Physics · Electrostatic Potential And Capacitance · NEET
Charge does add up n times (Q = nq), so you might expect potential to be n times bigger. But potential is V = kQ/R, and R also grows. Since volume is conserved, R = n^(1/3) × r. So V_big = k(nq) / (n^(1/3) r) = n / n^(1/3) × (kq/r) = n^(2/3) × v. The larger radius pulls the potential back down, giving n^(2/3), not n.
Use volume conservation. The liquid does not disappear, so the total volume of n small drops equals the volume of the one big drop: n × (4/3)π r^3 = (4/3)π R^3. Cancel (4/3)π: n r^3 = R^3, so R = n^(1/3) × r. For n = 27, R = 3r; for n = 8, R = 2r; for n = 1000, R = 10r.
Yes. Charge cannot be created or destroyed. If each small drop carries charge q, the big drop carries Q = nq. This is the key input, along with volume conservation, that gives the n^(2/3) result.
Surface field is E = kQ/R^2 = k(nq)/(n^(1/3) r)^2 = n^(1/3) × (kq/r^2) = n^(1/3) × e. So the big drop's surface field is n^(1/3) times a small drop's field. Note: potential scales as n^(2/3) but surface field scales as n^(1/3) — a common NEET mix-up.
Yes. n^(2/3) with n = 27 is (27)^(2/3) = (3^3)^(2/3) = 3^2 = 9. So the big drop has 9 times the potential of one small drop. If each small drop was at 220 V, the big drop is at 1980 V (the NEET 2021 answer).
Twenty seven drops of same size are charged at 220 V each. They combine to form a bigger drop. Calculate the potential of the bigger drop.
Try the real previous-year questions from this chapter — each with the answer and a full solution.
V_big = n^(2/3) × v, where v is the potential of one small drop. This comes from charge Q = nq and radius R = n^(1/3) × r (volume conserved).
R = n^(1/3) × r. Volume is conserved, so n r^3 = R^3. For 8 drops R = 2r, for 27 drops R = 3r, for 64 drops R = 4r.
Surface charge density σ = Q/(4πR^2) = nq/(4π (n^(1/3) r)^2) = n^(1/3) × σ_small. So it becomes n^(1/3) times the small drop's value.
It is a direct-formula MCQ that appears often (e.g., NEET 2021). Once you know V scales as n^(2/3), you solve it in seconds. It also tests conservation of charge and volume together, which are core electrostatics ideas.
For a single charged sphere, U ∝ Q^2/R = (nq)^2/(n^(1/3) r) = n^(5/3) × (q^2/r). So the big drop's self-energy is n^(5/3) times a small drop's self-energy — a higher-order twist NEET occasionally uses.