The Force Law for Simple Harmonic Motion — Question 3

Section 15-2 · Physics pages 2256–2257

Question 3 Turning on a constant force launches motion about a new center A horizontal mass m = 0.20 kg on an ideal spring k = 80 N/m is initially at rest at x = 0, its original equilibrium. At t = 0, a constant force F0 = 4.0 N in the positive direction is switched on and retained. There is no impulse at switch-on. m x Horizontal oscillator schematic; displacement is measured from equilibrium. (a) Find the new equilibrium and the complete motion x(t). (b) Find the first maximum displacement and maximum speed. Why does the particle not simply stop at the new equilibrium?
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Question 3 - Solution Turning on a constant force launches motion about a new center m x (a) Derivation and calculation m¨x + kx = F0, xe = F0/k = 4/80 = 0.0500 m. q = x −xe : ¨q + ω2q = 0, ω = √ 80/0.20 = 20 rad/s. q(0) = −xe, ˙q(0) = 0 ⇒x(t) = 0.0500[1 −cos 20t] m . (b) Result and interpretation v(t) = 20(0.0500) sin 20t = 1.00 sin 20t m/s. tmax = π 20 = 0.15708 s, xmax = 2xe = 0.100 m . vmax = 1.00 m/s , x = xe : Fnet = 0, a = 0, |v| = vmax. The equilibrium crossing has nonzero velocity, so the undamped mass overshoots. Physical check The force step changes acceleration but supplies no impulse: position and velocity remain continuous at t = 0.

Question 3

Turning on a constant force launches motion about a new center

A horizontal mass m=0.20kgm=0.20\,\mathrm{kg} on an ideal spring k=80N/mk=80\,\mathrm{N/m} is initially at rest at x=0x=0, its original equilibrium. At t=0t=0, a constant force F0=4.0NF_0=4.0\,\mathrm{N} in the positive direction is switched on and retained. There is no impulse at switch-on.

Diagram shown in the original SVG worksheet.

  1. Find the new equilibrium and the complete motion x(t)x(t).

  2. Find the first maximum displacement and maximum speed. Why does the particle not simply stop at the new equilibrium?

Question 3 - Solution

Turning on a constant force launches motion about a new center

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

mẍ+kx=F0,xe=F0/k=4/80=0.0500m.m\ddot x+kx=F_0,\qquad x_e=F_0/k=4/80=0.0500\,\mathrm m.q=x−xe:q̈+ω2q=0,ω=80/0.20=20rad/s.q=x-x_e:\quad\ddot q+\omega^2q=0,\quad\omega=\sqrt{80/0.20}=20\,\mathrm{rad/s}.q(0)=−xe,q̇(0)=0⇒x(t)=0.0500[1−cos⁡20t]m.q(0)=-x_e,\quad\dot q(0)=0\Rightarrow\boxed{x(t)=0.0500[1-\cos20t]\,\mathrm m}.

(b) Result and interpretation

v(t)=20(0.0500)sin⁡20t=1.00sin⁡20tm/s.v(t)=20(0.0500)\sin20t=1.00\sin20t\,\mathrm{m/s}.tmax=π20=0.15708s,xmax=2xe=0.100m.t_{\max}=\frac\pi{20}=0.15708\,\mathrm s,\qquad\boxed{x_{\max}=2x_e=0.100\,\mathrm m}.vmax=1.00m/s,x=xe:Fnet=0,a=0,|v|=vmax.\boxed{v_{\max}=1.00\,\mathrm{m/s}},\qquad x=x_e:\ F_{\mathrm{net}}=0,\ a=0,\ |v|=v_{\max}.The equilibrium crossing has nonzero velocity, so the undamped mass overshoots.

Physical check

The force step changes acceleration but supplies no impulse: position and velocity remain continuous at t=0t=0.