Step 1. Volume Conservation:
Since the total volume of the liquid remains constant, we equate the volume of the original drop to the combined volume of the 27 smaller drops.
For the original drop:
\(\frac{4}{3}\pi R^3\)
For the 27 smaller drops (each of radius \( r \)):
\(27 \times \frac{4}{3}\pi r^3\)
Equating the volumes:
\(\frac{4}{3}\pi R^3 = 27 \times \frac{4}{3}\pi r^3\)
\(R^3 = 27r^3 \implies r = \frac{R}{3}\)
Step 2. Calculate the Surface Areas:
- Surface area of the original drop:
\(A_{\text{initial}} = 4\pi R^2\)
- Surface area of the 27 smaller drops:
\(A_{\text{final}} = 27 \times 4\pi r^2 = 27 \times 4\pi \left(\frac{R}{3}\right)^2 = 27 \times 4\pi \frac{R^2}{9} = 12\pi R^2\)
Step 3. Calculate the Work Done :
The work done in increasing the surface area is given by: \(\text{Work done} = T\Delta A = T(A_{\text{final}} - A_{\text{initial}})\)
\(= T(12\pi R^2 - 4\pi R^2) = T \times 8\pi R^2\)
Thus, the work done in the process is \( 8\pi R^2 T \).
The Correct Answer is:\( 8\pi R^2 T \)
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 $ f: \mathbb{R} \to \mathbb{R} $ be a twice differentiable function such that $$ f''(x)\sin\left(\frac{x}{2}\right) + f'(2x - 2y) = (\cos x)\sin(y + 2x) + f(2x - 2y) $$ for all $ x, y \in \mathbb{R} $. If $ f(0) = 1 $, then the value of $ 24f^{(4)}\left(\frac{5\pi}{3}\right) $ is: