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Question: A galvanometer of resistance \(25\Omega \) is connected to a battery of \(2V\) along with a resistan...

A galvanometer of resistance 25Ω25\Omega is connected to a battery of 2V2V along with a resistance in series. When the value of this resistance is 3000Ω3000\Omega a full- scale deflection 30units30units is obtained in the galvanometer. To reduce this deflection to 20units20units, the resistance in series will be:
(A) 1991.66Ω1991.66\Omega
(B) 5413Ω5413\Omega
(C) 2000Ω2000\Omega
(D) 6000Ω6000\Omega

Explanation

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, rr is 25Ω25\Omega . The initial resistance in series is 3000Ω3000\Omega . 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 xx 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+ir2V = iR + ir .
The values of R=3000ΩR = 3000\Omega , and r=25Ωr = 25\Omega are given.
Substituting these values in the given equation, we get
2V=i(3000Ω+25Ω)\Rightarrow 2V = i(3000\Omega + 25\Omega )
i=23025A\Rightarrow i = \dfrac{2}{{3025}}A
This value is described as 30units30units when the deflection of the galvanometer is at full scale.
Thus if i=23025A=30unitsi = \dfrac{2}{{3025}}A = 30 units then
1unit1unit is 23025×30A\dfrac{2}{{3025 \times 30}}A.
Similarly, deflection 20units20units is equal to 2×203025×30A\dfrac{{2 \times 20}}{{3025 \times 30}}Acurrent flow through the circuit which is the new current II .
Thus keeping the numerator same, the denominator turns out to be
23025×1.5A=2V4537.5Ω\dfrac{2}{{3025 \times 1.5}}A = \dfrac{{2V}}{{4537.5\Omega }}
; i.e. the denominator turns out to be (4512.5+25)Ω(4512.5 + 25)\Omega .
We now get the required net resistance of the new circuit to be 4537.5Ω4537.5\Omega , 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)=2×203025×30(25Ω+R)2V = I(r + R) = \dfrac{{2 \times 20}}{{3025 \times 30}}(25\Omega + R).
On further simplifying we get,
2×3025×302×20=25+R\Rightarrow 2 \times \dfrac{{3025 \times 30}}{{2 \times 20}} = 25 + R
R+25Ω=(4512.5+25)Ω\therefore R + 25\Omega = (4512.5 + 25)\Omega
Thus we get the required value of the new resistance RR as 4512.5Ω4512.5\Omega .

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 RR changes as we wish to decrease the value of current passing through the galvanometer.