To solve this problem, we need to find the velocity of the particle when the acceleration becomes zero. Let's go through the problem step-by-step:
Given:
- Acceleration \( f = f_0 \left(1 - \frac{t}{T}\right) \)
- Initial velocity \( v_x(t=0) = 0 \)
- We need to find the velocity \( v_x \) at the instant \( t = T \) when \( f = 0 \).
Step 1: Find the time when acceleration is zero.
- Set \( f = 0 \) and solve for \( t \):
- \( f_0 \left(1 - \frac{t}{T}\right) = 0 \)
- This gives \( 1 - \frac{t}{T} = 0 \Rightarrow t = T \).
Step 2: Integrate acceleration to get velocity.
- The velocity is the integral of acceleration with respect to time:
- \( v_x = \int_0^T f \, dt = \int_0^T f_0 \left(1 - \frac{t}{T}\right) \, dt \)
- \( v_x = \int_0^T \left(f_0 - \frac{f_0}{T} t\right) \, dt \)
- This separates into: \( v_x = f_0 \int_0^T 1 \, dt - \frac{f_0}{T} \int_0^T t \, dt \)
- \( v_x = f_0 \left[t\right]_0^T - \frac{f_0}{T} \left[\frac{t^2}{2}\right]_0^T \)
Step 3: Evaluate the integrals.
- First term: \( f_0 [T - 0] = f_0 T \)
- Second term: \(- \frac{f_0}{T} \left[\frac{T^2}{2} - \frac{0^2}{2}\right] = - \frac{f_0}{T} \cdot \frac{T^2}{2} = - \frac{f_0 T}{2} \)
Step 4: Combine results to find velocity.
- Combining these results, we have:
- \( v_x = f_0 T - \frac{f_0 T}{2} = \frac{f_0 T}{2} \)
Conclusion:
- Thus, the velocity of the particle when the acceleration becomes zero is \( \frac{1}{2}f_0 T \).