| π‘ |
Shear Stress Components in a 2D Stress Field |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
2D Stress Field: Finding Shear Stress Components |
10 |
885 |
384.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
2d-stress-field-finding-shear-stress-components.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
3D Harmonic Oscillator with General Potential (Figure It Out) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
3D Harmonic Oscillator with General Potential |
13 |
1195 |
517.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
3d-harmonic-oscillator-with-general-potential.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Absolute & Relative Errors β Concept (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Absolute Value Inequalities and Intervals (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Atomic Spectra β Absorption Lines (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Atomic Spectra |
10 |
523 |
104.0s |
20 |
100.0% |
0 |
0 |
| π‘ |
AC Generator β How Rotating Coils Make Electricity (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
AC in Capacitors (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
AC in Inductors (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
AC in Resistive Circuits (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
AC Signal Representation (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Accelerated Charges as Sources (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Accelerating Liquid in Vessel: Finding Restraining Force |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Accelerating Liquid in Vessel: Finding Restraining Force |
12 |
1211 |
507.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
accelerating-liquid-in-vessel-finding-restraining-force.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Acceleration Due to Gravity g (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Acceleration from Slope (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
VelocityβTime Graphs |
12 |
484 |
190.0s |
22 |
100.0% |
0 |
2 |
| π‘ |
Acceleration in SHM (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Acoustic Waves in Fluids (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Newton's Third Law & Interaction Pairs |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Newton's Third Law & Interaction Pairs |
10 |
500 |
109.5s |
20 |
100.0% |
0 |
0 |
| π’ |
The Adiabatic Approximation |
10 |
642 |
110.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
Adiabatic Invariants (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Adiabatic vs Isothermal: What's Actually Different? |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Adiabatic vs Isothermal Processes |
11 |
631 |
264.6s |
25 |
100.0% |
0 |
0 |
| π‘ |
Why Adiabats Are Steeper Than Isotherms |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Adiabats vs Isotherms: Gradient Comparison |
12 |
1152 |
464.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
adiabats-vs-isotherms-gradient-comparison.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Advanced Counting β Inclusion-Exclusion Principle (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Aeolian Vibration: Why Power Lines Hum |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Aeolian Vibration: Why Power Lines Hum |
11 |
1084 |
436.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
aeolian-vibration-why-power-lines-hum.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
The Aharonov-Bohm Effect |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Aharonov-Bohm Effect |
12 |
772 |
334.7s |
23 |
100.0% |
0 |
0 |
| π‘ |
Why Air Molecules Push on a Wall |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Air Molecules Hitting a Wall |
11 |
1014 |
392.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
air-molecules-hitting-a-wall.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Air pressure and barometer accuracy in deep mines |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Air pressure and barometer accuracy in deep mines |
11 |
1050 |
445.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
air-pressure-and-barometer-accuracy-in-deep-mines.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Air Pressure Inside a Soap Bubble (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Air Pressure Inside a Soap Bubble |
11 |
923 |
360.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
air-pressure-inside-a-soap-bubble.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Airy Asymptotics & WKB Quantization |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Airy Function Asymptotics & WKB Quantization |
13 |
1327 |
536.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
airy-function-asymptotics-wkb-quantization.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Polynomials β Algebraic Identities (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Polynomials |
11 |
549 |
118.0s |
28 |
100.0% |
0 |
0 |
| π‘ |
Alpha, Beta, and Gamma Decay (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Alpha Decay & Quantum Tunneling: Escaping the Nucleus |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Alpha Decay & Quantum Tunneling |
11 |
603 |
242.3s |
21 |
100.0% |
0 |
0 |
| π‘ |
Alpha Decay (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Alpha Decay |
10 |
476 |
100.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
Alpha-Particle Scattering β Rutherford's Nuclear Model (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Alternating Current and RMS Values (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Ampère's Circuital Law: Reading the Magnetic Field from Enclosed Current |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Ampère's Circuital Law |
11 |
542 |
205.7s |
20 |
100.0% |
0 |
0 |
| π‘ |
Sound Wave Characteristics β Amplitude & Loudness (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Sound Wave Characteristics |
11 |
618 |
120.0s |
22 |
100.0% |
0 |
0 |
| π‘ |
Vector Addition & Component Resolution |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Vector Addition & Component Resolution |
11 |
518 |
109.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
Angular Frequency in HeβΊ's Second Bohr Orbit |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Angular Frequency in the Second Bohr Orbit of HeβΊ |
11 |
1122 |
457.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
angular-frequency-in-the-second-bohr-orbit-of-he.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Wave Description β Angular Frequency & Wavenumber (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Wave Description |
11 |
588 |
120.0s |
26 |
100.0% |
0 |
0 |
| π‘ |
Angular Momentum Conservation |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Angular Momentum Conservation |
14 |
524 |
229.3s |
22 |
100.0% |
0 |
0 |
| π’ |
Angular Momentum Operators in QM |
14 |
561 |
256.3s |
21 |
100.0% |
0 |
0 |
| π‘ |
Angular Momentum (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Angular Momentum |
10 |
464 |
102.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Why Does a Plumb Line Tilt on a Spinning Disk? |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Angular velocity from tilted plumb line on rotating disk |
11 |
994 |
406.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
angular-velocity-from-tilted-plumb-line-on-rotating-disk.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Angular Width on a Sphere: Intrinsic Geometry |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Angular Width on a Sphere: Intrinsic Geometry |
11 |
1116 |
458.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
angular-width-on-a-sphere-intrinsic-geometry.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Archimedes' Principle (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Archimedes' Principle |
12 |
622 |
126.5s |
25 |
100.0% |
3 |
1 |
| π‘ |
The Electromagnetic Spectrum β Applications & Hazards (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Electromagnetic Spectrum |
11 |
508 |
119.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Applications of Momentum Conservation (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Conservation Laws |
11 |
484 |
112.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
Ultrasound β Applications (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Ultrasound |
10 |
523 |
104.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
Rates of Change (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Rates of Change |
11 |
567 |
117.5s |
22 |
100.0% |
0 |
0 |
| π‘ |
Archimedes' Principle and Buoyancy (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Archimedes' Principle and Buoyancy |
11 |
544 |
113.5s |
23 |
100.0% |
0 |
0 |
| π‘ |
Archimedes' Principle: Why Objects Float |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Archimedes' Principle: Why Objects Float |
12 |
1160 |
457.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
archimedes-principle-why-objects-float.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Finding an Asteroid's Orbital Radius from Its Angular Velocity |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Asteroid Orbital Radius from Angular Velocity |
11 |
875 |
352.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
asteroid-orbital-radius-from-angular-velocity.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Atomic Nucleus Structure β Protons and Neutrons (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Atomic Nucleus Structure |
11 |
542 |
107.5s |
21 |
100.0% |
0 |
0 |
| π΄ |
Atomic Recoil from Photon Emission |
12 |
1152 |
475.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
atomic-recoil-from-photon-emission.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Atomic Spacing Under Tension |
11 |
1026 |
404.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
atomic-spacing-under-tension.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Atwood Machine: Finding Acceleration and Tension |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Atwood Machine: Acceleration & Tension |
12 |
1112 |
451.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
Average Acceleration β Concept (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
1D Acceleration: Definition & Interpretation |
10 |
487 |
197.5s |
20 |
100.0% |
0 |
1 |
| π‘ |
Power β Concept (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Power |
10 |
471 |
102.0s |
20 |
100.0% |
0 |
0 |
| π‘ |
Foundations of Force & Motion |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Foundations of Force & Motion |
10 |
497 |
101.0s |
20 |
100.0% |
0 |
0 |
| π‘ |
Balloon in Wind: Finding Terminal Velocity |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Balloon in Wind: Terminal Velocity Analysis |
12 |
1106 |
450.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
balloon-in-wind-terminal-velocity-analysis.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Why Some Materials Conduct and Others Don't |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Band Theory: Insulators, Semiconductors & Metals |
13 |
552 |
232.3s |
21 |
100.0% |
0 |
0 |
| π’ |
Banked Curves & Friction |
14 |
608 |
246.7s |
21 |
100.0% |
0 |
0 |
| π‘ |
Lines and Angles (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Lines and Angles |
12 |
514 |
121.0s |
23 |
100.0% |
0 |
0 |
| π‘ |
Battery EMF and Internal Resistance |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Battery EMF and Internal Resistance |
12 |
897 |
377.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
battery-emf-and-internal-resistance.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
BCS Theory of Superconductivity |
10 |
533 |
109.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
Wave Superposition β Beats (Figure It Out) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Wave Superposition |
11 |
550 |
121.5s |
21 |
100.0% |
0 |
0 |
| π’ |
Bernoulli's Equation |
12 |
526 |
209.0s |
22 |
100.0% |
0 |
0 |
| π’ |
Bernoulli's Principle |
11 |
470 |
108.0s |
20 |
100.0% |
0 |
0 |
| π’ |
Berry Phase in Adiabatic Evolution |
11 |
621 |
118.0s |
22 |
100.0% |
0 |
0 |
| π‘ |
Berry Phase (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Berry Phase |
11 |
595 |
229.8s |
21 |
100.0% |
0 |
0 |
| π‘ |
Bessel Functions: Waves Trapped in a Circle |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Bessel Functions: Waves in Circles |
11 |
1062 |
437.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
bessel-functions-waves-in-circles.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Beta decay and half-life: counting particles |
10 |
842 |
359.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
beta-decay-and-half-life-counting-particles.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
beta-decay-and-weak-interaction.json |
PARSE ERROR: parse: Expecting ',' delimiter: line 271 column 55 (char 13485) |
| π‘ |
The Big Bang Theory (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Big Bang Theory |
11 |
525 |
115.0s |
21 |
100.0% |
0 |
0 |
| π΄ |
Binary collapse time from orbital period |
11 |
946 |
385.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
binary-collapse-time-from-orbital-period.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Binary Star Orbital Period |
11 |
956 |
379.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
binary-star-orbital-period.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Magnetic Field from a Finite Straight Wire |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Biot-Savart Law β Finite Wire |
11 |
688 |
277.6s |
21 |
100.0% |
1 |
0 |
| π‘ |
Biot-Savart Law (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Biot-Savart Law |
12 |
664 |
128.0s |
22 |
100.0% |
0 |
0 |
| π’ |
Black-body Radiation |
15 |
625 |
256.6s |
23 |
100.0% |
0 |
0 |
| π‘ |
Blackbody Radiation: Why Classical Physics Broke β and Planck Fixed It |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Blackbody Radiation: From Heat to Quanta |
12 |
1086 |
455.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
blackbody-radiation-from-heat-to-quanta.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Bloch's Theorem |
11 |
676 |
131.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
Driven Oscillator: Finding Resonance Amplitude |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Block Leaving SHM Platform: Normal Force Analysis |
12 |
1187 |
521.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
block-leaving-shm-platform-normal-force-analysis.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Block on Incline: Finding Acceleration |
10 |
947 |
394.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
Blocking Half a Lens: What Happens to the Image? |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Blocking Half a Lens: What Happens to the Image? |
11 |
1148 |
422.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
blocking-half-a-lens-what-happens-to-the-image.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Bohr Model of the Hydrogen Atom |
14 |
670 |
303.2s |
23 |
100.0% |
0 |
0 |
| π‘ |
Boltzmann's H-Theorem: How Irreversibility Emerges from Reversible Mechanics |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Boltzmann's H-Theorem & Entropy |
14 |
621 |
264.3s |
22 |
100.0% |
0 |
0 |
| π‘ |
Bosons vs Fermions: Who Can Share a Seat? |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Bose-Einstein vs Fermi-Dirac Statistics |
14 |
635 |
271.9s |
23 |
100.0% |
0 |
0 |
| π΄ |
boundary-effects.json |
PARSE ERROR: parse: Expecting ',' delimiter: line 366 column 43 (char 19852) |
| π’ |
Bragg Diffraction |
12 |
619 |
261.8s |
23 |
100.0% |
0 |
0 |
| π‘ |
Brillouin Zones (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Brillouin Zones |
12 |
721 |
289.8s |
23 |
100.0% |
0 |
0 |
| π’ |
Buoyancy & Archimedes' Principle |
13 |
521 |
209.6s |
19 |
100.0% |
0 |
0 |
| π΄ |
Buoyancy & Water Level: The Steel Weight Paradox |
11 |
1086 |
422.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
buoyancy-water-level-the-steel-weight-paradox.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Burgers' Equation & Weak Discontinuity Structure |
12 |
1193 |
523.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
burgers-equation-weak-discontinuity-structure.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Canonical Transformations (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Canonical Transformations |
15 |
673 |
274.3s |
23 |
100.0% |
0 |
0 |
| π’ |
Capacitance: Parallel-Plate Capacitor |
15 |
667 |
275.8s |
23 |
100.0% |
0 |
0 |
| π’ |
Capacitor Charging & Discharging |
15 |
703 |
291.9s |
25 |
100.0% |
0 |
0 |
| π‘ |
Time-Dependent Circuits β Capacitor Charging in RC Circuits (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Time-Dependent Circuits |
12 |
580 |
125.0s |
24 |
100.0% |
0 |
0 |
| π‘ |
Time-Dependent Circuits β Capacitor Discharging in RC Circuits (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Time-Dependent Circuits |
13 |
658 |
133.0s |
26 |
100.0% |
0 |
0 |
| π‘ |
Capacitors and Capacitance (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Capacitors and Capacitance |
11 |
581 |
114.5s |
22 |
100.0% |
0 |
0 |
| π‘ |
Capacitance β Series & Parallel (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Capacitance |
11 |
529 |
113.0s |
21 |
100.0% |
0 |
0 |
| π΄ |
Capillary Pressure in Droplets and Bubbles |
11 |
1025 |
400.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
capillary-pressure-in-droplets-and-bubbles.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Heat Engines β Carnot Efficiency (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Heat Engines |
11 |
552 |
114.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Center of Mass: Why Objects Balance Where They Do |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Center of Mass & Balance |
13 |
539 |
191.6s |
19 |
100.0% |
0 |
0 |
| π‘ |
Bead on a Rotating Hoop: Finding the Equilibrium Angle |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Center of Mass of Isosceles Right Triangle |
12 |
1129 |
454.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
center-of-mass-of-isosceles-right-triangle.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Center of Mass (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Center of Mass |
10 |
476 |
97.0s |
18 |
100.0% |
0 |
0 |
| π‘ |
Kepler Orbits & Central Force Motion |
14 |
726 |
310.4s |
23 |
75.0% |
0 |
0 |
| π΄ |
Central Force Motion & Kepler Orbits |
14 |
663 |
283.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
Systems of Particles & Centre of Mass (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Systems of Particles & Centre of Mass |
11 |
629 |
119.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
Irodov 1.115: Velocity of a Particle in Non-Inertial Frame |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Centrifugal and Coriolis Forces at Break-off on Rotating Sphere |
11 |
1036 |
445.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
centrifugal-and-coriolis-forces-at-break-off-on-rotating-sph.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Uniform Circular Motion β Centripetal Acceleration (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Uniform Circular Motion |
12 |
550 |
123.5s |
23 |
100.0% |
0 |
0 |
| π’ |
Centripetal Force & Circular Motion |
14 |
613 |
243.0s |
24 |
100.0% |
0 |
0 |
| π‘ |
Circular & Orbital Motion Dynamics |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Circular & Orbital Motion Dynamics |
10 |
507 |
107.0s |
19 |
100.0% |
0 |
0 |
| π΄ |
Chain on Table: Finding Coefficient of Static Friction |
11 |
984 |
384.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
chain-on-table-finding-coefficient-of-static-friction.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Chain Rule |
10 |
539 |
100.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
Orbital Speed of a Satellite from First Principles |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Chaos in the Driven Damped Pendulum |
11 |
1036 |
448.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
chaos-in-the-driven-damped-pendulum.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Finding the Wavelength and Frequency of a Radio Wave |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Charge Motion in EM Waves |
12 |
1196 |
500.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
charge-motion-in-em-waves.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Charge on parallel conductors from field |
10 |
846 |
353.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
charge-on-parallel-conductors-from-field.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Charge Velocity and Current in a Wire |
11 |
1075 |
426.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
charge-velocity-and-current-in-a-wire.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Chemical Potential & Equilibrium |
15 |
614 |
258.1s |
22 |
100.0% |
0 |
0 |
| π‘ |
The Chern Number: Counting Twists in Quantum Geometry |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Chern Number & Band Topology |
