Question
Question: A series combination of two capacitances of value \[0.1\,\mu F\] and \[1\,\mu F\] is connected with ...
A series combination of two capacitances of value 0.1μF and 1μF is connected with a source of voltage 500 volts. The potential difference in volts across the capacitor of value 0.1μF will be:
A. 50
B. 500
C. 45.5
D. 454.5
Solution
In series circuit, the charge through the circuit does not change. Use the formula for voltage across the capacitor in terms of capacitance and charge to express the charge across both capacitors. In a series circuit, the total potential difference is the potential difference across each component.
Formula used:
Q=CV
Here, Q is the charge, C is capacitance and V is the voltage across the capacitor.
Complete step by step answer:
We have given that two capacitors are connected in series. We know that, according to the law of conservation of charge, in series connection the charges remain conserved. Therefore, the charge across both capacitors is the same.
We know the charge flowing through the capacitor is,
Q=CV
Here, Q is the charge and V is the voltage across the capacitor.
We assume the first capacitor is C1=0.1μF and the second capacitor is C2=1μF.
Therefore, we can write,
Q=C1V1=C2V2
⇒V2=C2C1V1 …… (1)
This is the potential difference across the1μF capacitor.
Now, we know that the total potential difference in the circuit is the sum of potential differences across C1 and C2.
Therefore, we can write,
V=V1+V2
Here, V1 is the potential difference across C1.
We can use equation (1) to rewrite the above equation.
V=V1+C2C1V1
⇒V=V1(1+C2C1)
⇒V=V1(C2C2+C1)
⇒V1=C1+C2C2V
Substitute 1μF for C2, 500 V for V and 0.1μF for C1 in the above equation.
⇒V1=0.1+1(1)(500)
⇒V1=454.5V
So, the correct answer is “Option D”.
Note:
To answer such types of questions, the key is to remember voltage, charge and current in series and parallel circuits. In a parallel circuit, the voltage across the capacitor remains constant but charge does not remain conserved. In a series circuit, the voltage drops at each component but the charge remains conserved.