For given circuit, charges on capacitor \[{{C}_{1}}\text{ and }{{\text{C}}_{2}}\] in steady state will be equal to:
\[\begin{align}
& \text{A) }{{\text{C}}_{1}}|{{V}_{A}}-{{V}_{C}}|,{{C}_{2}} |{{V}_{C}}-{{V}_{B}}|\text{ respectively} \\
& \text{B) }{{\text{C}}_{1}}|{{V}_{A}}-{{V}_{B}}|, {{C}_{2}}|{{V}_{A}}-{{V}_{B}}|\text{ respectively} \\
& \text{C) (}{{\text{C}}_{1}}+{{C}_{2}})|{{V}_{A}}-{{V}_{B}}|\text{ on each capacitor} \\
& \text{D) }\left( \dfrac{{{C}_{1}}{{C}_{2}}}{{{C}_{1}}+{{C}_{2}}} \right)|{{V}_{A}}-{{V}_{B}}|\text{ on each capacitor} \\
\end{align}\]
Answer
638.1k+ views
Hint: The charge accumulated on a capacitor is directly proportional to the capacitance C and voltage across the capacitance V. We are given the different values of potential at each end which has a net effect on each capacitance in the whole network.
Complete step-by-step solution:
We know that the capacitance of a capacitor is the ability of a pair of parallel plates to store the electrical charges on the plates at a given voltage. The capacitance is related to the charge accumulated on the plates and the voltage as –
\[C=\dfrac{Q}{V}\]
The charge accumulated on a parallel plate capacitor is, therefore, given as –
\[Q=CV\]
Now, let us consider the situation given to us in which the capacitors \[{{C}_{1}}\text{ and }{{\text{C}}_{2}}\] are connected to external sources \[{{\text{V}}_{\text{A}}}\text{,}{{\text{V}}_{\text{B }}}\text{and }{{\text{V}}_{\text{C}}}\] through the resistor R as shown in the circuit given below.
Now, we understand that in the given circuit the node joining the capacitors has a potential which is equal to the \[{{\text{V}}_{C}}\].
So, we can understand that the potential across the capacitors \[{{C}_{1}}\text{ and }{{\text{C}}_{2}}\] can be given as –
Across the capacitor \[{{C}_{1}}\], the voltage is –
\[{{V}_{1}}={{V}_{A}}-{{V}_{C}}\]
Across the capacitor \[{{C}_{2}}\], the voltage is –
\[{{V}_{2}}={{V}_{B}}-{{V}_{C}}\]
Now, we can find the charge in each of the capacitor by using the relation between the voltage and the capacitance of the capacitor as explained earlier –
\[Q=CV\]
For the capacitor \[{{C}_{1}}\], the charge accumulated is given as –
\[\begin{align}
& {{Q}_{1}}={{C}_{1}}{{V}_{1}} \\
& \therefore {{Q}_{1}}={{C}_{1}}({{V}_{A}}-{{V}_{C}}) \\
\end{align}\]
For the capacitor \[{{C}_{2}}\], the charge accumulated is given as –
\[\begin{align}
& {{Q}_{2}}={{C}_{2}}{{V}_{2}} \\
& \therefore {{Q}_{2}}={{C}_{2}}({{V}_{B}}-{{V}_{C}}) \\
\end{align}\]
So, we get the charge accumulated on both the capacitors.
The correct answer is option A.
Note: The resistance used in the circuit avoids the shorting of the circuit in case the capacitors reach a breakdown. The electric field developing inside the capacitor can exceed the ionizing energy of the electric field in the air resulting in conduction without resistance.
Complete step-by-step solution:
We know that the capacitance of a capacitor is the ability of a pair of parallel plates to store the electrical charges on the plates at a given voltage. The capacitance is related to the charge accumulated on the plates and the voltage as –
\[C=\dfrac{Q}{V}\]
The charge accumulated on a parallel plate capacitor is, therefore, given as –
\[Q=CV\]
Now, let us consider the situation given to us in which the capacitors \[{{C}_{1}}\text{ and }{{\text{C}}_{2}}\] are connected to external sources \[{{\text{V}}_{\text{A}}}\text{,}{{\text{V}}_{\text{B }}}\text{and }{{\text{V}}_{\text{C}}}\] through the resistor R as shown in the circuit given below.
Now, we understand that in the given circuit the node joining the capacitors has a potential which is equal to the \[{{\text{V}}_{C}}\].
So, we can understand that the potential across the capacitors \[{{C}_{1}}\text{ and }{{\text{C}}_{2}}\] can be given as –
Across the capacitor \[{{C}_{1}}\], the voltage is –
\[{{V}_{1}}={{V}_{A}}-{{V}_{C}}\]
Across the capacitor \[{{C}_{2}}\], the voltage is –
\[{{V}_{2}}={{V}_{B}}-{{V}_{C}}\]
Now, we can find the charge in each of the capacitor by using the relation between the voltage and the capacitance of the capacitor as explained earlier –
\[Q=CV\]
For the capacitor \[{{C}_{1}}\], the charge accumulated is given as –
\[\begin{align}
& {{Q}_{1}}={{C}_{1}}{{V}_{1}} \\
& \therefore {{Q}_{1}}={{C}_{1}}({{V}_{A}}-{{V}_{C}}) \\
\end{align}\]
For the capacitor \[{{C}_{2}}\], the charge accumulated is given as –
\[\begin{align}
& {{Q}_{2}}={{C}_{2}}{{V}_{2}} \\
& \therefore {{Q}_{2}}={{C}_{2}}({{V}_{B}}-{{V}_{C}}) \\
\end{align}\]
So, we get the charge accumulated on both the capacitors.
The correct answer is option A.
Note: The resistance used in the circuit avoids the shorting of the circuit in case the capacitors reach a breakdown. The electric field developing inside the capacitor can exceed the ionizing energy of the electric field in the air resulting in conduction without resistance.
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