JEE PYQ: Motion in a Straight Line - Question ID e1d5bb605b90 (JEE Main 2019)

ID: e1d5bb605b90JEE Main 2019Single Correct MCQ
In a car race on straight road, car A takes a time t less than car B at the finish and passes finishing point with a speed 'υ\upsilon' more than that of car B. Both the cars start from rest and travel with constant acceleration a1 and a2 respectively. Then 'υ\upsilon' is equal to :

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Step-by-step Explanation

Core Formula & Concept:

In problems involving motion with constant acceleration, the following kinematic relations are fundamental:

  • Displacement (ss) as a function of time (tt) and acceleration (aa): s=ut+12at2s = ut + \tfrac{1}{2} a t^2 where uu is the initial velocity.
  • Final velocity (vv) as a function of initial velocity, acceleration, and time: v=u+atv = u + a t
  • Relation between displacement, initial velocity, final velocity, and acceleration (without explicit time): v2=u2+2asv^2 = u^2 + 2 a s

Since both cars start from rest, their initial velocities are zero (u=0u = 0). The key idea is to express the race distance in terms of each car’s acceleration and travel time, then relate the time difference and speed difference at the finish.

Step-by-Step Derivation:

Let:

  • a1a_1 = acceleration of car A
  • a2a_2 = acceleration of car B
  • tAt_A = time taken by car A to finish
  • tBt_B = time taken by car B to finish
  • vAv_A = speed of car A at finish
  • vBv_B = speed of car B at finish

1. Express the race distance ss in two ways:

Since both cars cover the same distance ss from rest:

s=12a1tA2(for car A)s = \tfrac{1}{2} a_1 t_A^2 \quad \text{(for car A)} s=12a2tB2(for car B)s = \tfrac{1}{2} a_2 t_B^2 \quad \text{(for car B)}

Equate the two expressions:

12a1tA2=12a2tB2\tfrac{1}{2} a_1 t_A^2 = \tfrac{1}{2} a_2 t_B^2 a1tA2=a2tB2(1)\Rightarrow a_1 t_A^2 = a_2 t_B^2 \quad \text{(1)}

2. Relate the time difference:

Car A finishes tt seconds earlier than car B:

tB=tA+t(2)t_B = t_A + t \quad \text{(2)}

3. Express the speed difference at finish:

Since both cars start from rest, their final speeds are:

vA=a1tAv_A = a_1 t_A vB=a2tBv_B = a_2 t_B

The problem states that car A passes the finish with speed vv more than car B:

vA=vB+vv_A = v_B + v a1tA=a2tB+v(3)\Rightarrow a_1 t_A = a_2 t_B + v \quad \text{(3)}

4. Substitute tBt_B from (2) into (1):

a1tA2=a2(tA+t)2a_1 t_A^2 = a_2 (t_A + t)^2 Expand the right side: a1tA2=a2(tA2+2tAt+t2)a_1 t_A^2 = a_2 (t_A^2 + 2 t_A t + t^2) a1tA2=a2tA2+2a2tAt+a2t2a_1 t_A^2 = a_2 t_A^2 + 2 a_2 t_A t + a_2 t^2 Bring all terms to one side: (a1a2)tA22a2ttAa2t2=0(a_1 - a_2) t_A^2 - 2 a_2 t t_A - a_2 t^2 = 0

This is a quadratic in tAt_A. However, instead of solving for tAt_A, we use equation (3) to eliminate tAt_A.

5. Express vv in terms of tAt_A and tt:

From (3): v=a1tAa2tBv = a_1 t_A - a_2 t_B Substitute tB=tA+tt_B = t_A + t: v=a1tAa2(tA+t)v = a_1 t_A - a_2 (t_A + t) v=(a1a2)tAa2t(4)v = (a_1 - a_2) t_A - a_2 t \quad \text{(4)}

6. Solve for tAt_A from equation (1):

From (1): a1tA2=a2tB2a_1 t_A^2 = a_2 t_B^2 tA2=a2a1tB2\Rightarrow t_A^2 = \frac{a_2}{a_1} t_B^2 tA=a2a1tB\Rightarrow t_A = \sqrt{\frac{a_2}{a_1}} t_B Substitute tB=tA+tt_B = t_A + t: tA=a2a1(tA+t)t_A = \sqrt{\frac{a_2}{a_1}} (t_A + t) Square both sides: tA2=a2a1(tA+t)2t_A^2 = \frac{a_2}{a_1} (t_A + t)^2 a1tA2=a2(tA+t)2a_1 t_A^2 = a_2 (t_A + t)^2 This brings us back to the earlier quadratic. Instead, let’s use a substitution to simplify.

