The Force Law for Simple Harmonic Motion — Question 1

Section 15-2 · Physics pages 2252–2253

Question 1 Gravity shifts the spring equilibrium without changing its frequency A mass m = 0.50 kg hangs from an ideal spring with k = 200 N/m. Let downward extension from the natural length be y and take g = 10 m/s2. The mass is released from rest at the natural length. The spring can exert both tension and compression. m y mg ky Vertical spring oscillator; positive extension is downward. (a) Derive the equilibrium extension and the motion equation using displacement from equilibrium. (b) Find the amplitude about equilibrium, angular frequency and greatest extension.
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Question 1 - Solution Gravity shifts the spring equilibrium without changing its frequency m y mg ky (a) Derivation and calculation Balance forces with downward positive: m¨y = mg −ky, 0 = mg −kye. ye = mg k = 0.50(10) 200 = 0.0250 m . Shift to x = y −ye: m¨x = mg −k(x + ye) = −kx, ¨x + k mx = 0 . (b) Result and interpretation ω = √ k/m = √ 200/0.50 = 20 rad/s . x(0) = −ye, ˙x(0) = 0 ⇒x(t) = −0.0250 cos 20t. A = 0.0250 m , y(t) = 0.0250(1 −cos 20t), ymax = 0.0500 m . Physical check Gravity contributes a constant force that cancels at the shifted equilibrium; the linear force slope remains −k.

Question 1

Gravity shifts the spring equilibrium without changing its frequency

A mass m=0.50kgm=0.50\,\mathrm{kg} hangs from an ideal spring with k=200N/mk=200\,\mathrm{N/m}. Let downward extension from the natural length be yy and take g=10m/s2g=10\,\mathrm{m/s^2}. The mass is released from rest at the natural length. The spring can exert both tension and compression.

Diagram shown in the original SVG worksheet.

  1. Derive the equilibrium extension and the motion equation using displacement from equilibrium.

  2. Find the amplitude about equilibrium, angular frequency and greatest extension.

Question 1 - Solution

Gravity shifts the spring equilibrium without changing its frequency

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Balance forces with downward positive:mÿ=mg−ky,0=mg−kye.m\ddot y=mg-ky,\qquad0=mg-ky_e.ye=mgk=0.50(10)200=0.0250m.\boxed{y_e=\frac{mg}{k}=\frac{0.50(10)}{200}=0.0250\,\mathrm m}.Shift to x=y−yex=y-y_e:mẍ=mg−k(x+ye)=−kx,ẍ+kmx=0.m\ddot x=mg-k(x+y_e)=-kx,\qquad\boxed{\ddot x+\frac{k}{m}x=0}.

(b) Result and interpretation

ω=k/m=200/0.50=20rad/s.\omega=\sqrt{k/m}=\sqrt{200/0.50}=\boxed{20\,\mathrm{rad/s}}.x(0)=−ye,ẋ(0)=0⇒x(t)=−0.0250cos⁡20t.x(0)=-y_e,\quad\dot x(0)=0\Rightarrow x(t)=-0.0250\cos20t.A=0.0250m,y(t)=0.0250(1−cos⁡20t),ymax=0.0500m.\boxed{A=0.0250\,\mathrm m},\qquad y(t)=0.0250(1-\cos20t),\quad\boxed{y_{\max}=0.0500\,\mathrm m}.

Physical check

Gravity contributes a constant force that cancels at the shifted equilibrium; the linear force slope remains −k-k.