
In the circuit shown, a potential difference of $60V$is applied across $AB$. The potential difference between the points $M$ and $N$ is:

A) $60V$
B) $15V$
C) $20V$
D) $30V$
Answer
218.7k+ views
Hint: The charges on the capacitors in series are the same. The electric potential across the capacitors or the combination of the capacitors in parallel are the same.
Complete step by step solution:

When capacitors are in series then the equivalent capacitance can be calculated as,
$\dfrac{1}{{{C}_{eq}}}=\dfrac{1}{{{C}_{1}}}+\dfrac{1}{{{C}_{2}}}+\dfrac{1}{{{C}_{3}}}+\cdots \cdots +\dfrac{1}{{{C}_{n}}}$
Here, ${{C}_{1}},{{C}_{2}},{{C}_{3}}\ldots \ldots {{C}_{n}}$ are the capacitances of the capacitors connected in series, and ${{C}_{eq}}$is the equivalent value of the capacitance.
When capacitors are in series then the equivalent capacitance can be calculated as,
$\dfrac{1}{{{C}_{eq}}}=\dfrac{1}{{{C}_{1}}}+\dfrac{1}{{{C}_{2}}}+\dfrac{1}{{{C}_{3}}}+\cdots \cdots +\dfrac{1}{{{C}_{n}}}$
Here, ${{C}_{1}},{{C}_{2}},{{C}_{3}}\ldots \ldots {{C}_{n}}$ are the capacitances of the capacitors connected in parallel, and ${{C}_{eq}}$ is the equivalent value of the capacitance.
From the electric circuit given, the capacitors in the right branch are in series.
Let equivalent capacitance of the capacitors in the right branch is ${{C}_{1}}$
Using the formula of the equivalent capacitance in series,
$\begin{array}{*{35}{l}}
{} & \dfrac{1}{{{C}_{1}}}=\dfrac{1}{2C}+\dfrac{1}{C}+\dfrac{1}{2C} \\
{} & \Rightarrow \dfrac{1}{{{C}_{1}}}=\dfrac{1+2+1}{2C} \\
{} & \Rightarrow \dfrac{1}{{{C}_{1}}}=\dfrac{4}{2C} \\
{} & \Rightarrow {{C}_{1}}=\dfrac{2C}{4} \\
{} & \therefore {{C}_{1}}=\dfrac{C}{2}\text{ }\!\!~\!\!\text{ }\!\!~\!\!\text{ } \\
\end{array}$
Now, ${{C}_{1}}$ is in parallel with the capacitor on the left branch.
Let ${{C}_{eq}}$ is the equivalent capacitance of the given circuit.
Using the equivalent capacitance in parallel combination,
$\begin{array}{*{20}{l}}
{}&{{C_{eq}} = {C_1} + C} \\
{}&{ \Rightarrow {C_{eq}} = \dfrac{C}{2} + C} \\
{}&{ \Rightarrow {C_{eq}} = \dfrac{{C + 2C}}{2}} \\
{}&{\therefore {C_{eq}} = \dfrac{{3C}}{2}{\text{ }}\;{\text{ }}\;{\text{ }}}
\end{array}$
The equivalent capacitance of the given electric circuit is $\dfrac{3C}{2}$
Let $Q$ is the total charge flown from the battery connected.
$\begin{array}{*{35}{l}}
{} & Q={{C}_{eq}}V \\
{} & \Rightarrow Q=\left( \dfrac{3C}{2} \right)\left( 60V \right) \\
{} & \therefore Q=90CV\text{ }\!\!~\!\!\text{ }\!\!~\!\!\text{ } \\
\end{array}$
The total charge gets distributed between the two branches.
${{Q}_{1}}+{{Q}_{2}}=Q\ldots \ldots \left( i \right)$
As right and the left branches are in parallel, so the electrical potential across both must be the same.
$\begin{array}{*{35}{l}}
{} & {{V}_{1}}={{V}_{2}} \\
{} & \Rightarrow \dfrac{{{Q}_{1}}}{C}=\dfrac{{{Q}_{2}}}{\left( \dfrac{C}{2} \right)} \\
{} & \Rightarrow {{Q}_{1}}=2{{Q}_{2}}\left( \dfrac{C}{C} \right) \\
{} & \therefore {{Q}_{1}}=2{{Q}_{2}}\ldots \ldots \left( ii \right) \\
\text{ }\!\!~\!\!\text{ } & {} \\
\end{array}$
From equations $\left( i \right)$ and $\left( ii \right)$,
$\begin{array}{*{35}{l}}
{} & \left( 2{{Q}_{2}} \right)+{{Q}_{2}}=Q \\
{} & \Rightarrow 3{{Q}_{2}}=Q \\
{} & \therefore {{Q}_{2}}=\dfrac{Q}{3}\text{ }\!\!~\!\!\text{ }\!\!~\!\!\text{ } \\
\end{array}$
Charge on the capacitor between M and N is ${{Q}_{2}}$
The potential difference between the point M and N is ${{V}_{MN}}=\dfrac{{{Q}_{2}}}{C}$
$\begin{array}{*{35}{l}}
\text{ }\!\!~\!\!\text{ }\!\!~\!\!\text{ } & {{V}_{MN}}=\dfrac{\left( \dfrac{Q}{3} \right)}{C} \\
{} & \Rightarrow {{V}_{MN}}=\dfrac{Q}{3C} \\
\text{ }\!\!~\!\!\text{ }\!\!~\!\!\text{ } & \Rightarrow {{V}_{MN}}=\dfrac{90CV}{3C} \\
{} & \therefore {{V}_{MN}}=30V\text{ }\!\!~\!\!\text{ }\!\!~\!\!\text{ } \\
\end{array}$
Hence, the potential difference between M and N is $30V$.
Note: The net potential drop in the right loop which comprises the capacitor $2C,C,2C\text{ and }C$. Total charge gets distributed between right and the left branch because they are connected in parallel. The charges on the capacitors in series are the same.
Complete step by step solution:

