Derive center and relative energy for an internal release
Explain how translational kinetic energy can increase without an external momentum impulse.
Learning outcome: Compare w=0,3,5 at V=2, then reverse V. Reconstruct both fragment velocities and the center-frame momenta, retain the internal-energy decrease and explain why the event is not an isolated creation of energy.
Starting recap
Integrate net external force, preserve vector and system boundaries, and test collision and evidence assumptions independently.
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Try
V=2,w=3 gives total P 10 kg m/s, center K 10 J and relative K 5.4 J, for total 15.4 J. The increase 5.4 J must come from the stated internal store.
Open the experimentPredict
Can translational kinetic energy increase while total momentum stays fixed?
Experiment
Compare w=0,3,5 at V=2, then reverse V. Reconstruct both fragment velocities and the center-frame momenta, retain the internal-energy decrease and explain why the event is not an isolated creation of energy.
Partition center and relative kinetic energy
Worked teaching model · synthetic values · Virtual two-fragment internal-energy release with masses2 and3 kg and no external impulse. Final v1−v2=w, center velocity fixed. No explosive materials, construction or physical release is requested. Extra translational energy comes from an unspecified internal store.
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Relative energy versus separation speed
Axes rescale independently. Curves join sampled coordinates; a joining segment is not additional measured evidence. Read physical units rather than screen angles or apparent slopes.
Relative energy versus separation speed: numerical coordinates
| relative speed (m/s) | energy (J) |
|---|---|
| 0 | 0 |
| 0.125 | 0.009375 |
| 0.25 | 0.0375 |
| 0.375 | 0.084375 |
| 0.5 | 0.15 |
| 0.625 | 0.234375 |
| 0.75 | 0.3375 |
| 0.875 | 0.459375 |
| 1 | 0.6 |
| 1.125 | 0.759375 |
| 1.25 | 0.9375 |
| 1.375 | 1.13437 |
| 1.5 | 1.35 |
| 1.625 | 1.58437 |
| 1.75 | 1.8375 |
| 1.875 | 2.10938 |
| 2 | 2.4 |
| 2.125 | 2.70937 |
| 2.25 | 3.0375 |
| 2.375 | 3.38437 |
| 2.5 | 3.75 |
| 2.625 | 4.13437 |
| 2.75 | 4.5375 |
| 2.875 | 4.95937 |
| 3 | 5.4 |
| 3.125 | 5.85938 |
| 3.25 | 6.3375 |
| 3.375 | 6.83437 |
| 3.5 | 7.35 |
| 3.625 | 7.88437 |
| 3.75 | 8.4375 |
| 3.875 | 9.00937 |
| 4 | 9.6 |
| 4.125 | 10.2094 |
| 4.25 | 10.8375 |
| 4.375 | 11.4844 |
| 4.5 | 12.15 |
| 4.625 | 12.8344 |
| 4.75 | 13.5375 |
| 4.875 | 14.2594 |
| 5 | 15 |
| Quantity | Value | Unit |
|---|---|---|
| First fragment velocity | 3.8 | m/s |
| Second fragment velocity | 0.8 | m/s |
| Conserved momentum | 10 | kg m/s |
| Center kinetic energy | 10 | J |
| Relative kinetic energy | 5.4 | J |
| Total final kinetic energy | 15.4 | J |
| Internal store energy converted | 5.4 | J |
An internal energy conversion can change translational kinetic energy while conserving momentum.
For masses2 and3, reduced mass is6/5 kg and relative K is one-half reduced mass times w². The center contribution is the minimum K at fixed total momentum. The energy source is explicitly an unspecified internal store; there is no real release or explosive procedure.
Derive before checking. Retain contrasting captures and explain one assumption that could fail; calculated evidence is not actual laboratory work.
An internal energy conversion can change translational kinetic energy while conserving momentum.
For masses2 and3, reduced mass is6/5 kg and relative K is one-half reduced mass times w². The center contribution is the minimum K at fixed total momentum. The energy source is explicitly an unspecified internal store; there is no real release or explosive procedure.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
Understand
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Public practice checks a specific claim. It does not establish independent mastery.
Why can both fragments move in the same laboratory direction while separating from each other?
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