2015: Problems 12-13

Topic: Dynamics
Concepts: Circular motion, Conservation of energy, Newton’s laws


Solution:

The pendulum feels the forces of tension and gravity. Applying Newton’s 2nd law in the tangential direction,

mat=mgsinθma_t=mg\sin\theta
at=gsinθa_t=g\sin\theta

Since the pendulum is undergoing circular motion, the radial acceleration is given by

ar=v2La_r=\frac{v^2}{L}

The magnitude of the total acceleration is

a=at2+ar2=(gsinθ)2+(v2/L)2a=\sqrt{a_t^2+a_r^2}=\sqrt{(g\sin\theta)^2+(v^2/L)^2}

Now we go through the possible answer choices.

  • A) Not correct since the magnitude of the acceleration depends on θ\theta and vv which are both changing.
  • B) Not correct since the magnitude of the acceleration at the lowest point θ=0\theta=0 is

    a=v2/La=v^2/L

    and we have from energy conservation,

    12mv2=mgL(1cosθmax)\frac{1}{2}mv^2=mgL(1-\cos\theta_{\text{max}})
    v2/L=2g(1cosθmax)v^2/L=2g(1-\cos\theta_{\text{max}})

    which is not (in general) equal to gg.
  • C) Not correct since v=0v=0 (no radial acceleration) only at θ=θmax\theta=\theta_{\text{max}} (where there is a tangential acceleration) so a0a \neq 0 at any point.
  • D) Not correct since the mass has a tangential acceleration at=gsinθa_t=g\sin\theta.
  • E) Correct since at the lowest point θ=0\theta=0 there is no tangential acceleration at=0a_t=0.

Thus, the answer is E.

Topic: Dynamics
Concepts: Circular motion


Solution:

The pendulum is undergoing circular motion, so the radial acceleration ar\vec{a}_r points toward the center of the circle. The pendulum is slowing down as it moves higher so the tangential acceleration at\vec{a}_t points opposite the velocity. The total acceleration

a=ar+at\vec{a}=\vec{a}_r+\vec{a}_t

is the vector sum of these two components. Thus, the answer is D.

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