When capacitors are in series then the equivalent capacitance can be calculated as,
$\dfrac{1}{{{C}_{eq}}}=\dfrac{1}{{{C}_{1}}}+\dfrac{1}{{{C}_{2}}}+\dfrac{1}{{{C}_{3}}}+\cdots \cdots +\dfrac{1}{{{C}_{n}}}$
Here, ${{C}_{1}},{{C}_{2}},{{C}_{3}}\ldots \ldots {{C}_{n}}$ are the capacitances of the capacitors connected in series, and ${{C}_{eq}}$is the equivalent value of the capacitance.
When capacitors are in series then the equivalent capacitance can be calculated as,
$\dfrac{1}{{{C}_{eq}}}=\dfrac{1}{{{C}_{1}}}+\dfrac{1}{{{C}_{2}}}+\dfrac{1}{{{C}_{3}}}+\cdots \cdots +\dfrac{1}{{{C}_{n}}}$
Here, ${{C}_{1}},{{C}_{2}},{{C}_{3}}\ldots \ldots {{C}_{n}}$ are the capacitances of the capacitors connected in parallel, and ${{C}_{eq}}$ is the equivalent value of the capacitance.
From the electric circuit given, the capacitors in the right branch are in series.
Let equivalent capacitance of the capacitors in the right branch is ${{C}_{1}}$
Using the formula of the equivalent capacitance in series,
$\begin{array}{*{35}{l}}
{} & \dfrac{1}{{{C}_{1}}}=\dfrac{1}{2C}+\dfrac{1}{C}+\dfrac{1}{2C} \\
{} & \Rightarrow \dfrac{1}{{{C}_{1}}}=\dfrac{1+2+1}{2C} \\
{} & \Rightarrow \dfrac{1}{{{C}_{1}}}=\dfrac{4}{2C} \\
{} & \Rightarrow {{C}_{1}}=\dfrac{2C}{4} \\
{} & \therefore {{C}_{1}}=\dfrac{C}{2}\text{ }\!\!~\!\!\text{ }\!\!~\!\!\text{ } \\
\end{array}$
Now, ${{C}_{1}}$ is in parallel with the capacitor on the left branch.
Let ${{C}_{eq}}$ is the equivalent capacitance of the given circuit.
Using the equivalent capacitance in parallel combination,
$\begin{array}{*{20}{l}}
{}&{{C_{eq}} = {C_1} + C} \\
{}&{ \Rightarrow {C_{eq}} = \dfrac{C}{2} + C} \\
{}&{ \Rightarrow {C_{eq}} = \dfrac{{C + 2C}}{2}} \\
{}&{\therefore {C_{eq}} = \dfrac{{3C}}{2}{\text{ }}\;{\text{ }}\;{\text{ }}}
\end{array}$
The equivalent capacitance of the given electric circuit is $\dfrac{3C}{2}$
Let $Q$ is the total charge flown from the battery connected.
$\begin{array}{*{35}{l}}
{} & Q={{C}_{eq}}V \\
{} & \Rightarrow Q=\left( \dfrac{3C}{2} \right)\left( 60V \right) \\
{} & \therefore Q=90CV\text{ }\!\!~\!\!\text{ }\!\!~\!\!\text{ } \\
\end{array}$
The total charge gets distributed between the two branches.
${{Q}_{1}}+{{Q}_{2}}=Q\ldots \ldots \left( i \right)$
As right and the left branches are in parallel, so the electrical potential across both must be the same.
$\begin{array}{*{35}{l}}
{} & {{V}_{1}}={{V}_{2}} \\
{} & \Rightarrow \dfrac{{{Q}_{1}}}{C}=\dfrac{{{Q}_{2}}}{\left( \dfrac{C}{2} \right)} \\
{} & \Rightarrow {{Q}_{1}}=2{{Q}_{2}}\left( \dfrac{C}{C} \right) \\
