The equation of the wave is given by \( y = A \sin (kx + \omega t) \), where \( A = 0.02 \) m, \( k \) is the wave number, and \( \omega \) is the angular frequency. The general relation for the wave number is \( k = \frac{2\pi}{\lambda} \), and the relation for the angular frequency is \( \omega = 2\pi f \), where \( \lambda \) is the wavelength and \( f \) is the frequency.
Step 1: From the given equation, we have \( k = \pi \) and \( \omega = 8\pi \). Now, using the relation \( k = \frac{2\pi}{\lambda} \), we can find \( \lambda \): \[ \pi = \frac{2\pi}{\lambda} \quad \Rightarrow \quad \lambda = 2 \, \text{m}. \]
Step 2: Next, we use the relation \( v = f\lambda \), where \( v \) is the speed of the wave. We can find the speed using the angular frequency relation \( \omega = 2\pi f \): \[ \omega = 8\pi \quad \Rightarrow \quad f = 4 \, \text{Hz}. \] Now, the speed \( v = f \lambda \) is \[ v = 4 \, \text{Hz} \times 2 \, \text{m} = 8 \, \text{ms}^{-1}. \]
A player can throw a ball to a maximum horizontal distance of 80 m. If he throws the ball vertically with the same velocity, then the maximum height reached by the ball is:
If a man of mass 50 kg is in a lift moving down with a acceleration equal to acceleration due to gravity, then the apparent weight of the man is:
A ball falls freely from a height h on a rigid horizontal plane. If the coefficient of resolution is e, then the total distance travelled by the ball before hitting the plane second time is:
A man weighing 75 kg is standing in a lift. The weight of the man standing on a weighing machine kept in the lift when the lift is moving downwards freely under gravity is: