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How does the impulse of a force change the momentum of an object?

Relate impulse to the change in momentum of an object using J=FΔt=Δp\vec{J} = \vec{F}\Delta t = \Delta \vec{p}, and interpret force-time graphs.

Defining momentum and impulse, the impulse-momentum theorem, reading impulse from a force-time graph, and how impulse explains safety features.

Generated by Claude Opus 4.77 min answer

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  1. What this dot point is asking
  2. Momentum
  3. Impulse and the impulse-momentum theorem
  4. Force-time graphs
  5. Why safety features work

What this dot point is asking

You need to define momentum and impulse, state and apply the impulse-momentum theorem, find impulse as the area under a force-time graph, and use these ideas to explain safety features such as crumple zones and airbags.

Momentum

Because momentum is a vector, direction matters. A ball bouncing back reverses its momentum, so its change in momentum is larger than if it simply stopped.

Impulse and the impulse-momentum theorem

Newton's second law can be written in terms of momentum: the net force equals the rate of change of momentum,

Fnet=ΔpΔt.\vec{F}_{\text{net}} = \frac{\Delta\vec{p}}{\Delta t}.

Rearranging gives the impulse-momentum theorem:
J=FnetΔt=Δp=mvmu.\vec{J} = \vec{F}_{\text{net}}\,\Delta t = \Delta\vec{p} = m\vec{v} - m\vec{u}.

Impulse and momentum change have the same units, N s = kg m s1^{-1}. The key insight is the trade-off between force and time: for a fixed change in momentum, increasing the contact time decreases the average force.

Force-time graphs

When a force varies during a collision, the impulse is the area under the force-time graph:

J=Fdt=area under the F-t graph.J = \int F\,dt = \text{area under the } F\text{-}t \text{ graph}.

For a triangular force pulse, the area is 12(base)(height)\tfrac{1}{2}(\text{base})(\text{height}). The average force is the constant force that would give the same area (same impulse) over the same time.

Why safety features work

Crumple zones, airbags, helmet padding and crash mats all work the same way. In a collision the change in momentum (the impulse) is essentially fixed - the occupant must be brought to rest. By extending the contact time Δt\Delta t, these devices reduce the average force F=Δp/ΔtF = \Delta p / \Delta t on the body. A longer, gentler deceleration replaces a short, violent one, reducing injury.

The same principle explains why a cricketer "gives" with the ball when catching, and why falling onto a soft surface hurts less than onto concrete.

Exam-style practice questions

Practice questions written in the style of SACE Board exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

2025 SACE Stage 23 marksA stationary object explodes into three pieces: A, B, and C. The momentum vectors of pieces A and B immediately after the explosion are shown on a diagram. Use the law of conservation of momentum to determine the momentum vector of piece C immediately after the explosion.
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Before the explosion the object is stationary, so the total momentum of the system is zero.

Momentum is conserved, so the vector sum of the momenta of the three pieces after the explosion must also be zero: pA + pB + pC = 0.

Therefore pC = -(pA + pB). Add the vectors pA and pB tip-to-tail to find their resultant, then pC is a vector of equal magnitude pointing in exactly the opposite direction to that resultant.

1 mark for stating total momentum before and after is zero, 1 mark for pC = -(pA + pB), 1 mark for drawing pC with the correct magnitude and opposite direction.

2023 SACE Stage 24 marksA photon of wavelength 508 nm is incident on a solar sail at 30.0 degrees from the surface and is reflected at 30.0 degrees. The magnitude of the initial momentum of the photon is 1.31 x 10^-27 kg m s-1. Use a vector diagram to determine the magnitude and direction of the change in momentum of this photon.
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Photon momentum p = h / wavelength. Both the incident and reflected photons have the same magnitude, p = 1.31 x 10^-27 kg m s-1.

The photon strikes at 30.0 degrees to the surface, so it is 60.0 degrees from the normal. By symmetry the component of momentum parallel to the sail surface is unchanged, while the component perpendicular to the surface reverses.

The perpendicular component of each photon is p sin 30.0 = 1.31 x 10^-27 x 0.500 = 6.55 x 10^-28. The change in momentum is twice this: delta p = 2 p sin 30.0 = 2 x 6.55 x 10^-28 = 1.31 x 10^-27 kg m s-1.

The change in momentum is directed perpendicular to the sail surface, away from the sail (into the sail's normal direction). 1 mark for the vector diagram, 1 mark for using only the perpendicular component, 1 mark for the magnitude, 1 mark for the direction.