Work Done by a General Variable Force — Question 7

Section 7-7 · Physics pages 984–985

Question 7 A finite force step does not create a kinetic-energy jump A 1 kg particle starts at x=0 moving right at 2 m/s. The net force is +4 N for 0 ≤x < 1 m and −2 N for 1 < x ≤3 m. The value at x=1 itself is finite but otherwise arbitrary. Fx (N) x (m) 4 −2 1 3 The dashed vertical guide marks the force step; it contributes no area. (a) Find kinetic energy just before and just after x=1 m. (b) Find speed at x=3 m. (c) Explain which of force, acceleration, velocity, and kinetic energy can jump at the boundary.
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Question 7 - Solution A finite force step does not create a kinetic-energy jump Fx (N) x (m) 4 −2 1 3 (a) A single point contributes no finite area. The governing relation is K(x) = K0 + ∫x 0 Fx(s) ds Work through x=1 is 4 J, so K(1−) = K(1+) = 2 + 4 = 6 J. Changing a bounded force at one point does not change its integral. (b) Subtract work over the second interval. K(3) = 6 −2(2) = 2 J, so v(3) = 2 m/s. K remains positive on the route. (c) Distinguish a force step from an impulse. Force and acceleration jump from +4 to −2 in their respective units. Velocity and kinetic energy remain continuous. A finite step is not an infinite impulse acting in zero time.

Question 7

A finite force step does not create a kinetic-energy jump

A 1 kg particle starts at x=0 moving right at 2 m/s. The net force is +4+4 N for 0≤x<10\le x<1 m and −2-2 N for 1<x≤31<x\le3 m. The value at x=1 itself is finite but otherwise arbitrary.

Diagram shown in the original SVG worksheet.

  1. Find kinetic energy just before and just after x=1 m.

  2. Find speed at x=3 m.

  3. Explain which of force, acceleration, velocity, and kinetic energy can jump at the boundary.

Question 7 - Solution

A finite force step does not create a kinetic-energy jump

Diagram shown in the original SVG worksheet.

(a) A single point contributes no finite area.

The governing relation is K(x)=K0+∫0xFx(s)ds\boxed{K(x)=K_0+\int_0^xF_x(s)\,ds} Work through x=1 is 4 J, so K(1−)=K(1+)=2+4=6J.K(1^-)=K(1^+)=2+4=6\ \mathrm J. Changing a bounded force at one point does not change its integral.

(b) Subtract work over the second interval.

K(3)=6−2(2)=2J,K(3)=6-2(2)=2\ \mathrm J, so v(3)=2m/s.v(3)=2\ \mathrm{m/s}. K remains positive on the route.

(c) Distinguish a force step from an impulse.

Force and acceleration jump from +4 to −2-2 in their respective units. Velocity and kinetic energy remain continuous. A finite step is not an infinite impulse acting in zero time.