To find the height where the acceleration due to gravity is reduced to \( g/16 \), we use the formula:
\( g_h = g \left( \frac{R}{R + h} \right)^2 \)
Here, \( g_h = \frac{g}{16} \). Substituting into the equation:
\( \frac{g}{16} = g \left( \frac{R}{R + h} \right)^2 \)
Cancel \( g \) on both sides:
\( \frac{1}{16} = \left( \frac{R}{R + h} \right)^2 \)
Take the square root of both sides:
\( \frac{1}{4} = \frac{R}{R + h} \)
Rearranging for \( R + h \):
\( R + h = 4R \)
Solve for \( h \):
\( h = 4R - R = 3R \)
Thus, the height above the Earth's surface where gravity is reduced to \( g/16 \) is:
\( h = 3R \)
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