To solve for the distance \(Z_0\) below the free surface of water where the pressure equals the pressure inside a soap bubble, we need to consider the formula for excess pressure inside a soap bubble and equate it to the hydrostatic pressure at depth \(Z_0\).
The excess pressure inside a soap bubble is given by:
\( \Delta P = \frac{4T}{R} \)
where \(T\) is the surface tension of the soap solution and \(R\) is the radius of the bubble. In the given problem:
Substituting these values, we find:
\( \Delta P = \frac{4 \times 2.5 \times 10^{-2}}{1 \times 10^{-3}} = 100 \, \frac{N}{m^2} \)
Now, equate this excess pressure to the hydrostatic pressure at depth \(Z_0\) in water:
\( P = \rho g Z_0 \)
where \(\rho = 103 \, kg/m^3\) is the density of water and \(g = 10 \, m/s^2\).
Thus, \(\rho g Z_0 = 100\)
Substituting the given values:
\( 103 \times 10 \times Z_0 = 100 \)
Solving for \(Z_0\) gives:
\( Z_0 = \frac{100}{1030} \approx 0.097 \, m = 1 \, cm \)
Therefore, the correct value of \(Z_0\) is \(1 \, cm\). The correct answer is \(1 \, cm\).
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) 