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.
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:
∈\(-N {\triangle \phi \over \triangle t}\)