Rather than comparing forces directly, compare the two accelerations a coin would feel: Earth pulls it down with acceleration \( g \), while the other coin pulls it sideways with acceleration \( a' = \dfrac{Gm}{r^2} \) (only one mass appears here, since acceleration doesn't depend on the mass being accelerated). Since both forces act on the same coin, the ratio of forces equals the ratio of accelerations, so \( \dfrac{W}{F} = \dfrac{g}{a'} \).
Computing \( a' = \dfrac{(6.67 \times 10^{-11})(0.008)}{(0.5)^2} = \dfrac{5.336 \times 10^{-13}}{0.25} = 2.134 \times 10^{-12} \, \text{m/s}^2 \), an acceleration many trillion times smaller than \( g = 9.81 \, \text{m/s}^2 \).
Taking the ratio: \( \dfrac{g}{a'} = \dfrac{9.81}{2.134 \times 10^{-12}} \approx 4.6 \times 10^{12} \), confirming the same result reached from the force comparison.\[ \boxed{4.6 \times 10^{12}} \]