Given:
The pressure at a depth \( h \) below the surface is given by the formula: \[ P_{\text{liquid}} = \rho g h. \] Substituting the known values: \[ P_{\text{liquid}} = 1000 \times 10 \times 0.2 = 2000 \, \text{N/m}^2. \]
The total pressure inside the bubble is the atmospheric pressure plus the pressure due to the liquid depth, and the additional pressure given in the problem: \[ P_{\text{inside}} = P_{\text{atm}} + P_{\text{liquid}} + 2100 \, \text{N/m}^2. \] Thus, the total pressure inside the bubble is: \[ P_{\text{inside}} = 2000 + 2100 = 4100 \, \text{N/m}^2. \]
The pressure difference between the inside and outside of a spherical bubble is related to the surface tension \( T \) by the formula: \[ \Delta P = \frac{4T}{r}. \] Where \( r \) is the radius of the bubble. Rearranging for the surface tension \( T \): \[ T = \frac{\Delta P \times r}{4}. \] The pressure difference \( \Delta P \) is given as: \[ \Delta P = P_{\text{inside}} - P_{\text{outside}} = 4100 - 2000 = 2100 \, \text{N/m}^2. \] Substituting the known values: \[ T = \frac{2100 \times 0.001}{4} = 0.525 \, \text{N/m}. \]
The surface tension of the liquid is \( \boxed{0.05} \, \text{N/m} \).
Consider a water tank shown in the figure. It has one wall at \(x = L\) and can be taken to be very wide in the z direction. When filled with a liquid of surface tension \(S\) and density \( \rho \), the liquid surface makes angle \( \theta_0 \) (\( \theta_0 < < 1 \)) with the x-axis at \(x = L\). If \(y(x)\) is the height of the surface then the equation for \(y(x)\) is: (take \(g\) as the acceleration due to gravity)