{} & \therefore {{Q}_{1}}=2{{Q}_{2}}\ldots \ldots \left( ii \right) \\
\text{ }\!\!~\!\!\text{ } & {} \\
\end{array}$
From equations $\left( i \right)$ and $\left( ii \right)$,
$\begin{array}{*{35}{l}}
{} & \left( 2{{Q}_{2}} \right)+{{Q}_{2}}=Q \\
{} & \Rightarrow 3{{Q}_{2}}=Q \\
{} & \therefore {{Q}_{2}}=\dfrac{Q}{3}\text{ }\!\!~\!\!\text{ }\!\!~\!\!\text{ } \\
\end{array}$
Charge on the capacitor between M and N is ${{Q}_{2}}$
The potential difference between the point M and N is ${{V}_{MN}}=\dfrac{{{Q}_{2}}}{C}$
$\begin{array}{*{35}{l}}
\text{ }\!\!~\!\!\text{ }\!\!~\!\!\text{ } & {{V}_{MN}}=\dfrac{\left( \dfrac{Q}{3} \right)}{C} \\
{} & \Rightarrow {{V}_{MN}}=\dfrac{Q}{3C} \\
\text{ }\!\!~\!\!\text{ }\!\!~\!\!\text{ } & \Rightarrow {{V}_{MN}}=\dfrac{90CV}{3C} \\
{} & \therefore {{V}_{MN}}=30V\text{ }\!\!~\!\!\text{ }\!\!~\!\!\text{ } \\
\end{array}$
Hence, the potential difference between M and N is $30V$.
Note: The net potential drop in the right loop which comprises the capacitor $2C,C,2C\text{ and }C$. Total charge gets distributed between right and the left branch because they are connected in parallel. The charges on the capacitors in series are the same.
Recently Updated Pages
A square frame of side 10 cm and a long straight wire class 12 physics JEE_Main

The work done in slowly moving an electron of charge class 12 physics JEE_Main

Two identical charged spheres suspended from a common class 12 physics JEE_Main

According to Bohrs theory the timeaveraged magnetic class 12 physics JEE_Main

ill in the blanks Pure tungsten has A Low resistivity class 12 physics JEE_Main

The value of the resistor RS needed in the DC voltage class 12 physics JEE_Main

Trending doubts
JEE Main 2026: Application Form Open, Exam Dates, Syllabus, Eligibility & Question Papers

Derivation of Equation of Trajectory Explained for Students

Hybridisation in Chemistry – Concept, Types & Applications

Understanding the Angle of Deviation in a Prism

Understanding Collisions: Types and Examples for Students

Understanding Atomic Structure for Beginners

Other Pages
JEE Advanced Marks vs Ranks 2025: Understanding Category-wise Qualifying Marks and Previous Year Cut-offs

How to Convert a Galvanometer into an Ammeter or Voltmeter

Understanding Centrifugal Force in Physics

JEE Main Marking Scheme 2026- Paper-Wise Marks Distribution and Negative Marking Details

Degree of Dissociation: Meaning, Formula, Calculation & Uses

Understanding Electromagnetic Waves and Their Importance

