Unit: Work, Energy, and Power

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Part 1

A simple pendulum consists of a small bob of mass m=0.5m = 0.5 kg attached to a light string of length L=2.4L = 2.4 m. The bob is pulled aside until the string makes an angle of θ0=33\theta_0 = 33^\circ with the vertical and then released from rest. Neglect air resistance. Take the lowest point of the swing as the zero of gravitational potential energy. Take g=9.8g = 9.8 m/s2^2.

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Find the speed vbottomv_{\text{bottom}} of the bob as it passes through the lowest point.

Correct!

Solution:

Solution

We apply conservation of mechanical energy between the release point and the lowest point. The bob is released from rest at angle θ0=33\theta_0 = 33^\circ.

At the release point, the height above the lowest point is:

h=LLcosθ0=L(1cosθ0)h = L - L \cos \theta_0 = L(1 - \cos \theta_0)

The total mechanical energy at release (taking the lowest point as zero potential energy):

Einitial=Kinitial+Uinitial=0+mgh=mgL(1cosθ0)E_{\text{initial}} = K_{\text{initial}} + U_{\text{initial}} = 0 + mgh = mgL(1 - \cos \theta_0)

At the lowest point:

Ebottom=Kbottom+Ubottom=12mvbottom2+0E_{\text{bottom}} = K_{\text{bottom}} + U_{\text{bottom}} = \frac{1}{2}mv_{\text{bottom}}^2 + 0

By conservation of energy:

mgL(1cosθ0)=12mvbottom2mgL(1 - \cos \theta_0) = \frac{1}{2}mv_{\text{bottom}}^2

Solving for vbottomv_{\text{bottom}}:

vbottom=2gL(1cosθ0)v_{\text{bottom}} = \sqrt{2gL(1 - \cos \theta_0)}

Substituting the values g=9.8g = 9.8 m/s2^2, L=2.4L = 2.4 m, and θ0=33\theta_0 = 33^\circ:

vbottom=29.82.4(1cos33)=2.75 m/sv_{\text{bottom}} = \sqrt{2 \cdot 9.8 \cdot 2.4 \cdot (1 - \cos 33^\circ)} = 2.75 \text{ m/s}

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