Work and Kinetic Energy — Question 5

Section 7-4 · Physics pages 920–921

Question 5 Endpoint speeds can reveal an unmeasured resistance Use the work–kinetic-energy theorem Wnet = ∆K for the specified particle in an inertial frame. A 2 kg block moves 5 m horizontally right. Its speed rises from 2 to 6 m/s while a constant 20 N pull acts 30◦above horizontal. A constant horizontal resistance opposes the motion. No other force does work. cart 20 N R Horizontal displacement; the pull is 30 degrees above horizontal. (a) Find the net work required by the speed change. (b) Find the work and magnitude of the resistance. (c) Check whether a proposed resistance of 12 N is compatible with the measured speeds.
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Question 5 - Solution Endpoint speeds can reveal an unmeasured resistance cart 20 N R (a) Convert both endpoint speeds to energies. The governing relation is 1 2m(v2 f −v2 i ) = Fd cos θ −Rd Wnet = 1 2(2)(36 −4) = 32 J. (b) Subtract the known pull contribution. WP = 20(5) cos 30◦= 50 √ 3 J. Thus WR = 32 −50 √ 3 ≈−54.603 J, R = (50 √ 3 −32)/5 = 10 √ 3 −6.4 ≈10.921 N. (c) Predict rather than refit. If R=12 N, net work is 50 √ 3 −60 ≈26.603 J. Then Kf = 4 + 26.603 = 30.603 J and speed is about 5.532 m/s, not 6 m/s. The proposal conflicts with the observations.

Question 5

Endpoint speeds can reveal an unmeasured resistance

Use the work–kinetic-energy theorem Wnet=ΔKW_{\mathrm{net}}=\Delta K for the specified particle in an inertial frame. A 2 kg block moves 5 m horizontally right. Its speed rises from 2 to 6 m/s while a constant 20 N pull acts 30∘30^\circ above horizontal. A constant horizontal resistance opposes the motion. No other force does work.

Diagram shown in the original SVG worksheet.

  1. Find the net work required by the speed change.

  2. Find the work and magnitude of the resistance.

  3. Check whether a proposed resistance of 12 N is compatible with the measured speeds.

Question 5 - Solution

Endpoint speeds can reveal an unmeasured resistance

Diagram shown in the original SVG worksheet.

(a) Convert both endpoint speeds to energies.

The governing relation is 12m(vf2−vi2)=Fdcos⁡θ−Rd\boxed{\tfrac12m(v_f^2-v_i^2)=Fd\cos\theta-Rd}

Wnet=12(2)(36−4)=32J.W_{\mathrm{net}}=\tfrac12(2)(36-4)=32\ \mathrm J.

(b) Subtract the known pull contribution.

WP=20(5)cos⁡30∘=503J.W_P=20(5)\cos30^\circ=50\sqrt3\ \mathrm J. Thus WR=32−503≈−54.603J,R=(503−32)/5=103−6.4≈10.921N.W_R=32-50\sqrt3\approx-54.603\ \mathrm J,\qquad R=(50\sqrt3-32)/5=10\sqrt3-6.4\approx10.921\ \mathrm N.

(c) Predict rather than refit.

If R=12 N, net work is 503−60≈26.603J50\sqrt3-60\approx26.603\ \mathrm J. Then Kf=4+26.603=30.603JK_f=4+26.603=30.603\ \mathrm J and speed is about 5.532 m/s, not 6 m/s. The proposal conflicts with the observations.