11 |
603 |
119.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
Circles β Chords and Angles (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Circles |
11 |
515 |
107.5s |
20 |
100.0% |
0 |
0 |
| π’ |
Chromatic Aberration in Lenses |
12 |
546 |
219.1s |
23 |
100.0% |
0 |
0 |
| π‘ |
Angular Momentum of a Skewed Rotating Rod |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Circling Stick: CM Frame Analysis |
11 |
1002 |
398.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
circling-stick-cm-frame-analysis.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Circular Motion & Centripetal Force (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Circular Motion & Centripetal Force |
11 |
532 |
108.0s |
22 |
100.0% |
0 |
0 |
| π‘ |
Satellites & Orbital Motion |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Satellites & Orbital Motion |
11 |
690 |
127.5s |
22 |
100.0% |
0 |
0 |
| π‘ |
Classical vs Relativistic KE: Reading the Graph |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Classical vs Relativistic Kinetic Energy |
11 |
1071 |
439.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
classical-vs-relativistic-kinetic-energy.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
The Real Number System (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Real Number System |
10 |
455 |
97.5s |
19 |
100.0% |
0 |
0 |
| π‘ |
The Clausius-Clapeyron Equation: Why Pressure Changes Boiling Points |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Clausius-Clapeyron Equation |
14 |
652 |
281.8s |
22 |
100.0% |
0 |
0 |
| π‘ |
Adding Two Spin-1/2 Particles: Triplet and Singlet States |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
ClebschβGordan coefficients for angular momentum coupling |
12 |
1079 |
485.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
clebsch-gordan-coefficients-for-angular-momentum-coupling.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Coefficient of Restitution and Energy Loss in Ball Bounce |
11 |
970 |
384.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
coefficient-of-restitution-and-energy-loss-in-ball-bounce.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Coherence and Interference (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Coherence and Interference |
12 |
562 |
123.5s |
24 |
100.0% |
0 |
0 |
| π΄ |
Collision Rate in Adiabatic Expansion |
12 |
1227 |
505.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
collision-rate-in-adiabatic-expansion.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Collision with 90Β° deflection: energy loss calculation |
11 |
918 |
402.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
collision-with-90-deflection-energy-loss-calculation.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Color & Dispersion Through a Prism |
15 |
567 |
237.4s |
22 |
100.0% |
0 |
0 |
| π‘ |
Color-Ordered Rules & N=1 Component Fields |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Color-Ordered Feynman Rules and N=1 Component Fields |
11 |
1066 |
481.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
color-ordered-feynman-rules-and-n-1-component-fields.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Commutator of Dot Products with Angular Momentum |
10 |
836 |
379.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
commutator-of-dot-products-with-angular-momentum.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Complex Numbers in Polar Form |
12 |
635 |
121.0s |
23 |
100.0% |
0 |
0 |
| π‘ |
Steady Flow Force on a Pipe Bend |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Compressible Flow in an Insulated Tube |
11 |
960 |
403.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
compressible-flow-in-an-insulated-tube.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Compression of a Granite Column Under Its Own Weight |
9 |
807 |
340.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
compression-of-a-granite-column-under-its-own-weight.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Compton Scattering |
13 |
628 |
271.3s |
25 |
100.0% |
0 |
0 |
| π‘ |
Compton Scattering (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Compton Scattering |
15 |
645 |
278.5s |
25 |
100.0% |
0 |
0 |
| π’ |
Concave & Convex Mirrors |
15 |
760 |
291.0s |
27 |
100.0% |
0 |
0 |
| π‘ |
Centre of Gravity (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Centre of Gravity |
11 |
563 |
112.0s |
22 |
100.0% |
0 |
0 |
| π‘ |
Triangle Congruence (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Triangle Congruence |
11 |
523 |
112.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Escape Velocity (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Escape Velocity |
11 |
602 |
117.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Torque β What Makes Things Spin (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Torque |
10 |
478 |
101.0s |
21 |
100.0% |
2 |
10 |
| π‘ |
Heat Transfer β Conduction (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Heat Transfer |
10 |
554 |
107.0s |
20 |
100.0% |
0 |
0 |
| π‘ |
Triangle Congruence (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Triangle Congruence |
12 |
519 |
117.5s |
22 |
100.0% |
0 |
0 |
| π‘ |
Bead on a Rotating Hoop β Finding Conservation Laws |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Conical pendulum with shortening string |
13 |
1197 |
479.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
conical-pendulum-with-shortening-string.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Particle Physics β Conservation Laws (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Particle Physics |
10 |
540 |
109.0s |
24 |
100.0% |
0 |
0 |
| π‘ |
Angular Momentum β Conservation (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Angular Momentum |
11 |
517 |
110.5s |
21 |
100.0% |
1 |
0 |
| π‘ |
Electric Charge β Conservation of Charge (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Electric Charge |
11 |
492 |
116.0s |
21 |
100.0% |
0 |
0 |
| π΄ |
Energy Conservation: Roller Coaster Loop |
13 |
496 |
177.6s |
0 |
0.0% |
0 |
0 |
| π’ |
Conservation of Energy: Roller Coaster Loop |
14 |
665 |
257.3s |
28 |
100.0% |
0 |
0 |
| π’ |
Conservation of Momentum in Collisions |
14 |
862 |
397.7s |
29 |
100.0% |
0 |
0 |
| π‘ |
Irodov 1.159 β Man and raft (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Irodov 1.159 β Man and raft (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Conservation of Momentum: Man and Raft on Water |
12 |
1040 |
435.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
conservation-of-momentum-man-and-raft-on-water.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Conservation of Momentum: Splitting Core |
9 |
756 |
304.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
conservation-of-momentum-splitting-core.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Conservation of Momentum (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Conservation of Momentum |
12 |
409 |
164.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
Conservative & Non-Conservative Forces |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Conservative & Non-Conservative Forces |
10 |
513 |
104.5s |
20 |
100.0% |
0 |
0 |
| π‘ |
Law of Conservation of Energy (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Law of Conservation of Energy |
10 |
462 |
105.0s |
20 |
100.0% |
0 |
0 |
| π‘ |
Constant Acceleration β Core Concept (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Uniform Motion & Constant Acceleration |
12 |
568 |
231.1s |
23 |
100.0% |
0 |
0 |
| π΄ |
Constructing the Hamiltonian from Lagrangian formulation |
11 |
939 |
426.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
constructing-the-hamiltonian-from-lagrangian-formulation.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Magnetic Field of a Uniformly Charged Rotating Sphere |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Convection Current from a Moving Charged Cylinder |
9 |
770 |
312.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
convection-current-from-a-moving-charged-cylinder.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Heat Transfer β Convection (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Heat Transfer |
11 |
606 |
122.0s |
20 |
100.0% |
0 |
0 |
| π΄ |
Cosmic Velocities and Orbital Periods |
12 |
1166 |
456.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
cosmic-velocities-and-orbital-periods.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Coulomb's Law |
14 |
749 |
307.4s |
24 |
100.0% |
0 |
0 |
| π‘ |
Coulomb's Law (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Coulomb's Law |
16 |
765 |
312.9s |
24 |
100.0% |
0 |
0 |
| π’ |
Coupled Oscillators & Normal Modes |
14 |
781 |
329.3s |
37 |
100.0% |
0 |
0 |
| π’ |
Coupled Oscillators & Normal Modes |
16 |
800 |
336.3s |
37 |
100.0% |
0 |
0 |
| π‘ |
Coupled Oscillators (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Coupled Oscillators |
11 |
631 |
124.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
Creation & Annihilation Operators: Building and Destroying Quantum States |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Creation & Annihilation Operators |
11 |
611 |
120.5s |
22 |
100.0% |
0 |
0 |
| π‘ |
Total Internal Reflection (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Total Internal Reflection |
10 |
472 |
98.5s |
19 |
100.0% |
0 |
0 |
| π’ |
Crystal Momentum |
11 |
711 |
122.0s |
22 |
100.0% |
0 |
0 |
| π‘ |
Crystal Structure and Lattices (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Crystal Structure and Lattices |
10 |
489 |
108.0s |
20 |
100.0% |
0 |
0 |
| π‘ |
Curl & Stokes' Theorem |
12 |
718 |
127.5s |
26 |
100.0% |
2 |
0 |
| π΄ |
Current density and charge in a moving wire |
11 |
1028 |
433.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
current-density-and-charge-in-a-moving-wire.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Current in a Capacitor as Dielectric is Withdrawn |
11 |
1147 |
465.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
current-in-a-capacitor-as-dielectric-is-withdrawn.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Current, Resistance & Ohm's Law |
10 |
472 |
100.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
Cyclic Quadrilaterals (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Circles |
11 |
513 |
112.0s |
20 |
100.0% |
0 |
0 |
| π΄ |
Cylindrical Capacitor Capacity |
12 |
1067 |
441.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
cylindrical-capacitor-capacity.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Damped Harmonic Oscillator |
14 |
674 |
294.4s |
21 |
100.0% |
0 |
0 |
| π‘ |
Advanced Oscillations β Damped Oscillations (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Advanced Oscillations |
10 |
516 |
109.5s |
19 |
100.0% |
0 |
0 |
| π’ |
Davisson-Germer Experiment |
10 |
543 |
237.3s |
20 |
100.0% |
0 |
0 |
| π‘ |
Matter Waves (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Matter Waves |
10 |
542 |
105.0s |
20 |
100.0% |
0 |
0 |
| π΄ |
de Broglie Wavelength: Matter Waves Explained |
12 |
1091 |
455.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
de Broglie Wavelength of Hβ at Room Temperature |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
de Broglie Wavelength of Hβ at Room Temperature |
12 |
1083 |
441.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
de-broglie-wavelength-of-h-at-room-temperature.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
de Broglie Wavelength (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
de Broglie Wavelength |
10 |
600 |
108.0s |
21 |
100.0% |
0 |
0 |
| π΄ |
de Broglie wavelengths at equal kinetic energy |
11 |
947 |
410.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
de-broglie-wavelengths-at-equal-kinetic-energy.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
The Real Number System (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Real Number System |
9 |
445 |
94.5s |
17 |
100.0% |
0 |
0 |
| π’ |
Definite Integral as Area Under a Curve |
10 |
474 |
102.0s |
18 |
100.0% |
0 |
0 |
| π‘ |
Kinetic Energy (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Kinetic Energy |
10 |
367 |
93.0s |
17 |
100.0% |
0 |
0 |
| π΄ |
Degeneracy of a 3D State in Lithium |
10 |
872 |
350.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
degeneracy-of-a-3d-state-in-lithium.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Degeneracy of Term Symbols with Maximum J |
10 |
840 |
347.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
degeneracy-of-term-symbols-with-maximum-j.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Delbruck Scattering: Light Scattering Light |
11 |
1032 |
463.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
delbruck-scattering-light-scattering-light.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Density fluctuations in a negatively curved, low-matter universe |
12 |
1105 |
476.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
density-fluctuations-in-a-negatively-curved-low-matter-unive.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Fluid Properties β Density & Structure (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Fluid Properties |
11 |
491 |
104.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
Derivation & Meaning of Equations (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Kinematic Equations for Uniform Acceleration |
12 |
599 |
247.5s |
23 |
100.0% |
0 |
0 |
| π’ |
Derivative from First Principles |
10 |
561 |
101.0s |
20 |
100.0% |
0 |
0 |
| π΄ |
Deriving Equation (5.61) via Laguerre Polynomials |
12 |
1224 |
510.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
deriving-equation-5-61-via-laguerre-polynomials.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Deriving the z-component of angular momentum |
11 |
930 |
401.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
deriving-the-z-component-of-angular-momentum.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Designing a Curve for Isochronous Oscillations |
12 |
1215 |
500.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
designing-a-curve-for-isochronous-oscillations.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Determinant of a Matrix |
12 |
509 |
123.0s |
24 |
100.0% |
0 |
0 |
| π’ |
Diffraction by a Circular Aperture |
14 |
651 |
276.2s |
22 |
100.0% |
0 |
0 |
| π’ |
Diffraction Gratings & Resolving Power |
16 |
688 |
307.0s |
25 |
100.0% |
0 |
0 |
| π‘ |
Diffusion and Brownian Motion (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Diffusion and Brownian Motion |
11 |
673 |
116.0s |
22 |
100.0% |
0 |
0 |
| π΄ |
Dimensional Analysis: Building the Compton Wavelength |
12 |
1057 |
425.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
dimensional-analysis-building-the-compton-wavelength.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Dimensional Equations (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Dimensional Analysis |
12 |
573 |
235.4s |
22 |
100.0% |
0 |
0 |
| π‘ |
Dimensions of Physical Quantities (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Dimensional Analysis |
12 |
573 |
235.4s |
22 |
100.0% |
0 |
0 |
| π‘ |
The Dirac Delta Function |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Dirac Delta Function |
10 |
610 |
233.4s |
21 |
100.0% |
0 |
0 |
| π‘ |
The Dirac Equation (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Dirac Equation |
12 |
625 |
271.4s |
23 |
100.0% |
0 |
0 |
| π΄ |
Dirac Matrices: Traceless, Even Dimension, Β±1 Eigenvalues |
11 |
1044 |
431.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
dirac-matrices-traceless-even-dimension-1-eigenvalues.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Electric Charge & Current β Direction of Conventional Current (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Electric Charge & Current |
10 |
429 |
98.0s |
17 |
100.0% |
0 |
0 |
| π‘ |
Dispersion and Prisms (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Dispersion and Prisms |
10 |
538 |
103.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
Dispersion of Light (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Dispersion of Light |
11 |
530 |
112.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Displacement Current (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Displacement Current |
10 |
565 |
235.5s |
20 |
100.0% |
0 |
0 |
| π‘ |
VelocityβTime Graphs β Displacement from Area (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
VelocityβTime Graphs |
10 |
407 |
98.0s |
20 |
100.0% |
0 |
0 |
| π‘ |
Displacement Vector (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Position, Displacement & Vector Equality |
11 |
542 |
210.7s |
20 |
100.0% |
0 |
0 |
| π‘ |
Distance, Displacement, Speed & Velocity |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Distance, Displacement, Speed & Velocity |
10 |
526 |
206.5s |
19 |
100.0% |
0 |
0 |
| π‘ |
Mass, Weight & Apparent Weight (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Mass, Weight & Apparent Weight |
10 |
486 |
103.0s |
20 |
100.0% |
0 |
0 |
| π’ |
Divergence & the Divergence Theorem |
12 |
629 |
122.0s |
22 |
100.0% |
0 |
0 |
| π΄ |
Does Kinetic Energy Have a Speed Limit? |
11 |
1056 |
445.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
does-kinetic-energy-have-a-speed-limit.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Echo Frequency from a Moving Source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Doppler Effect & Echo: Double Shift |
12 |
1105 |
452.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
doppler-effect-echo-double-shift.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Doppler Effect for Light: Redshift |
14 |
595 |
240.9s |
21 |
100.0% |
0 |
0 |
| π΄ |
Doppler Effect: Moving Light Sources |
12 |
1195 |
505.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
doppler-effect-moving-light-sources.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Doppler Effect: Frequency Shift of an Approaching Train |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Doppler Effect: Train Horn Approach |
11 |
988 |
404.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
doppler-effect-train-horn-approach.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Doppler Shift and Relativistic Energy: Pulsar Observations |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Doppler Shift and Relativistic Energy: Pulsar Observations |
12 |
1186 |
477.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
doppler-shift-and-relativistic-energy-pulsar-observations.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
The Doppler Effect (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Doppler Effect |
10 |
489 |
101.5s |
19 |
100.0% |
0 |
0 |
| π‘ |
Drag Force & Terminal Velocity (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Drag Force & Terminal Velocity |
11 |
516 |
111.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Free-Body Diagrams & Force Modeling |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Free-Body Diagrams & Force Modeling |
10 |
464 |
96.5s |
20 |
100.0% |
0 |
0 |
| π΄ |
Drift Velocity in Crossed Electric and Magnetic Fields |
12 |
1105 |
458.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
drift-velocity-in-crossed-electric-and-magnetic-fields.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Driven Oscillations & Resonance |
14 |
566 |
241.4s |
21 |
100.0% |
0 |
0 |
| π‘ |
Roller Coaster Loop: Finding Speed at the Top |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Driven Oscillator Near Resonance |
12 |
1064 |
465.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
driven-oscillator-near-resonance.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Driven Oscillators & Resonance |
13 |
546 |
224.7s |
21 |
100.0% |
0 |
0 |
| π‘ |
Drude Model of Electrical Conduction |
14 |
587 |
243.2s |
21 |
100.0% |
1 |
0 |
| π‘ |
WaveβParticle Duality (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
WaveβParticle Duality |
11 |
579 |
113.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
The Solar System β Earth's Rotation & Orbit (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Solar System |
11 |
612 |
112.0s |
22 |
100.0% |
0 |
0 |
| π‘ |
Sound Reflection Phenomena (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Sound Reflection Phenomena |
10 |
494 |
104.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
Energy Losses & Efficiency (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Energy Losses & Efficiency |
12 |
560 |
119.0s |
22 |
100.0% |
0 |
0 |
| π‘ |
Ehrenfest Theorem: Why Quantum Averages Obey Newton |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Ehrenfest Theorem: Classical Mechanics Meets Quantum |
11 |
1106 |
453.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
ehrenfest-theorem-classical-mechanics-meets-quantum.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Eigenvalues & Eigenvectors |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Eigenvalues & Eigenvectors |
11 |
532 |
