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  1. AP Physics C Mechanics
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Change in Momentum and Impulse

Ethan Williams

Ethan Williams

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Next Topic - Conservation of Linear Momentum

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Study Guide Overview

This study guide covers momentum, impulse, and the impulse-momentum theorem. Key concepts include: the relationship between net external force and rate of momentum change, calculating impulse using integrals and force-time graphs, understanding impulse as a vector, the relationship between impulse and change in momentum, and applying these concepts to problem-solving, including those involving changing mass. It also provides practice questions and exam tips.

#AP Physics C: Mechanics - Momentum and Impulse 🚀

Hey there, future AP Physics C champ! Let's dive into momentum and impulse – two concepts that are absolutely key to understanding how forces change motion. Think of this as your ultimate cheat sheet for acing the exam. Let's get started!

This topic is super important! Expect to see it in both multiple-choice and free-response questions. It's a core concept that links force, time, and motion. Understanding it well will boost your confidence and your score.

#Impulse Delivery 🏃‍♂️

#Rate of Momentum Change

  • The net external force acting on a system dictates how quickly its momentum changes. 💡
  • This is captured by the equation: F⃗net =dp⃗dt\vec{F}_{\text {net }}=\frac{d \vec{p}}{d t}Fnet ​=dtdp​​
    • F⃗net \vec{F}_{\text {net }}Fnet ​ is the net external force vector.
    • dp⃗dt\frac{d \vec{p}}{d t}dtdp​​ is the rate of change of momentum with respect to time.
Key Concept

Remember, force is the cause of momentum change. The greater the force, the faster the momentum changes. It's all about how forces affect motion over time.

#Impulse Definition

  • Impulse is the effect of a force acting over a time interval. Think of it as a 'push' that changes momentum.
  • Calculated using the integral: J⃗=∫t1t2F⃗net (t)dt\vec{J}=\int_{t_{1}}^{t_{2}} \vec{F}_{\text {net }}(t) d tJ=∫t1​t2​​Fnet ​(t)dt
    • J⃗\vec{J}J is the impulse vector.
    • F⃗net (t)\vec{F}_{\text {net }}(t)Fnet ​(t) is the net external force as a function of time.
    • t1t_1t1​ and t2t_2t2​ are the start and end times of the interval.

#Impulse Direction

  • Impulse is a vector, meaning it has both magnitude and direction.
  • It always points in the same direction as the net force applied.

#Impulse and Force-Time Graphs 📈

  • The area under a force-time graph gives you the impulse delivered. It's a visual way to see the total 'push'.
  • This area is the integral of the net force over time.
Memory Aid

Think of the area under the curve as the 'total push' – the bigger the area, the bigger the impulse. This visual helps you connect graphs to physical concepts.

#Force and Momentum-Time Graphs

  • The slope of a momentum-time graph at any point is the net external force at that moment.
  • Steeper slopes mean larger forces.
  • Constant slopes mean constant forces.
  • Changes in slope show how the force changes over time.
Exam Tip

For graphs, remember: Area under force-time = impulse, and slope of momentum-time = force. Use these relationships to quickly solve problems.

#Impulse-Momentum Relationship 🎯

#Change in Momentum

  • Change in momentum (Δp⃗\Delta \vec{p}Δp​) is the difference between final and initial momentum.
  • It's calculated as: Δp⃗=p⃗−p⃗0\Delta \vec{p}=\vec{p}-\vec{p}_{0}Δp​=p​−p​0​
    • Δp⃗\Delta \vec{p}Δp​ is the change in momentum vector.
    • p⃗\vec{p}p​ is the final momentum vector.
    • p⃗0\vec{p}_0p​0​ is the initial momentum vector.

#Impulse-Momentum Theorem

  • This theorem is a big deal: Impulse = Change in Momentum.
  • Mathematically: J⃗=∫t1t2F⃗net (t)dt=Δp⃗\vec{J}=\int_{t_{1}}^{t_{2}} \vec{F}_{\text {net }}(t) d t=\Delta \vec{p}J=∫t1​t2​​Fnet ​(t)dt=Δp​
    • J⃗\vec{J}J is the impulse vector.
    • F⃗net (t)\vec{F}_{\text {net }}(t)Fnet ​(t) is the net external force as a function of time.
    • Δp⃗\Delta \vec{p}Δp​ is the change in momentum vector.
  • Newton's second law (F⃗net =ma⃗\vec{F}_{\text {net }}=m \vec{a}Fnet ​=ma) comes from this theorem when mass is constant: F⃗net =dp⃗dt=mdv⃗dt=ma⃗\vec{F}_{\text {net }}=\frac{d \vec{p}}{d t}=m \frac{d \vec{v}}{d t}=m \vec{a}Fnet ​=dtdp​​=mdtdv​=ma
    • mmm is the constant mass.
    • dv⃗dt\frac{d \vec{v}}{d t}dtdv​ is the acceleration vector (a⃗\vec{a}a).
  • The theorem also applies when velocity is constant, but mass changes (like a rocket): F⃗net=dp⃗dt=dmdtv⃗\vec{F}_{\mathrm{net}}=\frac{d \vec{p}}{d t}=\frac{d m}{d t} \vec{v}Fnet​=dtdp​​=dtdm​v
    • dmdt\frac{d m}{d t}dtdm​ is the rate of mass change.
    • v⃗\vec{v}v is the constant velocity vector.
Memory Aid

Remember: Impulse is the 'push' (force over time), and change in momentum is the 'result' (change in motion). They are always equal! This helps connect the concepts.

