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.