221.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Elastic and Inelastic Collisions (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Elastic and Inelastic Collisions |
12 |
1049 |
460.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
elastic-and-inelastic-collisions.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Elastic Collision: Identifying the Mystery Nucleus |
12 |
1113 |
488.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
elastic-collision-identifying-the-mystery-nucleus.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Elastic Deformations (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Elastic Deformations |
11 |
542 |
110.5s |
20 |
100.0% |
0 |
0 |
| π’ |
Elastic & Inelastic Collisions in 1D |
15 |
692 |
295.4s |
28 |
100.0% |
0 |
0 |
| π΄ |
Elastic Rod Collisions & Compression Waves |
12 |
1162 |
485.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
elastic-rod-collisions-compression-waves.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Elastic vs Inelastic Collisions: Angle of Divergence |
11 |
1029 |
455.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
elastic-vs-inelastic-collisions-angle-of-divergence.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Electric and Magnetic Field Energy Density |
11 |
1034 |
405.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
electric-and-magnetic-field-energy-density.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Electric Charge & Current |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Electric Charge & Current |
9 |
518 |
96.0s |
16 |
100.0% |
0 |
0 |
| π‘ |
Electric Circuits: Series & Parallel (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Electric Circuits: Series & Parallel |
11 |
615 |
111.0s |
21 |
100.0% |
0 |
0 |
| π’ |
Electric Dipole in an External Field |
11 |
639 |
245.9s |
21 |
100.0% |
0 |
0 |
| π΄ |
Electric Field at Center of Charged Semicircular Rod |
12 |
1151 |
464.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
electric-field-at-center-of-charged-semicircular-rod.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Electric Field of a Point Charge |
14 |
894 |
388.1s |
24 |
100.0% |
0 |
0 |
| π΄ |
Electric Field on the Axis of a Charged Disk |
12 |
1163 |
466.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
electric-field-on-the-axis-of-a-charged-disk.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Electric Flux & Gauss's Law |
12 |
648 |
263.8s |
24 |
100.0% |
0 |
0 |
| π΄ |
Electric & Magnetic Fields in Waves: The E-B Relationship |
12 |
1191 |
475.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
electric-magnetic-fields-in-waves-the-e-b-relationship.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Electric Potential (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Electric Potential |
11 |
573 |
113.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
Electric Power & Energy Consumption (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Electric Power & Energy Consumption |
12 |
594 |
120.0s |
23 |
100.0% |
0 |
0 |
| π‘ |
Electric Power (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Electric Power |
10 |
531 |
105.5s |
24 |
100.0% |
0 |
0 |
| π’ |
Electric Power in Resistors |
14 |
633 |
252.6s |
23 |
100.0% |
0 |
0 |
| π‘ |
Electrical Conductivity & the Drude Model |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Electrical Conductivity & the Drude Model |
10 |
484 |
107.5s |
19 |
100.0% |
0 |
0 |
| π‘ |
Conductors, Insulators & Semiconductors (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Conductors, Insulators & Semiconductors |
11 |
508 |
113.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Electrical Energy (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Electrical Energy |
10 |
476 |
99.5s |
19 |
100.0% |
0 |
0 |
| π΄ |
Electrodynamics Triangle: Sources, Fields & Potentials |
12 |
1132 |
486.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
electrodynamics-triangle-sources-fields-potentials.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Electromagnetic Induction: Faraday's & Lenz's Laws |
12 |
1223 |
506.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
electromagnetic-induction-faraday-s-lenz-s-laws.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Electromagnetic Waves (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Electromagnetic Waves |
12 |
536 |
118.5s |
23 |
100.0% |
0 |
0 |
| π’ |
Electromagnets & Solenoids |
15 |
576 |
231.0s |
23 |
100.0% |
0 |
0 |
| π‘ |
Cells & EMF (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Cells & EMF |
11 |
499 |
109.0s |
20 |
100.0% |
0 |
0 |
| π΄ |
Electron Beam Self-Repulsion and Expansion |
13 |
1231 |
528.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
electron-beam-self-repulsion-and-expansion.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Magnetic Field of a Solenoid with a Moving Charge Inside |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Electron Helical Motion in Magnetic Field |
12 |
983 |
405.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
electron-helical-motion-in-magnetic-field.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Electron Speed in a Circular Orbit |
12 |
1198 |
504.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
electron-speed-in-a-circular-orbit.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Electron Spread in Wire-Grid Capacitor |
11 |
1097 |
456.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
electron-spread-in-wire-grid-capacitor.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Magnetic Field of a Solenoid with Varying Current |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Electron Trajectory in Wire's Magnetic Field |
12 |
1106 |
465.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
electron-trajectory-in-wire-s-magnetic-field.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Electrostatic repulsion and distance scaling |
10 |
871 |
354.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
electrostatic-repulsion-and-distance-scaling.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Escape Velocity (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Escape Velocity |
12 |
588 |
115.0s |
23 |
100.0% |
0 |
0 |
| π΄ |
Energy conditions and the equation-of-state parameter w |
10 |
878 |
372.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
energy-conditions-and-the-equation-of-state-parameter-w.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Energy Conservation: Roller Coaster Loop |
15 |
510 |
184.6s |
24 |
100.0% |
0 |
0 |
| π‘ |
Collisions & Momentum β Energy Considerations (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Collisions & Momentum |
12 |
574 |
125.0s |
23 |
100.0% |
0 |
0 |
| π’ |
Energy in Electric & Magnetic Fields |
12 |
558 |
228.9s |
22 |
100.0% |
0 |
0 |
| π‘ |
Energy in Simple Harmonic Motion (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Energy in Simple Harmonic Motion |
12 |
673 |
126.0s |
23 |
100.0% |
0 |
0 |
| π‘ |
The Electromagnetic Spectrum (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Electromagnetic Spectrum |
10 |
472 |
98.0s |
20 |
100.0% |
0 |
0 |
| π‘ |
Energy in Electromagnetic Fields (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Energy in Electromagnetic Fields |
12 |
660 |
129.0s |
23 |
100.0% |
0 |
0 |
| π‘ |
Applications & Systems: Newton's Laws in Action β Energy in Vertical Circular Motion (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Applications & Systems: Newton's Laws in Action |
11 |
545 |
111.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Gravitational Potential Energy (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Gravitational Potential Energy |
10 |
441 |
97.0s |
17 |
100.0% |
0 |
0 |
| π΄ |
Energy Stored in a Charged Disk |
11 |
1009 |
384.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
energy-stored-in-a-charged-disk.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Energy Stored in Capacitors (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Capacitance |
11 |
530 |
114.5s |
22 |
100.0% |
0 |
0 |
| π‘ |
Mechanical Energy (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Mechanical Energy |
11 |
503 |
111.0s |
22 |
100.0% |
0 |
1 |
| π΄ |
Engine Detonation and Efficiency Loss |
11 |
1125 |
484.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
engine-detonation-and-efficiency-loss.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Entropy increase during water vaporization |
8 |
679 |
293.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
entropy-increase-during-water-vaporization.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Entropy: The Arrow of Time |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Entropy: The Arrow of Time |
11 |
514 |
112.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Second Law & Entropy (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Second Law & Entropy |
11 |
630 |
117.5s |
23 |
100.0% |
0 |
0 |
| π‘ |
Entropy & Microstates: Reading Boltzmann's Formula |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Entropy & Microstates: Boltzmann's S = k log W |
15 |
652 |
273.5s |
24 |
100.0% |
0 |
0 |
| π‘ |
Entropy of a 2D Ideal Gas |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Entropy of a 2D Ideal Gas |
12 |
1261 |
519.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
entropy-of-a-2d-ideal-gas.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Entropy of Mixing |
12 |
538 |
230.3s |
24 |
100.0% |
0 |
0 |
| π’ |
Equipartition & Heat Capacity |
13 |
656 |
269.3s |
23 |
100.0% |
0 |
0 |
| π’ |
Equipartition Theorem & Heat Capacity |
13 |
596 |
278.0s |
19 |
100.0% |
0 |
0 |
| π’ |
Equipartition Theorem & Heat Capacity |
13 |
685 |
278.0s |
24 |
100.0% |
0 |
0 |
| π‘ |
Electric Potential β Equipotential Surfaces (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Electric Potential |
11 |
630 |
120.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
Measurement Errors β Addition & Subtraction (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Measurement Errors |
12 |
583 |
241.1s |
22 |
100.0% |
0 |
0 |
| π‘ |
Measurement Errors β Multiplication & Division (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Measurement Errors |
12 |
583 |
241.1s |
22 |
100.0% |
0 |
0 |
| π‘ |
Escape Velocity |
11 |
540 |
212.1s |
22 |
100.0% |
1 |
0 |
| π΄ |
Estimating Brβ Bond Enthalpy from Fig. 22.8 |
12 |
1117 |
470.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
estimating-br-bond-enthalpy-from-fig-22-8.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Estimating Dipole-Dipole Energy from Critical Temperature |
11 |
1045 |
448.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
estimating-dipole-dipole-energy-from-critical-temperature.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Estimating Molecular Diameter from Mean Free Path |
11 |
940 |
394.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
estimating-molecular-diameter-from-mean-free-path.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
The Art of Estimation |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Art of Estimation |
12 |
596 |
130.5s |
23 |
100.0% |
0 |
0 |
| π΄ |
Ethyl alcohol flow rate between wide tanks |
11 |
998 |
392.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
ethyl-alcohol-flow-rate-between-wide-tanks.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Foundations of Geometry |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Foundations of Geometry |
11 |
520 |
110.5s |
21 |
100.0% |
0 |
0 |
| π’ |
Euler's Formula |
11 |
604 |
122.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Exchange Splitting: Why Triplet and Singlet Energies Differ |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Exchange Splitting: Two-Electron Perturbation Theory |
12 |
1119 |
478.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
exchange-splitting-two-electron-perturbation-theory.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Exponential Functions & Laws of Exponents (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Exponential Functions & Laws of Exponents |
11 |
645 |
118.5s |
21 |
100.0% |
0 |
0 |
| π΄ |
Exponential Spirals & Central Force Motion |
12 |
1032 |
459.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
exponential-spirals-central-force-motion.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Newton's Second Law & Dynamics (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Newton's Second Law & Dynamics |
11 |
515 |
102.5s |
20 |
100.0% |
0 |
0 |
| π‘ |
Torque β Factors That Affect It (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Torque |
10 |
512 |
98.5s |
23 |
100.0% |
2 |
0 |
| π‘ |
The Photoelectric Effect β Why Classical Waves Fail (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Photoelectric Effect |
11 |
533 |
116.5s |
19 |
100.0% |
0 |
0 |
| π’ |
Faraday's Law of Induction |
11 |
604 |
115.5s |
22 |
100.0% |
0 |
0 |
| π‘ |
The Fermi-Dirac Distribution |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Fermi-Dirac Distribution |
11 |
623 |
260.7s |
24 |
100.0% |
0 |
0 |
| π‘ |
fermi-dirac-distribution.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Fermi's Golden Rule: Where Transition Rates Come From |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Fermi's Golden Rule |
11 |
649 |
124.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
The Fermi Surface (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Fermi Surface |
11 |
569 |
234.8s |
21 |
100.0% |
0 |
0 |
| π‘ |
Feynman's Path Integral: Every Path at Once |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Feynman's Path Integrals |
14 |
577 |
236.4s |
21 |
100.0% |
0 |
0 |
| π΄ |
Finding a Nitrogen-Oxide Formula from Gas Pressure |
10 |
845 |
358.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
finding-a-nitrogen-oxide-formula-from-gas-pressure.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Finding Atomic Diameter from Viscosity |
12 |
1170 |
487.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
finding-atomic-diameter-from-viscosity.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Finding Eigenfunctions of LΒ² and Lβ via Rotation |
11 |
936 |
416.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
finding-eigenfunctions-of-l-and-l-via-rotation.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Finding Electrostatic Potential from Given Field |
10 |
815 |
321.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
finding-electrostatic-potential-from-given-field.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Finding Elements by Electron Configuration |
11 |
941 |
390.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
finding-elements-by-electron-configuration.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Finding Elements from X-ray Wavelengths |
9 |
772 |
335.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
finding-elements-from-x-ray-wavelengths.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Finding Identical Charges from Coulomb's Law |
10 |
803 |
333.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
finding-identical-charges-from-coulomb-s-law.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Finding Speed from Momentum and Energy |
11 |
1088 |
446.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
finding-speed-from-momentum-and-energy.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Finding Zero Electric Field Between Two Point Charges |
12 |
1205 |
479.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
finding-zero-electric-field-between-two-point-charges.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Laws of Thermodynamics β First Law (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Laws of Thermodynamics |
10 |
472 |
102.5s |
19 |
100.0% |
0 |
0 |
| π’ |
First-Order ODEs |
12 |
634 |
128.0s |
23 |
100.0% |
0 |
0 |
| π’ |
Fission vs Fusion: Which Powers What |
14 |
644 |
282.7s |
24 |
100.0% |
0 |
0 |
| π‘ |
Draining Tank: Reynolds Transport Theorem for Mass |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Flow Through Elbows & Momentum Balance |
11 |
1031 |
428.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
flow-through-elbows-momentum-balance.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Bernoulli's Equation |
11 |
484 |
112.0s |
21 |
100.0% |
2 |
0 |
| π΄ |
Focal Distance Product for Concave Mirrors |
11 |
1045 |
427.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
focal-distance-product-for-concave-mirrors.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Foundations of Force & Motion |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Foundations of Force & Motion |
10 |
575 |
108.5s |
20 |
100.0% |
0 |
0 |
| π΄ |
Force Between Parallel Current-Carrying Buses |
12 |
1147 |
475.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
force-between-parallel-current-carrying-buses.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Force on Wall from Wedge with Friction |
11 |
1046 |
414.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
force-on-wall-from-wedge-with-friction.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Advanced Oscillations β Forced Oscillations & Resonance |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Advanced Oscillations |
11 |
524 |
115.5s |
22 |
100.0% |
0 |
0 |
| π΄ |
Foucault Pendulum: Evidence of Earth's Rotation |
12 |
1129 |
451.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
foucault-pendulum-evidence-of-earth-s-rotation.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Foucault Pendulum: Plane of Oscillation Rotation |
12 |
1144 |
491.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
foucault-pendulum-plane-of-oscillation-rotation.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Foucault Pendulum: Proof of Earth's Rotation |
10 |
965 |
379.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
foucault-pendulum-proof-of-earth-s-rotation.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Fourier Series of a Square Wave |
11 |
710 |
125.0s |
21 |
100.0% |
0 |
0 |
| π’ |
Fourier Transform Basics |
10 |
540 |
103.5s |
19 |
100.0% |
0 |
0 |
| π‘ |
Fraunhofer Single-Slit Intensity Distribution |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Fraunhofer Single-Slit Diffraction: Intensity |
12 |
1247 |
481.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
fraunhofer-single-slit-diffraction-intensity.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Free electrons per sodium atom at T = 0 |
10 |
817 |
338.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
free-electrons-per-sodium-atom-at-t-0.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Free Energy: Helmholtz vs Gibbs |
14 |
606 |
263.7s |
19 |
100.0% |
0 |
0 |
| π‘ |
Free-Fall & Vertical Motion |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Free-Fall & Vertical Motion |
11 |
482 |
108.0s |
19 |
100.0% |
0 |
0 |
| π΄ |
Free Fall from Rest: Time and Final Speed |
11 |
1022 |
416.8s |
0 |
0.0% |
0 |
0 |
| π’ |
Free Fall & Galileo's Insight |
15 |
572 |
233.8s |
22 |
100.0% |
0 |
0 |
| π΄ |
Frequency of Small Oscillations: Compound Pendulum |
12 |
1250 |
484.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
frequency-of-small-oscillations-compound-pendulum.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Sound Wave Characteristics β Frequency & Pitch (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Sound Wave Characteristics |
11 |
498 |
105.5s |
20 |
100.0% |
0 |
0 |
| π’ |
Fresnel Equations for Reflection |
11 |
643 |
276.3s |
24 |
100.0% |
0 |
0 |
| π‘ |
Friction and Normal Forces (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Friction and Normal Forces |
12 |
672 |
128.5s |
23 |
91.7% |
0 |
0 |
| π΄ |
Friction on a Slope |
12 |
1177 |
387.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
friction-on-a-slope.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Friction on an Inclined Plane |
14 |
554 |
221.7s |
21 |
100.0% |
0 |
0 |
| π‘ |
Common Forces in Mechanics β Static & Kinetic Friction (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Common Forces in Mechanics |
12 |
591 |
124.0s |
24 |
100.0% |
0 |
0 |
| π΄ |
Friction Work on Moving Conveyor Belt |
12 |
1275 |
517.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
friction-work-on-moving-conveyor-belt.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Gamma-ray recoil energy loss in nuclear decay |
11 |
949 |
420.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
gamma-ray-recoil-energy-loss-in-nuclear-decay.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Gas Pressure Change from Molecular Absorption |
12 |
1162 |
480.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
gas-pressure-change-from-molecular-absorption.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Gauge Invariance of Maxwell's Equations |
10 |
821 |
336.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
gauge-invariance-of-maxwell-s-equations.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Gauss's Law: Charge and Electric Flux |
12 |
1101 |
441.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
gauss-s-law-charge-and-electric-flux.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Gauss's Law β Charged Sphere |
