Work and Kinetic Energy — Question 4

Section 7-4 · Physics pages 918–919

Question 4 Zero net work permits a changing velocity vector Use the work–kinetic-energy theorem Wnet = ∆K for the specified particle in an inertial frame. A 2 kg particle is guided at constant speed 5 m/s through a quarter circle in a horizontal plane. It starts with velocity (5, 0) m/s and ends with (0, 5) m/s. The guide force is everywhere perpendicular to the motion.⃗ vi⃗ vf A fixed horizontal guide turns the velocity without changing its magnitude. (a) Find the kinetic-energy change and net work. (b) Find the change in velocity. (c) Why does zero net work not imply zero net force during the turn?
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Question 4 - Solution Zero net work permits a changing velocity vector⃗ vi⃗ vf (a) Compare the equal speed magnitudes. The governing relation is Wnet = ∆K = 1 2m(v2 f −v2 i ) Ki = Kf = 1 2(2)25 = 25 J, so ∆K = Wnet = 0. (b) Retain directional information. ∆⃗v = (−5, 5) m/s, |∆⃗v| = 5 √ 2 m/s. (c) Distinguish tangential from normal acceleration. The nonzero inward force changes velocity direction while remaining perpendicular to each infinitesimal displacement. It does no work. The theorem constrains changes in speed, not every component of acceleration.

Question 4

Zero net work permits a changing velocity vector

Use the work–kinetic-energy theorem Wnet=ΔKW_{\mathrm{net}}=\Delta K for the specified particle in an inertial frame. A 2 kg particle is guided at constant speed 5 m/s through a quarter circle in a horizontal plane. It starts with velocity (5,0)(5,0) m/s and ends with (0,5)(0,5) m/s. The guide force is everywhere perpendicular to the motion.

Diagram shown in the original SVG worksheet.

  1. Find the kinetic-energy change and net work.

  2. Find the change in velocity.

  3. Why does zero net work not imply zero net force during the turn?

Question 4 - Solution

Zero net work permits a changing velocity vector

Diagram shown in the original SVG worksheet.

(a) Compare the equal speed magnitudes.

The governing relation is Wnet=ΔK=12m(vf2−vi2)\boxed{W_{\mathrm{net}}=\Delta K=\tfrac12m(v_f^2-v_i^2)}

Ki=Kf=12(2)25=25J,K_i=K_f=\tfrac12(2)25=25\ \mathrm J, so ΔK=Wnet=0.\Delta K=W_{\mathrm{net}}=0.

(b) Retain directional information.

Δv→=(−5,5)m/s,|Δv→|=52m/s.\Delta\vec v=(-5,5)\ \mathrm{m/s},\qquad |\Delta\vec v|=5\sqrt2\ \mathrm{m/s}.

(c) Distinguish tangential from normal acceleration.

The nonzero inward force changes velocity direction while remaining perpendicular to each infinitesimal displacement. It does no work. The theorem constrains changes in speed, not every component of acceleration.