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Question: In a car race, car A takes time \( t \) less than car B at the finish and passes the finishing point...

In a car race, car A takes time tt less than car B at the finish and passes the finishing point with speed vv more than that of the car B. Assuming both the cars starts from rest and travel with the constant acceleration a1{a_1} and a2{a_2} respectively. Show that v=a1a2tv = \sqrt {{a_1}{a_2}} t .

Explanation

Solution

We need to use Newton’s laws of kinematics, v2u2=2as{v^2} - {u^2} = 2as and s=ut+12at2s = ut + \dfrac{1}{2}a{t^2} . Since these are two bodies in motion, these laws of kinematics can be used for each car separately to find a relation between the two.

Formulas used We will be using the formula v2u2=2as{v^2} - {u^2} = 2as where vv is the final velocity of the body, uu is the initial velocity of the body, aa is the acceleration the body acquired and ss the displacement travelled by the body. Also we would be using s=ut+12at2s = ut + \dfrac{1}{2}a{t^2} where tt will be the time taken to travel the distance ss .

Complete Answer:
We all know that there are few laws of kinematics that will be used to solve most of the problems that are related to kinematics. The third law of kinematics states v2u2=2as{v^2} - {u^2} = 2as . But if you investigate in accordance with this problem you can see that the bodies are starting from rest and hence u=0u = 0
If u=0u = 0 then the law would be, v20=2as{v^2} - 0 = 2as . Simplifying the equation further and applying square root on both sides we get,
v=2asv = \sqrt {2as} .
Similarly, you can find that the second law of kinematics states, s=ut+12at2s = ut + \dfrac{1}{2}a{t^2} . Again, here u=0u = 0 because the cars begin at rest. Hence the equation becomes, s=(0)t+12at2s = (0)t + \dfrac{1}{2}a{t^2} . Simplifying it further,
t2=2sa\Rightarrow {t^2} = \dfrac{{2s}}{a} or t=2sat = \sqrt {\dfrac{{2s}}{a}} .
Now, in the problem, since Car A takes time tt less than car B, let us assume that the time taken by car B is TT and so time taken by car A becomes TtT - t . It also passes the finish line with a speed vv more than B. So let the speed of car B be vv' and the speed of car A be v+vv + v' .
Now let us apply the laws of kinematics on each car, starting with car A,
v+v=2a1sv + v' = \sqrt {2{a_1}s} and Tt=2sa1T - t = \sqrt {\dfrac{{2s}}{{{a_1}}}}
For car B,
v=2a2sv' = \sqrt {2{a_2}s} and T=2sa2T = \sqrt {\dfrac{{2s}}{{{a_2}}}}
Now substitute the values of v=2a2sv' = \sqrt {2{a_2}s} and T=2sa2T = \sqrt {\dfrac{{2s}}{{{a_2}}}} in the equations for car A.
v+(2a2s)=2a1sv + (\sqrt {2{a_2}s} ) = \sqrt {2{a_1}s} and 2sa2t=2sa1\sqrt {\dfrac{{2s}}{{{a_2}}}} - t = \sqrt {\dfrac{{2s}}{{{a_1}}}}
v=2a1s2a2s\Rightarrow v = \sqrt {2{a_1}s} - \sqrt {2{a_2}s} and 2sa22sa1=t\sqrt {\dfrac{{2s}}{{{a_2}}}} - \sqrt {\dfrac{{2s}}{{{a_1}}}} = t
Divide the final equations to give you the value of vt\dfrac{v}{t}
2a1s2a2s2sa22sa1=vt\dfrac{{\sqrt {2{a_1}s} - \sqrt {2{a_2}s} }}{{\sqrt {\dfrac{{2s}}{{{a_2}}}} - \sqrt {\dfrac{{2s}}{{{a_1}}}} }} = \dfrac{v}{t}
vt=a1a21a21a1×2s2s\Rightarrow \dfrac{v}{t} = \dfrac{{\sqrt {{a_1}} - \sqrt {{a_2}} }}{{\sqrt {\dfrac{1}{{{a_2}}}} - \sqrt {\dfrac{1}{{{a_1}}}} }} \times \dfrac{{\sqrt {2s} }}{{\sqrt {2s} }}
Taking L.C.M of the denominator and solving further we get,
vt=a1a2a1a2×a1a2\dfrac{v}{t} = \dfrac{{\sqrt {{a_1}} - \sqrt {{a_2}} }}{{\sqrt {{a_1}} - \sqrt {{a_2}} }} \times \sqrt {{a_1}{a_2}}
Eliminating the common terms, we get,
vt=a1a2\dfrac{v}{t} = \sqrt {{a_1}{a_2}}
v=a1a2×t\Rightarrow v = \sqrt {{a_1}{a_2}} \times t .

Note:
Although we changed most of the terms for each car A and B, we can see that the distance was never changed, this is because both the cars travelled the same distance from rest to complete the rest.