Let \( g_0 \) be the acceleration due to gravity at the earth's surface. The acceleration due to gravity at a height \( h \) above the surface is given by:
\( g_h = \frac{g_0}{(1 + \frac{h}{R_e})^2} \)
The acceleration due to gravity at a depth \( d = \alpha h \) below the surface is given by:
\( g_d = g_0 \left(1 - \frac{\alpha h}{R_e}\right) \)
According to the problem, \( g_h = g_d \). Therefore:
\[\frac{g_0}{(1 + \frac{h}{R_e})^2} = g_0 \left(1 - \frac{\alpha h}{R_e}\right)\]
We can cancel \( g_0 \) from both sides and solve the resulting equation:
\[\frac{1}{(1 + \frac{h}{R_e})^2} = 1 - \frac{\alpha h}{R_e}\]
For simplicity, let's approximate \((1+\frac{h}{R_e})^2\) using binomial expansion, considering \( h \ll R_e \):
\((1 + \frac{h}{R_e})^2 \approx 1 + \frac{2h}{R_e}\)
Thus, the equation simplifies to:
\[\frac{1}{1 + \frac{2h}{R_e}} \approx 1 - \frac{\alpha h}{R_e}\]
Expanding the left side using binomial approximation again:
\[1 - \frac{2h}{R_e} \approx 1 - \frac{\alpha h}{R_e}\]
Equating coefficients of \(\frac{h}{R_e}\):
\[2 = \alpha\]
Thus, the value of \(\alpha\) is \(2\), which fits within the given range of \(2,2\).
\(g(1 - \frac{2h}{R}) = g(1 - \frac{d}{R})\)
\(⇒ 2h = d\)
\(⇒ α = 2\)
So, the answer is 2.
In mechanics, the universal force of attraction acting between all matter is known as Gravity, also called gravitation, . It is the weakest known force in nature.
According to Newton’s law of gravitation, “Every particle in the universe attracts every other particle with a force whose magnitude is,
On combining equations (1) and (2) we get,
F ∝ M1M2/r2
F = G × [M1M2]/r2 . . . . (7)
Or, f(r) = GM1M2/r2
The dimension formula of G is [M-1L3T-2].