The surface energy of a droplet is defined as the product of its surface tension and surface area, represented by the equation: \( E = \sigma \times A \).
Here, \( \sigma \) denotes the surface tension and \( A \) represents the surface area.
Consider a small drop with radius \( r \). Its surface area is calculated as: \( A_1 = 4 \pi r^2 \).
For a collection of 1000 such small drops, the aggregate surface area is: \( A_1(\text{total}) = 1000 \times 4 \pi r^2 = 4000 \pi r^2 \).
The total surface energy of these 1000 small drops is: \( E_1 = \sigma \times A_1(\text{total}) = \sigma \times 4000 \pi r^2 \).
When these 1000 small drops merge, their total volume is conserved. The volume of a single small drop is: \( V_{\text{small}} = \frac{4}{3} \pi r^3 \).
Consequently, the combined volume of 1000 small drops is: \( V_{\text{total}} = 1000 \times \frac{4}{3} \pi r^3 = \frac{4}{3} \pi (1000 r^3) \).
Let \( R \) be the radius of the resultant large drop. Its volume is expressed as: \( V_{\text{large}} = \frac{4}{3} \pi R^3 \).
Equating the total volume of the small drops to the volume of the large drop yields: \( \frac{4}{3} \pi R^3 = \frac{4}{3} \pi (1000 r^3) \).
This equation simplifies to: \( R^3 = 1000 r^3 \), from which we derive \( R = 10r \).
The surface area of the large drop is therefore: \( A_2 = 4 \pi R^2 = 4 \pi (10r)^2 = 4 \pi \times 100r^2 = 400 \pi r^2 \).
The surface energy of the large drop is: \( E_2 = \sigma \times A_2 = \sigma \times 400 \pi r^2 \).
The ratio of the total surface energy of the small drops to the surface energy of the large drop is calculated as: \( \frac{E_1}{E_2} = \frac{\sigma \times 4000 \pi r^2}{\sigma \times 400 \pi r^2} \).
Upon simplification, this ratio becomes: \( \frac{E_1}{E_2} = \frac{4000}{400} = 10 \).
Final Answer: The ratio of surface energies is: 10.
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) 