To solve this problem, we need to find the maximum velocity acquired by a car that accelerates from rest at a constant rate \( \alpha \), and then decelerates at a constant rate \( \beta \), with the total time elapsed being \( t \).
- Let \( V \) be the maximum velocity achieved by the car.
- During the acceleration phase, using the equation of motion:
\( V = \alpha \cdot t_1 \),
where \( t_1 \) is the time period of acceleration.
- During the deceleration phase, the car slows down to rest, so:
\( 0 = V - \beta \cdot t_2 \),
where \( t_2 \) is the time period of deceleration.
Hence,
\( V = \beta \cdot t_2 \).
- Since the car comes to rest from its maximum velocity,
\( \alpha \cdot t_1 = \beta \cdot t_2 \).
- The total time \( t \) is the sum of the acceleration and deceleration times:
\( t = t_1 + t_2 \).
- From the equation \( \alpha \cdot t_1 = \beta \cdot t_2 \), we get:
\( t_1 = \frac{\beta}{\alpha} \cdot t_2 \).
- Substitute \( t_1 = \frac{\beta}{\alpha} \cdot t_2 \) in the total time equation:
\( t = \frac{\beta}{\alpha} \cdot t_2 + t_2 = t_2\left(\frac{\beta}{\alpha} + 1\right) = t_2\left(\frac{\beta + \alpha}{\alpha}\right).\)
- Simplifying gives:
\( t_2 = \frac{\alpha}{\alpha + \beta} \cdot t.\)
- Substitute the value of \( t_2 \) into the equation \( V = \beta \cdot t_2 \):
\( V = \beta \cdot \frac{\alpha}{\alpha + \beta} \cdot t = \frac{\alpha \beta}{\alpha + \beta} \cdot t.\)
Therefore, the maximum velocity acquired by the car is
\( \frac{\alpha \beta}{\alpha + \beta} \cdot t \).
Hence, the correct answer is:
\( \left(\frac{\alpha \beta}{\alpha+\beta}\right) t \).