Work Done by a General Variable Force — Question 6

Section 7-7 · Physics pages 982–983

Question 6 Two integral measurements identify a linear force A force is known to have the form Fx = a + bx. Its work from 0 to 1 m is 5 J; from 1 to 2 m it is 1 J. Treat the data as exact. x (m) Fx = a + bx ∫ Fx dx = 5 J ∫ Fx dx = 1 J 1 2 Each labeled integral covers its own 1 m interval; the force line is to be inferred. (a) Find a and b, including their units. (b) Locate the force zero. (c) Find work from 0 to 3 m and explain how it can be smaller than work from 0 to 2 m.
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Question 6 - Solution Two integral measurements identify a linear force x (m) Fx = a + bx ∫ Fx dx = 5 J ∫ Fx dx = 1 J 1 2 (a) Translate each interval into an equation. The governing relation is Wp→q = a(q −p) + 1 2b(q2 −p2) a(1 m) + 1 2b(1 m2) = 5 J, a(1 m) + 3 2b(1 m2) = 1 J. Subtraction gives b = −4 N/m and then a = 7 N. (b) Set the reconstructed force to zero. 7 −4x = 0 at x=1.75 m. The force opposes rightward motion beyond this position. (c) Integrate over the longer interval. W0→3 = [7x −2x2]3 0 = 3 J. Work through 2 m is 6 J; the additional interval contributes −3 J. A longer displacement need not increase signed work.

Question 6

Two integral measurements identify a linear force

A force is known to have the form Fx=a+bxF_x=a+bx. Its work from 0 to 1 m is 5 J; from 1 to 2 m it is 1 J. Treat the data as exact.

Diagram shown in the original SVG worksheet.

  1. Find a and b, including their units.

  2. Locate the force zero.

  3. Find work from 0 to 3 m and explain how it can be smaller than work from 0 to 2 m.

Question 6 - Solution

Two integral measurements identify a linear force

Diagram shown in the original SVG worksheet.

(a) Translate each interval into an equation.

The governing relation is Wp→q=a(q−p)+12b(q2−p2)\boxed{W_{p\to q}=a(q-p)+\tfrac12b(q^2-p^2)}

a(1m)+12b(1m2)=5J,a(1m)+32b(1m2)=1J.a(1\,\mathrm m)+\tfrac12b(1\,\mathrm m^2)=5\ \mathrm J,\qquad a(1\,\mathrm m)+\tfrac32b(1\,\mathrm m^2)=1\ \mathrm J. Subtraction gives b=−4N/mb=-4\ \mathrm{N/m} and then a=7N.a=7\ \mathrm N.

(b) Set the reconstructed force to zero.

7−4x=07-4x=0 at x=1.75 m. The force opposes rightward motion beyond this position.

(c) Integrate over the longer interval.

W0→3=[7x−2x2]03=3J.W_{0\to3}=[7x-2x^2]_0^3=3\ \mathrm J. Work through 2 m is 6 J; the additional interval contributes −3J-3\ \mathrm J. A longer displacement need not increase signed work.