JEE PYQ: Motion in a Straight Line - Question ID aa08c2dca467 (JEE Main 2022)

ID: aa08c2dca467JEE Main 2022Single Correct MCQ

A ball is thrown up vertically with a certain velocity so that, it reaches a maximum height h. Find the ratio of the times in which it is at height h3\frac{h}{3} while going up and coming down respectively.

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Step-by-step Explanation

Core Formula & Concept:

To solve this problem, we rely on the kinematic equations of motion under constant acceleration (gravity, gg, acting downward). The key concepts and formulas are:

  • Equation of motion for displacement: s=ut+12at2s = ut + \frac{1}{2} a t^2 Here, ss is displacement, uu is initial velocity, aa is acceleration, and tt is time.
  • Velocity at maximum height: At the highest point, the velocity becomes zero. Using v2=u2+2asv^2 = u^2 + 2as, with v=0v = 0, a=ga = -g, and s=hs = h, we get: 0=u22ghu=2gh0 = u^2 - 2gh \Rightarrow u = \sqrt{2gh} This gives the initial velocity in terms of maximum height hh.
  • Time to reach height yy: We want the time taken to reach height y=h3y = \frac{h}{3} during ascent and descent. Using the displacement equation: y=ut12gt2y = ut - \frac{1}{2} g t^2 This is a quadratic in tt, yielding two roots — one for the upward journey (smaller tt) and one for the downward journey (larger tt).

Our goal is to find the ratio: t1t2\frac{t_1}{t_2} where t1t_1 is the time to reach h3\frac{h}{3} on the way up, and t2t_2 is the time to reach the same height on the way down.

--- Step-by-Step Derivation:

Let’s denote:

  • uu: initial upward velocity
  • hh: maximum height reached
  • gg: acceleration due to gravity (acting downward)

Step 1: Express uu in terms of hh
At maximum height, velocity v=0v = 0. Using v2=u22ghv^2 = u^2 - 2gh: 0=u22ghu2=2ghu=2gh0 = u^2 - 2gh \Rightarrow u^2 = 2gh \Rightarrow u = \sqrt{2gh}

Step 2: Write the displacement equation for height y=h3y = \frac{h}{3}
We use: y=ut12gt2y = ut - \frac{1}{2} g t^2 Substitute y=h3y = \frac{h}{3} and u=2ghu = \sqrt{2gh}: h3=2ght12gt2\frac{h}{3} = \sqrt{2gh} \cdot t - \frac{1}{2} g t^2 Divide both sides by hh: 13=2ghtg2ht2\frac{1}{3} = \sqrt{\frac{2g}{h}} \cdot t - \frac{g}{2h} t^2 Let’s define a dimensionless time variable τ=tg2h\tau = t \sqrt{\frac{g}{2h}}. Then: g2ht2=(tg2h)2=τ2\frac{g}{2h} t^2 = \left( t \sqrt{\frac{g}{2h}} \right)^2 = \tau^2 and 2ght=2ghτg/(2h)=2ghτ2hg=2τ\sqrt{\frac{2g}{h}} \cdot t = \sqrt{\frac{2g}{h}} \cdot \frac{\tau}{\sqrt{g/(2h)}} = \sqrt{\frac{2g}{h}} \cdot \tau \cdot \sqrt{\frac{2h}{g}} = 2\tau So the equation becomes: 13=2ττ2\frac{1}{3} = 2\tau - \tau^2 Rearranged: τ22τ+13=0\tau^2 - 2\tau + \frac{1}{3} = 0

Step 3: Solve the quadratic equation for τ\tau
τ22τ+13=0\tau^2 - 2\tau + \frac{1}{3} = 0 Multiply through by 3 to eliminate fraction: 3τ26τ+1=03\tau^2 - 6\tau + 1 = 0 Use quadratic formula: τ=6±36126=6±246=6±266=1±63\tau = \frac{6 \pm \sqrt{36 - 12}}{6} = \frac{6 \pm \sqrt{24}}{6} = \frac{6 \pm 2\sqrt{6}}{6} = 1 \pm \frac{\sqrt{6}}{3} Simplify 24=26\sqrt{24} = 2\sqrt{6}, so: τ=1±63=3±63\tau = 1 \pm \frac{\sqrt{6}}{3} = \frac{3 \pm \sqrt{6}}{3}

Step 4: Identify τ1\tau_1 and τ2\tau_2
The two roots correspond to the two times when the ball is at h3\frac{h}{3}:

  • τ1=363\tau_1 = \frac{3 - \sqrt{6}}{3} (smaller time, on the way up)
  • τ2=3+63\tau_2 = \frac{3 + \sqrt{6}}{3} (larger time, on the way down)

Step 5: Compute the ratio t1t2\frac{t_1}{t_2}
Recall t=τ2hgt = \tau \sqrt{\frac{2h}{g}}, so: t1t2=τ1τ2=363+6\frac{t_1}{t_2} = \frac{\tau_1}{\tau_2} = \frac{3 - \sqrt{6}}{3 + \sqrt{6}} Now rationalize the denominator: Multiply numerator and denominator by 363 - \sqrt{6}: (36)2(3)2(6)2=966+696=15663=526\frac{(3 - \sqrt{6})^2}{(3)^2 - (\sqrt{6})^2} = \frac{9 - 6\sqrt{6} + 6}{9 - 6} = \frac{15 - 6\sqrt{6}}{3} = 5 - 2\sqrt{6} Wait — this seems messy. Let’s re-express the ratio in a cleaner form.

Instead, let’s write: 363+6=33633+6\frac{3 - \sqrt{6}}{3 + \sqrt{6}} = \frac{\sqrt{3} \cdot \sqrt{3} - \sqrt{6}}{\sqrt{3} \cdot \sqrt{3} + \sqrt{6}} But 6=23\sqrt{6} = \sqrt{2} \cdot \sqrt{3}, so: =3(32)3(3+2)=323+2= \frac{\sqrt{3}(\sqrt{3} - \sqrt{2})}{\sqrt{3}(\sqrt{3} + \sqrt{2})} = \frac{\sqrt{3} - \sqrt{2}}{\sqrt{3} + \sqrt{2}} This matches option B.

Conclusion: The ratio of the times is: tuptdown=323+2\frac{t_{\text{up}}}{t_{\text{down}}} = \frac{\sqrt{3} - \sqrt{2}}{\sqrt{3} + \sqrt{2}}

--- Common Traps & Exam Tip:

Trap 1: Misidentifying the roots.
Students often confuse which root corresponds to upward and downward motion. The smaller root is always the time during ascent, and the larger one during descent.

Trap 2: Forgetting to rationalize or simplify.
The answer appears in a form that must be simplified or rationalized to match the given options. Directly comparing 363+6\frac{3 - \sqrt{6}}{3 + \sqrt{6}} with options is difficult — it must be rewritten in terms of 2\sqrt{2} and 3\sqrt{3}.

Trap 3: Using wrong sign for acceleration.
It’s crucial to take gg as negative when upward is positive. A sign error here leads to incorrect quadratic solutions.

Exam Tip:
Always express time in terms of a dimensionless variable (like τ\tau) to simplify algebra. Also, verify units and consistency — the ratio must be dimensionless and less than 1, which all options satisfy.

Final Answer: Option B is correct.

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