Newton's Second Law — Question 4

Section 5-5 · Physics pages 698–699

Question 4 A force switch requires a piecewise motion history Use ∑⃗F = m⃗a for constant mass in an inertial frame. A 2 kg cart begins at rest at x=0. Net force is +4 N for 2 s, then -2 N for the following 3 s. t (s) Fx (N) 4 −2 2 5 Force history; the switch changes acceleration, with no impulsive force. (a) Find position and velocity at the switch. (b) Find the final position and velocity. (c) Does velocity jump when the finite force changes abruptly?
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Question 4 - Solution A force switch requires a piecewise motion history t (s) Fx (N) 4 −2 2 5 (a) Solve the first stage. a1 = 4/2 = 2, v1 = 2(2) = 4 m/s, x1 = 1 2(2)(2)2 = 4 m a1 = 2 m/s2, so at t=2 s, v = 4 m/s and x = 4 m. (b) Use the switch state as new initial data. a2 = −2/2 = −1, vf = 4 −3 = 1 m/s , xf = 4 + 4(3) −1 2(3)2 = 11.5 m a2 = −1 m/s2. Over the next 3 s, ∆x = 4(3) −1 2(3)2 = 7.5 m and v = 1 m/s. Final x is 11.5 m. (c) Separate acceleration from velocity. v(2+) −v(2−) = lim ϵ→0 1 m ∫2+ϵ 2−ϵ F(t) dt = 0 Acceleration changes instantly in this ideal piecewise model, but a bounded force acting for zero elapsed time produces no finite velocity jump. Position and velocity remain continuous at the switch.

Question 4

A force switch requires a piecewise motion history

Use ∑F→=ma→\sum\vec F=m\vec a for constant mass in an inertial frame. A 2 kg cart begins at rest at x=0. Net force is +4 N for 2 s, then -2 N for the following 3 s.

Diagram shown in the original SVG worksheet.

  1. Find position and velocity at the switch.

  2. Find the final position and velocity.

  3. Does velocity jump when the finite force changes abruptly?

Question 4 - Solution

A force switch requires a piecewise motion history

Diagram shown in the original SVG worksheet.

(a) Solve the first stage.

a1=4/2=2,v1=2(2)=4m/s,x1=12(2)(2)2=4ma_1=4/2=2,\quad v_1=2(2)=4\,\mathrm{m/s},\quad x_1=\tfrac12(2)(2)^2=4\,\mathrm m a1=2a_1=2 m/s2^2, so at t=2 s, v=4v=4 m/s and x=4x=4 m.

(b) Use the switch state as new initial data.

a2=−2/2=−1,vf=4−3=1m/s,xf=4+4(3)−12(3)2=11.5ma_2=-2/2=-1,\quad\boxed{v_f=4-3=1\,\mathrm{m/s}},\quad x_f=4+4(3)-\tfrac12(3)^2=11.5\,\mathrm m a2=−1a_2=-1 m/s2^2. Over the next 3 s, Δx=4(3)−12(3)2=7.5\Delta x=4(3)-\tfrac12(3)^2=7.5 m and v=1v=1 m/s. Final x is 11.5 m.

(c) Separate acceleration from velocity.

v(2+)−v(2−)=limϵ→01m∫2−ϵ2+ϵF(t)dt=0v(2^+)-v(2^-)=\lim_{\epsilon\to0}\frac1m\int_{2-\epsilon}^{2+\epsilon}F(t)\,dt=0 Acceleration changes instantly in this ideal piecewise model, but a bounded force acting for zero elapsed time produces no finite velocity jump. Position and velocity remain continuous at the switch.