JEE PYQ: Motion in a Straight Line - Question ID 1f68aae45b62 (JEE Main 2021)

ID: 1f68aae45b62JEE Main 2021Numerical Value
Two spherical balls having equal masses with radius of 5 cm each are thrown upwards along the same vertical direction at an interval of 3s with the same initial velocity of 35 m/s, then these balls collide at a height of ............... m. (Take g = 10 m/s2)
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Step-by-step Explanation

Core Formula & Concept:

This problem involves the motion of two spherical balls under constant gravitational acceleration (g=10m/s2g = 10 \, \text{m/s}^2 downward). The key concepts and formulas used are:

  • Kinematic Equation for Vertical Motion: For an object thrown upward with initial velocity uu, its displacement ss at time tt is given by: s=ut12gt2s = ut - \frac{1}{2}gt^2 This equation accounts for the deceleration due to gravity.
  • Relative Motion: Since both balls are thrown along the same vertical line with the same initial velocity but at different times, we analyze their positions as functions of time and find the instant when they meet (collide).
  • Time Interval Consideration: The second ball is thrown 3s3 \, \text{s} after the first. Thus, if tt is the time elapsed since the first ball was thrown, the second ball has been in motion for (t3)s(t - 3) \, \text{s}.
Step-by-Step Derivation:

Let’s define:

  • u=35m/su = 35 \, \text{m/s} (initial velocity of both balls)
  • g=10m/s2g = 10 \, \text{m/s}^2 (acceleration due to gravity)
  • tt = time elapsed since the first ball was thrown (in seconds)
  • h1(t)h_1(t) = height of the first ball at time tt
  • h2(t)h_2(t) = height of the second ball at time tt

The second ball is thrown at t=3st = 3 \, \text{s}, so for t<3t < 3, h2(t)=0h_2(t) = 0 (not yet thrown). For t3t \geq 3, the second ball has been in motion for (t3)s(t - 3) \, \text{s}.

Using the kinematic equation for vertical motion:

h1(t)=ut12gt2=35t5t2h_1(t) = ut - \frac{1}{2}gt^2 = 35t - 5t^2 h_2(t) = u(t - 3) - \frac{1}{2}g(t - 3)^2 = 35(t - 3) - 5(t - 3)^2 \quad \text{(fort \geq 3)}

The balls collide when h1(t)=h2(t)h_1(t) = h_2(t). Thus, we set:

35t5t2=35(t3)5(t3)235t - 5t^2 = 35(t - 3) - 5(t - 3)^2

Simplify the right-hand side (RHS):

35(t3)=35t10535(t - 3) = 35t - 105 5(t3)2=5(t26t+9)=5t230t+455(t - 3)^2 = 5(t^2 - 6t + 9) = 5t^2 - 30t + 45

Substitute back into the equation:

35t5t2=(35t105)(5t230t+45)35t - 5t^2 = (35t - 105) - (5t^2 - 30t + 45) 35t5t2=35t1055t2+30t4535t - 5t^2 = 35t - 105 - 5t^2 + 30t - 45

Combine like terms on the RHS:

35t5t2=(35t+30t)5t2+(10545)35t - 5t^2 = (35t + 30t) - 5t^2 + (-105 - 45) 35t5t2=65t5t215035t - 5t^2 = 65t - 5t^2 - 150

Subtract (35t5t2)(35t - 5t^2) from both sides:

0=30t1500 = 30t - 150 30t=15030t = 150 t=5st = 5 \, \text{s}

Thus, the balls collide at t=5st = 5 \, \text{s} after the first ball is thrown.

Now, compute the height at t=5st = 5 \, \text{s} using h1(t)h_1(t):

h=35(5)5(5)2=175125=50mh = 35(5) - 5(5)^2 = 175 - 125 = 50 \, \text{m}

Verification: Check h2(t)h_2(t) at t=5st = 5 \, \text{s}:

h2(5)=35(53)5(53)2=35(2)5(4)=7020=50mh_2(5) = 35(5 - 3) - 5(5 - 3)^2 = 35(2) - 5(4) = 70 - 20 = 50 \, \text{m}

Both heights match, confirming the collision at 50m50 \, \text{m}.

Common Traps & Exam Tip:

  1. Incorrect Time Reference: Students often confuse the time variables. The second ball’s motion must be referenced to its own launch time (t3t - 3), not the absolute time tt. Failing to adjust for the 3s3 \, \text{s} delay leads to incorrect equations.
  2. Sign Errors in Kinematic Equation: The equation s=ut12gt2s = ut - \frac{1}{2}gt^2 assumes upward as positive. Some students mistakenly use +12gt2+ \frac{1}{2}gt^2, which reverses the direction of gravity and yields wrong results.
  3. Algebraic Mistakes: Expanding (t3)2(t - 3)^2 incorrectly or miscombining terms during simplification can lead to wrong values for tt. Double-check each algebraic step.
  4. Ignoring Physical Constraints: The collision must occur after the second ball is thrown (t3t \geq 3). If solving yields t<3t < 3, it implies no collision, which is not the case here. Always verify the solution’s physical validity.

Exam Tip: For problems involving relative motion with time delays, always define a clear time reference (e.g., t=0t = 0 when the first object is launched). Write separate equations for each object’s position as a function of tt, then equate them to find the collision time. This systematic approach minimizes errors.

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