Common Mistake

Don't forget that momentum and impulse are vectors! Always consider direction when solving problems, especially in collisions. A common mistake is to treat them as scalars.

#Final Exam Focus

Alright, let's talk strategy for the exam. Here’s what you should really focus on:

  • High-Priority Topics: The impulse-momentum theorem is HUGE. Make sure you can apply it to various situations, including collisions and systems with changing mass. Also, be very comfortable with force-time and momentum-time graphs.
  • Common Question Types: Expect questions that ask you to calculate impulse, change in momentum, or forces using graphs or integrals. Also, look out for problems that combine these concepts with conservation of energy or other mechanics topics.
  • Time Management: Don't spend too long on one problem. If you're stuck, move on and come back later. Make sure you allocate enough time for free-response questions, which often require more detailed solutions.
  • Common Pitfalls: Watch out for vector directions and units. Always double-check your work to avoid careless errors. Be careful with the signs of the forces and momentums.
  • Strategies: Practice, practice, practice! The more problems you solve, the more comfortable you'll become with these concepts. Review your mistakes and focus on areas where you struggle.
Exam Tip

When tackling free-response questions, start with the basic principles and equations. Show all your work, even if it seems obvious. This will help you earn partial credit even if you make a mistake along the way.

#Practice Questions

Practice Question

#Multiple Choice Questions

  1. A 2 kg object is moving with a velocity of 5 m/s. A force is applied to it, and its velocity changes to 10 m/s in the same direction. What is the magnitude of the impulse delivered to the object? (A) 5 N⋅s (B) 10 N⋅s (C) 15 N⋅s (D) 20 N⋅s (E) 25 N⋅s

  2. A force-time graph shows a triangular pulse with a peak force of 10 N lasting for 2 seconds. What is the impulse delivered by this force? (A) 5 N⋅s (B) 10 N⋅s (C) 20 N⋅s (D) 40 N⋅s (E) Cannot be determined without knowing the mass

  3. A 1 kg ball moving at 10 m/s hits a wall and bounces back with a speed of 8 m/s. What is the magnitude of the change in momentum of the ball? (A) 2 kg⋅m/s (B) 8 kg⋅m/s (C) 10 kg⋅m/s (D) 18 kg⋅m/s (E) 80 kg⋅m/s

#Free Response Question

A 0.5 kg cart is initially at rest on a horizontal, frictionless surface. A time-dependent force given by F(t)=10t−2t2F(t) = 10t - 2t^2F(t)=10t−2t2 (where F is in Newtons, and t is in seconds) is applied to the cart in the positive direction for 5 seconds.

(a) Calculate the impulse delivered to the cart during the 5-second interval.

(b) Determine the final velocity of the cart after the 5-second interval.

(c) Sketch a graph of the force as a function of time for the 5-second interval.

(d) At what time is the force maximum?

Scoring Breakdown:

(a) (5 points) - 1 point: Correctly setting up the integral for impulse: J=∫05(10t−2t2)dtJ = \int_{0}^{5} (10t - 2t^2) dtJ=∫05​(10t−2t2)dt - 2 points: Correctly integrating the force function: J=[5t2−(2/3)t3]05J = [5t^2 - (2/3)t^3]_{0}^{5}J=[5t2−(2/3)t3]05​ - 2 points: Correctly evaluating the integral: J=5(5)2−(2/3)(5)3=125−250/3=125/3≈41.67 NsJ = 5(5)^2 - (2/3)(5)^3 = 125 - 250/3 = 125/3 \approx 41.67 \text{ Ns}J=5(5)2−(2/3)(5)3=125−250/3=125/3≈41.67 Ns

(b) (3 points) - 1 point: Using the impulse-momentum theorem: J=Δp=mΔvJ = \Delta p = m\Delta vJ=Δp=mΔv - 1 point: Correctly relating impulse to change in velocity: 41.67=0.5Δv41.67 = 0.5 \Delta v41.67=0.5Δv - 1 point: Correctly finding the final velocity: Δv=41.67/0.5=83.34 m/s\Delta v = 41.67 / 0.5 = 83.34 \text{ m/s}Δv=41.67/0.5=83.34 m/s

(c) (2 points) - 1 point: Correctly plotting the force as a function of time. The graph should be a parabola opening downwards, starting at 0, reaching a peak, and returning to 0. - 1 point: The graph should be labeled with correct units and scales on both axes.

(d) (2 points) - 1 point: Taking the derivative of the force function and setting it to zero to find the maximum: F′(t)=10−4t=0F'(t) = 10 - 4t = 0F′(t)=10−4t=0 - 1 point: Correctly solving for the time at which the force is maximum: t=10/4=2.5 st = 10/4 = 2.5 \text{ s}t=10/4=2.5 s

Remember, you've got this! Keep practicing, stay focused, and you'll do great on the exam. Good luck! 🎉

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Question 1 of 13

A 2 kg ball is pushed with a constant force of 10 N for 2 seconds. What is the magnitude of the impulse delivered to the ball? 🚀

5 N⋅s

10 N⋅s

20 N⋅s

40 N⋅s