This can be written as:
\[T = \frac{2\pi}{\sqrt{G \cdot M}} \cdot R^{3/2}\]
where:
- \(T\) is the orbital period,
- \(G\) is the gravitational constant,
- \(M\) is the mass of the central body (in this case, Earth),
- \(R\) is the radius of the orbit.
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