Concept:When two conducting spheres are brought into contact, charges redistribute until their electric potentials become equal.
Explanation:For a metal sphere,
Q=σ⋅4πr2.
Initially, both spheres have the same surface charge density
σ.
For the smaller sphere of radius
R:
Q1=σ⋅4πR2.
For the bigger sphere of radius
3R:
Q2=σ⋅4π(3R)2=9σ⋅4πR2.
On contact, charge flows from one sphere to the other until potentials become equal.
For a conducting sphere,
V=rkQ.
After contact, equate the potentials:
RkQ1′=3RkQ2′.
Cancelling
k and
R gives
Q2′=3Q1′.
After separation, the new surface charge densities are:
σ1=4πR2Q1′ and
σ2=4π(3R)2Q2′.
Substitute
Q2′=3Q1′:
σ2=36πR23Q1′=12πR2Q1′.
Thus,
σ2σ1=12πR2Q1′4πR2Q1′=3.
Answer:The ratio
σ2σ1 is
3, which is option D.