JEE PYQ: Motion in a Plane - Question ID a51f2e8c9ee5 (JEE Main 2021)

ID: a51f2e8c9ee5JEE Main 2021Single Correct MCQ
The trajectory of a projectile in a vertical plane is y = α\alphax - β\betax2, where α\alpha and β\beta are constants and x & y are respectively the horizontal and vertical distances of the projectile from the point of projection. The angle of projection θ\theta and the maximum height attained H are respectively given by :

Select Option

Step-by-step Explanation

Core Formula & Concept:

In projectile motion, the trajectory of a particle launched from the origin with initial velocity v0v_0 at an angle θ\theta with the horizontal is described by the equation:

y=xtanθgx22v02cos2θy = x \tan \theta - \frac{g x^2}{2 v_0^2 \cos^2 \theta}

This equation is derived by eliminating time from the horizontal and vertical motion equations:

  • Horizontal motion: x=v0cosθtx = v_0 \cos \theta \cdot t
  • Vertical motion: y=v0sinθt12gt2y = v_0 \sin \theta \cdot t - \frac{1}{2} g t^2

The given trajectory equation is y=αxβx2y = \alpha x - \beta x^2. By comparing this with the standard trajectory equation, we can extract the angle of projection θ\theta and the maximum height HH.

Step-by-Step Derivation:

Step 1: Compare the given trajectory with the standard form

Given trajectory: y=αxβx2y = \alpha x - \beta x^2 Standard trajectory: y=xtanθgx22v02cos2θy = x \tan \theta - \frac{g x^2}{2 v_0^2 \cos^2 \theta}

By comparing coefficients of xx and x2x^2 in both equations, we get:

tanθ=α(1)\tan \theta = \alpha \quad \text{(1)} g2v02cos2θ=β(2)\frac{g}{2 v_0^2 \cos^2 \theta} = \beta \quad \text{(2)}

Step 2: Find the angle of projection θ\theta

From equation (1), we directly obtain: θ=tan1α\theta = \tan^{-1} \alpha

Step 3: Express v02v_0^2 in terms of α\alpha and β\beta

Recall that cos2θ=11+tan2θ=11+α2\cos^2 \theta = \frac{1}{1 + \tan^2 \theta} = \frac{1}{1 + \alpha^2}. Substituting this into equation (2):

β=g2v02(1+α2)\beta = \frac{g}{2 v_0^2} (1 + \alpha^2)

Solving for v02v_0^2:

v02=g(1+α2)2βv_0^2 = \frac{g (1 + \alpha^2)}{2 \beta}

Step 4: Find the maximum height HH

The maximum height HH in projectile motion is given by:

H=v02sin2θ2gH = \frac{v_0^2 \sin^2 \theta}{2g}

We know sinθ=tanθ1+tan2θ=α1+α2\sin \theta = \frac{\tan \theta}{\sqrt{1 + \tan^2 \theta}} = \frac{\alpha}{\sqrt{1 + \alpha^2}}. Thus:

sin2θ=α21+α2\sin^2 \theta = \frac{\alpha^2}{1 + \alpha^2}

Substituting v02v_0^2 and sin2θ\sin^2 \theta into the expression for HH:

H=(g(1+α2)2β)(α21+α2)2g=α24βH = \frac{\left( \frac{g (1 + \alpha^2)}{2 \beta} \right) \left( \frac{\alpha^2}{1 + \alpha^2} \right)}{2g} = \frac{\alpha^2}{4 \beta}

Step 5: Match with the given options

From the above derivations:

  • Angle of projection: θ=tan1α\theta = \tan^{-1} \alpha
  • Maximum height: H=α24βH = \frac{\alpha^2}{4 \beta}

This matches Option A.

Common Traps & Exam Tip:

1. Misidentifying coefficients: Students often confuse the coefficients of xx and x2x^2 in the trajectory equation, leading to incorrect expressions for tanθ\tan \theta or β\beta. Always compare the given equation with the standard form carefully.

2. Incorrect trigonometric identities: Forgetting that cos2θ=11+tan2θ\cos^2 \theta = \frac{1}{1 + \tan^2 \theta} or misapplying sinθ\sin \theta in terms of tanθ\tan \theta can lead to errors in calculating HH. Practice deriving these identities to avoid mistakes.

3. Algebraic errors: Simplifying expressions like v02v_0^2 or HH requires careful algebra. Double-check each step to ensure no terms are dropped or miscalculated.

4. Unit consistency: While this problem does not involve units explicitly, ensure that all physical quantities are consistent (e.g., gg is in m/s2m/s^2 if v0v_0 is in m/sm/s).

Exam Tip: For trajectory-based problems, always start by writing the standard trajectory equation and then compare it with the given equation. This systematic approach minimizes errors and saves time.