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Concepts Of Physics MCQ Edition [Volume 1]
Exam
Concepts Of Physics MCQ Edition [Volume 1]
Subject
Physics
Chapter
Simple Harmonic Motion

Concepts Of Physics MCQ Edition [Volume 1] · Physics · Simple Harmonic Motion

Initially, all the springs displayed in the figure are unstretched...

Initially, all the springs displayed in the figure are unstretched when a man begins pulling the block. The man applies a constant force FF to the block. Determine the amplitude and the frequency of the block's motion.
Initially, all the springs displayed in the figure are unstretched when a man begins pulling the block. The man applies

Options

  1. AAmplitude: F(k2+k3)k1k2+k2k3+k3k1\dfrac{F(k_2 + k_3)}{k_1 k_2 + k_2 k_3 + k_3 k_1}, Frequency: 12πM(k2+k3)k1k2+k2k3+k3k1\dfrac{1}{2\pi} \sqrt{\dfrac{M(k_2 + k_3)}{k_1 k_2 + k_2 k_3 + k_3 k_1}}
  2. BAmplitude: F(k1+k2)k1k2+k2k3+k3k1\dfrac{F(k_1 + k_2)}{k_1 k_2 + k_2 k_3 + k_3 k_1}, Frequency: 12πk1k2+k2k3+k3k1M(k1+k2)\dfrac{1}{2\pi} \sqrt{\dfrac{k_1 k_2 + k_2 k_3 + k_3 k_1}{M(k_1 + k_2)}}
  3. CAmplitude: F(k2+k3)k1k2+k2k3+k3k1\dfrac{F(k_2 + k_3)}{k_1 k_2 + k_2 k_3 + k_3 k_1}, Frequency: 12πk1k2+k2k3+k3k1M(k2+k3)\dfrac{1}{2\pi} \sqrt{\dfrac{k_1 k_2 + k_2 k_3 + k_3 k_1}{M(k_2 + k_3)}}
  4. DAmplitude: Fk1+k2+k3\dfrac{F}{k_1 + k_2 + k_3}, Frequency: 12πk1+k2+k3M\dfrac{1}{2\pi} \sqrt{\dfrac{k_1 + k_2 + k_3}{M}}

Correct answer

C. Amplitude: F(k2+k3)k1k2+k2k3+k3k1\dfrac{F(k_2 + k_3)}{k_1 k_2 + k_2 k_3 + k_3 k_1}, Frequency: 12πk1k2+k2k3+k3k1M(k2+k3)\dfrac{1}{2\pi} \sqrt{\dfrac{k_1 k_2 + k_2 k_3 + k_3 k_1}{M(k_2 + k_3)}}

Step-by-step solution

The springs k2k_2 and k3k_3 are connected in series. Their equivalent spring constant is:

k23=k2k3k2+k3k_{23} = \dfrac{k_2 k_3}{k_2 + k_3}

This combination is connected in parallel with spring k1k_1. The total equivalent spring constant of the system is:

keq=k1+k23=k1+k2k3k2+k3=k1k2+k2k3+k3k1k2+k3k_{eq} = k_1 + k_{23} = k_1 + \dfrac{k_2 k_3}{k_2 + k_3} = \dfrac{k_1 k_2 + k_2 k_3 + k_3 k_1}{k_2 + k_3}

When a constant force FF is applied to the block, the equilibrium position shifts by a distance x0x_0 given by:

x0=Fkeqx_0 = \dfrac{F}{k_{eq}}

Since the block is initially at rest at the unstretched position, it will perform simple harmonic motion about the new equilibrium position. The amplitude AA of this motion is equal to the shift in the equilibrium position:

A=x0=Fkeq=F(k2+k3)k1k2+k2k3+k3k1A = x_0 = \dfrac{F}{k_{eq}} = \dfrac{F(k_2 + k_3)}{k_1 k_2 + k_2 k_3 + k_3 k_1}

The frequency of the oscillation is given by:

f=12πkeqM=12πk1k2+k2k3+k3k1M(k2+k3)f = \dfrac{1}{2\pi} \sqrt{\dfrac{k_{eq}}{M}} = \dfrac{1}{2\pi} \sqrt{\dfrac{k_1 k_2 + k_2 k_3 + k_3 k_1}{M(k_2 + k_3)}}
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