(a) Initially, the capacitance is :
$$C_0=\dfrac{ε_0A}{d}=\dfrac{(8.85\times10^{-12}C^2/N.m^2)(0.12 m^2)}{1.2\times10^{-2}m^2}=89pF$$
(b) Working through Sample Problem — “Dielectric partially filling the gap in a capacitor” algebraically, we find :
$$C=\dfrac{ε_0Aκ}{κ(d-b)+b}=\dfrac{(8.85\times10^{-12}C^2/N.m^2)(0.12m^2)(4.8)}{4.8)(1.2-0.40)(10^{-2}m)+(4.0\times10^{-3}m)}=1.2\times10^2pF.$$
(c) Before the insertion, $$q$$ = $$C_0$$$$V$$$$ (89 pF)(120 V)$$ = $$11 nC$$.
(d) Since the battery is disconnected, q will remain the same after the insertion of the slab,with $$q$$ = $$11 nC$$ .
(e) $$E=q/ε_0A=11\times10^{-9}C/(8.85\times10^{-12}C^2/N.m^2)(0.12m^2)=10kV/m$$
(f) $$ E'=E/κ=(10kV/m)/4.8=2.1kV/m.$$
(g) The potential difference across the plates is :
$$V$$ = $$E(d – b) + E'b$$ = $$(10 kV/m)(0.012 m – 0.0040 m)+ (2.1 kV/m)(0.40 × 10^{–3} m)$$ = $$88 V$$.
(h) The work done is :
$$W_{ext}=\Delta U=\dfrac{q^2}{2}\left( \dfrac{1}{C}-\dfrac{1}{C_0}\right) =\dfrac{(11\times10^{-9}C)^2}{2} \left( \dfrac{1}{89\times10^{-12}F}-\dfrac{1}{120\times10^{-12}F} \right) =-1.7\times10^{-7}J. $$