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Question: In the circuit shown, the symbols have their usual meanings. The cell has emf \(\varepsilon \). \(X\...

In the circuit shown, the symbols have their usual meanings. The cell has emf ε\varepsilon . XX is initially joined to YY for a long time. Then, XX is joined to ZZ. The maximum charge on CC at any later time will be

A. εRLC\dfrac{\varepsilon }{{R\sqrt {LC} }}
B. εR2LC\dfrac{{\varepsilon R}}{{2\sqrt {LC} }}
C. εLCR\dfrac{{\varepsilon \sqrt {LC} }}{R}
D. εLC2R\dfrac{{\varepsilon \sqrt {LC} }}{{2R}}

Explanation

Solution

To give the answer this problem we must know about the concept of LC circuit. In this problem first we determine the current flow through the circuit, then find the energy stored, and charge in the circuit, and finally apply the law of conservation of energy to obtain the required result.

Complete step by step answer:
In the given circuit, the LL represents the inductance, RR represents the resistance, and CC represents the capacitance.When initially the circuit is connected with YY then the charge is started to store in inductance, and at the steady state the current flow through the circuit will be as follows.
i=εRi = \dfrac{\varepsilon }{R}
The energy stored at the steady state will be as follows.
E=12Li2E = \dfrac{1}{2}L{i^2}
When the circuit is connected with ZZ then it will become an LC circuit. As we know that in LC circuits oscillation occurs. In the oscillation if the LL is fully charged initially then energy transferred to CC and when CC is completely charged then it slowly starts discharging and the process charging and discharging of LL and CC is going on in LC circuit.The charge stored in LCLC circuit will be maximum only when energy is maximum in that circuit.
The charge stored in the circuit is given by,
Charge  stored=Q22C{\rm{Charge}}\;{\rm{stored}} = \dfrac{{{Q^2}}}{{2C}}
From the conservation of energy,

12Li2=Q22C Q=iLC\dfrac{1}{2}L{i^2} = \dfrac{{{Q^2}}}{{2C}}\\\ Q = i\sqrt {LC}

By substituting εR\dfrac{\varepsilon }{R} for ii in the equation Q=iLCQ = i\sqrt {LC} , we get,
Q=εRLC\therefore Q = \dfrac{\varepsilon }{R}\sqrt {LC}

Therefore, the option C is the correct answer.

Note: The key concept of this problem is that initially there was no energy in the capacitor, so, by the law of conservation of energy, the energy stored in the LL will be equal to the charge stored in CC.