To address this issue, we will employ the principles of pressure differential and surface tension. The pressure differential stemming from surface tension for an air bubble is quantified by the following equation:
\(P_{\text{inside}} - P_{\text{outside}} = \frac{4T}{r}\)
In this formula, \(T\) represents the liquid's surface tension, and \(r\) denotes the air bubble's radius.
Given that the internal pressure of the bubble exceeds atmospheric pressure by 2100 N/m\(^2\), we can express this as:
\(P_{\text{inside}} - P_{\text{outside}} = 2100 \, \text{N/m}^2\)
Furthermore, with the radius specified as \(r = 0.1 \, \text{cm}\), which converts to 0.001 m, we can integrate these values into the equation:
\(2100 = \frac{4T}{0.001}\)
Rearranging to solve for \(T\) yields:
\(T = \frac{2100 \times 0.001}{4} = \frac{2.1}{4} = 0.525 \times 0.1 = 0.05 \, \text{N/m}\)
Consequently, the surface tension of the liquid is determined to be \(0.05 \, \text{N/m}\).
The calculated surface tension is 0.05.
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) 