(a) Consider the left side:
The plate area of the left part with the dielectric is
bn.
Its capacitance,
C1=K1ε0bnd
And without dielectric
C2=ε0b(L1−n)d
These are connected in parallel, so the equivalent capacitance,
C=C1+C2=ε0bd[L1+n(K1−1)] .......(1)
Let the potential difference or emf of the battery
V1.
Suppose, dielectric slab is attracted by electric field and an external force
F.
Consider the part
dn which makes inside further, As the potential differences remains constant as
V.
The charge supply,
dq=(dC)V to the capacitor.
The work done by the battery is
dWb=Vdq=(dC)V2
The external force
F does a work
dWe=(−F.dn) during a small displacement.
The total work done will be
dWb+dWe=(dC)V2−Fdn
This should be equal to the increase
dV in the stored energy.
Thus,
12(dC)V2=(dC)V2−Fdn
⇒F=12V2dCdn
From equation (1)
F=ε0bV22d(K1−1)
⇒V21=F×2dε0b(K1−1)
⇒V1=√F×2dε0b(K1−1)
Similarly, for right side potential difference,
⇒V2=√F×2dε0b(K2−1)
∴V1V2=√F×2dε0b(K1−1)√F×2dε0b(K2−1)
⇒V1V2=√K2−1√K1−1
Given,
K1=2 and
K2=5
⇒V1V2=√5−1√2−1=2
Accepted answer: 2, 2.0, 2.00