Maximum Velocity with Two-Phase Motion – Rankers Physics

Graphs of Motion: Practice Problem & Solution

A car accelerates from rest at a constant rate \(\alpha\) for some time after which it decelerates at a constant rate \(\beta\) and comes to rest. If total time elapsed is t, then maximum velocity acquired by car will be: (1994)
\(\frac{(\alpha^2 - \beta^2)t}{\alpha\beta}\)
\(\frac{(\alpha^2 + \beta^2)t}{\alpha\beta}\)
\(\frac{(\alpha + \beta)t}{\alpha\beta}\)
\(\frac{\alpha\beta t}{\alpha + \beta}\)

Solution Explained:

To solve this problem, we apply the core principles of Graphs of Motion. Understanding the underlying formula is key to arriving at the correct answer below:

Let (v_{max}) be the maximum velocity. Time to accelerate: \(t_1 = \frac{v_{max}}{\alpha}). Time to decelerate: (t_2 = \frac{v_{max}}{\beta}). Total time (t = t_1 + t_2 = \frac{v_{max}}{alpha} + \frac{v_{max}}{beta} = v_{max}\left(\frac{1}{alpha} + \frac{1}{\beta}\right) = v_{max}\left(\frac{\beta + \alpha}{\alpha\beta}\right)). Solving for \(v_{max}): (v_{max} = \frac{\alpha\beta t}{\alpha + \beta}).

Leave a Reply

Your email address will not be published. Required fields are marked *