To solve this problem, we need to find the ratio of the radius of gyration of a solid sphere to that of a thin hollow sphere, both having the same mass \(M\) and radius \(R\).
1. Radius of gyration: The radius of gyration \(K\) of an object is defined as the distance from the axis of rotation at which the entire mass of the body can be assumed to be concentrated to provide a moment of inertia \(I\). Mathematically, \(K = \sqrt{\frac{I}{M}}\).
2. Solid sphere: For a solid sphere, the moment of inertia about its axis is \(I_s = \frac{2}{5}MR^2\). Thus, the radius of gyration \(K_s\) is:
\(K_s = \sqrt{\frac{\frac{2}{5}MR^2}{M}} = \sqrt{\frac{2}{5}R^2} = \frac{R}{\sqrt{5}}\).
3. Thin hollow sphere: For a thin hollow sphere, the moment of inertia about its axis is \(I_h = \frac{2}{3}MR^2\). Thus, the radius of gyration \(K_h\) is:
\(K_h = \sqrt{\frac{\frac{2}{3}MR^2}{M}} = \sqrt{\frac{2}{3}R^2} = \frac{R}{\sqrt{3}}\).
4. Ratio: The ratio of the radii of gyration of the solid sphere to the hollow sphere is given by:
\(\frac{K_s}{K_h} = \frac{\frac{R}{\sqrt{5}}}{\frac{R}{\sqrt{3}}} = \frac{\sqrt{3}}{\sqrt{5}}\).
Simplifying, we multiply both numerator and denominator by \(\sqrt{15}\) to get:
\(\frac{\sqrt{3}}{\sqrt{5}} \times \frac{\sqrt{15}}{\sqrt{15}} = \frac{3}{5}\).
The ratio is therefore 3:5, which matches the given correct option.
A string of length \( L \) is fixed at one end and carries a mass of \( M \) at the other end. The mass makes \( \frac{3}{\pi} \) rotations per second about the vertical axis passing through the end of the string as shown. The tension in the string is ________________ ML.
Consider a water tank shown in the figure. It has one wall at \(x = L\) and can be taken to be very wide in the z direction. When filled with a liquid of surface tension \(S\) and density \( \rho \), the liquid surface makes angle \( \theta_0 \) (\( \theta_0 < < 1 \)) with the x-axis at \(x = L\). If \(y(x)\) is the height of the surface then the equation for \(y(x)\) is: (take \(g\) as the acceleration due to gravity)
A bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) is :
Moment of inertia is defined as the quantity expressed by the body resisting angular acceleration which is the sum of the product of the mass of every particle with its square of a distance from the axis of rotation.
In general form, the moment of inertia can be expressed as,
I = m × r²
Where,
I = Moment of inertia.
m = sum of the product of the mass.
r = distance from the axis of the rotation.
M¹ L² T° is the dimensional formula of the moment of inertia.
The equation for moment of inertia is given by,
I = I = ∑mi ri²
To calculate the moment of inertia, we use two important theorems-