To determine the speed of water in the stream, we analyze the velocity components of the swimmer relative to the water.
Step 1: Given Data
- Speed of the swimmer relative to water: \( v_s = 0.5 \) m/s
- Angle of swimming with respect to the direction of water flow: \( \theta = 120^\circ \)
- The swimmer aims to reach directly opposite, meaning the net velocity component along the stream should cancel out the water velocity.
Step 2: Resolving the Velocity Components
The swimmer's velocity can be resolved into two components:
- Perpendicular to the stream (across the river): This component determines the actual movement towards the opposite bank.
\[ v_{\perp} = v_s \sin \theta \] - Parallel to the stream (along the river): This component should be equal and opposite to the velocity of water \( v_w \) to cancel out drift.
\[ v_{\parallel} = v_s \cos \theta \] Step 3: Calculating the Speed of Water
Since the swimmer reaches exactly the opposite point, the drift velocity \( v_{\parallel} \) must be equal to the speed of the stream \( v_w \).
\[ v_w = v_s \cos 120^\circ \] Using \( \cos 120^\circ = -\frac{1}{2} \), we substitute:
\[ v_w = 0.5 \times \left(-\frac{1}{2} \right) \] \[ v_w = -0.25 { m/s} \] Since speed is always positive, we take:
\[ v_w = 0.25 { m/s} \] Step 4: Conclusion
Thus, the speed of water in the stream is:
\[ {0.25 { m/s}} \]
Given below are two statements. One is labelled as Assertion (A) and the other is labelled as Reason (R):
Assertion (A): In an insulated container, a gas is adiabatically shrunk to half of its initial volume. The temperature of the gas decreases.
Reason (R): Free expansion of an ideal gas is an irreversible and an adiabatic process. \text{In the light of the above statements, choose the correct answer from the options given below:}
For the circuit shown above, the equivalent gate is:
Find the equivalent resistance between two ends of the following circuit:
The circuit consists of three resistors, two of \(\frac{r}{3}\) in series connected in parallel with another resistor of \(r\).