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IB DP Physics Impulse and force-time graphs Study Notes

IB DP Physics Impulse and force-time graphs Study Notes - 2025 Syllabus

IB DP Physics Impulse and force-time graphs Study Notes

IB DP Physics Impulse and force-time graphs Study Notes at  IITian Academy  focus on  specific topic and type of questions asked in actual exam. Study Notes focus on IB Physics syllabus with guiding questions of

  • that a resultant external force applied to a system constitutes an impulse J as given by J = FΔt where F is the average resultant force and Δt is the time of contact
  • that the applied external impulse equals the change in momentum of the system

Standard level and higher level: 10  hours
Additional higher level: There is no additional higher level content

IB DP Physics 2025 -Study Notes -All Topics

Impulse and Change in Momentum

 A resultant external force applied to a system constitutes an impulse \( J \) as given by:

\( J = F \Delta t \)

  • Impulse is the product of the average resultant external force \( F \) and the time duration \( \Delta t \) the force acts.
  • It is a vector quantity and has the same direction as the force applied.
  • The SI unit of impulse is newton-second (N·s) or equivalently kg·m/s.
  • Impulse is not a “thing” but an action that alters momentum – it’s how a force causes a momentum change over time.

Example:

A tennis ball of mass \( 0.06 \, \text{kg} \) is initially at rest. It is struck by a racket with an average force of \( 40 \, \text{N} \) for a contact time of \( 0.02 \, \text{s} \). What is the impulse imparted and the final speed of the ball?

▶️Answer/Explanation

Use impulse formula

\( J = F \Delta t = 40 \times 0.02 = \boxed{0.8 \, \text{N·s}} \)

 Use impulse-momentum theorem

\( J = \Delta p = m v – m u \Rightarrow v = \frac{J}{m} = \frac{0.8}{0.06} = \boxed{13.33 \, \text{m/s}} \)

 The applied external impulse equals the change in momentum of the system:

\( J = \Delta p = m v – m u \)

  • This is known as the impulse-momentum theorem.
  • It says that impulse causes a change in momentum.
  • If no external force acts (\( F = 0 \)), then \( \Delta p = 0 \) ⇒ momentum is conserved.
  • Applicable to any motion: linear, recoil, stopping a vehicle, kicking a ball, rocket propulsion, etc.

Example: 

A truck of mass \( 2000 \, \text{kg} \) is moving at \( 15 \, \text{m/s} \) and brakes to a stop in \( 5 \, \text{s} \). Find the impulse and average braking force.

▶️Answer/Explanation

Change in momentum

\( \Delta p = m (v – u) = 2000(0 – 15) = -30,000 \, \text{kg·m/s} \)

 Impulse equals change in momentum

\( J = \Delta p = -30,000 \, \text{N·s} \)

 Use \( J = F \Delta t \) to find force

\( F = \frac{J}{\Delta t} = \frac{-30,000}{5} = \boxed{-6000 \, \text{N}} \) (Negative sign: force opposes motion)

Example: 

A force is applied to a cart for 4 seconds, and the graph of the force versus time is shown below.

If the maximum force is \( F_{\text{max}} = 20 \, \text{N} \) and it increases linearly from 0 to 20 N in 4 s, find the impulse delivered to the cart.

▶️Answer/Explanation

This is a triangular force–time graph, so the impulse is the area under the curve.

Use area of triangle:

\( \text{Impulse} = \text{Area} = \frac{1}{2} \times \text{base} \times \text{height} = \frac{1}{2} \times 4 \, \text{s} \times 20 \, \text{N} \)

\( \Rightarrow J = \boxed{40 \, \text{N·s}} \)

Interpretation:

  • The cart gained \( 40 \, \text{kg·m/s} \) of momentum.
  • If its mass was known, you could calculate its final speed from this impulse.
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