Answer:
Solid angle subtended by the sun at
a point on earth, \[\Omega =\frac{\pi R_{S}^{2}}{R_{SE}^{2}}\]
Solid angle subtended by the moon at
appoint on earth \[\Omega =\frac{\pi R_{m}^{2}}{R_{ME}^{2}}\].
\[\therefore \]\[\frac{\pi
R_{S}^{2}}{R_{SE}^{2}}=\frac{\pi R_{M}^{2}}{R_{ME}^{2}}\] or \[\frac{{{R}_{s}}}{{{R}_{M}}}=\frac{{{R}_{SE}}}{{{R}_{ME}}}\]
\[\therefore \] \[\frac{\text{Radius}\,\text{of}\,\,\text{the}\,\text{sun}}{\text{Radium}\,\,\text{of}\,\,\text{the}\,\,\text{moon}}\]
\[\text{=}\frac{\text{Distance of the sun
from the earth}}{\text{Distance of the moon from the earth}}\]
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