1.8 Relativistic Mechanics
Irodov Problems 1.340 to 1.388.
- 49problems
- 110figures
- Difficulty2.7avgDifficulty: 2 rated 1, 20 rated 2, 20 rated 3, 7 rated 4, 0 rated 5; mean 2.7.
- Uniqueness3.1avgUniqueness: 2 rated 1, 9 rated 2, 20 rated 3, 17 rated 4, 1 rated 5; mean 3.1.
| No. | Title | Difficulty | Uniqueness | Methods |
|---|---|---|---|---|
| 1.340 | Small Contraction, Not Small Speed | length contraction · approximation expansion · limiting cases | ||
| 1.341 | Each Side Shrinks by Its Angle | length contraction · vector decomposition · limiting cases | ||
| 1.342 | Only One Leg of the Rod Shrinks | length contraction · vector decomposition · lorentz transformation | ||
| 1.343 | Only the Height Is Contracted | length contraction · vector decomposition · limiting cases | ||
| 1.344 | How Fast to Lose Two Percent | time dilation · frames of reference · limiting cases | ||
| 1.345 | Two Timings Fix One Proper Length | length contraction · time dilation · frames of reference | ||
| 1.346 | The Lifetime Ratio Is Gamma | time dilation · invariant interval · frames of reference | ||
| 1.347 | The Muon Sees a Shorter Distance | time dilation · length contraction · frames of reference | ||
| 1.348 | One Clock Times a Contracted Gap | length contraction · time dilation · frames of reference | ||
| 1.349 | Two Simultaneities, Two Lengths, One Rod | length contraction · lorentz transformation · frames of reference | ||
| 1.350 | Two Rods, One Clock, One Gap | length contraction · relative motion · frames of reference | ||
| 1.351 | Simultaneous for Them, Not for Us | lorentz transformation · length contraction · frames of reference | ||
| 1.352 | Two Marks Made at Two Different Times | length contraction · frames of reference · lorentz transformation | ||
| 1.353 | Each Rod Sees the Other Lag | time dilation · length contraction · lorentz transformation · frames of reference | ||
| 1.354 | Same Moment, Two Different Answers | lorentz transformation · frames of reference · length contraction | ||
| 1.355 | The Point Where Both Clocks Agree | lorentz transformation · frames of reference · limiting cases | ||
| 1.356 | No Boost Outruns a Cause | lorentz transformation · frames of reference · invariant interval | ||
| 1.357 | The Interval Answers Both Questions | invariant interval · lorentz transformation · frames of reference | ||
| 1.358 | The Transverse Component Changes Too | lorentz transformation · frames of reference · vector decomposition | ||
| 1.359 | The Gap Closes Faster Than Anything Moves | relative motion · frames of reference · lorentz transformation | ||
| 1.360 | Compose the Speeds, Then Contract | length contraction · lorentz transformation · relative motion | ||
| 1.361 | Pythagoras Loses a Relativistic Term | lorentz transformation · relative motion · vector decomposition | ||
| 1.362 | Two Gammas Multiply Across the Boost | lorentz transformation · time dilation · frames of reference | ||
| 1.363 | The Angle a Boost Bends | lorentz transformation · frames of reference · vector decomposition · relative motion | ||
| 1.364 | A Rod Tilted by Disagreeing Clocks | lorentz transformation · length contraction · frames of reference | ||
| 1.365 | The Clock Transforms Too | lorentz transformation · frames of reference · calculus of motion | ||
| 1.366 | A Year at Ten Gravities | relativistic dynamics · differential equation · frames of reference · approximation expansion | ||
| 1.367 | The Crew Ages Only Logarithmically | time dilation · relativistic dynamics · calculus of motion | ||
| 1.368 | Inertia from the Square Root's Edge | relativistic dynamics · approximation expansion | ||
| 1.369 | Rest Mass over a Shrinking Box | length contraction · relativistic dynamics | ||
| 1.370 | Half a Percent Short of Light | relativistic dynamics · invariant interval · approximation expansion | ||
| 1.371 | The Excess Factor Is Just Gamma | relativistic dynamics · limiting cases | ||
| 1.372 | The Same Two Tenths of c Cost Three Times More | work energy · relativistic dynamics · approximation expansion | ||
| 1.373 | Where Motion Doubles a Particle's Energy | relativistic dynamics · limiting cases | ||
| 1.374 | How Slow Is Slow Enough | relativistic dynamics · approximation expansion · limiting cases | ||
| 1.375 | Momentum from Kinetic Energy Alone | relativistic dynamics · invariant interval · limiting cases | ||
| 1.376 | Momentum and Energy per Unit Time | momentum flux · relativistic dynamics · limiting cases | ||
| 1.377 | Both Frames Agree on the Pressure | momentum flux · length contraction · frames of reference · relativistic dynamics | ||
| 1.378 | Momentum Grows Forever, Speed Saturates | relativistic dynamics · impulse · calculus of motion · limiting cases | ||
| 1.379 | Hyperbolic Motion Hides a Constant Force | relativistic dynamics · calculus of motion · limiting cases | ||
| 1.380 | Two Inertias, One Rest Mass | relativistic dynamics · vector decomposition · limiting cases | ||
| 1.381 | Energy and Momentum Are One Vector | lorentz transformation · four vectors · relativistic dynamics · invariant interval | ||
| 1.382 | Chasing a Photon Lowers Its Energy | lorentz transformation · relativistic doppler · four vectors | ||
| 1.383 | Every Frame Agrees on Rest Mass | relativistic dynamics · invariant interval · four vectors | ||
| 1.384 | The Frame Where Momentum Vanishes | relativistic dynamics · invariant interval · frames of reference · collisions | ||
| 1.385 | Sticking Together Creates New Rest Mass | relativistic dynamics · four vectors · collisions · momentum conservation | ||
| 1.386 | The Price of a Stationary Target | relativistic dynamics · invariant interval · frames of reference · collisions | ||
| 1.387 | When the Other Two Move Together | relativistic dynamics · invariant interval · optimization · momentum conservation | ||
| 1.388 | The Rocket Adds Rapidity Not Speed | variable mass · relativistic dynamics · lorentz transformation · differential equation |
