A galvanometer of resistance G has voltage range Vg. Resistance required to convert it to read voltage up to V is
(V-\(\frac {V_g}{V}\))G
G(\(\frac {V}{V_g}\)-1)
G*\(\frac {V_g}{V}\)
(V+\(\frac {V_g}{V}\))G
The total resistance in the circuit is given by the sum of the galvanometer resistance and the series resistor: G + R.
Using Ohm's Law, the current passing through the galvanometer can be calculated as I =\(\frac { V}{G + R}\)
Since we want to limit the current to be within the galvanometer's range, we have: I ≤ \(\frac { V_g}{G}\).
Substituting the expression for I and rearranging the inequality, we get:
\(\frac { V}{G + R}\) ≤ \(\frac { V_g}{G}\)
Multiplying both sides by G and rearranging, we have:
V ≤ \((\frac { V_g}{G})\) * (G + R)
V ≤ Vg + \((\frac { V_g}{G})\) * R
Now, subtracting Vg from both sides, we get:
V - Vg ≤ \((\frac { V_g}{G})\) * R
Dividing both sides by \((\frac { V_g}{G})\), we have:
\(\frac { (V - Vg)}{(Vg / G)}\) ≤ R
R ≥ (V - Vg) * \(\frac {G}{V_g}\)
R ≥\(\frac { VG - V_gG}{V_g }\)
R ≥ \(\frac {V*G}{V_g}\) - G
R ≥ G*(\(\frac { V}{V_g}\)- 1)
Therefore, the correct option is (B) G(\(\frac { V}{V_g}\) - 1), which represents the resistance required to convert the galvanometer to read voltage up to V.

Which part of root absorb mineral?
There are two laws, given by Faraday which explain the phenomena of electromagnetic induction:
Whenever a conductor is placed in a varying magnetic field, an emf is induced. If the conductor circuit is closed, a current is induced, known as the induced current.
The Emf induced inside a coil is equal to the rate of change of associated magnetic flux.
This law can be mathematically written as:
∈\(-N {\triangle \phi \over \triangle t}\)
