galvanometer
A galvanometer is a type of sensitive ammeter: an instrument for detecting electric current. It is an analog electromechanical actuator that produces a rotary deflection of some type of pointer in response to electric current through its coil in a magnetic field
A galvanometer is a type of sensitive ammeter: an instrument for detecting electric current. It is an analog electromechanical actuator that produces a rotary deflection of some type of pointer in response to electric current through its coil in a magnetic field
D'Arsonval/Weston galvanometer movement - with the moving coil
shown in orange
Now our interest is to
convert a galvanometer to voltmeter to measure the potential difference
across any component in a circuit. This can be done by adding a suitable
high resistance in series with galvanometer. When high resistance is
connect in series with the galvanometer, very negligible current flow
through it.
The
figure show a galvanometer G connected in series with high resistor R
across a component in the circuit. We are interested to know the
potential difference Δ V across the component. If I is the maximum current through the galvanometer then according ohms law
Δ V = (R +G) I.
Resistance that is to be connected in series is
R =ΔVI - G
≃ 100kΩ . We can build any range of
voltmeter by suitable high resistance in series to the galvanometer.
Here R is the resistance that is connected in series with galvanometer resistance G. From the above equation
(R +G) = ΔVI
Resistance that is to be connected in series is
R =
Now we will decide what would be the value of the resistance
that is connected in series with the galvanometer. Let’s say we need a
voltmeter of to measure voltage between 0 -10V, and we have galvanometer
specifying that its resistance is 20ohms and maximum permissible
current is 0.1mA.
R = 10V0.1×10−3 - 20 Ω
= 99980Ω
≃ 100k ω .
The high resistance needed is = 99980
CONVERSION
OF GALVANOMETER
INTO AMMETER |
|
| Since Galvanometer is a very sensitive instrument therefore it can’t measure heavy currents. In order to convert a Galvanometer into an Ammeter, a very low resistance known as "shunt" resistance is connected in parallel to Galvanometer. Value of shunt is so adjusted that most of the current passes through the shunt. In this way a Galvanometer is converted into Ammeter and can measure heavy currents without fully deflected. | |
|
VALUE
OF SHUNT RESISTANCE
|
|
| Let resistance of galvanometer = Rg and it gives full-scale deflection when current Ig is passed through it. Then, | |
|
Vg
= IgRg -------(i)
|
|
| Let a shunt of resistance (Rs) is connected in parallel to galvanometer. If total current through the circuit is I. | |
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|
| Then current through shunt: | |
|
Is
= (I-Ig)
|
|
| potential difference across the shunt: | |
|
Vs=
IsRs
|
|
|
or
Vs = (I – Ig)Rs -------(ii) |
|
| But | |
|
Vs
=Vg
(I - Ig)Rs = IgRg ![]() | |


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