JEE PYQ: Motion in a Plane - Question ID 2193aa4e7b8d (JEE Main 2023)

ID: 2193aa4e7b8dJEE Main 2023Numerical Value

A projectile fired at 3030^{\circ} to the ground is observed to be at same height at time 3 s3 \mathrm{~s} and 5 s5 \mathrm{~s} after projection, during its flight. The speed of projection of the projectile is ___________ m s1\mathrm{m} ~\mathrm{s}^{-1}.

(Given g=10 ms2g=10 \mathrm{~ms}^{-2} )

Your Answer

Step-by-step Explanation

Core Formula & Concept:

In projectile motion, the vertical component of the motion is governed by the equations of uniformly accelerated motion under gravity. The key idea here is that the projectile reaches the same height at two different times during its flight. This symmetry implies that the two times are equidistant from the time at which the projectile reaches its maximum height.

Let:

  • uu = initial speed of projection (unknown)
  • θ=30\theta = 30^\circ = angle of projection with the horizontal
  • g=10 m s2g = 10 \text{ m s}^{-2} = acceleration due to gravity
  • t1=3 st_1 = 3 \text{ s} and t2=5 st_2 = 5 \text{ s} = two times at which the projectile is at the same height

The vertical displacement y(t)y(t) at any time tt is given by: y(t)=usinθt12gt2y(t) = u \sin \theta \cdot t - \frac{1}{2} g t^2 Since y(t1)=y(t2)y(t_1) = y(t_2), we have: usinθt112gt12=usinθt212gt22u \sin \theta \cdot t_1 - \frac{1}{2} g t_1^2 = u \sin \theta \cdot t_2 - \frac{1}{2} g t_2^2 This equation can be simplified to find a relationship involving uu.

Step-by-Step Derivation:

Step 1: Equate vertical displacements at t1t_1 and t2t_2
Given y(t1)=y(t2)y(t_1) = y(t_2), we write: usin303121032=usin305121052u \sin 30^\circ \cdot 3 - \frac{1}{2} \cdot 10 \cdot 3^2 = u \sin 30^\circ \cdot 5 - \frac{1}{2} \cdot 10 \cdot 5^2

Step 2: Simplify the equation
Substitute sin30=12\sin 30^\circ = \frac{1}{2} and compute the terms: u12359=u125525u \cdot \frac{1}{2} \cdot 3 - 5 \cdot 9 = u \cdot \frac{1}{2} \cdot 5 - 5 \cdot 25 3u245=5u2125\frac{3u}{2} - 45 = \frac{5u}{2} - 125

Step 3: Solve for uu
Bring all terms involving uu to one side and constants to the other: 3u25u2=125+45\frac{3u}{2} - \frac{5u}{2} = -125 + 45 2u2=80-\frac{2u}{2} = -80 u=80    u=80 m s1-u = -80 \implies u = 80 \text{ m s}^{-1}

Verification:
The time at which the projectile reaches its maximum height is the average of t1t_1 and t2t_2: tmax=t1+t22=3+52=4 st_{\text{max}} = \frac{t_1 + t_2}{2} = \frac{3 + 5}{2} = 4 \text{ s} Using the vertical motion equation at t=tmaxt = t_{\text{max}}, the vertical component of velocity becomes zero: usin30gtmax=0u \sin 30^\circ - g t_{\text{max}} = 0 u12104=0u \cdot \frac{1}{2} - 10 \cdot 4 = 0 u2=40    u=80 m s1\frac{u}{2} = 40 \implies u = 80 \text{ m s}^{-1} This confirms our result.

Common Traps & Exam Tip:

  • Misapplying symmetry: Students often forget that the two times at which the projectile is at the same height are symmetric about the time of maximum height. This symmetry is crucial for solving the problem efficiently.
  • Incorrect sign convention: Ensure that the acceleration due to gravity is taken as negative if upward direction is positive (or vice versa). Consistency in sign convention is key.
  • Overcomplicating the problem: Avoid unnecessary calculations involving horizontal motion or range. The problem only requires vertical motion analysis.
  • Arithmetic errors: Simple arithmetic mistakes in solving the equation for uu can lead to incorrect answers. Double-check calculations.

Final Answer: The speed of projection is 80 m s180 \text{ m s}^{-1}.