We are asked to find the moment of inertia of a circular ring of mass \( M \) and diameter \( r \) about a tangential axis lying in the plane of the ring.
We use the Parallel Axis Theorem and the known moment of inertia of a ring about its central axes. For a circular ring of radius \( R \) and mass \( M \):
\[ I_{\text{center, diametral}} = \frac{1}{2}MR^2, \quad I_{\text{center, perpendicular}} = MR^2 \]
The Parallel Axis Theorem states:
\[ I = I_{\text{center}} + Md^2 \]
where \( d \) is the distance between the two parallel axes.
Step 1: Given diameter \( r \), so radius \( R = \dfrac{r}{2} \).
Step 2: The axis about which we need the moment of inertia is tangential and lies in the plane of the ring.
The moment of inertia about the diametral axis (through the center, in the plane of the ring) is:
\[ I_{\text{center, diametral}} = \frac{1}{2}MR^2 \]
Step 3: Using the parallel axis theorem to shift from the center to the tangent point (distance \( R \)):
\[ I_{\text{tangent, in-plane}} = I_{\text{center, diametral}} + MR^2 = \frac{1}{2}MR^2 + MR^2 = \frac{3}{2}MR^2 \]
Step 4: Substitute \( R = \frac{r}{2} \):
\[ I_{\text{tangent, in-plane}} = \frac{3}{2}M\left(\frac{r}{2}\right)^2 = \frac{3}{8}Mr^2 \]
The moment of inertia of the circular ring about a tangential axis lying in its plane is:
\[ \boxed{I = \frac{3}{8}Mr^2} \]
A, B and C are disc, solid sphere and spherical shell respectively with the same radii and masses. These masses are placed as shown in the figure. 
The moment of inertia of the given system about PQ is $ \frac{x}{15} I $, where $ I $ is the moment of inertia of the disc about its diameter. The value of $ x $ is:
A sphere of radius R is cut from a larger solid sphere of radius 2R as shown in the figure. The ratio of the moment of inertia of the smaller sphere to that of the rest part of the sphere about the Y-axis is : 
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is:
Two blocks of masses \( m \) and \( M \), \( (M > m) \), are placed on a frictionless table as shown in figure. A massless spring with spring constant \( k \) is attached with the lower block. If the system is slightly displaced and released then \( \mu = \) coefficient of friction between the two blocks.
(A) The time period of small oscillation of the two blocks is \( T = 2\pi \sqrt{\dfrac{(m + M)}{k}} \)
(B) The acceleration of the blocks is \( a = \dfrac{kx}{M + m} \)
(\( x = \) displacement of the blocks from the mean position)
(C) The magnitude of the frictional force on the upper block is \( \dfrac{m\mu |x|}{M + m} \)
(D) The maximum amplitude of the upper block, if it does not slip, is \( \dfrac{\mu (M + m) g}{k} \)
(E) Maximum frictional force can be \( \mu (M + m) g \)
Choose the correct answer from the options given below:
Let \( f : \mathbb{R} \to \mathbb{R} \) be a twice differentiable function such that \[ (\sin x \cos y)(f(2x + 2y) - f(2x - 2y)) = (\cos x \sin y)(f(2x + 2y) + f(2x - 2y)), \] for all \( x, y \in \mathbb{R}. \)
If \( f'(0) = \frac{1}{2} \), then the value of \( 24f''\left( \frac{5\pi}{3} \right) \) is: