Data: k = 1(air), A = 6 × 10
-3 m
2, d = 2
mm = 2 × 10
-3 m,V = 100V, t = 2 mm = d, k
1 = 6,
ε
0 = 8.85 × 10
-12 F/m
(i) The capacitance of the air capacitor, C
0 = \(\frac{\varepsilon_{0} A}{d}\)
= \(\frac{\left(8.85 \times 10^{-12}\right)\left(6 \times 10^{-3}\right)}{2 \times 10^{-3}}\)
= 26.55 × 10
-12 F = 26.55 pF
(ii) Q0 = C0V = (26.55 × 10-12)(100)
= 26.55 × 10-10 C = 2.655 nC
(iii) The dielectric of relative permittivity k1 completely fills the space between the plates (∵t = d), so that the new capacitance is C = k1C0.
With the supply still connected, V remains the same.
∴ Q = CV = kC0V = kQ0 =6(2.655 nF) = 15.93 nC
Therefore, the charge on the plates increases.