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
\(\theta=sin^{-1}(\frac{2gT^2}{\pi^2R})^{\frac{1}{2}}\)
\(\theta=cos^{-1}(\frac{gT^2}{\pi^2R})^{\frac{1}{2}}\)
\(\theta=cos^{-1}(\frac{\pi^2R}{gT^2})^{\frac{1}{2}}\)
\(\theta=sin^{-1}(\frac{\pi^2R}{gT^2})^{\frac{1}{2}}\)
To solve this problem, we need to relate the circular motion of a particle to its projectile motion. Let's break down the solution step-by-step:
Thus, the correct answer is:
\(\theta=sin^{-1}(\frac{2gT^2}{\pi^2R})^{\frac{1}{2}}\)
This option corresponds to the correct angle of projection that satisfies the given condition of maximum height being \( 4R \).