Question
Question: A galvanometer of resistance \(25\Omega \) is connected to a battery of \(2V\) along with a resistan...
A galvanometer of resistance 25Ω is connected to a battery of 2V along with a resistance in series. When the value of this resistance is 3000Ω a full- scale deflection 30units is obtained in the galvanometer. To reduce this deflection to 20units, the resistance in series will be:
(A) 1991.66Ω
(B) 5413Ω
(C) 2000Ω
(D) 6000Ω
Solution
Hint From the diagram, we can see that the battery, the galvanometer, and the resistance are in series with each other. The internal resistance of the galvanometer, r is 25Ω. The initial resistance in series is 3000Ω. Thus we apply Kirchhoff’s Voltage Law in the above circuit to get the current flowing through the circuit. Next, we insert a new resistance x in series with the previous resistance to get the new current flow.
Complete Step by step solution Applying Kirchhoff’s Voltage Law in the above circuit, we get
2V=iR+ir .
The values of R=3000Ω, and r=25Ω are given.
Substituting these values in the given equation, we get
⇒2V=i(3000Ω+25Ω)
⇒i=30252A
This value is described as 30units when the deflection of the galvanometer is at full scale.
Thus if i=30252A=30units then
1unit is 3025×302A.
Similarly, deflection 20units is equal to 3025×302×20Acurrent flow through the circuit which is the new current I .
Thus keeping the numerator same, the denominator turns out to be
3025×1.52A=4537.5Ω2V
; i.e. the denominator turns out to be (4512.5+25)Ω.
We now get the required net resistance of the new circuit to be 4537.5Ω, which is including the internal resistance of the galvanometer.
This is because we can compare this equation with the K.V.L. equation of the new circuit, where 2V=I(r+R)=3025×302×20(25Ω+R).
On further simplifying we get,
⇒2×2×203025×30=25+R
∴R+25Ω=(4512.5+25)Ω
Thus we get the required value of the new resistance R as 4512.5Ω.
Therefore the correct option is not present in the given question.
Note A galvanometer measures the amount of current flowing through a given circuit. Here the galvanometer resistance is constant since we use the same galvanometer for both the readings. The value of the resistance R changes as we wish to decrease the value of current passing through the galvanometer.