Let I=Moment of inertia of a solid cone about an axis through its C.O.M
To calculate I
Consider a solid cone of mass M, base radius R , and Height as h
As shown in figure I is about the x axis and through its C.O.M

Now take an elemental disc of mass dm at a distance x from top as shown in figure

As The density of the cone is $\rho=\frac{M}{V}=\frac{M}{\frac{1}{3} \pi R^2 h}$
So, $d m=\rho d V=\rho\left(\pi r^2 d x\right)$
Using similar triangle method we have
$$
\frac{r}{x}=\frac{R}{h}
$$
$\mathrm{So}_{,} x=\frac{r h}{R} \Rightarrow d x=\frac{h d r}{R}$
For an elemental disc moment of inertia about $x$ - axis is given by
$$
d I=\frac{1}{2} * d m r^2
$$
For an elemental disc moment of inertia about the x-axis is given by
$$
d I=\frac{1}{2} * d m r^2
$$
So,
$$
\begin{aligned}
& d I=\frac{1}{2} * d m r^2 \\
& d I=\frac{1}{2} \rho \pi r^2 d x * r^2 \\
& d I=\frac{1}{2} \rho \pi r^2 * r^2 * \frac{h}{R} d r \\
& \int d I=\frac{1}{2} \rho \pi \frac{h}{R} \int r^4 d r \\
& \int d I=\frac{1}{2} * \frac{3 M}{\pi R^2 h} \pi \frac{h}{R} \int_0^R r^4 d r \\
& I=\frac{3}{2} * \frac{M}{R^3} * \frac{R^5}{5} \\
& \mathbf{I}=\frac{\mathbf{3}}{\mathbf{1 0}} * \mathbf{M R}^2
\end{aligned}
$$
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