13 |
416 |
168.7s |
0 |
0.0% |
0 |
0 |
| π’ |
Gauss's Law for a Charged Sphere |
16 |
849 |
349.3s |
25 |
100.0% |
0 |
0 |
| π’ |
Gauss's Law for a Charged Sphere |
14 |
830 |
342.3s |
25 |
100.0% |
0 |
0 |
| π΄ |
Gauss's Law & Relativity: The Tilted Sheet |
12 |
1200 |
496.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
gauss-s-law-relativity-the-tilted-sheet.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Gauss's Law: Uniformly Charged Sphere |
14 |
727 |
293.4s |
28 |
100.0% |
0 |
0 |
| π‘ |
Geometric Optics (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Geometric Optics |
11 |
612 |
115.0s |
21 |
100.0% |
0 |
0 |
| π’ |
Geometric Series & Convergence |
11 |
525 |
110.0s |
21 |
100.0% |
0 |
0 |
| π΄ |
GPS Satellite Orbits: Gravity and Circular Motion |
11 |
1064 |
435.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
gps-satellite-orbits-gravity-and-circular-motion.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Gradient of a Scalar Field |
11 |
606 |
115.5s |
20 |
100.0% |
0 |
0 |
| π‘ |
Vector Addition & Component Resolution |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Vector Addition & Component Resolution |
11 |
575 |
111.5s |
22 |
100.0% |
0 |
0 |
| π‘ |
Linear Equations in Two Variables (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Linear Equations in Two Variables |
11 |
522 |
107.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Universal Law of Gravitation (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Universal Law of Gravitation |
11 |
534 |
116.5s |
20 |
100.0% |
0 |
0 |
| π΄ |
Gravitational Deflection of Spacecraft |
12 |
995 |
420.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
gravitational-deflection-of-spacecraft.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Gravitational Potential Energy (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Gravitational Potential Energy |
10 |
458 |
101.5s |
20 |
100.0% |
0 |
0 |
| π΄ |
Gravitational Potential Energy & the mgh Approximation |
12 |
1156 |
473.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
gravitational-potential-energy-the-mgh-approximation.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Gravitational Potential Energy (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Gravitational Potential Energy |
11 |
515 |
110.0s |
23 |
100.0% |
0 |
0 |
| π‘ |
Gravitational Time Dilation |
15 |
749 |
299.9s |
22 |
100.0% |
1 |
0 |
| π’ |
Gravity and Kepler's Laws |
11 |
550 |
116.5s |
21 |
100.0% |
0 |
0 |
| π΄ |
Gravity & Mass: Why Orbits Feel Weightless |
11 |
1073 |
440.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
gravity-mass-why-orbits-feel-weightless.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Gyroscopic Precession |
12 |
652 |
269.4s |
24 |
100.0% |
0 |
0 |
| π‘ |
Particle Physics β Hadrons, Baryons & Mesons |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Particle Physics |
10 |
390 |
97.0s |
20 |
100.0% |
0 |
0 |
| π‘ |
The Hall Effect |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
The Hall Effect |
11 |
639 |
123.0s |
22 |
100.0% |
1 |
0 |
| π’ |
Hamiltonian Mechanics: The Pendulum |
14 |
770 |
327.0s |
23 |
100.0% |
0 |
0 |
| π’ |
Hamiltonian Mechanics & the Pendulum |
14 |
686 |
299.1s |
21 |
100.0% |
0 |
0 |
| π΄ |
Harmonic Forces: Driven Oscillations in Real Systems |
10 |
984 |
411.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
harmonic-forces-driven-oscillations-in-real-systems.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Heat and Work (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Heat and Work |
10 |
499 |
103.0s |
18 |
90.0% |
0 |
0 |
| π΄ |
Heat Capacity of Hβ: From Classicism to Quantum |
11 |
1068 |
487.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
heat-capacity-of-h-from-classicism-to-quantum.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Heat Capacity of Solids: Einstein & Debye Models |
15 |
773 |
320.9s |
23 |
100.0% |
0 |
0 |
| π’ |
Heat Capacity & Specific Heat |
14 |
578 |
241.5s |
21 |
100.0% |
0 |
0 |
| π’ |
Heat Engine Efficiency |
11 |
488 |
201.9s |
21 |
100.0% |
0 |
0 |
| π‘ |
Heat Engines and Efficiency (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Heat Engines and Efficiency |
10 |
513 |
109.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
Heat Engines (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Heat for Surface Layer Formation in Carnot Cycle |
11 |
1015 |
431.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
heat-for-surface-layer-formation-in-carnot-cycle.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Heat Transfer β Conduction, Convection, Radiation (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Heat Transfer |
10 |
545 |
109.0s |
19 |
100.0% |
0 |
0 |
| π΄ |
Heat & Work in Isobaric Gas Expansion |
12 |
1127 |
465.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
heat-work-in-isobaric-gas-expansion.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Internal Energy, Heat & Work (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Internal Energy |
11 |
477 |
107.0s |
22 |
100.0% |
0 |
0 |
| π‘ |
Heisenberg vs SchrΓΆdinger: Where Does the Time Go? |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Heisenberg vs SchrΓΆdinger Picture |
11 |
608 |
124.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
The Heisenberg Uncertainty Principle: Why Nature Hides Its Cards |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Heisenberg Uncertainty Principle |
13 |
581 |
229.6s |
20 |
100.0% |
0 |
0 |
| π΄ |
HeliumβNitrogen Mixture Concentration |
10 |
869 |
397.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
helium-nitrogen-mixture-concentration.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Adsorption on a Surface: Gibbs Distribution for a Single Site |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Hemoglobin Oβ Binding: Multiple Occupancy Probabilities |
11 |
1031 |
433.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
hemoglobin-o-binding-multiple-occupancy-probabilities.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Orbital Speed of a Satellite Near Earth's Surface |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Henon Map: Initial Conditions & Attractor Shape |
11 |
959 |
397.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
henon-map-initial-conditions-attractor-shape.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Will This Reaction Happen? Using ΞG to Decide |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Henry's Law Constant for Oβ using van't Hoff Equation |
12 |
1098 |
466.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
henry-s-law-constant-for-o-using-van-t-hoff-equation.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Area of Triangles β Heron's Formula (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Area of Triangles |
10 |
462 |
99.5s |
20 |
100.0% |
0 |
0 |
| π’ |
Hooke's Law |
12 |
418 |
212.7s |
25 |
100.0% |
0 |
0 |
| π‘ |
Hooke's Law (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Hooke's Law |
13 |
598 |
237.9s |
29 |
100.0% |
0 |
0 |
| π‘ |
Escape Velocity from a Planetary Surface |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Hoop rolling on sliding inclined plane |
12 |
1061 |
448.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
hoop-rolling-on-sliding-inclined-plane.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Projectile Motion β Horizontal & Vertical Decomposition (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Projectile Motion |
11 |
563 |
112.0s |
21 |
100.0% |
0 |
0 |
| π΄ |
Hot-Air Soap Bubble Equilibrium |
12 |
1051 |
442.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
hot-air-soap-bubble-equilibrium.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
How Earth's Year Changes with Different Planetary Mass |
11 |
1012 |
396.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
how-earth-s-year-changes-with-different-planetary-mass.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
How Wire Properties Change Fundamental Frequency |
11 |
1003 |
415.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
how-wire-properties-change-fundamental-frequency.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
How a Spinning Coil Generates AC Voltage |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Impedance of AC Circuit Elements |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Impedance of Resistors, Capacitors, and Inductors |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Why AC Voltage Oscillates: Understanding the Sine Wave |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Why AC Voltage Oscillates β and What We Mean by 'RMS' |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
What Is Electrical Energy, Really? |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Why the Sky is Blue: Rayleigh Scattering |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
What Acceleration Really Means in 1D |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
What Is Capacitance, Really? |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
What Is Capacitance, Really? |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Angular Momentum: What It Is and Why It's Conserved |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Coupled Oscillators and Normal Modes |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
What Is Angular Momentum, Really? |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Thin Lens Equation & Ray Diagrams |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Why Satellites Don't Fall: Orbital Motion Unpacked |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Distance vs. Displacement β What's the Difference? |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
How Capacitors Behave in DC Circuits |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Thin Lens Equation & Ray Diagrams |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Superposition & Standing Waves: Where Waves Add Up |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
How a Hydraulic Lift Multiplies Force |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Coupled Oscillators and Normal Modes |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
How Energy Spreads: The Drive Toward Equilibrium |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
How Energy Spreads: Understanding Energy Distribution |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
What Is Electrical Energy, Really? |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
2D Motion: Breaking It Into Two 1D Problems |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
What Acceleration Actually Means in 1D |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Impedance in AC Circuits: Resistance, Reactance, and Phase |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Bridging Kinematics to Dynamics: Why F = ma Is the Link |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Impedance in AC Circuits: Resistance, Reactance, and Phase |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Impedance in AC Circuits: Resistance, Reactance, and Phase |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Why the Sky is Blue (and Sunsets are Red) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Distance vs. Displacement β What's the Difference? |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Why Waves Reflect and Transmit at Boundaries |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
What Happens at a Boundary: Reflection & Transmission |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
How a Transformer Works: Induction Across Coils |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Breaking Vectors Into Components |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Breaking Down 2D Motion: Two Independent Axes |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Breaking Vectors into Components |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Superposition & Standing Waves: Building Intuition |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Sound Perception β Human Range of Hearing (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Sound Perception |
10 |
527 |
109.0s |
20 |
100.0% |
0 |
0 |
| π΄ |
Hydrogen-like Spectra and Atomic Number |
11 |
1046 |
434.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
hydrogen-like-spectra-and-atomic-number.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Hydrostatic Pressure in Layered Fluids |
11 |
1056 |
461.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
hydrostatic-pressure-in-layered-fluids.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Ideal Gas Law β Concept (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Ideal Gas Law |
9 |
485 |
93.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
Free-Body Diagrams & Force Modeling |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Free-Body Diagrams & Force Modeling |
10 |
448 |
105.5s |
23 |
100.0% |
0 |
0 |
| π‘ |
Newton's Third Law & Interaction Pairs |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Newton's Third Law & Interaction Pairs |
10 |
488 |
102.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
Newton's Second Law & Dynamics β Identifying Net Force (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Newton's Second Law & Dynamics |
11 |
520 |
113.0s |
20 |
100.0% |
0 |
0 |
| π΄ |
Identities: div(curl) and curl(grad) |
12 |
1201 |
494.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
identities-div-curl-and-curl-grad.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Improper Integrals & Convergence |
12 |
668 |
132.5s |
29 |
100.0% |
0 |
0 |
| π‘ |
Impulse and Momentum (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Impulse and Momentum |
12 |
541 |
119.5s |
23 |
100.0% |
0 |
0 |
| π‘ |
Impulse-Momentum Theorem (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Impulse-Momentum Theorem |
10 |
583 |
229.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
2D Motion with Constant Acceleration (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
2D Motion with Constant Acceleration |
11 |
541 |
116.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
Inductance & Mutual Inductance (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Inductance & Mutual Inductance |
10 |
446 |
103.5s |
19 |
100.0% |
0 |
0 |
| π΄ |
Inelastic Collisions: Momentum & Energy Loss |
12 |
1071 |
445.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
Newton's First Law & Inertia |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Newton's First Law & Inertia |
10 |
521 |
105.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
Charged Sphere Rolling in a Magnetic Field |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Infinite Ladder RC Circuit: Capacitor Charges |
12 |
1058 |
431.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
infinite-ladder-rc-circuit-capacitor-charges.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Infrared & Visible Light (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Infrared & Visible Light |
11 |
538 |
114.0s |
23 |
100.0% |
0 |
0 |
| π‘ |
1D Acceleration: Definition & Interpretation |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
1D Acceleration: Definition & Interpretation |
9 |
426 |
91.0s |
18 |
100.0% |
0 |
0 |
| π‘ |
Power (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Power |
10 |
481 |
105.0s |
20 |
100.0% |
0 |
0 |
| π‘ |
Integration by Parts (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Integration by Parts |
10 |
541 |
204.1s |
19 |
100.0% |
0 |
0 |
| π’ |
Integration by Substitution |
11 |
533 |
112.0s |
21 |
100.0% |
0 |
0 |
| π΄ |
Interactions in Relativistic Quantum Mechanics |
11 |
1104 |
485.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
interactions-in-relativistic-quantum-mechanics.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Interference and Diffraction (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Interference and Diffraction |
12 |
632 |
121.5s |
25 |
100.0% |
1 |
0 |
| π΄ |
Internal Energy of Air at Normal Conditions |
11 |
972 |
406.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
internal-energy-of-air-at-normal-conditions.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Compound Circuits β Internal Resistance (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Compound Circuits |
12 |
570 |
126.0s |
23 |
100.0% |
0 |
0 |
| π΄ |
Introduction to Quantum Mechanics: The Wave Function |
11 |
1076 |
445.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
introduction-to-quantum-mechanics-the-wave-function.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Introduction to Quantum Mechanics: Wave Functions & SchrΓΆdinger |
11 |
1011 |
438.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
introduction-to-quantum-mechanics-wave-functions-schr-dinger.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Universal Law of Gravitation (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Universal Law of Gravitation |
11 |
492 |
110.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Normal Shock Wave: Finding Post-Shock Conditions |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Isentropic Flow in Ducts: Continuity & State Relations |
12 |
1081 |
461.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
isentropic-flow-in-ducts-continuity-state-relations.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Isothermal Expansion & Work Done by Gas |
12 |
1102 |
464.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
isothermal-expansion-work-done-by-gas.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Jam-powered roof climb: energy and power |
11 |
874 |
350.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
jam-powered-roof-climb-energy-and-power.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Jet Force on Deflecting Plates |
12 |
1097 |
443.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
jet-force-on-deflecting-plates.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Jet Impact Force on Stationary Vane |
9 |
823 |
323.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
jet-impact-force-on-stationary-vane.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
The Josephson Effect |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Josephson Effect |
11 |
649 |
277.7s |
26 |
100.0% |
0 |
0 |
| π‘ |
Kepler Orbits & Central Force Motion |
16 |
745 |
317.7s |
23 |
75.0% |
0 |
0 |
| π΄ |
Kepler's Equation: Successive Approximations via Taylor Series |
12 |
1043 |
437.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
kepler-s-equation-successive-approximations-via-taylor-serie.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Kepler's Laws of Planetary Motion |
13 |
515 |
214.7s |
21 |
100.0% |
0 |
0 |
| π‘ |
Planetary Motion & Orbits β Kepler's Third Law (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Planetary Motion & Orbits |
11 |
658 |
117.5s |
22 |
100.0% |
0 |
0 |
| π’ |
Kinematics: Constant Acceleration |
15 |
610 |
245.0s |
23 |
100.0% |
0 |
0 |
| π΄ |
Kinematics: Velocity, Acceleration, and Rest Points |
11 |
889 |
354.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
kinematics-velocity-acceleration-and-rest-points.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Kinetic Energy: Center of Mass + Internal Motion |
12 |
1072 |
459.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
kinetic-energy-center-of-mass-internal-motion.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Rolling Without Slipping: Finding Acceleration of a Cylinder on an Incline |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Kinetic Energy of a Rolling Cone with Fixed Vertex |
12 |
1130 |
480.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
kinetic-energy-of-a-rolling-cone-with-fixed-vertex.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Kinetic Energy of Two-Rod Sliding System |
12 |
1066 |
444.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
kinetic-energy-of-two-rod-sliding-system.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Kinetic Theory Of Gases (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Kirchhoff's Laws |
12 |
657 |
130.0s |
23 |
100.0% |
0 |
0 |
| π‘ |
The Klein-Gordon Equation |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Klein-Gordon Equation |
11 |
561 |
243.0s |
22 |
100.0% |
0 |
0 |
| π’ |
Lagrange Multipliers |
11 |
621 |
118.0s |
21 |
100.0% |
0 |
0 |
| π’ |
Lagrangian Mechanics: The Simple Pendulum |
13 |
723 |
283.0s |
21 |
100.0% |
0 |
0 |
| π’ |
Lagrangian Mechanics II |
15 |
623 |
265.3s |
23 |
100.0% |
0 |
0 |
| π΄ |
Lagrangian Mechanics: Simple Pendulum via Euler-Lagrange |
14 |
739 |
312.8s |
0 |
0.0% |
0 |
0 |
| π΄ |
Lagrangian Mechanics: Spring-Suspended Swinging Bar |
12 |
1217 |
502.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
lagrangian-mechanics-spring-suspended-swinging-bar.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Lagrangian Mechanics: The Simple Pendulum |
15 |
729 |
318.9s |
24 |
100.0% |
0 |
0 |
| π‘ |
