Suppose a mountain at location A is in isostatic equilibrium with a column at location B, which is at sea-level, as shown in the figure. The height of the mountain is 4 km and the thickness of the crust at B is 1 km. Given that the densities of crust and mantle are 2700 kg/m\(^3\) and 3300 kg/m\(^3\), respectively, the thickness of the mountain root (r1) is km. (Answer in integer)


Step 3: Buoyant Force by Root
Given:
The crustal root provides a buoyant force by displacing mantle material: \[ \text{Buoyant force} = r_1 \times (\rho_m - \rho_c) = r_1 \times (3300 - 2700) = r_1 \times 600 \]
Step 4: Equating Mass and Buoyant Force
For isostatic equilibrium: \[ h_{\text{mountain}} \times \rho_c = r_1 \times (\rho_m - \rho_c) \] \[ 4 \times 2700 = r_1 \times 600 \quad \Rightarrow \quad 10800 = r_1 \times 600 \]
Step 5: Solving for \( r_1 \)
\[ r_1 = \frac{10800}{600} = 18 \, \text{km} \]
Consider a medium of uniform resistivity with a pair of source and sink electrodes separated by a distance \( L \), as shown in the figure. The fraction of the input current \( (I) \) that flows horizontally \( (I_x) \) across the median plane between depths \( z_1 = \frac{L}{2} \) and \( z_2 = \frac{L\sqrt{3}}{2} \), is given by \( \frac{I_x}{I} = \frac{L}{\pi} \int_{z_1}^{z_2} \frac{dz}{(L^2/4 + z^2)} \). The value of \( \frac{I_x}{I} \) is equal to 
Suppose a mountain at location A is in isostatic equilibrium with a column at location B, which is at sea-level, as shown in the figure. The height of the mountain is 4 km and the thickness of the crust at B is 1 km. Given that the densities of crust and mantle are 2700 kg/m\(^3\) and 3300 kg/m\(^3\), respectively, the thickness of the mountain root (r1) is km. (Answer in integer)