7. Introduce a ratio variable:

Let k=tAtk = \frac{t_A}{t}. Then tA=ktt_A = k t, and from (2): tB=tA+t=kt+t=(k+1)tt_B = t_A + t = k t + t = (k + 1) t Substitute into (1): a1(kt)2=a2((k+1)t)2a_1 (k t)^2 = a_2 ((k + 1) t)^2 a1k2t2=a2(k+1)2t2a_1 k^2 t^2 = a_2 (k + 1)^2 t^2 Cancel t2t^2: a1k2=a2(k+1)2a_1 k^2 = a_2 (k + 1)^2 a1a2=(k+1)2k2\Rightarrow \frac{a_1}{a_2} = \frac{(k + 1)^2}{k^2} Take square roots (assuming positive accelerations and times): a1a2=k+1k\sqrt{\frac{a_1}{a_2}} = \frac{k + 1}{k} ka1a2=k+1\Rightarrow k \sqrt{\frac{a_1}{a_2}} = k + 1 k(a1a21)=1\Rightarrow k \left( \sqrt{\frac{a_1}{a_2}} - 1 \right) = 1 k=1a1a21=a2a1a2\Rightarrow k = \frac{1}{\sqrt{\frac{a_1}{a_2}} - 1} = \frac{\sqrt{a_2}}{\sqrt{a_1} - \sqrt{a_2}}

8. Express vv in terms of kk and tt:

From (4): v=(a1a2)tAa2tv = (a_1 - a_2) t_A - a_2 t Substitute tA=ktt_A = k t: v=(a1a2)kta2tv = (a_1 - a_2) k t - a_2 t v=t[(a1a2)ka2]v = t \left[ (a_1 - a_2) k - a_2 \right] Substitute k=a2a1a2k = \frac{\sqrt{a_2}}{\sqrt{a_1} - \sqrt{a_2}}: v=t[(a1a2)a2a1a2a2]v = t \left[ (a_1 - a_2) \frac{\sqrt{a_2}}{\sqrt{a_1} - \sqrt{a_2}} - a_2 \right] Simplify the numerator: (a1a2)=(a1a2)(a1+a2)(a_1 - a_2) = (\sqrt{a_1} - \sqrt{a_2})(\sqrt{a_1} + \sqrt{a_2}) Thus: (a1a2)a2a1a2=(a1+a2)a2(a_1 - a_2) \frac{\sqrt{a_2}}{\sqrt{a_1} - \sqrt{a_2}} = (\sqrt{a_1} + \sqrt{a_2}) \sqrt{a_2} So: v=t[(a1+a2)a2a2]v = t \left[ (\sqrt{a_1} + \sqrt{a_2}) \sqrt{a_2} - a_2 \right] v=t[a1a2+a2a2]v = t \left[ \sqrt{a_1 a_2} + a_2 - a_2 \right] v=ta1a2v = t \sqrt{a_1 a_2}

Thus, the correct expression for vv is:

v=a1a2tv = \sqrt{a_1 a_2} t Common Traps & Exam Tip:

Students often make these mistakes:

  • Incorrectly relating time and speed: Many assume that the speed difference is directly proportional to the acceleration difference, ignoring the quadratic relation between time and distance.
  • Algebraic errors in substitution: The quadratic in tAt_A can be messy; substituting a ratio variable (like k=tA/tk = t_A / t) simplifies the algebra.
  • Misapplying kinematic equations: Forgetting that both cars start from rest and using incorrect initial conditions leads to wrong expressions.
  • Overcomplicating the problem: Some students try to solve for tAt_A explicitly, which is unnecessary. The key is to express everything in terms of the given time difference tt.

Exam Tip: Always start by writing down known quantities and relations. Use symmetry and substitution to reduce variables. In this problem, introducing k=tA/tk = t_A / t simplifies the algebra significantly.

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