The Lamb Shift |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Lamb Shift |
10 |
514 |
224.1s |
20 |
100.0% |
0 |
0 |
| π’ |
Larmor Formula: Radiation from an Accelerating Charge |
14 |
607 |
267.1s |
23 |
100.0% |
0 |
0 |
| π’ |
Latent Heat of Vaporization |
11 |
588 |
231.7s |
23 |
100.0% |
0 |
0 |
| π‘ |
Phase Change β Latent Heat (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Phase Change |
10 |
463 |
102.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
Newton's First Law & Inertia (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Newton's First Law & Inertia |
10 |
446 |
96.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
Laws of Exponents β The Real Number System (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Real Number System |
11 |
515 |
119.0s |
23 |
100.0% |
0 |
0 |
| π‘ |
Reflection of Light (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Reflection of Light |
10 |
525 |
109.5s |
22 |
100.0% |
0 |
0 |
| π΄ |
Leaning triangular panel: wall and floor reactions |
13 |
1118 |
483.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
leaning-triangular-panel-wall-and-floor-reactions.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Lenz's Law |
11 |
557 |
112.5s |
22 |
100.0% |
1 |
0 |
| π΄ |
Length Contraction: Why Moving Objects Shrink |
10 |
968 |
406.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
length-contraction-why-moving-objects-shrink.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Lens Diameter & Solar Image Illumination |
11 |
1181 |
465.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
lens-diameter-solar-image-illumination.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Lens Focal Length & Optical Power |
10 |
792 |
339.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
lens-focal-length-optical-power.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Lenz's Law |
11 |
537 |
226.9s |
20 |
100.0% |
0 |
0 |
| π’ |
Lenz's Law |
10 |
532 |
204.4s |
20 |
100.0% |
0 |
0 |
| π‘ |
Lenz's Law & Electromagnetic Induction |
14 |
757 |
323.8s |
28 |
83.3% |
0 |
0 |
| π’ |
Lenz's Law & Faraday's Law |
16 |
747 |
313.7s |
25 |
100.0% |
0 |
0 |
| π’ |
Lenz's Law & Faraday's Law |
14 |
733 |
307.0s |
25 |
100.0% |
0 |
0 |
| π‘ |
lenz-s-law-of-electromagnetic-induction.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Lenz's Law: Opposition in Electromagnetic Induction |
11 |
1009 |
410.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
lenz-s-law-opposition-in-electromagnetic-induction.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Lenz's Law (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Lenz's Law |
11 |
601 |
226.9s |
20 |
100.0% |
0 |
0 |
| π‘ |
Particle Physics β Leptons, Quarks & Antiquarks |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Particle Physics |
10 |
460 |
103.0s |
19 |
100.0% |
0 |
0 |
| π’ |
Limits & the Epsilon-Delta Definition |
11 |
644 |
121.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
Linear Momentum and Collisions (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Linear Momentum and Collisions |
11 |
571 |
116.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
System Momentum β Concept (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
System Momentum |
11 |
477 |
114.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Linear Momentum β Concept (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Thermal Expansion (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Thermal Expansion |
11 |
556 |
113.0s |
21 |
100.0% |
0 |
0 |
| π’ |
Liouville's Theorem: Phase Space |
15 |
671 |
274.1s |
23 |
100.0% |
0 |
0 |
| π‘ |
Sound: Production & Nature (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Sound: Production & Nature |
11 |
555 |
116.5s |
23 |
100.0% |
0 |
0 |
| π΄ |
Lorentz Force for Magnetic Monopoles |
12 |
497 |
207.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
lorentz-force-for-magnetic-monopoles.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Lorentz Force & Particle Acceleration |
12 |
1166 |
469.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
lorentz-force-particle-acceleration.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Lorentz Transformation: Space and Time Bend |
12 |
1229 |
530.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
lorentz-transformation-space-and-time-bend.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Lorentz Transformations & 4-Vectors |
15 |
679 |
287.3s |
23 |
100.0% |
0 |
0 |
| π‘ |
Two Trains, Two Clocks: Simultaneity in Relative Motion |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Loss of Simultaneity in Special Relativity |
11 |
1038 |
436.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
loss-of-simultaneity-in-special-relativity.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Maclaurin Series |
11 |
630 |
118.5s |
21 |
100.0% |
0 |
0 |
| π΄ |
Magnetic Field Around an Infinite Wire |
12 |
1149 |
439.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
magnetic-field-around-an-infinite-wire.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Magnetic Fields (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Magnetic Fields |
11 |
608 |
114.0s |
21 |
100.0% |
0 |
0 |
| π΄ |
Magnetic Field from a Current Ring |
12 |
1175 |
472.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
magnetic-field-from-a-current-ring.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Magnetic field in bent current ring |
11 |
1017 |
397.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
magnetic-field-in-bent-current-ring.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Magnetic Field of a Current-Carrying Wire |
12 |
413 |
161.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
Fields due to Currents β Magnetic Field of a Straight Conductor (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Fields due to Currents |
10 |
562 |
108.0s |
19 |
100.0% |
0 |
0 |
| π΄ |
Magnetic Field of a Current-Carrying Wire (AI Β· with voice) |
12 |
412 |
158.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
Foundations of Induction β Magnetic Flux (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Foundations of Induction |
11 |
553 |
120.0s |
21 |
100.0% |
0 |
0 |
| π΄ |
Magnetic flux through half a wire's cross-section |
11 |
973 |
379.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
magnetic-flux-through-half-a-wire-s-cross-section.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Magnetic Force on Currents |
13 |
546 |
209.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
Bead on a Rotating Hoop: Finding the Equilibrium Angle |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Magnetic Forces & Conservation Laws in Particle Systems |
11 |
1064 |
452.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
magnetic-forces-conservation-laws-in-particle-systems.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Colliding Carts: Finding the Final Velocity |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Magnetic Monopoles: Force Law & Symmetry |
12 |
1362 |
552.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
magnetic-monopoles-force-law-symmetry.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Newton's First Law & Inertia (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Newton's First Law & Inertia |
10 |
447 |
101.5s |
18 |
100.0% |
0 |
0 |
| π‘ |
Simple Harmonic Motion β Mass-Spring Systems (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Simple Harmonic Motion |
11 |
493 |
115.0s |
21 |
100.0% |
0 |
0 |
| π’ |
Mathematical Proof Techniques |
12 |
543 |
124.0s |
25 |
100.0% |
0 |
0 |
| π΄ |
Matrix Invariants Under Similarity Transformations |
12 |
1078 |
503.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
matrix-invariants-under-similarity-transformations.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Matrix Inverse via Cofactors |
11 |
541 |
109.5s |
22 |
100.0% |
0 |
0 |
| π‘ |
Spinning Skater: Conservation of Angular Momentum |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Matrix of Jz in the y-basis and expectation value |
11 |
914 |
366.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
matrix-of-jz-in-the-y-basis-and-expectation-value.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Maximum Power Transfer in Generators |
12 |
1180 |
488.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
maximum-power-transfer-in-generators.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Maximum Separation Angle in Two-Body Decay |
12 |
1130 |
475.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
maximum-separation-angle-in-two-body-decay.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Maximum Speed of a Deflected Pendulum |
12 |
1125 |
422.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
maximum-speed-of-a-deflected-pendulum.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Maximum Temperature in Ideal Gas Processes |
12 |
1144 |
487.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
maximum-temperature-in-ideal-gas-processes.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Maxwell-Boltzmann Distribution |
12 |
643 |
268.2s |
26 |
100.0% |
0 |
0 |
| π’ |
Maxwell-Boltzmann Distribution |
14 |
658 |
275.2s |
26 |
100.0% |
0 |
0 |
| π’ |
Maxwell's Equations in Differential Form |
14 |
822 |
344.0s |
23 |
100.0% |
0 |
0 |
| π‘ |
maxwell-s-equations-overview.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Maxwell's Equations |
13 |
570 |
243.6s |
0 |
0.0% |
0 |
0 |
| π’ |
Maxwell's First Equation |
11 |
593 |
120.2s |
22 |
100.0% |
0 |
0 |
| π’ |
Maxwell's Relations in Thermodynamics |
14 |
641 |
260.7s |
23 |
100.0% |
0 |
0 |
| π‘ |
Maxwell's Equations Overview (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Maxwell's Equations Overview |
12 |
751 |
329.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
maxwells-equations-overview.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Temperature & Heat β Concept Guide |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Temperature & Heat |
11 |
537 |
114.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
Mechanical Energy (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Mechanical Energy |
10 |
520 |
105.0s |
19 |
100.0% |
0 |
0 |
| π΄ |
mechanical-waves.json |
PARSE ERROR: parse: Expecting ',' delimiter: line 323 column 30 (char 16452) |
| π’ |
The Michelson Interferometer |
10 |
488 |
101.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
Quadrilaterals β Midpoint Theorem (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Quadrilaterals |
11 |
491 |
111.5s |
23 |
100.0% |
0 |
0 |
| π’ |
Millikan Oil-Drop Experiment |
11 |
658 |
121.0s |
23 |
100.0% |
0 |
0 |
| π΄ |
Minimum exhaust velocity for rocket liftoff |
11 |
935 |
369.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
minimum-exhaust-velocity-for-rocket-liftoff.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Minimum Height to Complete a Vertical Loop |
11 |
1039 |
394.4s |
0 |
0.0% |
0 |
0 |
| π΄ |
Minimum Mirror Height for Full-Length Reflection |
12 |
1202 |
437.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
minimum-mirror-height-for-full-length-reflection.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Minkowski Diagram Units and Interval Invariance |
11 |
1061 |
447.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
minkowski-diagram-units-and-interval-invariance.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Microscopic Current Model (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Microscopic Current Model |
12 |
587 |
126.5s |
25 |
100.0% |
0 |
0 |
| π΄ |
Molar mass and degrees of freedom from heat capacities |
10 |
811 |
341.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
molar-mass-and-degrees-of-freedom-from-heat-capacities.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Mole Fractions at Reduced Pressure: Gas Mixture Analysis |
12 |
1177 |
498.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
mole-fractions-at-reduced-pressure-gas-mixture-analysis.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Molecular Collisions: How Density & Temperature Change Collision Rate |
11 |
1067 |
446.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
molecular-collisions-how-density-temperature-change-collisio.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Moment of Inertia (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Moment of Inertia |
14 |
545 |
222.4s |
21 |
100.0% |
0 |
0 |
| π‘ |
Collisions & Momentum |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Collisions & Momentum |
10 |
450 |
107.0s |
21 |
100.0% |
0 |
0 |
| π΄ |
Momentum Conservation: Man and Raft on a Lake |
11 |
499 |
209.5s |
0 |
0.0% |
0 |
0 |
| π΄ |
Momentum Conservation: Man and Raft on Water |
11 |
993 |
395.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
Linear Momentum of a System of Particles (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Linear Momentum |
11 |
546 |
113.0s |
22 |
100.0% |
0 |
0 |
| π΄ |
Momentum Transfer from Reflected Light |
11 |
965 |
397.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
momentum-transfer-from-reflected-light.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Finding Orbital Speed from Radius |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Moon's Elliptical Orbit: Finding Apogee Distance |
12 |
1050 |
451.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
moon-s-elliptical-orbit-finding-apogee-distance.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Moseley's Law: X-ray wavelengths for Ka lines |
10 |
759 |
313.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
moseley-s-law-x-ray-wavelengths-for-ka-lines.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Most Probable de Broglie Wavelength of Hβ at Room Temperature |
11 |
1102 |
466.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
most-probable-de-broglie-wavelength-of-h-at-room-temperature.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Most Probable Velocities in Gas Mixtures |
11 |
1047 |
417.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
most-probable-velocities-in-gas-mixtures.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Moving charge in capacitor: current induced |
12 |
1115 |
437.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
moving-charge-in-capacitor-current-induced.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Multiple Integrals |
11 |
656 |
116.0s |
21 |
100.0% |
0 |
0 |
| π΄ |
Multipole expansion of a non-uniform charged sphere |
12 |
1102 |
465.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
multipole-expansion-of-a-non-uniform-charged-sphere.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Mutual Inductance of Two Coils on a Shared Core |
9 |
773 |
313.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
mutual-inductance-of-two-coils-on-a-shared-core.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Mutual Inductance (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Mutual Inductance |
10 |
547 |
219.7s |
22 |
100.0% |
0 |
0 |
| π‘ |
Electric Charge β Nature of Charge (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Electric Charge |
11 |
551 |
115.5s |
21 |
100.0% |
0 |
0 |
| π΄ |
Navier-Stokes: Newton's Second Law for Fluids |
11 |
1037 |
434.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
navier-stokes-newton-s-second-law-for-fluids.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Bead on a Rotating Hoop |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Net Torque Independence from Reference Frame |
11 |
976 |
376.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
net-torque-independence-from-reference-frame.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Neutrino Oscillations (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Neutrino Oscillations |
11 |
648 |
283.3s |
23 |
100.0% |
0 |
0 |
| π’ |
Newton's Law of Universal Gravitation |
14 |
813 |
346.7s |
23 |
100.0% |
0 |
0 |
| π΄ |
Newton's Laws of Motion: Forces and Acceleration |
11 |
1075 |
348.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
newton-s-laws-of-motion-forces-and-acceleration.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Rotational Dynamics β Newton's Second Law for Rotation (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Rotational Dynamics |
11 |
563 |
114.5s |
21 |
100.0% |
0 |
0 |
| π’ |
Newton's Second Law |
14 |
668 |
260.8s |
22 |
100.0% |
0 |
0 |
| π‘ |
Newton's Second Law: Force, Mass, and Acceleration |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Newton's Second Law |
15 |
678 |
263.3s |
22 |
100.0% |
0 |
0 |
| π’ |
Newton's Third Law |
14 |
417 |
165.5s |
26 |
100.0% |
0 |
0 |
| π’ |
Newton's Third Law |
12 |
403 |
158.5s |
26 |
100.0% |
0 |
0 |
| π‘ |
Nodes and Antinodes in Standing Waves (Figure It Out) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Nodes and Antinodes in Standing Waves |
12 |
1183 |
469.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
nodes-and-antinodes-in-standing-waves.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Noether's Theorem: Symmetry & Conservation |
13 |
641 |
267.6s |
23 |
100.0% |
0 |
0 |
| π’ |
Noether's Theorem: Symmetry & Conservation |
15 |
657 |
274.4s |
23 |
100.0% |
0 |
0 |
| π‘ |
Conservative & Non-Conservative Forces (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Conservative & Non-Conservative Forces |
12 |
594 |
129.0s |
25 |
100.0% |
0 |
2 |
| π’ |
Normal Force in an Accelerating Elevator |
10 |
430 |
100.5s |
20 |
100.0% |
0 |
0 |
| π‘ |
Common Forces in Mechanics β Normal Force (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Common Forces in Mechanics |
12 |
561 |
121.0s |
25 |
100.0% |
0 |
0 |
| π‘ |
Ballistic Pendulum: Finding Bullet Speed |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Normal modes of two masses and three springs |
12 |
1014 |
456.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
normal-modes-of-two-masses-and-three-springs.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Normal Modes (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Normal Modes |
12 |
642 |
129.0s |
23 |
100.0% |
0 |
0 |
| π‘ |
Nuclear Binding Energy (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Nuclear Binding Energy |
11 |
607 |
122.5s |
21 |
100.0% |
0 |
0 |
| π΄ |
Nuclear decay in a moving beam: perpendicular velocity |
12 |
1027 |
442.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
nuclear-decay-in-a-moving-beam-perpendicular-velocity.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Nuclear Fusion in Stars |
11 |
554 |
109.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Number Systems β Natural, Integer, Rational, Real, Complex (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Number Systems |
12 |
566 |
118.5s |
22 |
100.0% |
0 |
0 |
| π‘ |
Optical Instruments (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Optical Instruments |
12 |
565 |
117.0s |
23 |
100.0% |
0 |
0 |
| π‘ |
Optics: Reflection & Refraction (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Optics: Reflection & Refraction |
11 |
573 |
115.0s |
21 |
100.0% |
0 |
0 |
| π΄ |
Optimal Running Path Around a Triangular House |
12 |
1090 |
424.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
optimal-running-path-around-a-triangular-house.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Orbital Mechanics (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π |
Orbital Mechanics |
11 |
552 |
115.0s |
23 |
100.0% |
4 |
0 |
| π΄ |
Orbital Motion and Planetary Mass: Phobos & Mars |
11 |
964 |
402.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
orbital-motion-and-planetary-mass-phobos-mars.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Orbital Motion of Satellites (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Orbital Motion |
11 |
581 |
119.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
The Real Number System β Order of Operations (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Real Number System |
12 |
614 |
122.0s |
22 |
100.0% |
0 |
0 |
| π‘ |
Roller Coaster Loop: Will It Make It? |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Overdamped Oscillator: Finding Trajectory & Origin Passage |
12 |
1069 |
420.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
overdamped-oscillator-finding-trajectory-origin-passage.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
The p-n Junction (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The p-n Junction |
11 |
519 |
112.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Partial Derivatives (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Partial Derivatives |
10 |
526 |
192.6s |
19 |
100.0% |
0 |
0 |
| π’ |
Partial Fractions Decomposition |
10 |
505 |
105.5s |
18 |
100.0% |
0 |
0 |
| π‘ |
Why Only Certain Energies Fit Inside a Box |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π |
Particle in a Box |
16 |
628 |
264.8s |
13 |
58.3% |
0 |
0 |
| π‘ |
Particle in a Linear Potential: Meeting the Airy Function |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Particle in a Linear Potential: Airy Functions |
11 |
1138 |
480.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
