Problem 18
Question
Imagine a light planet revolving around a very massive star in a circular orbit of radius \(R\) with a period of revolution \(T\). If the gravitational force of attraction between the planet and the star is proportional to \(R^{-5 / 2}\), \(T^{2}\) is proportional to (A) \(R^{3}\) (B) \(R^{7 / 2}\) (C) \(R^{3 / 2}\) (D) \(R^{3.75}\)
Step-by-Step Solution
Verified Answer
The relationship between \(T^2\) and R is given by:
\[T^2 \propto R^{3/2}\]
Hence, the correct answer is (C).
1Step 1: Analyzing the Centripetal Force
The centripetal force acting on the planet must balance the gravitational force to keep it in a stable circular orbit. The centripetal force can be given as:
\[F_c = \frac{m_p v^2}{R}\]
where \(m_p\) is the mass of the planet, and v is the orbital velocity of the planet.
The orbital velocity can be determined from the circumference of the orbit and the period of the revolution, as follows.
\[v = \frac{2 \pi R}{T}\]
2Step 2: Equating Gravitational Force and Centripetal Force
Now we will equate the centripetal force with the gravitational force:
\[F_g = k R^{-5/2}\]
where k is a proportionality constant. Therefore,
\[\frac{m_p v^2}{R} = k R^{-5/2}\]
Now, substitute the expression for velocity from step 1:
\[\frac{m_p (2 \pi R / T)^2}{R} = k R^{-5/2}\]
3Step 3: Simplifying the Equation and Solving for T^2
We will now simplify the equation and solve for \(T^2\):
\[\frac{4m_p \pi^2 R^2}{T^2 R} = k R^{-5/2}\]
\[4m_p \pi^2 R = k R^{1/2}T^2\]
Now, rearrange the equation to find the proportionality between \(T^2\) and R:
\[T^2 = \frac{4m_p \pi^2 R^{3/2}}{k}\]
From this expression, we can clearly see that the relationship between \(T^2\) and R is given by:
\[T^2 \propto R^{3/2}\]
This corresponds to the answer choice (C) in the given options.
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