Electrodynamometer Type Wattmeter

Electrodynamometer Wattmeter Definition

An electrodynamometer type wattmeter measures electrical power by using the interaction between magnetic fields and electric currents.

Working Principle

Now let us look at constructional details of electrodynamometer. It consists of following parts.There are two types of coils present in the electrodynamometer. They are :

Moving Coil

The moving coil moves the pointer with the help of a spring control instrument. To prevent overheating, a limited current flows through the moving coil by connecting a high-value resistor in series. The air-cored moving coil is mounted on a pivoted spindle and can move freely. In an electrodynamometer type wattmeter, the moving coil acts as a pressure coil and is connected across the voltage, so the current through it is proportional to the voltage.

Fixed Coil

The fixed coil is divided into two equal parts and these are connected in series with the load, therefore the load current will flow through these coils. Now the reason is very obvious of using two fixed coils instead of one, so that it can be constructed to carry considerable amount of electric current.

These coils are called the current coils of electrodynamometer type wattmeter. Earlier these fixed coils are designed to carry the current of about 100 amperes but now the modern wattmeter are designed to carry current of about 20 amperes in order to save power.

Control System

Out of two controlling systems i.e.

Gravity control

Spring control, only spring controlled systems are used in these types of wattmeter. Gravity controlled system cannot be employed because there will be appreciable amount of errors.

Damping System

Air friction damping is used because eddy current damping can distort the weak operating magnetic field, leading to errors.

There is uniform scale which is used in these types of instrument as moving coil moves linearly over a range of 40 degrees to 50 degrees on either side.

Now let us derive the expressions for the controlling torque and deflecting torques. In order to derive these expressions let us consider the circuit diagram given below:

We know that instantaneous torque in electrodynamic type instruments is directly proportional to the product of instantaneous values of currents flowing through both the coils and the rate of change of flux linked with the circuit.

Let I1 and I2 be the instantaneous values of currents in pressure and current coils respectively. So the expression for the torque can be written as:

Where, x is the angle.

Now let the applied value of voltage across the pressure coil be

Since the electrical resistance of the pressure coil is very high, we can neglect its reactance compared to its resistance. Thus, the impedance is equal to its electrical resistance, making it purely resistive.

The expression for instantaneous current can be written as I2 = v / Rp where Rp is the resistance of pressure coil.

If there is phase difference between voltage and electric current, then expression for instantaneous current through current coil can be written as

As current through the pressure coil is very very small compared to the current through current coil hence current through the current coil can be considered as equal to total load current.Hence the instantaneous value of torque can be written as

Average value of deflecting torque can be obtained by integrating the instantaneous torque from limit 0 to T, where T is the time period of the cycle.