AP Physics C Mechanics Work FRQ

Work AP  Physics C Mechanics FRQ – Exam Style Questions etc.

Work AP  Physics C Mechanics FRQ

Unit 3: Work, Energy, and Power

Weightage : 15-25%

AP Physics C Mechanics Exam Style Questions – All Topics

Question

 A block of mass m is pulled across a rough horizontal table by a string connected to a motor that is attached to the floor. The string passes over a pulley with negligible friction that is vertically aligned with the left edge of the table as shown. The string and pulley both have negligible mass. The pulley is at height H above the table. The motor exerts a constant force of tension \(F_{T}\) on the string, and the block remains in contact with the table at all times as the block slides across the table from x = L to x = 0. The coefficient of kinetic friction between the table and the block is \(\mu _{k}\). Express all algebraic answers in terms of m, H, \(F _{T}\) , x, \(\mu _{k}\), L, and physical constants as appropriate.

(a) On the dot below that represents the block, draw and label the forces (not components) that act on the block when the block is at x = L. Each force must be represented by a distinct arrow starting on, and pointing away from, the dot.

(b) Derive an expression for the angle \(\Theta \) that the string makes with the horizontal as a function of x.

(c)
     i. Derive an expression for the normal force \(F_{N}\) exerted on the block by the table as a function of the block’s position x.

    ii. Derive an expression for the magnitude of the net horizontal force \(F_{net}\) exerted on the block as a function of the position x.

(d) Write, but do not solve, an integral expression that could be used to solve for the work W done by the string on the block as the block moves from x = L to x = 0.

(e) Does the string do more, less, or the same amount of work on the block as the block moves from x = L to \(x = \frac{L}{2}\)  compared to when the block moves from x = L to \(x = \frac{L}{2}\) to x = 0 ?
______ More work when the block moves from x = L to \(x = \frac{L}{2}\)
______ Less work when the block moves from x = L to \(x = \frac{L}{2}\)
______The same amount of work when the block moves from x = L to \(x = \frac{L}{2}\)
Justify your answer

▶️Answer/Explanation

1(a) Example Response 

  • Scoring Note: Examples of appropriate labels for the force due to gravity include: \(F_{G}\), \(F_{g}\),  \(F_{grav}\), W , mg , Mg , “grav force”, “F Earth on block”, “F on block by Earth”, \(F_{Earth\\\ on\\\ Block}\),  \(F_{E\\\ ,\\\ Block}\). The labels G and g are not appropriate labels for the force due to gravity. \(F_{n}\), \(F_{N}\), N , “normal force”, “ground force”, or similar labels may be used for the normal force. \(F_{string}\), \(F_{s}\), \(F_{T}\), \(F_{Tension}\), T, “string force,” “tension force,” or similar labels may be used for the tension force exerted by the string.
  • A response with extraneous forces or vectors can earn a maximum of two points.

1(b) Example Responses

1(c)(i) Example Responses

For using Newton’s second law to sum the forces in the vertical direction and write an equation that is consistent with part (a)

\(\sum F_{y} = ma\)

\(F_{net, y} = F_{N} + F_{T,y} – F_{g} = 0\)

\(F_{N} = F_{g} – F_{T, y}\)

For correctly substituting the vertical component of the tension in terms of the given variables consistent with part (b)

\(F_{N} = mg -F_{T} sin\Theta\)

\(F_{N} = mg -F_{T}\left ( \frac{H}{\sqrt{H^{2} + x^{2}}} \right )\)

1(c)(ii) Example Response 

For using Newton’s second law to sum the forces in the horizontal direction and write an equation that is consistent with part (a)

\(F_{net, x} = F_{T, x} – F_{f}\)

For correctly substituting the horizontal component of the force of tension in terms of the given variables consistent with part (b)

\( F_{net, x} = F_{T}cos\Theta – F_{f}\)

\(F_{net, x} = F_{T}(\frac{(x)}{\sqrt{H^{2}+x^{2}}}) – F_{f}\)

For correctly substituting the expression for the normal force from part (c)(i) into the expression for the force of friction

\(F_{net, x} = F_{T}(\frac{(x)}{\sqrt{H^{2}+x^{2}}}) – \mu _{k}F_{N}\)

\(F_{net, x} = F_{T}(\frac{(x)}{\sqrt{H^{2}+x^{2}}}) – \mu _{k}(mg – F_{r(\frac{H}{\sqrt{H^{2}+x^{2}}})})\)

1(d)Example Response

For any indication that the work done on the block by the string is due only to the horizontal component of the tension in the string 

\( W = \int F_{T, x}dx\)

For using the horizontal component of the force of tension consistent with part (c)

For indicating that work is the integral of the force with respect to x, including limits or a constant of integration

\( W = \int_{x=L}^{x = 0} – F_{T}(\frac{x}{\sqrt{H^{2}+x^{2}}})dx\)

1(e)Example Response

\(F_{T}\) stays the same for both halves, the displacement is the same in both halves, but from x = L to x = L /2 the angle is smaller, resulting in a larger component of the tension force that aligns with the displacement 

Question

A uniform chain of mass M and length l hangs from a hook in the ceiling. The bottom link is now raised vertically and hung on the hook as shown above on the right.
a. Determine the increase in gravitational potential energy of the chain by considering the change in position of the center of mass of the chain.
b. Write an equation for the upward external force F(y) required to lift the chain slowly as a function of the vertical distance y.
c. Find the work done on the chain by direct integration of ∫ 𝐹𝑑𝑦.

Answer/Explanation

Ans:

a. using the ceiling as a reference point: Ui = – ½ mgl; Uf = – ¼ mgl
∆U = Uf – Ui = ¼ mgl
b. λ = m/l, the weight of the piece being held is λsg = mgs/l; s = y/2 so F(y) = mgy/2l

c. \(\int_{0}^{l}Fdy = \frac{mg}{2l}\int_{0}^{l}ydy = \frac{mg}{2l}\frac{l^{2}}{2}= \frac{1}{4}mgl\)

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