The acceleration due to gravity near the surface of a planet of radius $R$ and density $d$ is proportional to
The acceleration due to gravity near the surface of a planet of radius $R$ and density $d$ is proportional to
- A
$\frac{d}{{{R^2}}}$
- B
$d{R^2}$
- C
$dR$
- D
$\frac{d}{R}$
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