Tom and Jerry relive!

Tom , on seeing jerry at a distance d d , starts with velocity u u and moves with acceleration α \alpha in order to catch it . While jerry with acceleration β \beta starts from rest. For what value of β \beta will the tom overtake the jerry ?

\bullet d = 5 m \displaystyle d= 5\text{ m}
\bullet u = 5 m/s \displaystyle u= 5\text{ m/s}
\bullet α = 2.5 m/s 2 \displaystyle \alpha= 2.5\text{ m/s}^2
\bullet g = 10 m/s 2 \displaystyle g=10\text{ m/s}^2


The answer is 5.

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2 solutions

Parth Sankhe
Oct 9, 2018

I think the question means at what value of B will jerry just escape. This can be solved with the help of relative motion. Just assume Jerry is stationary and just give his acceleration to Tom in the opposite direction. We would have 2 equations, (B - A)t = u ; d = ut + 0.5(B - A)t^2. Solving these would give you the value of B as 5

i agree with you. or the question can be : 'For what maximum value of β \beta will Tom overtake Jerry ?'

The Linh Nguyen - 2 years, 1 month ago
Tom Engelsman
May 1, 2021

Let us utilize the equation x = v 0 t + 1 2 a t 2 x = v_{0}t + \frac{1}{2}at^2 from uniform acceleration kinematics. If Jerry runs a distance x x in t t seconds, then Tom runs a distance d + x d+x to catch him in t t seconds. This can be modeled via:

Tom: d + x = u t + 1 2 α t 2 d+x = ut + \frac{1}{2}\alpha t^2 (i)

Jerry: x = 1 2 β t 2 x = \frac{1}{2}\beta t^2 (ii)

If we substitute (ii) into (i), we end up with a quadratic equation in t t :

d + 1 2 β t 2 = u t + 1 2 α t 2 d + \frac{1}{2}\beta t^2 = ut + \frac{1}{2}\alpha t^2 ;

or 1 2 ( β α ) t 2 u t + d = 0 ; \frac{1}{2}(\beta - \alpha) t^2 - ut + d = 0;

or t = u ± u 2 4 ( d ) ( ( β α ) / 2 ) β α \large t = \frac{u \pm \sqrt{u^2 - 4(d)((\beta-\alpha)/2)}}{\beta-\alpha} (iii).

Tom will just capture Jerry when the discriminant in (iii) equals zero, or:

u 2 4 ( d ) ( ( β α ) / 2 ) = 0 \sqrt{u^2 - 4(d)((\beta-\alpha)/2)} = 0 ;

or 5 2 4 ( 5 ) ( β 2.5 ) ( 1 / 2 ) = 0 ; \sqrt{5^2 - 4(5)(\beta - 2.5)(1/2)} = 0;

or 50 10 β = 0 ; \sqrt{50-10\beta} = 0;

or β = 5 m / s 2 \boxed{\beta = 5 m/s^{2} } .

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