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NEET PHYSICSMedium

A car accelerates from rest at a constant rate α\alpha for some time, after which it decelerates at a constant rate β\beta and comes to rest. If the total time elapsed is tt, then the maximum velocity acquired by the car is:

A

(α2+β2αβ)t\left( \frac{\alpha^2 + \beta^2}{\alpha\beta} \right) t

B

(α2β2αβ)t\left( \frac{\alpha^2 - \beta^2}{\alpha\beta} \right) t

C

(α+β)tαβ\frac{(\alpha + \beta) t}{\alpha\beta}

D

αβtα+β\frac{\alpha\beta t}{\alpha + \beta}

Step-by-Step Solution

  1. Define Variables: Let the maximum velocity acquired be vmaxv_{max}. Let the time taken to accelerate be t1t_1 and the time taken to decelerate be t2t_2. The total time is t=t1+t2t = t_1 + t_2.
  2. Analyze Acceleration Phase: The car starts from rest (u=0u=0) and accelerates at α\alpha. Using the first equation of motion (v=u+atv = u + at) : vmax=0+αt1    t1=vmaxαv_{max} = 0 + \alpha t_1 \implies t_1 = \frac{v_{max}}{\alpha}
  3. Analyze Deceleration Phase: The car starts from vmaxv_{max} and decelerates at β\beta to rest (v=0v=0). 0=vmaxβt2    vmax=βt2    t2=vmaxβ0 = v_{max} - \beta t_2 \implies v_{max} = \beta t_2 \implies t_2 = \frac{v_{max}}{\beta}
  4. Combine and Solve: Substitute t1t_1 and t2t_2 into the total time equation: t=t1+t2=vmaxα+vmaxβt = t_1 + t_2 = \frac{v_{max}}{\alpha} + \frac{v_{max}}{\beta} t=vmax(1α+1β)=vmax(α+βαβ)t = v_{max} \left( \frac{1}{\alpha} + \frac{1}{\beta} \right) = v_{max} \left( \frac{\alpha + \beta}{\alpha\beta} \right) vmax=αβtα+βv_{max} = \frac{\alpha\beta t}{\alpha + \beta}
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