Provided:
\[ V = \frac{2\pi R}{T} \]
The equation for the maximum height achieved by the particle is:
\[ H = \frac{v^2 \sin^2 \theta}{2g} \]
It is given that:
\[ 4R = \frac{4\pi^2 R^2 \sin^2 \theta}{T^2 \cdot 2g} \]
After simplification:
\[ \sin^2 \theta = \frac{2gT^2}{\pi^2 R} \]
Taking the square root yields:
\[ \sin \theta = \sqrt{\frac{2gT^2}{\pi^2 R}} \]
Therefore:
\[ \theta = \sin^{-1} \left( \sqrt{\frac{2gT^2}{\pi^2 R}} \right) \]