Cuesta College, San Luis Obispo, CA
Cf. Young and Freeman, University Physics, 11/e, Problem 9.86
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(A) 0.45 m.
(B) 0.90 m.
(C) 1.4 m.
(D) 2.3 m.
Correct answer: (D)
No external work is done on this system, so the decrease in gravitational potential energy of the box is equal to the sum of the increases of the translational kinetic energy of the box, and the rotational kinetic energy of the disk. The translational speed of the box v is related to the angular speed of the disk via v = r·ω. With initial conditions vi = 0, and ωi = 0; final conditions vf = r·ωf, and yf = 0; and the moment of inertia of the disk is Idisk = (1/2)·mdisk·r2, the energy conservation transfer-balance equation is:
Wnc = ∆Ktr + ∆Krot + ∆Ugrav + ∆Uelas,
0 = (1/2)·mbox·(vf2 - 02) + (1/2)·Idisk·(ωf2 - 02) + mbox·g·(0 - yi) + 0,
0 = (1/2)·mbox·vf2 + (1/2)·((1/2)·mdisk·r2)·(vf/r)2 - mbox·g·yi,
0 = (1/2)·mbox·vf2 + (1/4)·mdisk·vf2 - mbox·g·yi,
Solving for yi:
yi = ((1/2)·mbox + (1/4)·mdisk)·vf2/mbox·g = 2.25 m,
or to two significant figures, 2.3 m.
Choice (A) stems from a sign error in the kinetic energy terms. Neglecting the rotational kinetic energy of the disk results in (B); neglecting the translational kinetic energy of the box results in (C).
Student responses:
(A) : 6 students
(B) : 12 students
(C) : 10 students
(D) : 2 students
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