particle-in-a-linear-potential-airy-functions.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Particle on a Cardioid with Constant Speed |
13 |
1247 |
552.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
particle-on-a-cardioid-with-constant-speed.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Finding Free Energy from the Partition Function |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Partition Function for Two Independent Systems |
10 |
888 |
360.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
partition-function-for-two-independent-systems.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Pauli Exclusion Principle & Electron Shells |
14 |
576 |
235.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Percentages (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Percentages |
9 |
460 |
96.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
Percentages β Figure It Out |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Resonance in a Driven Mass-Spring System |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Period of a Hoop Oscillating on a Nail |
11 |
975 |
386.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
period-of-a-hoop-oscillating-on-a-nail.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Period of a Simple Pendulum |
14 |
588 |
242.6s |
22 |
100.0% |
0 |
0 |
| π΄ |
Period of Spring Oscillation: Independence from Amplitude |
11 |
1074 |
408.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
period-of-spring-oscillation-independence-from-amplitude.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Perpendicular Reflection & Refraction at Water |
12 |
1027 |
438.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
perpendicular-reflection-refraction-at-water.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Perturbation Theory |
15 |
786 |
346.4s |
23 |
100.0% |
0 |
0 |
| π‘ |
Phase Changes & Latent Heat |
14 |
578 |
233.4s |
23 |
100.0% |
1 |
0 |
| π‘ |
Resonance in a Driven Spring-Mass System |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Phase Space Portraits of Linear Oscillators |
11 |
1142 |
481.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
phase-space-portraits-of-linear-oscillators.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Wave Description β Phase, Wavelength & Frequency (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Wave Description |
11 |
538 |
111.5s |
22 |
100.0% |
0 |
0 |
| π΄ |
Photoelectric Effect: Light Knocks Out Electrons |
11 |
1097 |
474.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
photoelectric-effect-light-knocks-out-electrons.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Photon Absorption by a Stationary Atom |
12 |
1129 |
495.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
photon-absorption-by-a-stationary-atom.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Pendulums β Physical Pendulum (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Pendulums |
11 |
564 |
214.8s |
19 |
90.0% |
1 |
11 |
| π‘ |
Measurement Systems (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Measurement Systems |
10 |
386 |
154.7s |
19 |
100.0% |
0 |
0 |
| π΄ |
Pion-Muon Race: Relativistic Speed Comparison |
10 |
883 |
379.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
pion-muon-race-relativistic-speed-comparison.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Pipe Reduction: Force on Flange Bolts |
10 |
889 |
392.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
pipe-reduction-force-on-flange-bolts.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Finding the Electric Field of a Charged Spherical Shell |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Floating Duck in Layered Oil and Water |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Resistance of a Uniform Metallic Sphere |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Finding the Pin Position for a Given Image Location |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Polarization by Reflection: Brewster's Angle & Degree of Polarization |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Period of a Mass-Spring System |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Electric Field of an Infinite Line Charge |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Packing Tetrahedra: What Fraction of Space Can They Fill? |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
X-Ray Diffraction: Finding Lattice Spacing from Bragg's Law |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Lenslet Array: Finding the System's Effective Focal Length |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Finding the Equilibrium Position of a Block on a Spring |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Net Force on a Block While in Contact with a Spring |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Entropy Change When Two Ideal Gases Mix Irreversibly |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Carnot Engine: Finding Efficiency and Heat Flows |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Neutron & Moderator Speeds in the Center-of-Mass Frame |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Molecular Speed Distribution: Applying the Maxwell-Boltzmann Expression |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Lapse Rate from First Principles |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Evening Dew Point: Will Dew Form Tonight? |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Binding Energy per Nucleon of Helium-4 |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Angle Between a Surface Intersection Line and a Particle Trajectory |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Cup Anemometer: Finding Wind Speed from Rotation Rate |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Parallel Beam Through a Prism: Finding the Transmitted Wavelength Range |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Proton Accelerated Through a Potential Difference |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
IPhO 1967 P3: Charged Particle in Magnetic Field |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Elastic Energy Stored in a Bent Rod |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Urban Walk: Average Speed Over Mixed Terrain |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
IPhO 1976 P2: Floating Cylinder in Two Liquids |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Racing Light: Cherenkov Radiation Angle |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Sphere Inside a Shell: Finding the Electrostatic Force |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
IPhO 1983 P5: Cylinder Rolling Inside a Sphere |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
IPhO 1989 P2: Optical Fiber & Total Internal Reflection |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Floating Ice with a Stone: Does the Water Level Change? |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Force to Lift a Piston Inside a Submerged Tube |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Finding the Schwarzschild Radius of a Black Hole |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Trolleybus Snaps Its Wire: Braking & Coasting to a Stop |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Formula Car on the Ceiling: How Fast to Stay Up? |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Snell's Law from Huygens's Principle |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Point Charge Near a Conducting Plane |
12 |
1148 |
455.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
point-charge-near-a-conducting-plane.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Polarization & Malus' Law |
13 |
436 |
185.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
Polarization of Light (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Polarization of Light |
11 |
1018 |
439.7s |
0 |
0.0% |
0 |
0 |
| π’ |
Polarizers and Waveplates |
13 |
588 |
247.7s |
19 |
100.0% |
0 |
0 |
| π’ |
Polaroid Stacks & Malus's Law |
11 |
478 |
111.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Polynomials β Guide Me |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Polynomials |
12 |
520 |
117.0s |
22 |
100.0% |
0 |
1 |
| π‘ |
Polynomials β Definition & Degree (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Polynomials |
11 |
591 |
115.0s |
22 |
100.0% |
0 |
0 |
| π‘ |
Position, Displacement & Vector Equality |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Position, Displacement & Vector Equality |
11 |
542 |
210.7s |
20 |
100.0% |
0 |
0 |
| π‘ |
Compound Circuits β Potential Dividers (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Compound Circuits |
12 |
581 |
121.5s |
23 |
100.0% |
0 |
0 |
| π‘ |
Potential Energy & Conservation of Energy (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Potential Energy & Conservation of Energy |
11 |
558 |
117.0s |
23 |
100.0% |
0 |
0 |
| π΄ |
Potential Energy in a 3D Cubic Ionic Crystal |
10 |
948 |
380.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
potential-energy-in-a-3d-cubic-ionic-crystal.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Potential energy per ion in a 1D ionic crystal |
9 |
822 |
335.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
potential-energy-per-ion-in-a-1d-ionic-crystal.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Potential of Charged Sphere: Boundary Value Problems |
12 |
1073 |
492.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
potential-of-charged-sphere-boundary-value-problems.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Potential of Concentric Charged Spheres |
9 |
769 |
329.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
potential-of-concentric-charged-spheres.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Potential of Uncharged Conducting Sphere with External Point Charge |
12 |
1144 |
450.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
potential-of-uncharged-conducting-sphere-with-external-point.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Power & Mechanical Efficiency |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Power & Mechanical Efficiency |
11 |
549 |
109.5s |
22 |
100.0% |
1 |
0 |
| π‘ |
Irodov 1.126: Disk Rolling Without Slipping β Velocity of a Point |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Power from Time-Varying Centripetal Acceleration |
11 |
942 |
386.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
power-from-time-varying-centripetal-acceleration.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Power in Battery Charging: Useful vs. Thermal |
12 |
1136 |
464.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
power-in-battery-charging-useful-vs-thermal.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Electric Power (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Electric Power |
10 |
521 |
102.5s |
19 |
100.0% |
0 |
0 |
| π΄ |
Power to Drive a Conveyor Belt with Falling Gravel |
10 |
955 |
388.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
power-to-drive-a-conveyor-belt-with-falling-gravel.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Power, Work & Energy Efficiency |
13 |
516 |
198.8s |
19 |
100.0% |
0 |
0 |
| π’ |
Poynting Vector: Energy Flow in EM Fields |
14 |
671 |
266.7s |
24 |
100.0% |
0 |
0 |
| π’ |
Poynting Vector: Energy Flow in EM Fields |
14 |
644 |
248.0s |
21 |
100.0% |
0 |
0 |
| π΄ |
Predicting Turbulent Transition in Oil Flow |
12 |
1192 |
530.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
predicting-turbulent-transition-in-oil-flow.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Pressure and Pascal's Principle |
10 |
509 |
101.0s |
19 |
100.0% |
0 |
0 |
| π΄ |
Pressure Head: Converting Pressure to Fluid Column Height |
12 |
1121 |
486.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
pressure-head-converting-pressure-to-fluid-column-height.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Fluid Statics β Pressure in Fluids (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Fluid Statics |
11 |
697 |
118.0s |
22 |
100.0% |
0 |
0 |
| π’ |
Pressure & Pascal's Principle |
14 |
535 |
215.1s |
21 |
100.0% |
0 |
0 |
| π΄ |
Principal Planes & Focal Length of Thick Lenses |
12 |
1206 |
500.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
principal-planes-focal-length-of-thick-lenses.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Rotational Equilibrium β Principle of Moments (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Rotational Equilibrium |
12 |
570 |
120.5s |
22 |
100.0% |
0 |
0 |
| π‘ |
Atwood Machine: Finding Acceleration & Tension |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Atwood machine β acceleration and tension |
6 |
372 |
150.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
Block on Inclined Plane with Friction |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Block on an inclined plane with friction |
7 |
397 |
163.6s |
0 |
0.0% |
0 |
0 |
| π΄ |
Loop the loop β minimum starting height |
7 |
503 |
188.9s |
0 |
0.0% |
0 |
0 |
| π΄ |
Perfectly inelastic cart collision |
6 |
319 |
136.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
Spring-block oscillator β Guide Me |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Spring-block oscillator β Guide Me |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Spring-block oscillator β period and max speed |
7 |
435 |
186.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
Free-Body Diagrams & Force Modeling (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Free-Body Diagrams & Force Modeling |
12 |
640 |
129.5s |
23 |
100.0% |
0 |
0 |
| π’ |
Product & Quotient Rules |
11 |
748 |
126.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
Projectile Motion on an Incline |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Projectile Motion: Range & Maximum Height |
13 |
586 |
248.2s |
23 |
100.0% |
0 |
0 |
| π‘ |
Projectile Motion (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Projectile Motion |
11 |
454 |
110.0s |
24 |
100.0% |
0 |
0 |
| π‘ |
Projectile Range: Hitting a Distant Target |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Projectile Range: Hitting a Distant Target |
11 |
1072 |
443.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
projectile-range-hitting-a-distant-target.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Proper Lifetime from Decay Distance |
12 |
1136 |
454.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
proper-lifetime-from-decay-distance.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Triangle Properties (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Triangle Properties |
11 |
565 |
117.5s |
23 |
100.0% |
0 |
0 |
| π‘ |
Polarized Light Through Two Polaroids: Malus's Law Twice |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Pulley-Mass-Spring System Oscillation Frequency |
12 |
1054 |
443.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
pulley-mass-spring-system-oscillation-frequency.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
DistanceβTime Graphs (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
DistanceβTime Graphs |
11 |
460 |
183.9s |
23 |
100.0% |
1 |
0 |
| π‘ |
Precision & Reporting (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Precision & Reporting |
11 |
490 |
110.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
Matter Waves β Quantisation via Standing Waves (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Matter Waves |
11 |
496 |
114.5s |
20 |
100.0% |
0 |
0 |
| π΄ |
Quantum Bouncing Ball: From Classical to Quantum |
12 |
1077 |
443.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
quantum-bouncing-ball-from-classical-to-quantum.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Spinning Skater: Conservation of Angular Momentum |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Quantum Bound State in a Delta Potential |
12 |
1174 |
489.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
quantum-bound-state-in-a-delta-potential.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Quantum Darwinism: How the Quantum World Becomes Classical |
12 |
1149 |
407.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
quantum-darwinism-how-the-quantum-world-becomes-classical.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Quantum Darwinism: Why the Quantum World Looks Classical |
11 |
465 |
161.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
quantum-darwinism-why-the-quantum-world-looks-classical.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Quantum Entanglement & Bell's Inequality |
14 |
617 |
267.5s |
0 |
0.0% |
0 |
0 |
| π΄ |
Quantum Entanglement: Spooky Action Explained |
11 |
1020 |
370.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
quantum-entanglement-spooky-action-explained.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
The Quantum Hall Effect |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Quantum Hall Effect |
11 |
589 |
242.3s |
22 |
100.0% |
0 |
0 |
| π΄ |
Quantum Harmonic Oscillator: Energy Levels and Zero-Point Motion |
12 |
1152 |
503.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
quantum-harmonic-oscillator-energy-levels-and-zero-point-mot.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Quantum Harmonic Oscillator: Ladder Operators |
14 |
665 |
287.8s |
22 |
100.0% |
0 |
0 |
| π‘ |
Quantum Harmonic Oscillator |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Quantum Harmonic Oscillator |
11 |
651 |
118.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
Quantum Numbers & Atomic Orbitals |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Quantum Numbers & Atomic Orbitals |
10 |
576 |
106.0s |
20 |
100.0% |
0 |
0 |
| π΄ |
Quantum Tunneling: Particles Breaking the Rules |
11 |
1050 |
434.9s |
0 |
0.0% |
0 |
0 |
| π΄ |
Quantum Tunneling: Particles Through Barriers |
11 |
1107 |
476.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
quantum-tunneling-particles-through-barriers.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Quantum Tunneling |
14 |
708 |
277.6s |
23 |
100.0% |
0 |
0 |
| π‘ |
Quantum Tunneling (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Quantum Tunneling |
16 |
724 |
284.5s |
23 |
100.0% |
0 |
0 |
| π΄ |
Quantum Tunnelling: Particles Through Barriers |
11 |
1062 |
451.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
quantum-tunnelling-particles-through-barriers.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Quark Confinement (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Quark Confinement |
11 |
546 |
218.1s |
23 |
100.0% |
0 |
0 |
| π‘ |
Quarks and Leptons |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Quarks and Leptons |
10 |
498 |
105.5s |
19 |
100.0% |
0 |
0 |
| π΄ |
Radiation Pressure from EM Waves on Conductors |
11 |
1090 |
442.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
radiation-pressure-from-em-waves-on-conductors.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Heat Transfer β Radiation (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Heat Transfer |
11 |
506 |
112.5s |
23 |
100.0% |
1 |
0 |
| π‘ |
The Real Number System β Radicals and Surds (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Real Number System |
11 |
563 |
109.5s |
21 |
100.0% |
0 |
0 |
| π΄ |
Radio Signal Travel Time from JWST to Earth |
8 |
691 |
276.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
radio-signal-travel-time-from-jwst-to-earth.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Radioactive Decay & Half-Life |
13 |
467 |
206.4s |
19 |
100.0% |
0 |
0 |
| π‘ |
Radioactive Decay (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Radioactive Decay |
11 |
495 |
107.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Ratio and Proportion |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Ratio and Proportion |
11 |
476 |
103.0s |
20 |
100.0% |
0 |
0 |
| π’ |
RC Circuit Time Constant |
11 |
547 |
119.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
RC Circuits & Time Constants (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
RC Circuits & Time Constants |
11 |
615 |
120.0s |
22 |
100.0% |
0 |
0 |
| π‘ |
Band Gaps from Bragg Reflection: Why Forbidden Energies Exist |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Reciprocal Lattices & Bravais Lattice Duality |
12 |
1127 |
507.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
reciprocal-lattices-bravais-lattice-duality.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Reflection & the Law of Reflection (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Reflection & the Law of Reflection |
11 |
486 |
99.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Sound Reflection Phenomena (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Sound Reflection Phenomena |
10 |
509 |
99.5s |
19 |
100.0% |
0 |
0 |
| π’ |
Refraction & Snell's Law |
11 |
565 |
115.0s |
23 |
100.0% |
0 |
0 |
| π΄ |
Refraction at a Glass-Water Boundary |
13 |
737 |
330.1s |
0 |
0.0% |
0 |
0 |
| π΄ |
Refraction at a Glass-Water Boundary |
12 |
415 |
159.9s |
0 |
0.0% |
0 |
0 |
| π’ |
Refraction & Snell's Law |
16 |
815 |
358.5s |
23 |
100.0% |
0 |
0 |
| π‘ |
Refraction of Light (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Refraction of Light |
11 |
611 |
130.0s |
24 |
100.0% |
0 |
0 |
| π‘ |
Refrigerators and Heat Pumps (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Refrigerators and Heat Pumps |
11 |
569 |
112.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
Relativistic Doppler Effect (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Relativistic Doppler Effect |
14 |
595 |
240.6s |
23 |
100.0% |
0 |
0 |
| π΄ |
Relativistic Drift in Crossed E and B Fields |
12 |
1191 |
481.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
relativistic-drift-in-crossed-e-and-b-fields.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Relativistic Mass and Momentum for Two Particles |
11 |
959 |
403.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
relativistic-mass-and-momentum-for-two-particles.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Relativistic Momentum & Energy (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Relativistic Momentum & Energy |
12 |
627 |
131.0s |
23 |
100.0% |
0 |
0 |
| π’ |
Relativistic Momentum |
13 |
536 |
224.9s |
21 |
100.0% |
0 |
0 |
| π΄ |
Relativistic Muon Velocity from Momentum and Energy |
10 |
897 |
387.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
relativistic-muon-velocity-from-momentum-and-energy.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Relativistic Proton in Interstellar Magnetic Field |
11 |
104 |
40.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
relativistic-proton-in-interstellar-magnetic-field.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Relativistic Proton in Magnetic Field |
12 |
1061 |
457.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
relativistic-proton-in-magnetic-field.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Relativistic spaceship travel time |
12 |
1201 |
477.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
relativistic-spaceship-travel-time.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Relativistic Velocity Addition and Ξ³ Factor |
10 |
861 |
373.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
relativistic-velocity-addition-and-factor.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Relativity: Ball Collision via Frame Simultaneity |
12 |
1241 |
513.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
relativity-ball-collision-via-frame-simultaneity.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Resistance, Voltage & Ohm's Law |
13 |
463 |
177.7s |
19 |
100.0% |
0 |
0 |
| π‘ |
Resistance & Resistivity (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Resistance & Resistivity |
11 |
462 |
107.0s |
20 |
100.0% |
0 |
0 |
| π‘ |
Resistor Networks β Parallel Combinations (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Resistor Networks |
12 |
641 |
127.5s |
23 |
100.0% |
0 |
0 |
| π‘ |
Resistor Networks β Series Circuits (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Resistor Networks |
11 |
598 |
121.0s |
25 |
100.0% |
0 |
0 |
| π‘ |
Vector Addition & Component Resolution (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Vector Addition & Component Resolution |
11 |
507 |
112.5s |
22 |
100.0% |
0 |
0 |
| π’ |
Resonance in Air Columns |
14 |
607 |
245.6s |
22 |
100.0% |
0 |
0 |
| π‘ |
Simple Harmonic Motion β Restoring Force Law (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Simple Harmonic Motion |
12 |
540 |
122.0s |
24 |
100.0% |
0 |
0 |
| π‘ |
Triangle Congruence β RHS (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Triangle Congruence |
12 |
600 |
112.5s |
23 |
100.0% |
0 |
0 |
| π‘ |
Rigid Body Dynamics (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Rigid Body Dynamics |
12 |
583 |
122.0s |
22 |
100.0% |
0 |
0 |
| π‘ |
Rigid Body Rotation (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Rigid Body Rotation |
11 |
574 |
111.5s |
21 |
100.0% |
0 |
0 |
| π’ |
RL Circuit Current Rise |
12 |
547 |
120.0s |
23 |
100.0% |
0 |
0 |
| π’ |
RLC Circuit Resonance |
11 |
547 |
114.0s |
22 |
100.0% |
0 |
0 |
| π΄ |
RMS Velocity & Mass in Brownian Motion |
11 |
976 |
387.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
rms-velocity-mass-in-brownian-motion.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Rocket Liftoff Condition & Thrust Analysis |
12 |
1027 |
431.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
rocket-liftoff-condition-thrust-analysis.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Rolling Friction β Common Forces in Mechanics (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Common Forces in Mechanics |
12 |
624 |
129.5s |
24 |
100.0% |
0 |
0 |
| π΄ |
Rolling vs. Sliding: Why Rotation Matters for Stopping Distance |
12 |
1166 |
474.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
rolling-vs-sliding-why-rotation-matters-for-stopping-distanc.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Orbit Shape from Energy and Angular Momentum |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Rotating Circle & Effective Gravity Analogy |
11 |
980 |
386.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
rotating-circle-effective-gravity-analogy.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Rotating Coil: Peak and RMS EMF |
10 |
909 |
371.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
rotating-coil-peak-and-rms-emf.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Rotating Frames: Centrifugal & Coriolis Forces |
15 |
652 |
263.2s |
23 |
100.0% |
0 |
0 |
| π΄ |
Rotating Rod on Strings: Torque and Energy Analysis |
11 |
1195 |
465.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
rotating-rod-on-strings-torque-and-energy-analysis.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Rotation Operator Identity: Exponential Form via Taylor Series |
12 |
1172 |
500.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
rotation-operator-identity-exponential-form-via-taylor-serie.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Rotational Dynamics & Torque |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Rotational Dynamics & Torque |
11 |
631 |
118.0s |
22 |
100.0% |
0 |
0 |
| π‘ |
Rotational Equilibrium of a Ladder |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Rotational Kinematics (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Rotational Kinematics |
12 |
607 |
125.0s |
27 |
100.0% |
0 |
0 |
| π‘ |
Rotational Kinematics (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Rotational Kinetic Energy of a Rolling Object |
12 |
664 |
127.0s |
25 |
100.0% |
2 |
0 |
| π‘ |
Atomic Structure β Rutherford Nuclear Model (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Atomic Structure |
10 |
492 |
106.0s |
19 |
100.0% |
0 |
0 |
| π΄ |
Sample Space & Basic Probability: Building the Foundation |
12 |
1153 |
367.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
sample-space-basic-probability-building-the-foundation.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Satellite Descent: From Circular to Elliptical Orbit |
12 |
1070 |
457.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
satellite-descent-from-circular-to-elliptical-orbit.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Satellite Orbit Eccentricity from Velocity Constraints |
11 |
1048 |
436.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
satellite-orbit-eccentricity-from-velocity-constraints.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Scalars, Vectors & Basic Definitions (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Scalars, Vectors & Basic Definitions |
10 |
484 |
191.9s |
20 |
100.0% |
0 |
0 |
| π΄ |
Scattering angle & differential cross section for soft repulsive potential |
12 |
1147 |
491.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
scattering-angle-differential-cross-section-for-soft-repulsi.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Scattering angle from repulsive potentials at high energy |
13 |
1301 |
556.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
scattering-angle-from-repulsive-potentials-at-high-energy.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Bead on a Rotating Hoop β Finding the Equilibrium Angle |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Scattering cross section for inverse-cube force |
11 |
1115 |
471.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
scattering-cross-section-for-inverse-cube-force.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Scattering cross section for repulsive central force |
12 |
1170 |
488.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
scattering-cross-section-for-repulsive-central-force.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
SchrΓΆdinger Equation: Hydrogen Atom |
14 |
572 |
244.1s |
21 |
100.0% |
0 |
0 |
| π‘ |
Why Particle-in-a-Box Energy Levels Are Quantized |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π |
Particle in a Box |
14 |
613 |
257.8s |
13 |
58.3% |
0 |
0 |
| π‘ |
The SchrΓΆdinger Equation (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The SchrΓΆdinger Equation |
13 |
705 |
142.0s |
25 |
100.0% |
0 |
0 |
| π’ |
Schwarzschild Radius & Black Holes |
14 |
514 |
198.6s |
22 |
100.0% |
0 |
0 |
| π‘ |
Second Law & Entropy (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Second Law & Entropy |
11 |
491 |
105.5s |
23 |
100.0% |
0 |
11 |
| π’ |
Second-Order Linear ODEs |
12 |
649 |
130.0s |
23 |
100.0% |
0 |
0 |
| π’ |
Second Quantization for Bosons |
12 |
587 |
120.5s |
24 |
100.0% |
0 |
0 |
| π‘ |
Selection Rules in Atomic Transitions (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Selection Rules in Atomic Transitions |
11 |
597 |
235.1s |
21 |
100.0% |
0 |
0 |
| π’ |
Self-Inductance of a Solenoid |
12 |
565 |
119.0s |
24 |
100.0% |
0 |
0 |
| π’ |
Semiconductor Doping |
11 |
584 |
120.0s |
22 |
100.0% |
0 |
0 |
| π‘ |
Semiconductors & Band Gaps (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Semiconductors & Band Gaps |
10 |
459 |
104.0s |
19 |
100.0% |
0 |
0 |
| π’ |
Series & Parallel Resistors |
14 |
608 |
254.3s |
23 |
100.0% |
0 |
0 |
| π΄ |
Shear Stress in Perfect Cubic Crystals |
11 |
1157 |
482.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
shear-stress-in-perfect-cubic-crystals.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Measurement Systems β SI Base Units (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Measurement Systems |
10 |
386 |
154.7s |
19 |
100.0% |
0 |
0 |
| π‘ |
Measurement Systems β SI Derived Units (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Measurement Systems |
10 |
386 |
154.7s |
19 |
100.0% |
0 |
0 |
| π‘ |
Precision & Reporting β Significant Figures (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Precision & Reporting |
10 |
542 |
221.3s |
19 |
100.0% |
0 |
0 |
| π΄ |
Simple Harmonic Motion: Oscillations Explained |
11 |
186 |
62.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
simple-harmonic-motion-oscillations-explained.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Simple Harmonic Motion: Period, Speed & Acceleration |
12 |
1181 |
515.2s |
0 |
0.0% |
0 |
0 |
| π΄ |
Simple Harmonic Motion: The Universal Oscillation |
11 |
1084 |
450.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
simple-harmonic-motion-the-universal-oscillation.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Simple Harmonic Motion (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Simple Harmonic Motion |
11 |
579 |
226.0s |
20 |
100.0% |
0 |
0 |
| π‘ |
The Simple Pendulum |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Simple Pendulum |
12 |
535 |
117.0s |
23 |
100.0% |
0 |
0 |
| π‘ |
Diffraction Gratings & Resolving Power (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Diffraction Gratings & Resolving Power |
14 |
675 |
300.0s |
25 |
100.0% |
0 |
0 |
| π΄ |
Sliding Bar on Rails: Electromagnetic Induction |
12 |
1185 |
486.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
sliding-bar-on-rails-electromagnetic-induction.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Bead on a Rotating Hoop β Finding Constants of Motion |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Sliding to Rolling: Friction and Angular Momentum |
12 |
1091 |
449.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
sliding-to-rolling-friction-and-angular-momentum.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
DistanceβTime Graphs (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
DistanceβTime Graphs |
11 |
460 |
183.9s |
23 |
100.0% |
1 |
0 |
| π΄ |
Small-angle pendulum: restoring force and potential energy |
11 |
980 |
395.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
small-angle-pendulum-restoring-force-and-potential-energy.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Small Oscillations (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Small Oscillations |
10 |
510 |
109.5s |
21 |
100.0% |
0 |
0 |
| π’ |
Snell's Law from Fermat's Principle |
15 |
718 |
294.6s |
24 |
100.0% |
0 |
0 |
| π΄ |
Sound Absorption by Small Spheres |
12 |
1218 |
519.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
sound-absorption-by-small-spheres.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Sound: Production & Nature (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Sound: Production & Nature |
10 |
515 |
101.5s |
23 |
100.0% |
0 |
0 |
| π’ |
Sound Intensity & Decibels |
14 |
583 |
227.3s |
20 |
100.0% |
0 |
0 |
| π‘ |
Sound Waves & Acoustics (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Sound Waves & Acoustics |
11 |
557 |
116.5s |
23 |
100.0% |
0 |
0 |
| π΄ |
Source near a wall: finding optimal placement |
11 |
273 |
102.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
source-near-a-wall-finding-optimal-placement.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Source Near a Wall: Maximum Velocity Design |
12 |
1223 |
495.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
source-near-a-wall-maximum-velocity-design.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Special Relativity: Time Dilation & Length Contraction |
14 |
655 |
338.8s |
29 |
100.0% |
0 |
0 |
| π’ |
Special Relativity: Time Dilation & Length Contraction |
15 |
813 |
342.8s |
25 |
100.0% |
0 |
0 |
| π΄ |
Special Relativity: Time & Space |
13 |
543 |
218.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
Specific Heat & Calorimetry (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Specific Heat & Calorimetry |
10 |
548 |
104.5s |
19 |
100.0% |
0 |
0 |
| π΄ |
Specific Heat Capacities of a Gas Mixture |
11 |
1010 |
435.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
specific-heat-capacities-of-a-gas-mixture.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Heat Capacity β Guide Me |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Heat Capacity |
10 |
485 |
105.0s |
20 |
100.0% |
0 |
0 |
| π΄ |
Spectral Term Designation with Quantum Numbers |
11 |
1085 |
434.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
spectral-term-designation-with-quantum-numbers.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Spectral Term Designations for n=3 in Hydrogen |
11 |
1161 |
485.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
spectral-term-designations-for-n-3-in-hydrogen.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Sound Wave Characteristics β Speed of Sound in Media (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Sound Wave Characteristics |
12 |
486 |
114.5s |
24 |
100.0% |
0 |
1 |
| π‘ |
Wave Speed on Stretched Strings (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Wave Speed |
10 |
458 |
100.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
Distance, Displacement, Speed & Velocity (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Distance, Displacement, Speed & Velocity |
10 |
526 |
206.5s |
19 |
100.0% |
0 |
0 |
| π΄ |
Spherical Harmonics: The Pure Tones of a Sphere |
11 |
1112 |
494.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
spherical-harmonics-the-pure-tones-of-a-sphere.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Spherical Harmonics: The Vibrations of a Sphere |
12 |
1204 |
490.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
spherical-harmonics-the-vibrations-of-a-sphere.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Gravitation & Weight β Spherical Mass Distributions (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Gravitation & Weight |
11 |
459 |
106.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Spin-Orbit Coupling (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Spin-Orbit Coupling |
11 |
536 |
215.7s |
21 |
100.0% |
0 |
0 |
| π’ |
Spin-Β½ & the Bloch Sphere |
13 |
616 |
244.1s |
19 |
100.0% |
0 |
0 |
| π΄ |
Spin-x Uncertainty & the |+xβ© Eigenstate |
12 |
1046 |
451.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
spin-x-uncertainty-the-x-eigenstate.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Spring Compression & Acceleration After Force Removal |
11 |
952 |
393.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
spring-compression-acceleration-after-force-removal.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Ballistic Pendulum: Finding Bullet Speed |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Spring Constant Change: Finding the New Oscillation |
11 |
1063 |
440.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
spring-constant-change-finding-the-new-oscillation.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Variable Forces & Graphical Methods (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Variable Forces & Graphical Methods |
10 |
543 |
104.5s |
19 |
100.0% |
0 |
0 |
| π‘ |
Common Forces in Mechanics β Spring Force (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Common Forces in Mechanics |
11 |
613 |
120.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
Spring Potential Energy (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Potential Energy |
10 |
445 |
99.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
Spinning Skater: Conservation of Angular Momentum |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Series RLC Circuit: Finding Resonant Frequency and Impedance |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Finite Square Well: Finding Bound State Energies |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Synchrotron Energy Gain per Revolution |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Angular Momentum of a Skewed Rotating Rod |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Finding COP of a Refrigerator Given Heat Flows |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Gravitational Time Dilation Near a Massive Body |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
WKB Bound States in a Symmetric Potential Well |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Angular Momentum of a Skewed Rotating Rod |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Elastic Collision: Finding Final Velocities |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Putting It All Together: A Synthesis Problem |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Latent Heat and the Clausius-Clapeyron Equation |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Two Coupled Pendulums: Finding Normal Modes |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Angular Momentum of a Skewed Rotating Rod |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
RLC Series Circuit: Finding Impedance and Phase Angle |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
RLC Series Circuit: Finding Impedance and Phase Angle |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Angular Momentum of a Skewed Rotating Rod |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Latent Heat and the Clausius-Clapeyron Equation |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Steady Pipe Flow: Forces on a Reducing Elbow |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Spinning Skater: Using Conservation of Angular Momentum |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Gas in a Piston: Finding Final Temperature |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
RLC Series Circuit: Finding Resonant Frequency and Impedance |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Rolling Cylinder on an Inclined Plane |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Why Hydrogen Sings at 21 Centimeters |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Action-Angle Variables: What They Are and Why They Work |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
What Makes Matter 'Active'? Self-Propulsion and Collective Motion |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Adiabatic Invariants: When Slow Change Preserves Something |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
How Adiabatic Quantum Computation Works |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
The ADM Split: Slicing Spacetime into Space + Time |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
AdS-CFT: How a Bulk Gravity Theory Encodes a Boundary QFT |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
AdS/CFT as a Tool for Strongly Coupled Matter |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
What RMS Really Means for AC Signals |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
The Anderson Impurity Model: A Magnetic Atom in a Metal |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
What Is Angular Momentum β and Why Does It Stay? |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Anomalies in QFT: When Symmetries Don't Survive Quantization |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
How a Half-Wave Dipole Radiates |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Antiferromagnetism: Opposing Spins, Zero Net Moment |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Entropy and Probability in Protein Folding |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
The Boltzmann Equation: How Systems Remember Where They've Been |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
The Bose-Einstein Distribution: How Bosons Share Energy Levels |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Chemical Potential: What It Really Means |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
The Clausius-Clapeyron Equation: Why Pressure Shifts Phase Boundaries |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Cluster Expansion: Building the Partition Function from Pair Interactions |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Critical Exponents and Why Universality is Surprising |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
The Real Number System β Standard Form & Scientific Notation (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Real Number System |
11 |
533 |
115.5s |
18 |
100.0% |
0 |
0 |
| π‘ |
Particle Physics β Exchange Particles (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Particle Physics |
10 |
452 |
104.5s |
21 |
100.0% |
0 |
0 |
| π’ |
The Standard Model of Particle Physics |
10 |
507 |
110.0s |
19 |
100.0% |
0 |
0 |
| π’ |
Standing Waves and Resonance |
11 |
566 |
113.0s |
19 |
100.0% |
0 |
0 |
| π’ |
Boundary Effects |
12 |
681 |
124.5s |
23 |
100.0% |
0 |
0 |
| π’ |
Standing Waves on a String |
14 |
582 |
235.1s |
22 |
100.0% |
0 |
0 |
| π‘ |
The Stark Effect |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Stark Effect |
11 |
617 |
247.2s |
22 |
100.0% |
0 |
0 |
| π‘ |
Archimedes' Principle |
11 |
468 |
110.5s |
20 |
100.0% |
2 |
0 |
| π’ |
Static Friction |
14 |
588 |
240.0s |
21 |
100.0% |
0 |
0 |
| π’ |
Statics and Equilibrium |
12 |
589 |
122.5s |
22 |
100.0% |
0 |
0 |
| π’ |
Stefan-Boltzmann Law |
14 |
624 |
256.0s |
21 |
100.0% |
0 |
0 |
| π’ |
Stellar Evolution |
12 |
649 |
127.0s |
23 |
100.0% |
0 |
0 |
| π’ |
Stern-Gerlach & Spin Quantization |
12 |
622 |
255.6s |
21 |
100.0% |
0 |
0 |
| π’ |
Stern-Gerlach & Spin Quantization |
14 |
637 |
262.6s |
21 |
100.0% |
0 |
0 |
| π’ |
Kinematic Equations for Uniform Acceleration |
12 |
573 |
125.0s |
24 |
100.0% |
0 |
0 |
| π΄ |
Stream Depth on an Inclined Plane |
11 |
1046 |
423.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
stream-depth-on-an-inclined-plane.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Fluid Dynamics |
12 |
586 |
123.0s |
26 |
100.0% |
0 |
0 |
| π’ |
Elasticity of Solids |
11 |
532 |
115.5s |
22 |
100.0% |
0 |
0 |
| π’ |
The Strong Force & Color Charge |
10 |
617 |
108.5s |
20 |
100.0% |
0 |
0 |
| π’ |
The Solar System |
11 |
596 |
117.0s |
22 |
100.0% |
0 |
0 |
| π’ |
Cartesian Coordinate System |
12 |
667 |
124.5s |
24 |
100.0% |
0 |
0 |
| π‘ |
Superconductivity & BCS Theory |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Superconductivity & BCS Theory |
14 |
529 |
228.5s |
0 |
0.0% |
0 |
0 |
| π’ |
Electric Force |
10 |
453 |
97.5s |
20 |
100.0% |
0 |
0 |
| π΄ |
Wave Superposition |
12 |
517 |
114.5s |
23 |
100.0% |
0 |
1 |
| π΄ |
Superposition & Separation of Variables |
11 |
1049 |
429.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
superposition-separation-of-variables.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Surface Tension from Merging Soap Bubbles |
12 |
1136 |
480.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
surface-tension-from-merging-soap-bubbles.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Symmetric collision with kinetic energy gain |
11 |
957 |
409.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
symmetric-collision-with-kinetic-energy-gain.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Taylor Series Expansion |
11 |
686 |
119.5s |
23 |
100.0% |
0 |
0 |
| π’ |
Temperature and Thermal Equilibrium |
11 |
537 |
116.5s |
21 |
100.0% |
0 |
0 |
| π’ |
Kinetic Theory of Gases |
12 |
610 |
117.0s |
23 |
100.0% |
0 |
0 |
| π΄ |
Temperature Scales: Kelvin vs. Celsius |
11 |
983 |
403.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
temperature-scales-kelvin-vs-celsius.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Common Forces in Mechanics |
12 |
558 |
122.0s |
23 |
100.0% |
0 |
0 |
| π΄ |
Terminal Velocity of a Falling Raindrop |
11 |
1087 |
450.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
terminal-velocity-of-a-falling-raindrop.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Terminal Velocity & Air Resistance |
11 |
509 |
114.0s |
22 |
100.0% |
0 |
0 |
| π’ |
Cells & EMF |
11 |
534 |
107.0s |
24 |
100.0% |
0 |
0 |
| π’ |
The Atwood Machine |
15 |
597 |
235.8s |
23 |
100.0% |
0 |
0 |
| π’ |
The Carnot Cycle & Heat Engine Efficiency |
16 |
815 |
360.4s |
28 |
100.0% |
0 |
0 |
| π‘ |
The Carnot Cycle & Heat Engine Efficiency |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Carnot Cycle & Heat Engine Efficiency |
14 |
801 |
353.8s |
28 |
100.0% |
0 |
0 |
| π‘ |
The Doppler Effect (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Doppler Effect |
13 |
560 |
235.3s |
19 |
100.0% |
0 |
0 |
| π’ |
The Electromagnetic Spectrum |
12 |
597 |
122.0s |
23 |
100.0% |
0 |
0 |
| π‘ |
The Equivalence Principle (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Equivalence Principle |
14 |
650 |
276.2s |
23 |
100.0% |
0 |
0 |
| π’ |
The Eye & Corrective Lenses |
15 |
702 |
275.3s |
24 |
100.0% |
0 |
0 |
| π‘ |
the-fermi-dirac-distribution.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
The Fermi Surface: Boundary of Filled States |
11 |
1046 |
414.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
the-fermi-surface-boundary-of-filled-states.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
The First Law of Thermodynamics |
10 |
595 |
112.0s |
20 |
100.0% |
2 |
0 |
| π’ |
The Greenhouse Effect |
13 |
549 |
236.9s |
21 |
100.0% |
0 |
0 |
| π’ |
The Hamilton-Jacobi Equation |
15 |
697 |
282.3s |
23 |
100.0% |
0 |
0 |
| π’ |
The Hydrogen Atom |
12 |
579 |
120.5s |
23 |
100.0% |
0 |
0 |
| π’ |
The Ideal Gas Law |
13 |
498 |
212.6s |
22 |
100.0% |
0 |
0 |
| π΄ |
The Munchausen Problem: Why You Can't Pull Yourself Up by Your Hair |
11 |
1104 |
420.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
the-munchausen-problem-why-you-can-t-pull-yourself-up-by-you.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The p-n Junction |
14 |
512 |
223.2s |
22 |
100.0% |
0 |
0 |
| π’ |
The Partition Function |
14 |
607 |
233.2s |
21 |
100.0% |
0 |
0 |
| π‘ |
The Photoelectric Effect (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
The Photoelectric Effect |
12 |
1170 |
490.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
the-photoelectric-effect.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The Photovoltaic Effect |
14 |
680 |
271.0s |
23 |
100.0% |
0 |
0 |
| π‘ |
The Quantum Harmonic Oscillator (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
The Quantum Harmonic Oscillator |
12 |
571 |
222.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
the-quantum-harmonic-oscillator.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
The SchrΓΆdinger Equation |
12 |
794 |
134.5s |
24 |
100.0% |
0 |
0 |
| π’ |
The Second Law of Thermodynamics |
11 |
593 |
112.0s |
21 |
100.0% |
0 |
0 |
| π’ |
Thermal Conductivity & Fourier's Law |
11 |
566 |
112.0s |
20 |
100.0% |
0 |
0 |
| π’ |
Thermal Equilibrium |
11 |
592 |
120.0s |
22 |
100.0% |
0 |
0 |
| π’ |
Thin-Film Interference: Soap Bubbles |
15 |
713 |
298.2s |
24 |
100.0% |
0 |
0 |
| π‘ |
Thin Lens Optics |
14 |
548 |
216.4s |
20 |
100.0% |
1 |
0 |
| π΄ |
Three-fragment explosion with momentum conservation |
10 |
892 |
402.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
three-fragment-explosion-with-momentum-conservation.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Thrust |
10 |
425 |
96.0s |
20 |
100.0% |
0 |
0 |
| π’ |
Tidal Forces & the Moon |
11 |
579 |
116.0s |
20 |
100.0% |
0 |
0 |
| π΄ |
Time-Dependent Force: Momentum & Displacement |
12 |
1143 |
477.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
time-dependent-force-momentum-displacement.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Time derivatives of vector expressions |
10 |
806 |
327.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
time-derivatives-of-vector-expressions.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Time Dilation and Particle Travel Distance |
11 |
1023 |
399.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
time-dilation-and-particle-travel-distance.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Time Dilation: What Clock B Measures in Carla's Frame |
11 |
1089 |
422.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
time-dilation-what-clock-b-measures-in-carla-s-frame.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Time evolution of ladder operator expectation values |
11 |
963 |
401.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
time-evolution-of-ladder-operator-expectation-values.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Topological Insulators β What Makes Them Special (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
topological-insulators.json |
PARSE ERROR: parse: Expecting ',' delimiter: line 136 column 47 (char 7078) |
| π’ |
Torque and Rotational Equilibrium |
13 |
470 |
181.0s |
20 |
100.0% |
0 |
0 |
| π‘ |
Total Internal Reflection (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π |
Transformers & AC Voltage |
14 |
673 |
284.6s |
26 |
100.0% |
4 |
0 |
| π΄ |
Transforming Planck's Formula: Angular Frequency to Frequency and Wavelength |
12 |
1172 |
479.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
transforming-planck-s-formula-angular-frequency-to-frequency.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Transition Probabilities & Wave Function Nodes |
12 |
1184 |
486.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
transition-probabilities-wave-function-nodes.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Transverse & Longitudinal Waves |
10 |
497 |
100.5s |
19 |
100.0% |
0 |
0 |
| π΄ |
Transverse Velocity of a Vibrating String |
10 |
1035 |
399.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
transverse-velocity-of-a-vibrating-string.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Truncated Coulomb Scattering: Angle & Cross Section |
11 |
1110 |
470.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
truncated-coulomb-scattering-angle-cross-section.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Twin Clock Paradox: Time Dilation in Relativity |
11 |
1053 |
436.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
twin-clock-paradox-time-dilation-in-relativity.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Two-body circular motion and centripetal force |
12 |
1059 |
417.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
two-body-circular-motion-and-centripetal-force.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
2D Collisions: Breaking Apart the Math |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
2D Collisions |
12 |
522 |
121.0s |
24 |
100.0% |
0 |
0 |
| π΄ |
Two-Body Kinetic Energy in Relative Coordinates |
12 |
1225 |
497.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
two-body-kinetic-energy-in-relative-coordinates.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Two-Particle Decay and Energy Conservation |
11 |
1061 |
432.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
two-particle-decay-and-energy-conservation.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Two Satellites Connected by a Tether in Circular Orbit |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Two Satellites Connected by Cable: Orbital Speed Comparison |
12 |
1055 |
459.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
two-satellites-connected-by-cable-orbital-speed-comparison.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Collisions & Momentum |
10 |
495 |
103.0s |
24 |
100.0% |
0 |
0 |
| π’ |
Spherical Mirrors |
10 |
579 |
107.0s |
19 |
100.0% |
0 |
0 |
| π΄ |
Quadrilaterals |
12 |
560 |
113.5s |
23 |
100.0% |
0 |
1 |
| π’ |
Thermodynamic Processes |
11 |
693 |
116.0s |
21 |
100.0% |
0 |
0 |
| π’ |
Free-Fall & Vertical Motion |
12 |
477 |
118.0s |
22 |
100.0% |
0 |
0 |
| π’ |
Gravitational Field & Acceleration |
11 |
594 |
114.0s |
22 |
100.0% |
0 |
0 |
| π‘ |
Projectile Launched from a Cliff |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Variational Method for Particle in Linear Potential |
11 |
1063 |
476.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
variational-method-for-particle-in-linear-potential.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Variational Method in Quantum Mechanics |
15 |
623 |
255.6s |
23 |
100.0% |
0 |
0 |
| π΄ |
Variational Method: Helium Atom |
11 |
531 |
120.5s |
0 |
0.0% |
0 |
0 |
| π’ |
Vector Cross Product & Area |
12 |
575 |
121.0s |
23 |
100.0% |
0 |
0 |
| π’ |
Vector Dot Product & Projection |
11 |
547 |
114.0s |
21 |
100.0% |
0 |
0 |
| π’ |
2D Motion with Constant Acceleration |
10 |
534 |
106.5s |
21 |
100.0% |
0 |
0 |
| π‘ |
Scalars, Vectors & Basic Definitions (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Scalars, Vectors & Basic Definitions |
10 |
484 |
191.9s |
20 |
100.0% |
0 |
0 |
| π΄ |
Vector Triple Product Identity via Component Proof |
12 |
1152 |
492.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
vector-triple-product-identity-via-component-proof.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Velocity Exchange in Collisions: Mass Ratio & Elasticity |
12 |
1073 |
462.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
velocity-exchange-in-collisions-mass-ratio-elasticity.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
SHM Kinematics |
12 |
531 |
119.5s |
22 |
100.0% |
0 |
0 |
| π‘ |
Electron Velocity in Crossed E and B Fields |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Velocity Selector: E and B Fields in Balance |
10 |
938 |
367.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
velocity-selector-e-and-b-fields-in-balance.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Measuring Instruments β Vernier Calipers & Screw Gauge (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Measuring Instruments |
11 |
499 |
195.4s |
20 |
100.0% |
0 |
0 |
| π’ |
Vertical Circular Motion: Top of the Loop |
12 |
564 |
115.0s |
21 |
100.0% |
0 |
0 |
| π΄ |
Vibrating Water Drop: Dimensional Analysis |
11 |
1062 |
437.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
vibrating-water-drop-dimensional-analysis.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Viscosity & Stokes' Drag |
11 |
508 |
113.0s |
21 |
100.0% |
0 |
0 |
| π΄ |
Viscosity of Liquid in Capillary Flow |
12 |
1129 |
448.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
viscosity-of-liquid-in-capillary-flow.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Viscous Drainage from a Tube |
11 |
1095 |
458.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
viscous-drainage-from-a-tube.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Water Discharge Over a Dam: How Height Affects Flow |
12 |
1105 |
440.0s |
0 |
0.0% |
0 |
0 |
| π‘ |
water-discharge-over-a-dam-how-height-affects-flow.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Water Pressure in a Charged Capacitor Gap |
11 |
988 |
414.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
water-pressure-in-a-charged-capacitor-gap.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Water Rising in a Cone: Deriving h(t) |
13 |
1202 |
499.5s |
0 |
0.0% |
0 |
0 |
| π‘ |
water-rising-in-a-cone-deriving-h-t.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Wave Equation from Maxwell's Equations |
15 |
586 |
243.6s |
24 |
100.0% |
0 |
0 |
| π΄ |
Wave Functions and Probability in Quantum Mechanics |
12 |
1230 |
383.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
wave-functions-and-probability-in-quantum-mechanics.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Wave Interference & Superposition |
14 |
624 |
260.8s |
21 |
100.0% |
0 |
0 |
| π’ |
Wave Optics |
11 |
559 |
114.5s |
22 |
100.0% |
0 |
0 |
| π’ |
Wave Properties |
11 |
516 |
116.5s |
21 |
100.0% |
0 |
0 |
| π΄ |
Wave Properties: Doppler, Diffraction, Coherence & Interference |
11 |
1001 |
447.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
wave-properties-doppler-diffraction-coherence-interference.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Wave speed on a seismic detection wire |
11 |
985 |
423.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
wave-speed-on-a-seismic-detection-wire.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Wave Speed |
11 |
467 |
113.5s |
20 |
100.0% |
0 |
1 |
| π’ |
Waves and Wave Mechanics |
10 |
581 |
111.0s |
21 |
100.0% |
0 |
0 |
| π΄ |
Waves on a Two-Segment String |
12 |
1090 |
446.2s |
0 |
0.0% |
0 |
0 |
| π‘ |
waves-on-a-two-segment-string.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Weak Energy Condition for Perfect Fluids |
11 |
1026 |
447.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
weak-energy-condition-for-perfect-fluids.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Weak Force & Beta Decay |
10 |
434 |
98.0s |
19 |
100.0% |
0 |
0 |
| π‘ |
Gravitation & Weight |
10 |
466 |
103.5s |
19 |
100.0% |
1 |
0 |
| π΄ |
Mass, Weight & Apparent Weight |
11 |
559 |
118.5s |
22 |
100.0% |
0 |
1 |
| π‘ |
Orbital Speed from Gravitational Force |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Weyl Tensor Bianchi Identity for n β₯ 4 |
11 |
986 |
390.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
weyl-tensor-bianchi-identity-for-n-4.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
When Does Internal Energy Stay Constant? |
11 |
983 |
423.3s |
0 |
0.0% |
0 |
0 |
| π‘ |
when-does-internal-energy-stay-constant.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Why Total Current Determines Mass in Electrolysis |
12 |
1177 |
494.8s |
0 |
0.0% |
0 |
0 |
| π‘ |
why-total-current-determines-mass-in-electrolysis.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Wien's Displacement Law |
13 |
525 |
220.0s |
21 |
100.0% |
0 |
0 |
| π‘ |
WKB Approximation (Guide Me) |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
wkb-approximation.json |
PARSE ERROR: parse: Expecting ',' delimiter: line 126 column 107 (char 6457) |
| π’ |
Energy Losses & Efficiency |
10 |
461 |
99.0s |
18 |
100.0% |
0 |
0 |
| π‘ |
Irodov 1.213: Gyroscopic Precession of a Spinning Top |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Work Against Gravity: Particle from Hemisphere to Infinity |
12 |
1185 |
508.1s |
0 |
0.0% |
0 |
0 |
| π‘ |
work-against-gravity-particle-from-hemisphere-to-infinity.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Work and Kinetic Energy |
11 |
485 |
110.0s |
21 |
100.0% |
0 |
0 |
| π’ |
Work: Fundamental Definition |
11 |
500 |
111.5s |
21 |
100.0% |
0 |
0 |
| π’ |
Work by Constant Forces |
10 |
530 |
104.0s |
22 |
100.0% |
0 |
0 |
| π΄ |
Work by Constant Forces |
10 |
500 |
96.5s |
19 |
100.0% |
0 |
10 |
| π΄ |
Variable Forces & Graphical Methods |
12 |
547 |
126.5s |
22 |
100.0% |
0 |
2 |
| π΄ |
Work Done by Gas: Isothermal vs Isobaric Expansion |
12 |
1145 |
473.9s |
0 |
0.0% |
0 |
0 |
| π‘ |
work-done-by-gas-isothermal-vs-isobaric-expansion.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Kinetic Energy |
11 |
524 |
114.5s |
24 |
100.0% |
0 |
0 |
| π΄ |
Work in isothermal expansion of Van der Waals gas |
11 |
1030 |
415.7s |
0 |
0.0% |
0 |
0 |
| π‘ |
work-in-isothermal-expansion-of-van-der-waals-gas.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Osmotic Pressure from van't Hoff Law |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π΄ |
Work to Blow a Soap Bubble: Surface Tension and Pressure |
12 |
1200 |
454.6s |
0 |
0.0% |
0 |
0 |
| π‘ |
work-to-blow-a-soap-bubble-surface-tension-and-pressure.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π‘ |
Young's Double-Slit Experiment |
11 |
568 |
120.5s |
21 |
100.0% |
1 |
0 |
| π’ |
Elastic Constants |
11 |
497 |
115.5s |
21 |
100.0% |
0 |
0 |
| π’ |
The Zeeman Effect |
10 |
470 |
208.1s |
20 |
100.0% |
0 |
0 |
| π΄ |
Zero-Point Energy of Copper from Debye Model |
11 |
880 |
388.4s |
0 |
0.0% |
0 |
0 |
| π‘ |
zero-point-energy-of-copper-from-debye-model.source |
0 |
0 |
0.0s |
0 |
β |
0 |
0 |
| π’ |
Polynomials |
10 |
462 |
97.0s |
19 |
100.0% |
0 |
0 |
| π’ |
Thermal Equilibrium |
11 |
557 |
112.5s |
21 |
100.0% |
0 |
0 |