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Question: The parallel combination of two air filled parallel plate capacitors of capacitance \[C\] and \[nC\]...

The parallel combination of two air filled parallel plate capacitors of capacitance CC and nCnC is connected to a battery of voltage VV. When the capacitors are fully charged, the battery is removed and after a dielectric material of dielectric constant KK is placed between the two plates of the first capacitor. The new potential difference of the combined system is?
(A) V(K+n)\dfrac{V}{{\left( {K + n} \right)}}
(B) VV
(C) (n+1)V(K+n)\dfrac{{\left( {n + 1} \right)V}}{{\left( {K + n} \right)}}
(D) nV(K+n)\dfrac{{nV}}{{\left( {K + n} \right)}}

Explanation

Solution

For parallel combination of capacitors, the equivalent or effective capacitance is the sum of all the capacitance of the parallel capacitors. When the battery of a capacitor is removed, the charge is kept constant under all conditions (as long as it is not discharged)
Formula used: In this solution we will be using the following formulae;
Q=CVQ = CV where QQ is the total charge stored in a capacitor, CC is the capacitance of the capacitor, and VV is the voltage across the capacitor.
Ceq=C1+C2{C_{eq}} = {C_1} + {C_2} where Ceq{C_{eq}} is the equivalent or effective capacitance of two capacitors in a parallel combination, C1{C_1} and C2{C_2} are the capacitances of the individual capacitors in the combination.

Complete Step-by-Step Solution:
When the capacitors are charged, the voltage across them is VV.
The charge on a capacitor is given as
Q=CVQ = CV where QQ is the total charge stored in a capacitor, CC is the capacitance of the capacitor, and VV is the voltage across the capacitor.
Hence, the charge on each capacitor after charge is
\Rightarrow Q1=CV{Q_1} = CV and
\Rightarrow Q2=nCV{Q_2} = nCV
Then the total charge in the system would be
\Rightarrow Q=Q1+Q2=CV+nCV=(n+1)CVQ = {Q_1} + {Q_2} = CV + nCV = \left( {n + 1} \right)CV
Now, a dielectric of dielectric constant KK is placed between the plates of the first capacitor, hence, the capacitance becomes
C1=KC{C_1} = KC
But the capacitance of the second remains C2=nC{C_2} = nC
For capacitors in parallel, the effective capacitance is given as
\Rightarrow Ceq=C1+C2{C_{eq}} = {C_1} + {C_2} where Ceq{C_{eq}} is the equivalent or effective capacitance of two capacitors in a parallel combination, C1{C_1} and C2{C_2} are the capacitances of the individual capacitors in the combination.
Hence,
\Rightarrow Ceq=KC+nC=C(K+n){C_{eq}} = KC + nC = C\left( {K + n} \right)
Then the new potential difference would be given as
\Rightarrow Vn=QCeq=(n+1)CVC(K+n){V_n} = \dfrac{Q}{{{C_{eq}}}} = \dfrac{{\left( {n + 1} \right)CV}}{{C\left( {K + n} \right)}}
By cancelling common terms, we have
\Rightarrow Vn=(n+1)V(K+n){V_n} = \dfrac{{\left( {n + 1} \right)V}}{{\left( {K + n} \right)}}

Hence, the correct option is C.

Note: For understanding, the formula Ceq=C1+C2{C_{eq}} = {C_1} + {C_2} can be proven from the knowledge that the total charge in the system is the sum of the charges in the two capacitors. Hence, since Q=CVQ = CV
We have that
\Rightarrow Q=Q1+Q2=C1V+C2VQ = {Q_1} + {Q_2} = {C_1}V + {C_2}V.
CeqV=C1V+C2V\Rightarrow {C_{eq}}V = {C_1}V + {C_2}V
It remains VV because potential across parallel components are equal, hence,
Ceq=C1+C2{C_{eq}} = {C_1} + {C_2}