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Question: Switch S is closed at \( t = 0 \) , \( {I_{10}} \) is the current supplied by the battery just after...

Switch S is closed at t=0t = 0 , I10{I_{10}} is the current supplied by the battery just after closing the switch S. Q1{Q_1} , Q2{Q_2} and Q3{Q_3} are the charges on the capacitors of 10μF10\mu F , 20μF20\mu F and 30μF30\mu F in steady state respectively. I20{I_{20}} is the current supplied by the battery in the circuit at steady state. Choose the correct statement(s).

(A) I10>I20{I_{10}} > {I_{20}}
(B) I10<I20{I_{10}} < {I_{20}}
(C) Q1<Q2<Q3{Q_1} < {Q_2} < {Q_3}
(D) Q1<Q3<Q2{Q_1} < {Q_3} < {Q_2}

Explanation

Solution

No current was flowing through the capacitors before the switch was closed at t=0t = 0 . We know that current is the flow of charge.

Formula Used: The formulae used in the solution are given here.
Current I=CdVdtI = C\dfrac{{dV}}{{dt}} , where CC the capacitance in Farad and voltage across the capacitor is VV .
Charge on the capacitor, Q=CVQ = CV .

Complete Step by Step Solution
No flow of charge to and from the capacitors plates was zero, prior to t=0t = 0 . Hence as charge on capacitor plates varies proportionally with the voltage across them, therefore voltage across them is zero before t=0t = 0 . We can say that the capacitor was short circuited or it behaved as if it was being short circuited.
We know, current through capacitor, II and voltage across the capacitor, VV , is related as
I=CdVdtI = C\dfrac{{dV}}{{dt}} , where CC is the capacitance in Farad.
Following from the above, when the switch is turned on at t=0t = 0 , the capacitor behaves as being short circuited , for the initial time being.
The circuit thus looks like,

On solving, we see that the resistances 10Ω10\Omega , 6Ω6\Omega , 15Ω15\Omega , 6Ω6\Omega are in parallel. So equivalent resistance,
1Req=110+16+115+16\dfrac{1}{{{R_{eq}}}} = \dfrac{1}{{10}} + \dfrac{1}{6} + \dfrac{1}{{15}} + \dfrac{1}{6}
1Req=12\Rightarrow \dfrac{1}{{{R_{eq}}}} = \dfrac{1}{2} .
So equivalent resistance, Req=2Ω{R_{eq}} = 2\Omega .
There is another resistance 2Ω2\Omega connected in series to the arrangement for which Req=2Ω{R_{eq}} = 2\Omega .
Thus, resistance R=4ΩR = 4\Omega .
By Ohm’s Law, V=IRV = IR .
Thus, I10=604=15A{I_{10}} = \dfrac{{60}}{4} = 15A .
At steady state, that is, after some time, the capacitor starts behaving like an open circuit.
Thus two 6Ω6\Omega resistors are in parallel with two 12Ω12\Omega resistors.
Equivalent resistance is thus,
1Req=12×6+12×12\dfrac{1}{{{R_{eq}}}} = \dfrac{1}{{2 \times 6}} + \dfrac{1}{{2 \times 12}}
1Req=18\Rightarrow \dfrac{1}{{{R_{eq}}}} = \dfrac{1}{8}
S, equivalent resistance Req=8Ω{R_{eq}} = 8\Omega .
There are two resistances 10Ω10\Omega and 2Ω2\Omega connected in series to the arrangement for which Req=8Ω{R_{eq}} = 8\Omega
By Ohm’s Law, V=IRV = IR .
At I20=6020=3A.{I_{20}} = \dfrac{{60}}{{20}} = 3A.
So I20>I10{I_{20}} > {I_{10}} .
Hence Option A is correct.
Now charge on the capacitor, Q=CVQ = CV .
Voltage across the 10μF10\mu F capacitor at steady state= 30V30V .
Q1=10μF×30{Q_1} = 10\mu F \times 30 .
Voltage across the 20μF20\mu F capacitor at steady state= 30V30V .
Q2=20μF×42{Q_2} = 20\mu F \times 42 .
Voltage across the 30μF30\mu F capacitor at steady state= 30V30V .
Q3=30μF×24{Q_3} = 30\mu F \times 24 .
It is quite apparent, Q3>Q2>Q1{Q_3} > {Q_2} > {Q_1} .
Hence Option D is also correct.

Note:
We can conclude that if voltage changes abruptly, current through the capacitor is spiked up. So, the tendency of the capacitor is to avoid the abrupt change in voltage across it.