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Center of Mass question

2021 · 22 Jul · Shift 2 · Q70
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  5. /2021 · 22 Jul · Shift 2 · Q70

Center of Mass question

2021 · 22 Jul · Shift 2 · Q70

JEE MainPhysicsCenter of MassNumerical+4 / −1
The position of the centre of mass of a uniform semi-circular wire of radius 'R' placed in x-y plane with its centre at the origin and the line joining its ends as x-axis is given by (0,xRπ)\left( {0,{{xR} \over \pi }} \right)(0,πxR​). Then, the value of | x | is ‾\underline{\hspace{2cm}}​.
Numerical answer
View written solutionFree

Correct answer: 2

  1. Understand the geometry

A uniform semicircular wire of radius RRR lies in the xxx-yyy plane.

  • Its centre is at the origin.
  • The line joining its ends is the xxx-axis.

So the semicircular arc is symmetric about the yyy-axis, and hence the centre of mass must lie on the yyy-axis.

Therefore, xCM=0x_{\text{CM}}=0xCM​=0 and we only need to find yCMy_{\text{CM}}yCM​.

  1. Use the centre of mass formula for a wire

For a uniform wire, yCM=1L∫y dly_{\text{CM}}=\frac{1}{L}\int y\,dlyCM​=L1​∫ydl where LLL is the total length of the wire.

For a semicircular wire of radius RRR, L=πRL=\pi RL=πR

  1. Parameterize the semicircle

Take the upper semicircle: x=Rcos⁡θ,y=Rsin⁡θ,0≤θ≤πx=R\cos\theta, \qquad y=R\sin\theta, \qquad 0\le \theta \le \pix=Rcosθ,y=Rsinθ,0≤θ≤π

The small arc length element is dl=R dθdl=R\,d\thetadl=Rdθ

  1. Compute yCMy_{\text{CM}}yCM​

Substitute into the formula: yCM=1πR∫0π(Rsin⁡θ)(R dθ)y_{\text{CM}}=\frac{1}{\pi R}\int_0^{\pi} (R\sin\theta)(R\,d\theta)yCM​=πR1​∫0π​(Rsinθ)(Rdθ)

yCM=R2πR∫0πsin⁡θ dθy_{\text{CM}}=\frac{R^2}{\pi R}\int_0^{\pi} \sin\theta\,d\thetayCM​=πRR2​∫0π​sinθdθ

yCM=Rπ[−cos⁡θ]0πy_{\text{CM}}=\frac{R}{\pi}\left[-\cos\theta\right]_0^{\pi}yCM​=πR​[−cosθ]0π​

yCM=Rπ[−cos⁡π+cos⁡0]y_{\text{CM}}=\frac{R}{\pi}\left[ -\cos\pi + \cos 0 \right]yCM​=πR​[−cosπ+cos0]

Since cos⁡π=−1\cos\pi=-1cosπ=−1 and cos⁡0=1\cos 0=1cos0=1, yCM=Rπ(1+1)=2Rπy_{\text{CM}}=\frac{R}{\pi}(1+1)=\frac{2R}{\pi}yCM​=πR​(1+1)=π2R​

  1. Compare with the given form

Given position of centre of mass: (0,xRπ)\left(0,\frac{xR}{\pi}\right)(0,πxR​)

We found: (0,2Rπ)\left(0,\frac{2R}{\pi}\right)(0,π2R​)

Thus, x=2x=2x=2 So, ∣x∣=2|x|=2∣x∣=2

  1. Comparison with stored answer

Stored correct answer: 222

Our derived answer matches it.

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