Track an internal energy release in two frames
Two points of masses 1 and 3 kg initially move together at ground velocity U. An internal store separates them with relative final speed u=v1−v2, with no external impulse. Their total momentum remains 4U even though their kinetic energy can increase. The energy source is the internal store, not a violation of momentum conservation.
Learning outcome: Hold relative speed fixed and change U. Compare ground and center-frame velocities, momenta and kinetic energies. Then double u and predict the energy-source requirement before checking.
Starting recap
Choose the system, interval and reference frame before using a conservation statement. Keep vector momentum, scalar energy and transferred power distinct.
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At U=0 and u=4 m/s, the final velocities are3 and−1 m/s. Their momenta cancel, while kinetic energy is 6 J. At U=2 the same relative release instead gives 5 and 1 m/s, adding the same6 J to the initial ground kinetic energy.
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With negligible external impulse, an internal release can:
Experiment
Hold relative speed fixed and change U. Compare ground and center-frame velocities, momenta and kinetic energies. Then double u and predict the energy-source requirement before checking.
Compare internal release in two inertial frames
Worked teaching model · synthetic values · Two virtual points of masses 1 and 3 kg initially share selected velocity. An internal store releases them with v1−v2 equal to selected nonnegative speed, no external impulse. Endpoint stored-energy loss supplies kinetic increase; no explosive or physical release procedure.
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Internal energy required for relative separation
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: reduced-mass energy (solid). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Internal energy required for relative separation
reduced-mass energy
| relative separation speed (m/s) | kinetic energy increase (J) |
|---|---|
| 0 | 0 |
| 0.1 | 0.00375 |
| 0.2 | 0.015 |
| 0.3 | 0.03375 |
| 0.4 | 0.06 |
| 0.5 | 0.09375 |
| 0.6 | 0.135 |
| 0.7 | 0.18375 |
| 0.8 | 0.24 |
| 0.9 | 0.30375 |
| 1 | 0.375 |
| 1.1 | 0.45375 |
| 1.2 | 0.54 |
| 1.3 | 0.63375 |
| 1.4 | 0.735 |
| 1.5 | 0.84375 |
| 1.6 | 0.96 |
| 1.7 | 1.08375 |
| 1.8 | 1.215 |
| 1.9 | 1.35375 |
| 2 | 1.5 |
| 2.1 | 1.65375 |
| 2.2 | 1.815 |
| 2.3 | 1.98375 |
| 2.4 | 2.16 |
| 2.5 | 2.34375 |
| 2.6 | 2.535 |
| 2.7 | 2.73375 |
| 2.8 | 2.94 |
| 2.9 | 3.15375 |
| 3 | 3.375 |
| 3.1 | 3.60375 |
| 3.2 | 3.84 |
| 3.3 | 4.08375 |
| 3.4 | 4.335 |
| 3.5 | 4.59375 |
| 3.6 | 4.86 |
| 3.7 | 5.13375 |
| 3.8 | 5.415 |
| 3.9 | 5.70375 |
| 4 | 6 |
At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.
| Quantity | Value | Unit |
|---|---|---|
| First final ground velocity | 2.5 | m/s |
| Second final ground velocity | 0.5 | m/s |
| Initial total momentum | 4 | kg m/s |
| Final total momentum | 4 | kg m/s |
| Initial ground kinetic energy | 2 | J |
| Final ground kinetic energy | 3.5 | J |
| Internal stored-energy decrease | 1.5 | J |
| Final center-of-mass-frame kinetic energy | 1.5 | J |
Internal energy can become kinetic energy without changing the total momentum.
Momentum and the specified relative speed give v1=U+3u/4 and v2=U−u/4. Subtracting the center-frame speed U leaves opposite component momenta but positive relative kinetic energy 3u²/8. The kinetic-energy increase is the same in these uniformly shifted frames because total momentum is unchanged. The supplied release speed needs an internal energy source; it is not free acceleration.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
Internal energy can become kinetic energy without changing the total momentum.
Momentum and the specified relative speed give v1=U+3u/4 and v2=U−u/4. Subtracting the center-frame speed U leaves opposite component momenta but positive relative kinetic energy 3u²/8. The kinetic-energy increase is the same in these uniformly shifted frames because total momentum is unchanged. The supplied release speed needs an internal energy source; it is not free acceleration.
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Why is the kinetic-energy increase invariant here even though kinetic energy itself depends on frame?
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