Given:
Step 1: Using Kinematic Equation
We use the third equation of motion:
\[ v^2 = v_0^2 + 2 a s \]
Solving for \( s \) (displacement):
\[ s = \frac{v^2 - v_0^2}{2a} \]
Step 2: Average Velocity Formula
Average velocity is given by:
\[ \bar{v} = \frac{\text{total displacement}}{\text{total time}} \]
\[ \bar{v} = \frac{s}{t} = \frac{v^2 - v_0^2}{2at} \]
Step 3: Conclusion
The correct answer is:
\[ \bar{v} = \frac{v^2 - v_0^2}{2at} \]
Answer: The correct option is C.
To find the average velocity, we use the formula for average velocity when acceleration is constant: \[ \bar{v} = \frac{v + v_0}{2} \] where:
\( v_0 \) is the initial velocity,
\( v \) is the final velocity after time \( t \).
Now, using the kinematic equation: \[ v^2 = v_0^2 + 2a \cdot d \] where:
\( v_0 \) is the initial velocity,
\( v \) is the final velocity,
\( a \) is the acceleration,
\( d \) is the distance traveled.
Thus, the average velocity formula is derived from the kinematic equation. We calculate the average velocity over the time interval \( t \) as: \[ \bar{v} = \frac{v^2 - v_0^2}{2at} \]
Therefore, the correct answer is (C).
The circuit shown in the figure contains two ideal diodes \( D_1 \) and \( D_2 \). If a cell of emf 3V and negligible internal resistance is connected as shown, then the current through \( 70 \, \Omega \) resistance (in amperes) is: 