Rotational Dynamics
Fig. shows a uniform solid block of mass $$M$$ and edge lengths $$a$$, $$b $$ and $$ c $$ . Its M.I about an axis passing through one corner and perpendicular (as shown) to the large face of the block is :
A uniform disc of radius $$R$$ has a round disc of radius $$R/3$$ cut as shown in fig. The mass of the remaining (shaded) portion of the disc equals $$M$$. Find the moment of inertia of such a disc relative to the axis passing through geometrical centre of original disc and perpendicular to the plane of the disc.
Given: A uniform disc of radius R has a round disc of radius R/3 cut as shown in fig. The mass of the remaining (shaded) portion of the disc equals M.
To find the moment of inertia of such a disc relative to the axis passing through geometrical centre of original disc and perpendicular to the plane of the disc.
Solution:
Moment of inertia of the disc,
$$I=I_{remain}+I_{R/3}\\\implies I_{remain}=I-I_{R/3}$$
Now using the values we get
$$I_{remain}=\dfrac {MR^2}{2}-\left[\dfrac {\dfrac M4\left(\dfrac R3\right)^2}{2}+\dfrac M4\left(\dfrac R3\right)^2\right]\\\implies I_{remain}=\dfrac {MR^2}{2}-\left[\dfrac {MR^2}{72}+\dfrac {MR^2}{36}\right]\\\implies I_{remain}=\dfrac {36MR^2-MR^2-2MR^2}{72}\\\implies I_{remain}=\dfrac {33MR^2}{72}\\\implies I_{remain}=\dfrac {11MR^2}{24}$$
is the the moment of inertia of such a disc relative to the axis passing through geometrical centre of original disc and perpendicular to the plane of the disc.
Fig. shows a uniform solid block of mass $$M$$ and edge lengths $$a$$, $$b $$ and $$ c $$ . Its M.I about an axis passing through one corner and perpendicular (as shown) to the large face of the block is :
The M.I of solid cylinder of mass $$'M'$$, length $$'l'$$ and radius $$'R'$$ about a transverse axis passing through its centre is :
The surface density ($$mass/area$$) of a circular disc of radius $$a$$ depends on the distance from the center of $$ \rho (r) = A + Br$$. Find its moment of inertia about the line perpendicular to the plane of the disc through its centre.
The moment of inertia of a uniform solid right circular cone of mass $$10\ kg$$, height $$2\ m$$ and vertical angle $$90^o$$ above a diameter of its base is:
The moment of inertia of the system about the center of ring will be
Two loops P and Q are made from a same uniform wire. The radii of P and Q are $$r_1$$ and $$r_2$$ respectively and their moments of inertia are $$l_1$$ and $$l_2$$ respectively. If $$\dfrac{l_2}{l_1}$$ = 4, then $$\dfrac{r_2}{r_1}$$ is equal to:
A disc of radius $$R$$, is cut from a disc of radius $$R_{2}$$ as shown in figure. if the disc left has mass $$M$$ then find the moment of inertia of the disc left about an axis passing through its centre and perpendicular to its plane
If the mass of the hydrogen atom is $$1.7\times 10^{-24}\ g$$ and interatomic distance in a molecule of hydrogen is $$4\times 10^{-8}\ cm$$, then the moment of inertia [in $$kg-m^{2}$$] of a molecule of hydrogen about the axis passing through the centre of mass and perpendicular to the line joining the atoms will be:-
A lamina is made by removing a small disc of diameter 2R from a bigger disc of uniform mass density and radius 2R, as shown in the figure. The moment of inertia of this lamina about axes passing through O and P is $$l_o $$ and $$l_p$$,respectively. Both these axes are perpendicular to the plane of the lamina. The ratio $$\dfrac {l_p}{l_o}$$ to the nearest integer is :