Simple Harmonic Motion and Uniform Circular Motion — Question 1

Section 15-6 · Physics pages 2332–2333

Question 1 A projected coordinate retains the direction through its velocity A point moves counterclockwise around a circle of radius A = .10 m with angular speed ω = 4 rad/s. At t = 0 its polar angle is π/3. Its horizontal projection is x. x y A Counterclockwise circular motion and its projection on the horizontal axis. (a) Write x(t) and find the initial projected velocity and acceleration. (b) Compare the projected speed with the actual speed at that instant. Is the projected acceleration always equal in magnitude to the centripetal acceleration?
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Question 1 - Solution A projected coordinate retains the direction through its velocity x y A (a) Derivation and calculation x(t) = .100 cos(4t + π/3) m . vx = −Aω sin ψ, ax = −Aω2 cos ψ = −ω2x. vx(0) = −.400 sin(π/3) = −.34641 m/s , ax(0) = −1.60 cos(π/3) = −.800 m/s2 . (b) Result and interpretation vcircle = Aω = .400 m/s, |vx(0)| vcircle = √ 3 2 . ac = Aω2 = 1.60 m/s2, |ax| = ac| cos ψ| ≤ac. Acceleration magnitudes agree only at x = ±A; the projected acceleration is zero at the center. Physical check The projection changes magnitude and direction even though the circle has constant speed.

Question 1

A projected coordinate retains the direction through its velocity

A point moves counterclockwise around a circle of radius A=.10mA=.10\,\mathrm{m} with angular speed ω=4rad/s\omega=4\,\mathrm{rad/s}. At t=0t=0 its polar angle is π/3\pi/3. Its horizontal projection is xx.

Diagram shown in the original SVG worksheet.

  1. Write x(t)x(t) and find the initial projected velocity and acceleration.

  2. Compare the projected speed with the actual speed at that instant. Is the projected acceleration always equal in magnitude to the centripetal acceleration?

Question 1 - Solution

A projected coordinate retains the direction through its velocity

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

x(t)=.100cos⁡(4t+π/3)m.\boxed{x(t)=.100\cos(4t+\pi/3)\,\mathrm m}.vx=−Aωsin⁡ψ,ax=−Aω2cos⁡ψ=−ω2x.v_x=-A\omega\sin\psi,\quad a_x=-A\omega^2\cos\psi=-\omega^2x.vx(0)=−.400sin⁡(π/3)=−.34641m/s,\boxed{v_x(0)=-.400\sin(\pi/3)=-.34641\,\mathrm{m/s}},ax(0)=−1.60cos⁡(π/3)=−.800m/s2.\boxed{a_x(0)=-1.60\cos(\pi/3)=-.800\,\mathrm{m/s^2}}.

(b) Result and interpretation

vcircle=Aω=.400m/s,|vx(0)|vcircle=32.v_{\mathrm{circle}}=A\omega=.400\,\mathrm{m/s},\quad\frac{|v_x(0)|}{v_{\mathrm{circle}}}=\frac{\sqrt3}{2}.ac=Aω2=1.60m/s2,|ax|=ac|cos⁡ψ|≤ac.a_c=A\omega^2=1.60\,\mathrm{m/s^2},\quad |a_x|=a_c|\cos\psi|\le a_c.Acceleration magnitudes agree only at x=±Ax=\pm A; the projected acceleration is zero at the center.

Physical check

The projection changes magnitude and direction even though the circle has constant speed.