
To solve the problem of finding the ratio of kinetic energies \( \frac{(\text{K.E.})_A}{(\text{K.E.})_B} \), we need to understand the physics involved in a simple pendulum executing circular motion.
The key points to consider are:
Let's go through the solution step-by-step:
The correct answer is therefore \(\frac{5}{1}\).
To solve this problem, we apply energy conservation between points \( A \) and \( B \).
Step 1: Energy conservation between \( A \) and \( B \):
\(\frac{1}{2} m V_L^2 = \frac{1}{2} m V_B^2 + mg(2L)\)
where:
- \( V_L \) is the velocity at point \( A \) (the lowest point),
- \( V_B \) is the velocity at point \( B \) (the highest point).
Rearranging the equation:
\(V_L^2 = V_B^2 + 4gL\)
Step 2: Calculate \( V_L \) (Minimum Velocity at \( A \)):
Since the bob must just complete the circular path, the minimum velocity at \( A \) must be such that:
\(V_L = \sqrt{5gL}\)
Step 3: Calculate \( V_B \):
Applying energy conservation:
\(\frac{1}{2} m V_L^2 = \frac{1}{2} m V_B^2 + mg(2L)\)
Substitute \(V_L = \sqrt{5gL}\):
\(\frac{1}{2} m (5gL) = \frac{1}{2} m V_B^2 + 2mgL\)
Simplifying:
\(\frac{5}{2} mgL = \frac{1}{2} m V_B^2 + 2mgL\)
\(\frac{1}{2} m V_B^2 = \frac{5}{2} mgL - 2mgL\)
\(V_B^2 = gL\)
\(V_B = \sqrt{gL}\)
Step 4: Calculate the ratio of kinetic energies:
\(\left(\frac{\text{(K.E.)}_A}{\text{(K.E.)}_B}\right) = \frac{\frac{1}{2} m V_L^2}{\frac{1}{2} m V_B^2} = \frac{V_L^2}{V_B^2} = \frac{5gL}{gL} = 5\)
Thus, the ratio of kinetic energies \( \left(\frac{\text{(K.E.)}_A}{\text{(K.E.)}_B}\right) \) is 5 : 1.
The Correct Answer is: 5 : 1
A body of mass $100 \;g$ is moving in a circular path of radius $2\; m$ on a vertical plane as shown in the figure. The velocity of the body at point A is $10 m/s.$ The ratio of its kinetic energies at point B and C is: (Take acceleration due to gravity as $10 m/s^2$)

A sportsman runs around a circular track of radius $ r $ such that he traverses the path ABAB. The distance travelled and displacement, respectively, are:


Consider the sound wave travelling in ideal gases of $\mathrm{He}, \mathrm{CH}_{4}$, and $\mathrm{CO}_{2}$. All the gases have the same ratio $\frac{\mathrm{P}}{\rho}$, where P is the pressure and $\rho$ is the density. The ratio of the speed of sound through the gases $\mathrm{v}_{\mathrm{He}}: \mathrm{v}_{\mathrm{CH}_{4}}: \mathrm{v}_{\mathrm{CO}_{2}}$ is given by