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Question: A galvanometer has a resistance \(G\) and a current \(i_{g}\) flowing in it produces full scale defl...

A galvanometer has a resistance GG and a current igi_{g} flowing in it produces full scale deflection. S1S_{1} is the value of shunt, which converts it into an ammeter of range 0I0-I and S2S_{2} is the value of shunt for the range 02I0-2I the ratio of S1S2\dfrac{S_{1}}{S_{2}} is

& A.\dfrac{{{S}_{1}}}{{{S}_{2}}}=\left[ \dfrac{2I-{{i}_{g}}}{I-{{i}_{g}}} \right] \\\ & B.\dfrac{{{S}_{1}}}{{{S}_{2}}}=\dfrac{1}{2}\left[ \dfrac{I-{{i}_{g}}}{2I-{{i}_{g}}} \right] \\\ & C.2 \\\ & D.1 \\\ \end{aligned}$$
Explanation

Solution

We know that a galvanometer is an instrument which can detect the electric current in a circuit. We can convert a moving coil galvanometer into a voltmeter or an ammeter by adding a resistance to the circuit.

Formula: S=G(ig)(iig)S=\dfrac{G(i_{g})}{(i-i_{g})}

Complete answer:
A galvanometer works on the principle of electromagnetic induction, which is when a current carrying conductor is placed in a magnetic field, it experiences a torque.
A galvanometer when connected in parallel to a circuit with low resistance, it can act as an ammeter and measure the current in that circuit. This low resistance is also called the shunt resistance.
Let us assume that a shunt SS is connected in parallel with a galvanometer with resistanceGG, then we know that the current in the circuit gets divided. If ii is the total current in the circuit and igi_{g} is the current in the galvanometer, then the current flowing through the shunt resistance is given as is=iigi_{s}=i-i_{g}
Since the voltage in both the circuits are equal, we also know from ohms law that V=IRV=IR.
Applying the same, we get S(iig)=G(ig)S(i-i_{g})=G(i_{g})
Or, S=G(ig)(iig)S=\dfrac{G(i_{g})}{(i-i_{g})}

Here it is given that the maximum current in the ammeter with shunt S1S_{1} as 0I0-I i.e. i=Ii=I
Then substituting the values we get, S1=G(ig)(Iig)S_{1}=\dfrac{G(i_{g})}{(I-i_{g})}
Also given that, the maximum current in the ammeter with shunt S2S_{2} is02I0-2Ii.e. i=2Ii=2I
Then substituting the values we get, S2=G(ig)(2Iig)S_{2}=\dfrac{G(i_{g})}{(2I-i_{g})}
But we need the ratioS1S2\dfrac{S_{1}}{S_{2}}
Then taking the ratio between S1S2\dfrac{S_{1}}{S_{2}} we get, S1S2=G(ig)(Iig)G(ig)(2Iig)=(2Iig)(Iig)\dfrac{S_{1}}{S_{2}}=\dfrac{\dfrac{G(i_{g})}{(I-i_{g})}} {\dfrac{G(i_{g})}{(2I-i_{g})}}=\dfrac{(2I-i_{g})}{(I-i_{g})}

Hence the answer is A.S1S2=[2IigIig]A.\dfrac{{{S}_{1}}}{{{S}_{2}}}=\left[ \dfrac{2I-{{i}_{g}}}{I-{{i}_{g}}} \right]

Note:
We know that the sensitivity of a galvanometer is its ability to give large deflections even for a small value of the current. And it is given as the ratio between the change deflections in the galvanometer to the change in current in the coil.