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Moment of inertia of a SOLID SPHERE is considered one the most difficult concept.
9 Questions around this concept.
Two identical spherical balls of mass M and radius R each are stuck on two ends of a rod of length 2R and mass M (see figure) The moment of inertia (MR2) of the system about the axis passing perpendicularly through the centre of the rod is :
Let I=Moment of inertia of a SOLID SPHERE about an axis through its centre
To calculate I
Consider a sphere of mass M, radius R and centre O. Mass per unit volume of the sphere = $
\rho=\frac{M}{\frac{4}{3} \pi R^3}
$
Take an elementary disc of mass dm, whose centre is C and which lies between two planes perpendicular to the axis at a distance x and x + dx from its centre
Disc has Radius=AC and thickness =dx. As shown in figure
So, $A C=\sqrt{R^2-x^2}$
So, $d V=\pi\left(R^2-x^2\right) d x$
$
d m=\rho d V=\frac{3 M}{4 \pi R^3} * \pi\left(R^2-x^2\right) d x=\frac{3 M}{4 R^3} *\left(R^2-x^2\right) d x
$
The moment of inertia of the elementary disc about the axis
$
d I=\int \frac{(A C)^2 d m}{2} \quad\left(\because I_{d i s c}=\frac{m R^2}{2}\right)
$
Now integrate this dl between the limits $x=-R$ to $x=+R$ |
$
\begin{aligned}
& I=\int d I=\int \frac{(A C)^2 d m}{2} \\
& =\int_{-R}^R\left(R^2-x^2\right) \frac{3 M}{8 R^3}\left(R^2-x^2\right) d x \\
& =\int_{-R}^R \frac{3 M}{8 R^3}\left(R^2-x^2\right)^2 d x \\
& =\frac{3 M}{8 R^3} \int_{-R}^R\left(R^4-2 R^2 x^2+x^4\right) d x \\
& \Rightarrow \mathbf{I}=\frac{2}{5} \mathbf{M R}^2
\end{aligned}
$
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