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AP Physics 1 6.3: Angular Momentum and Angular Impulse

Describe angular momentum about a chosen axis and connect angular impulse to changes in angular momentum during rotational interactions.

Syllabus
Effective Fall 2025
Course
AP Physics 1: Algebra-Based

Exam points

  • Calculate angular momentum about a specified axis for a rigid system or moving object.
  • Use angular impulse and change in angular momentum to describe a rotational interaction.

6.3 Angular Momentum and Angular Impulse question 1

[Maximum number: 6]

(12 points, suggested time 25 minutes)
The left end of a rod of length d and rotational inertia I is attached to a frictionless horizontal surface by a frictionless pivot, as shown above. Point C marks the center (midpoint) of the rod. The rod is initially motionless but is free to rotate around the pivot. A student will slide a disk of mass mdisk m_{\text {disk }} toward the rod with velocity v0v_{0} perpendicular to the rod, and the disk will stick to the rod a distance x from the pivot. The student wants the rod

disk system to end up with as much angular speed as possible.

Question (a)

(a)

Suppose the rod is much more massive than the disk. To give the rod as much angular speed as possible, should the student make the disk hit the rod to the left of point C, at point C, or to the right of point C ? To the left of C At C To the right of C
Briefly explain your reasoning without manipulating equations.

[ 1 ]

Question (b)

(b)

On the Internet, a student finds the following equation for the postcollision angular speed ω\omega of the rod in this situation: ω=mdisk xv0I\omega=\frac{m_{\text {disk }} x v_{0}}{I}. Regardless of whether this equation for angular speed is correct, does it agree with your qualitative reasoning in part (a) ? In other words, does this equation for ω\omega have the expected dependence as reasoned in part (a) ? Yes No
Briefly explain your reasoning without deriving an equation for ω\omega.

[ 2 ]

Question (c)

(c)

Another student deriving an equation for the postcollision angular speed ω\omega of the rod makes a mistake and comes up with ω=Ixv0mdisk d4\omega=\frac{I x v_{0}}{m_{\text {disk }} d^{4}}. Without deriving the correct equation, how can you tell that this equation is not plausible-in other words, that it does not make physical sense? Briefly explain your reasoning.

For parts (d) and (e), do NOT assume that the rod is much more massive than the disk.

[ 3 ]

6.3 Angular Momentum and Angular Impulse question 2

[Maximum number: 1]
Figure for Question 6.3 Angular Momentum and Angular Impulse question 2 — AP Physics 1: Algebra-Based

A string of negligible mass is wrapped around the rim of a solid disk that can rotate without friction about its center, as shown above. The string is pulled down with a force of constant magnitude F for an interval of time Δt\Delta t. If the disk starts from rest, which combination of F and Δt\Delta t will result in the greatest angular speed of the disk?

International Exam 2021 MCQ

A
Table for Question 6.3 Angular Momentum and Angular Impulse question 2 — AP Physics 1: Algebra-Based — Option A
B
Table for Question 6.3 Angular Momentum and Angular Impulse question 2 — AP Physics 1: Algebra-Based — Option B
C
Table for Question 6.3 Angular Momentum and Angular Impulse question 2 — AP Physics 1: Algebra-Based — Option C
D
Figure for Question 6.3 Angular Momentum and Angular Impulse question 2 — AP Physics 1: Algebra-Based — Option D

6.3 Angular Momentum and Angular Impulse question 3

[Maximum number: 6]

(7 points, suggested time 13 minutes)

A block of unknown mass is attached to a long, lightweight string that is wrapped several turns around a pulley mounted on a horizontal axis through its center, as shown. The pulley is a uniform solid disk of mass M and radius R. The rotational inertia of the pulley is described by the equation I=12MR2I=\frac{1}{2} M R^{2}. The pulley can rotate about its center with negligible friction. The string does not slip on the pulley as the block falls.

When the block is released from rest and as the block travels toward the ground, the magnitude of the tension exerted on the block by the string is FTF_{\mathrm{T}}.

Consider scenarios 1 and 2 at the end of time interval Δt\Delta t. In a clear, coherent paragraph-length response that may also contain equations and drawings, explain why the change in angular momentum of both pulleys is the same but the change in rotational kinetic energy is greater for the disk.

Figure 1

Figure 1

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