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AP Physics C Mechanics - 6.3 Angular Momentum and Angular Impulse- Exam Style questions- FRQs

Angular Momentum and Angular Impulse AP  Physics C Mechanics FRQ

Unit 6: Energy and Momentum of Rotating Systems

Weightage : 10-15%

AP Physics C Mechanics Exam Style Questions – All Topics

Question

A uniform rod of length \( d \) has one end fixed to the central axis of a horizontal, frictionless circular platform of radius \( R=2d \). Fixed at the other end of the rod is an ideal spring of negligible mass to which a block is attached. The block is set in frictionless grooves so that it can only move along a radius of the platform, as shown in Figure \( 1 \) above. The equilibrium length of the spring is \( d/2 \). Below is a table showing the mass of the block and the masses and rotational inertias of the rod and platform.
A motor begins to slowly rotate the platform counterclockwise as viewed from above until the platform reaches a constant angular speed \( \omega \). Under these conditions, the spring has stretched by an additional length \( d/2 \), as shown in Figure \( 2 \). Answer the following questions for the platform rotating at constant angular speed \( \omega \). Express all algebraic answers in terms of \( m \), \( d \), \( \omega \), and physical constants, as appropriate.
(a) Derive an expression for the spring constant of the spring.
(b)
i. Determine an expression for the rotational inertia of the block around the axis of the platform.
ii. Derive an expression for the rotational inertia of the entire system about the axis of the platform.
(c) Determine an expression for the angular momentum of the entire system about the axis of the platform.
While the system continues to rotate, a small mechanism in the pivot moves the rod slowly until the center of the rod is positioned on the axis, as shown in Figure \( 3 \) above. The same constant angular speed \( \omega \) is maintained by the motor driving the platform.
(d) Derive an expression for the distance \( x \) that the spring is stretched when the rod reaches the position shown in Figure \( 3 \) above.
For parts (e), (f), and (g), assume the center of the rod is still moving toward the axis of the platform.
(e) Is the angular momentum of the entire system increasing, decreasing, or staying the same?
_____ Increasing      _____ Decreasing      _____ Staying the same
Justify your answer.
(f) In order to keep the system rotating with constant angular speed \( \omega \), is the motor doing positive work, negative work, or no work on the rotating system?
_____ Positive      _____ Negative      _____ No work
Justify your answer.
(g) On the block in Figure \( 4 \) below, draw a single vector representing the direction of the acceleration of the block. Draw the vector so that it is starting on, and pointing away from, the block.

Most-appropriate topic codes (AP Physics C: Mechanics):

• Topic \( 2.8 \) — Spring Forces (Parts \( \mathrm{a} \), \( \mathrm{d} \))
• Topic \( 2.10 \) — Circular Motion (Parts \( \mathrm{a} \), \( \mathrm{d} \), \( \mathrm{g} \))
• Topic \( 5.4 \) — Rotational Inertia (Part \( \mathrm{b} \))
• Topic \( 6.1 \) — Rotational Kinetic Energy (Part \( \mathrm{f} \))
• Topic \( 6.3 \) — Angular Momentum and Angular Impulse (Parts \( \mathrm{c} \), \( \mathrm{e} \))
▶️ Answer/Explanation

(a)
To find the spring constant, we equate the restoring force of the spring to the centripetal force required to maintain the block’s circular motion. The total radius of the block’s path is the sum of the rod’s length, the spring’s equilibrium length, and its stretch.
\( F_S = F_C \)
\( kx = mr\omega^2 \)
\( k\left(\dfrac{d}{2}\right) = m(2d)\omega^2 \)
\( \boxed{k = 4m\omega^2} \)

(b) i.
The rotational inertia of a point mass at a distance \( r \) from the axis of rotation is calculated using \( I = mr^2 \). By substituting the total radius from part (a), we can find the block’s inertia.
\( I = mr^2 \)
\( I = m(2d)^2 \)
\( \boxed{I = 4md^2} \)

(b) ii.
The rotational inertia of the entire system is the sum of the individual rotational inertias of the platform, the rod, and the block. We simply substitute the given mass and radius expressions for each part and sum them up.
\( I_{\text{sys}} = I_{\text{P}} + I_{\text{R}} + I_{\text{B}} \)
\( I_{\text{sys}} = \dfrac{m_P R^2}{2} + \dfrac{m_R d^2}{3} + mr^2 \)
\( I_{\text{sys}} = \dfrac{(5m)(2d)^2}{2} + \dfrac{(3m)d^2}{3} + 4md^2 \)
\( I_{\text{sys}} = 10md^2 + md^2 + 4md^2 \)
\( \boxed{I_{\text{sys}} = 15md^2} \)

(c)
Angular momentum is the product of the system’s total rotational inertia and its angular velocity. Since we already have the total inertia, we just multiply it by the given angular speed \( \omega \).
\( L = I_{\text{sys}}\omega \)
\( \boxed{L = 15md^2\omega} \)

(d)
When the rod is centered on the axis, the new radius for the block is half the rod length \( d/2 \) plus the spring’s equilibrium length \( d/2 \) and its new stretch \( x \). We again equate the spring force to the centripetal force and solve for \( x \).
\( F_S = F_C \)
\( kx = m r_{\text{new}} \omega^2 \)
\( (4m\omega^2)x = m\left(\dfrac{d}{2} + \dfrac{d}{2} + x\right)\omega^2 \)
\( 4x = d + x \)
\( 3x = d \)
\( \boxed{x = d/3} \)

(e)
Correct choice:
\( \boxed{\text{Decreasing}} \)

As the rod moves toward the axis, the mass of the system is distributed closer to the center of rotation, which decreases the overall rotational inertia \( I \). Since the angular momentum is given by \( L = I\omega \) and the angular velocity \( \omega \) remains constant, the angular momentum must decrease.

(f)
Correct choice:
\( \boxed{\text{Negative}} \)

The rotational kinetic energy of the system is given by \( K = \frac{1}{2}I\omega^2 \). As the rotational inertia \( I \) decreases and \( \omega \) is kept constant, the system’s total rotational kinetic energy drops. According to the work-energy theorem, a decrease in kinetic energy indicates that the net work done on the rotating system by the motor is negative.

(g)


The block’s acceleration is made up of two distinct components. First, there is the centripetal acceleration directing it toward the center of the platform. Second, as it moves radially inward while rotating, there is a tangential component (the Coriolis acceleration) pointing in the direction of the rotation. The combination yields a net vector pointing diagonally.

\( \boxed{\text{An arrow starting on the box and pointing down and to the right}} \)

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