JEE PYQ: Motion in a Plane - Question ID 4dd866733ec2 (JEE Main 2022)

ID: 4dd866733ec2JEE Main 2022Single Correct MCQ

A projectile is launched at an angle 'α\alpha' with the horizontal with a velocity 20 ms-1. After 10 s, its inclination with horizontal is 'β\beta'. The value of tanβ\beta will be : (g = 10 ms-2).

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Step-by-step Explanation

Core Formula & Concept:

In projectile motion, the motion of an object launched at an angle can be resolved into two independent components:

  • Horizontal motion: Uniform motion with constant velocity since no acceleration acts horizontally (ignoring air resistance). The horizontal velocity component is: vx=v0cosαv_{x} = v_{0} \cos \alpha where v0v_{0} is the initial velocity and α\alpha is the launch angle.
  • Vertical motion: Uniformly accelerated motion under gravity. The vertical velocity component at any time tt is: vy=v0sinαgtv_{y} = v_{0} \sin \alpha - g t where g=10ms2g = 10 \, \text{ms}^{-2} is the acceleration due to gravity.

The inclination β\beta of the projectile with the horizontal at any time tt is the angle whose tangent is the ratio of the vertical velocity component to the horizontal velocity component: tanβ=vyvx\tan \beta = \frac{v_{y}}{v_{x}} This is the key formula we will use to find tanβ\tan \beta after 10 seconds.

--- Step-by-Step Derivation:

Step 1: Write down initial velocity components
Initial velocity v0=20ms1v_{0} = 20 \, \text{ms}^{-1}, angle α\alpha
Horizontal component: vx=v0cosα=20cosαv_{x} = v_{0} \cos \alpha = 20 \cos \alpha
Vertical component at t=0t = 0: vy0=v0sinα=20sinαv_{y0} = v_{0} \sin \alpha = 20 \sin \alpha

Step 2: Find vertical velocity at t=10t = 10 s
Using vy=vy0gtv_{y} = v_{y0} - g t, and g=10ms2g = 10 \, \text{ms}^{-2}
vy=20sinα10×10=20sinα100v_{y} = 20 \sin \alpha - 10 \times 10 = 20 \sin \alpha - 100

Step 3: Horizontal velocity remains constant
vx=20cosαv_{x} = 20 \cos \alpha (unchanged)

Step 4: Compute tanβ\tan \beta
tanβ=vyvx=20sinα10020cosα\tan \beta = \frac{v_{y}}{v_{x}} = \frac{20 \sin \alpha - 100}{20 \cos \alpha}
Simplify numerator: 20sinα100=20(sinα5)20 \sin \alpha - 100 = 20 (\sin \alpha - 5)
So, tanβ=20(sinα5)20cosα=sinα5cosα\tan \beta = \frac{20 (\sin \alpha - 5)}{20 \cos \alpha} = \frac{\sin \alpha - 5}{\cos \alpha} Split the fraction: tanβ=sinαcosα5cosα=tanα5secα\tan \beta = \frac{\sin \alpha}{\cos \alpha} - \frac{5}{\cos \alpha} = \tan \alpha - 5 \sec \alpha since secα=1cosα\sec \alpha = \frac{1}{\cos \alpha}

Step 5: Match with given options
We have derived: tanβ=tanα5secα\tan \beta = \tan \alpha - 5 \sec \alpha This matches Option B.

--- Common Traps & Exam Tip:

Trap 1: Forgetting that horizontal velocity is constant
Students often mistakenly apply acceleration to the horizontal component. Remember: vxv_{x} does not change.

Trap 2: Sign error in vertical velocity
The vertical velocity decreases due to gravity, so vy=v0sinαgtv_{y} = v_{0} \sin \alpha - g t. A common mistake is using +gt+g t, which would imply upward acceleration.

Trap 3: Misinterpreting tanβ\tan \beta
tanβ\tan \beta is the ratio of current vertical velocity to horizontal velocity, not initial velocity components.

Exam Tip: Always resolve motion into horizontal and vertical components. Use tanθ=vyvx\tan \theta = \frac{v_{y}}{v_{x}} for inclination at any instant. Double-check signs and units.