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5 Questions around this concept.
The position of the centre of mass of a uniform semi-circular wire of radius ${ }^{\prime} R^{\prime}$ placed in $x-y$ plane with its centre at the origin and the line joining its ends as $x$-axis is given by $\left(0, \frac{x R}{\pi}\right)$. Then, the value of $|x|$ is $\qquad$:
A train of mass M is moving on a circular track of radius ' R ' with constant speed V. The length of the train is half of the perimeter of the track. The linear momentum of the train will be
The distance of the center of mass of a semicircular ring from centre of the ring is
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Have a look at the figure of semicircular ring.
Since it is symmetrical about $y$-axis on both sides of the origin
So we can say that its $x_{c m}=0$
And its $z_{c m}=0$ as z-coordinate is zero for all particles of semicircular ring.
Now, we will calculate its $y_{\mathrm{cm}}$ which is given by
$
y_{c m}=\frac{\int y \cdot d m}{\int d m}
$
So, Take a small elemental arc of mass dm at an angle $\theta$ from the x -direction.
Its angular width $\mathrm{d} \theta$
If the radius of the ring is R then its y coordinate will be $\mathrm{R} \sin \theta$
So, $d m=\frac{M}{\pi R} * R d \theta=\frac{M}{\pi} d \theta$
As, $y_{c m}=\frac{\int y \cdot d m}{\int d m}$
So, $y_{c m}=\frac{\int_0^\pi \frac{M}{\pi R} \times R \times R \sin \theta d \theta}{M}=\frac{R}{\pi} \int_0^\pi \sin \theta d \theta=\frac{2 R}{\pi}$
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