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 \(\theta_0(\theta_0 \ll 1)\) with the \(x\)-axis at \(x = L\). If \(y(x)\) is the height of the surface then the equation for \(y(x)\) is :
(take \(\theta(x) = \sin\theta(x) = \tan\theta(x) = \frac{dy}{dx}\), \(g\) is the acceleration due to gravity)


























































