Moment of inertia of a SOLID SPHERE is considered one the most difficult concept.
8 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 :
Absorption of water by the plant cell walls by surface attraction is called
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 the figure
$\mathrm{So}_{,} A C=\sqrt{R^2-x^2}$
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
$$
d I=\int(A C)^2 d m
$$
Now integrate this dl between the limits $x=-R$ to $x=+R$
$$
\begin{aligned}
& I=\int d I=\int(A C)^2 d m \\
& =\int_{-R}^R\left(R^2-x^2\right) * \frac{3 M}{4 R^3} *\left(R^2-x^2\right) \cdot d x \\
& =\int_{-R}^R \frac{3 M}{4 R^3} *\left(R^2-x^2\right)^2 \cdot d x \\
& =\frac{3 M}{4 R^3} \int_{-R}^R\left(R^4-2 R^2 x^2+x^4\right) d x \\
& \Rightarrow \mathbf{I}=\frac{2}{5} * \mathbf{M R}^2
\end{aligned}
$$
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