In this problem, we need to determine the speed of a particle on the rim of a wheel rolling on a plane surface, at the same level as the center of the wheel. Let's break down the problem step-by-step:
\[ 2V = 8 \, \text{m/s} \]
\[ V = 4 \, \text{m/s} \]
\[ v_{\text{resultant}} = \sqrt{V^2 + V^2} = \sqrt{4^2 + 4^2} \]
\[ v_{\text{resultant}} = \sqrt{16 + 16} \]
\[ v_{\text{resultant}} = \sqrt{32} \]
\[ v_{\text{resultant}} = 4\sqrt{2} \, \text{m/s} \]
Given that the speed of the particle at the highest point of the rim is 8 m/s, and the wheel is rolling without slipping, the speed at any point on the rim is the sum of the velocity of the center of the wheel and the velocity due to the rotational motion.
Let:
- \( V_B = 8 \, \text{m/s} \) (speed at the highest point of the rim),
- \( V = 4 \, \text{m/s} \) (speed of the center of the wheel),
- \( V_P = \sqrt{2}V \) (velocity at point \( P \)).
Since the wheel is rolling without slipping, the speed at point \( P \) (which is the same level as the center of the wheel) will be: \[ V_P = \sqrt{2} \times 4 = 4\sqrt{2} \, \text{m/s} \]
Thus, the correct answer is (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:



Two cells of emf 1V and 2V and internal resistance 2 \( \Omega \) and 1 \( \Omega \), respectively, are connected in series with an external resistance of 6 \( \Omega \). The total current in the circuit is \( I_1 \). Now the same two cells in parallel configuration are connected to the same external resistance. In this case, the total current drawn is \( I_2 \). The value of \( \left( \frac{I_1}{I_2} \right) \) is \( \frac{x}{3} \). The value of x is 1cm.
If $ \theta \in [-2\pi,\ 2\pi] $, then the number of solutions of $$ 2\sqrt{2} \cos^2\theta + (2 - \sqrt{6}) \cos\theta - \sqrt{3} = 0 $$ is:
The term independent of $ x $ in the expansion of $$ \left( \frac{x + 1}{x^{3/2} + 1 - \sqrt{x}} \cdot \frac{x + 1}{x - \sqrt{x}} \right)^{10} $$ for $ x>1 $ is: