Work Done in Expanding a Soap Bubble:
The work \( W \) done in increasing the surface area of a soap bubble is given by:
\[ W = \Delta U = S \Delta A \] where \( S \) is the surface tension and \( \Delta A \) is the increase in surface area.
Calculate Initial and Final Surface Areas:
Initial radius \( r = 7 \, \text{cm} \).
Initial surface area \( A_i = 4\pi r^2 = 4\pi (7)^2 \, \text{cm}^2 \).
Suppose the new radius is \( R \). Then the final surface area \( A_f \) is:
\[ A_f = 4\pi R^2 \]
Calculate the Change in Surface Area \( \Delta A \):
\[ \Delta A = A_f - A_i = 4\pi R^2 - 4\pi (7)^2 = 4\pi (R^2 - 49) \]
Use the Work Done to Solve for \( R \):
Given \( W = 36960 \, \text{erg} \) and \( S = 40 \, \text{dyne/cm} \), we have:
\[ 36960 = 40 \times 4\pi (R^2 - 49) \]
Simplifying,
\[ 36960 = 160\pi (R^2 - 49) \]
Using \( \pi = \frac{22}{7} \):
\[ 36960 \, \text{erg} = \frac{40 \, \text{dyne}}{\text{cm}} 8\pi \left[(R)^2 - \left(\frac{7}{2}\right)^2\right] \, \text{cm}^2 \]
\[ r = 7 \, \text{cm} \]
Conclusion:
The new radius of the soap bubble is \( 7 \, \text{cm} \).
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)
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is: