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NEET2021Physics-Projectile Motion

NEET 2021 Physics Maximum Height Calculation MCQ Question

Type: MCQ-conceptual-Hard-Class 11

A particle moving in a circle of radius R with a uniform speed takes a time T to complete one revolution. If this particle were projected with the same speed at an angle 'θ' to the horizontal, the maximum height attained by it equals 4R. The angle of projection, θ, is then given by:

A

θ = cos⁻¹[(gT²)/(π²R)]^(1/2)

B

θ = cos⁻¹[(π²R)/(gT²)]^(1/2)

C

θ = sin⁻¹[(π²R)/(gT²)]^(1/2)

D

θ = sin⁻¹[(2gT²)/(π²R)]^(1/2)

Correct Answer

Option D

Detailed Explanation

To solve the problem, we need to analyze the motion of a particle moving in a circle and then being projected at an angle.

  1. Understanding the Circular Motion: When a particle moves in a circle of radius RR with uniform speed, we can find the speed vv of the particle using the relationship between the speed, radius, and time period TT:

    v=2πRTv = \frac{2\pi R}{T}

    This formula comes from the fact that the distance traveled in one complete revolution (circumference of the circle) is 2πR2\pi R, and dividing this by the time TT gives us the speed.

  2. Analyzing the Projectile Motion: When the particle is projected at an angle θ\theta to the horizontal with the same speed vv, we can find the maximum height HH attained during the projectile motion using the formula:

    H=v2sin⁡2θ2gH = \frac{v^2 \sin^2 \theta}{2g}

    where gg is the acceleration due to gravity.

  3. Setting Up the Equation: According to the problem, the maximum height attained by the projectile is given as 4R4R. Thus, we can set up the equation:

    4R=v2sin⁡2θ2g4R = \frac{v^2 \sin^2 \theta}{2g}
  4. Substituting vv: Now, substituting vv from our earlier calculation:

    4R=(2πRT)2sin⁡2θ2g4R = \frac{\left(\frac{2\pi R}{T}\right)^2 \sin^2 \theta}{2g}

    Simplifying this gives:

    4R=4π2R2sin⁡2θ2gT24R = \frac{4\pi^2 R^2 \sin^2 \theta}{2gT^2} 4R=2π2R2sin⁡2θgT24R = \frac{2\pi^2 R^2 \sin^2 \theta}{gT^2}
  5. Solving for sin⁡2θ\sin^2 \theta: Rearranging the equation to isolate sin⁡2θ\sin^2 \theta:

    sin⁡2θ=4gT22π2R\sin^2 \theta = \frac{4gT^2}{2\pi^2 R} sin⁡2θ=2gT2π2R\sin^2 \theta = \frac{2gT^2}{\pi^2 R}
  6. Finding θ\theta: Taking the square root to find sin⁡θ\sin \theta:

    sin⁡θ=2gT2π2R\sin \theta = \sqrt{\frac{2gT^2}{\pi^2 R}}

    Finally, we can express θ\theta:

    θ=sin⁡−1(2gT2π2R)\theta = \sin^{-1}\left(\sqrt{\frac{2gT^2}{\pi^2 R}}\right)

    Notice that this matches the form of option D when rearranging the expression:

    θ=sin⁡−1(2gT2π2R)1/2\theta = \sin^{-1}\left(\frac{2gT^2}{\pi^2 R}\right)^{1/2}

Why Other Options are Incorrect:

  • Option A: θ=cos⁡−1((gT2π2R)1/2)\theta = \cos^{-1}\left(\left(\frac{gT^2}{\pi^2 R}\right)^{1/2}\right) is incorrect because we derived a formula involving sine, not cosine.
  • Option B: θ=cos⁡−1((π2RgT2)1/2)\theta = \cos^{-1}\left(\left(\frac{\pi^2 R}{gT^2}\right)^{1/2}\right) is also incorrect as it does not relate to our derived expression.
  • Option C: θ=sin⁡−1((π2RgT2)1/2)\theta = \sin^{-1}\left(\left(\frac{\pi^2 R}{gT^2}\right)^{1/2}\right) does not match our derived expression either.

Conclusion:

The correct answer is D, as we derived it correctly from the conditions of the problem regarding the maximum height attained by the projectile.

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