Given: - A big drop is formed by combining 1000 small droplets.
Since the droplets coalesce to form one big drop, the total volume remains constant. Let \( r \) be the radius of each small droplet and \( R \) be the radius of the big drop.
The volume of one small droplet is:
\[ V_{\text{small}} = \frac{4}{3} \pi r^3 \]
The total volume of 1000 small droplets is:
\[ V_{\text{total}} = 1000 \times \frac{4}{3} \pi r^3 = \frac{4000}{3} \pi r^3 \]
The volume of the big drop is:
\[ V_{\text{big}} = \frac{4}{3} \pi R^3 \]
Equating the total volumes:
\[ \frac{4000}{3} \pi r^3 = \frac{4}{3} \pi R^3 \]
Simplifying:
\[ R^3 = 1000r^3 \]
Taking the cube root on both sides:
\[ R = 10r \]
The surface area of one small droplet is:
\[ A_{\text{small}} = 4 \pi r^2 \]
The total surface area of 1000 small droplets is:
\[ A_{\text{total}} = 1000 \times 4 \pi r^2 = 4000 \pi r^2 \]
The surface area of the big drop is:
\[ A_{\text{big}} = 4 \pi R^2 = 4 \pi (10r)^2 = 4 \pi \times 100r^2 = 400 \pi r^2 \]
Surface energy is directly proportional to the surface area. Let \( E_{\text{small}} \) and \( E_{\text{big}} \) be the surface energies of the small droplets and the big drop, respectively. The ratio of the surface energies is:
\[ \frac{E_{\text{big}}}{E_{\text{total}}} = \frac{A_{\text{big}}}{A_{\text{total}}} = \frac{400 \pi r^2}{4000 \pi r^2} = \frac{1}{10} \]
The surface energy will become \( \frac{1}{10} \)th of its original value.
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 \[ I(x) = \int \frac{dx}{(x-11)^{\frac{11}{13}} (x+15)^{\frac{15}{13}}} \] If \[ I(37) - I(24) = \frac{1}{4} \left( b^{\frac{1}{13}} - c^{\frac{1}{13}} \right) \] where \( b, c \in \mathbb{N} \), then \[ 3(b + c) \] is equal to:
For the thermal decomposition of \( N_2O_5(g) \) at constant volume, the following table can be formed, for the reaction mentioned below: \[ 2 N_2O_5(g) \rightarrow 2 N_2O_4(g) + O_2(g) \] Given: Rate constant for the reaction is \( 4.606 \times 10^{-2} \text{ s}^{-1} \).