To find the work done in breaking a big water drop into smaller drops, we need to understand the concept of surface tension and surface energy. The work done is essentially the increase in surface energy when the drop is broken into smaller drops.
Given that initially, we have a large drop of radius \( R \) and we need to break it into smaller drops, the formula for the surface energy is:
\(W = \Delta E = \text{{Surface tension}} \times \Delta A\)
where \(\Delta A\) is the change in surface area.
For a sphere, the surface area \((A)\) is given by \(A = 4 \pi r^2\).
**Step 1: Calculate the initial surface area of the large drop**
The surface area of the large drop is \(A_{large} = 4 \pi R^2\).
**Step 2: Calculate the surface area of the small drops**
If the large drop is divided into \( n \) small drops, each of radius \(r\), then:\) \(n \cdot (4 \pi r^2)\) is the total surface area of all small drops.
The volume of the big drop is equal to the total volume of all small drops:
\(\frac{4}{3} \pi R^3 = n \cdot \frac{4}{3} \pi r^3\)
From this, we get:
\(R^3 = n \cdot r^3\)
\(r = \frac{R}{n^{1/3}}\)
**Case 1: 27 Small Drops**
For the first scenario where \( n = 27 \):
\(r_{27} = \frac{R}{27^{1/3}} = \frac{R}{3}\)
New total surface area:
\(A_{27} = 27 \cdot 4 \pi \left(\frac{R}{3}\right)^2 = 12 \pi R^2\)
Change in surface area:
\(\Delta A_{27} = A_{27} - A_{large} = 12 \pi R^2 - 4 \pi R^2 = 8 \pi R^2\)
Using the given work done for 27 drops:
\(T\cdot 8 \pi R^2 = 10\space \text{J}\) (where T is surface tension)
**Case 2: 64 Small Drops**
For the second scenario where \( n = 64 \):
\(r_{64} = \frac{R}{64^{1/3}} = \frac{R}{4}\)
New total surface area:
\(A_{64} = 64 \cdot 4 \pi \left(\frac{R}{4}\right)^2 = 16 \pi R^2\)
Change in surface area:
\(\Delta A_{64} = A_{64} - A_{large} = 16 \pi R^2 - 4 \pi R^2 = 12 \pi R^2\)
Using the above relation:
\(T\cdot 12 \pi R^2 = 15\space \text{J}\)
Thus, the work done to break the big drop into 64 smaller drops is 15 J, which corresponds to the correct option: 15 J.
The work to break the large drop into 27 smaller drops is given by: \[ W_1 = s \times 4\pi \left( \frac{R}{3} \right)^2 \times 27 - 4\pi R^2 \times s. \] Simplifying: \[ W_1 = 4\pi R^2 \times s \times (2) = 10 \, \text{Joule}. \]
The work to break the large drop into 64 smaller drops is: \[ W_2 = s \times 4\pi R^2 \times (4 - 1) = 4\pi R^2 \times s \times 3. \] Using the value \( W_1 = 10 \) Joules, we substitute into the equation for \( W_2 \): \[ W_2 = 3 \times \frac{10}{2} = 15 \, \text{Joule}. \]
The work required to break the large drop into 64 smaller drops is \( \boxed{15} \, \text{Joule} \).


In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by: