Translate a force-time pulse into momentum change
For fixed mass, Newton’s second law can be written Fnet=Δp/Δt over an interval when Fnet is interpreted as the interval-average force. Multiplying gives impulse J=FavgΔt=Δp. For a varying force, impulse is the signed area under its force–time graph. The vector direction of impulse determines the direction of momentum change, not necessarily final velocity. Conversely, on a momentum-versus-time graph the interval slope Δp/Δt gives average net force; the local slope gives instantaneous net force. A rising, falling or horizontal momentum segment therefore indicates positive, negative or zero net force along the chosen axis, not necessarily positive, negative or zero momentum.
Learning outcome: Compare(8 N,0.5 s) with(4 N,1 s), then reverse the pulse sign. Calculate area, average force and final momentum before checking. Distinguish a zero final velocity from a zero force throughout the event. Sketch a momentum-time line rising from−2 to+2 kg m/s over2 s, then staying flat: the first segment has average net force+2 N and the flat segment zero, even though momentum remains+2 kg m/s.
Starting recap
Review signed velocity components, force-time areas, kinetic energy and system boundaries. Keep momentum vectors distinct from scalar energy.
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For a triangular+8 N pulse lasting 0.5 s, impulse is½×8×0.5=2 N s. The 2 kg object begins with momentum 2 kg m/s, ends with 4 kg m/s and therefore has final velocity 2 m/s. Reversing the peak to−8 N gives impulse−2 N s and brings it to rest.
Open the experimentPredict
If peak force doubles while duration halves, what happens to impulse and the final velocity in the same-mass case?
Experiment
Compare(8 N,0.5 s) with(4 N,1 s), then reverse the pulse sign. Calculate area, average force and final momentum before checking. Distinguish a zero final velocity from a zero force throughout the event. Sketch a momentum-time line rising from−2 to+2 kg m/s over2 s, then staying flat: the first segment has average net force+2 N and the flat segment zero, even though momentum remains+2 kg m/s.
Read a triangular force pulse
Worked teaching model · synthetic values · Net force rises linearly from zero to the selected peak halfway through the interval, then returns linearly to zero. A 2 kg object starts at +1 m/s. The pulse is prescribed in time; no contact material or injury response is modeled.
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| Quantity | Value | Unit |
|---|---|---|
| Signed impulse | 2 | N s |
| Average net force | 4 | N |
| Momentum change | 2 | kg m/s |
| Initial momentum | 2 | kg m/s |
| Final velocity | 2 | m/s |
Accessible plot coordinates
| time (s) | net force (N) |
|---|---|
| 0 | 0 |
| 0.25 | 8 |
| 0.5 | 0 |
The signed force-time area gives momentum change, not work.
For this triangular pulse J=½FpeakΔt. The average force is half the peak. Contact duration alone cannot determine peak force without a pulse shape or measurements.
The signed force-time area gives momentum change, not work.
For this triangular pulse J=½FpeakΔt. The average force is half the peak. Contact duration alone cannot determine peak force without a pulse shape or measurements.
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How would a rectangular pulse with the same peak and duration differ from the triangular pulse? Which measurement would be needed to distinguish them?
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