Now!
We study in detail about these two instruments and we will also see the difference between galvanometer and ammeter.
See also: Potential Difference Vs Electromotive Force
It is an electrical device that is used to detect the passage of current through a circuit.
Construction:
This device consists of the following parts:
See also: Factors affecting resistance
When the current is passed through the coil, a couple of two equal and opposite forces acting on two different points act on the coil and the coil tends to rotate. Such a couple is known as deflecting couple.
If N is the number of turns of the coil and A is the area then the torque due to the deflecting couple is given by:
τ = NIBA cosα
Since the pole pieces of the magnet are made concave to make the field radial, therefore the plane of the coil is always parallel to the field, so α =0º
τ = NIBA cos0º
τ = NIBA(1)
τ = NIBA …………………….(1)
Restoring torque
As the coil turns under the action of deflecting torque, the suspension wire is twisted which gives rise to the torsional couple which tends to untwist the suspension wire and restores the original position. This couple is known as a restoring couple.
The torque due to restoring the couple is proportional to the angle of deflection θ as long as the suspension wire obeys Hook’s law. Thus
Restoring torque ∝ θ
Restoring torque = Cθ —————(2)
Where C is the constant, known as twisting or torsional constant and it depends upon the nature of suspension wire.
When the deflecting couple balances the restoring couple then the coil will come to rest. So, in equilibrium.
Deflecting torque =Restoring torque
NIBA = Cθ
oR
I = Cθ/NBA
Since C/NBA =constant then:
I ∝ θ
So the current passing through the coil is directly proportional to deflection θ.
There are two methods to determine the angle of deflection of the coil.
In a sensitive galvanometer, the angle of deflection is observed by means of the small mirror attached to the coil along with the lamp.
A beam of light from the lamp falls on the mirror of the galvanometer. After reflection from the mirror, it produces a spot on a transparent scale placed at a distance of one-meter form the galvanometer. When the coil rotates, the mirror attached to the coil also rotates and the spot of light moves along the scale.
The displacement of the spot of light on the scale is proportional to the angle of deflection, provided the angle of deflection is small.
In this method, the coil is pivoted between two jeweled bearings. The restoring torque is provided by two hairsprings which also act as current leads. An aluminum pointer is attached to the coil which moves over a scale.
The angular twist per unit is called the current sensitivity of a galvanometer. It is expressed as:
Sensitivity = θ/I = BAN/C
We can make it sensitive by the following steps:
A type of galvanometer, in which the coil comes to rest quickly after passing of current through it, is called a stable or deadbeat galvanometer.
A sensitive coil is not stable; its coil oscillates many times before coming to rest, although the current through the coil is stopped. But in some galvanometers, the coil comes to rest very soon, as the current stops the flow through it.
When current passes through the coil is starts rotating about the central axis. The flux through the frame of coil changes so (by Faraday’s law) an emf and hence an (eddy) current is induced in the frame which opposes it cause (i.e. the rotation of coil).In this way, the oscillations are damped.
Ammeter
An electrical instrument that is used to measure the current passing through its circuit is called an ammeter.
Principle and Construction
Its principle and construction are similar to the moving coil galvanometer.
To current a galvanometer into an ammeter, a very small resistance is connected in the parallel with the galvanometer. This resistance is called shunt resistance (Rs).
Watch the video about the conversion!
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Thank you.
Some ideas of post galvanometer and ammeter were not given.