MEASURING INSTRUMENTS - AMMETER AND VOLTMETER

Measuring instruments are an important part of electrical engineering and they are essential for analyzing the electrical circuits. Some of the important instruments which are used occasionally are ammeter, voltmeter, wattmeter, energy meter etc. But in this article we are about to discuss the two most fundamental of all - Ammeter and Voltmeter. Ammeters and voltmeters are generally classed together because of the similarities in their operating principles, with some exceptions of course!

WHAT IS AN AMMETER?

An ammeter is an electrical measurement instrument which is used to measure current through a point or wire in a circuit. It is connected in series with the circuit whose current is to be measured. Therefore, they should have a low electrical resistance. This is essential in order that they cause a small voltage drop and consequently absorb small power.
Ammeter can also be made from a galvanometer by placing a shunt resistance in parallel with the galvanometer.

WHAT IS A VOLTMETER?

A voltmeter is an electrical measurement instrument which is used to measure voltage across two given points in a circuit. It is connected in parallel with the circuit or the part of the circuit whose voltage is to be measured. They should have high electrical resistance so that the current drawn by them is small and ultimately the power absorbed is small.
voltmeter can also be made from a galvanometer by placing a high resistance in series with the galvanometer.
Ammeters and voltmeters can be of different types based on their construction and working.

TYPES OF AMMETERS AND VOLTMETERS –

  1. Moving iron type (both for AC/DC)
      (a)  Attraction type
      (b) Repulsion type
  2. Moving coil type
      (a)  Permanent magnet type (for DC only)
      (b) Electrodynamic or dynamometer type (for DC/AC)
  3. Hot wire type (both for DC/AC)
  4. Induction type (for AC only)
      (a)  Split phase type
      (b) Shaded pole type
  5. Electrostatic type (for voltmeters only) – Both DC/AC

MOVING IRON TYPE –

In moving iron type, there are two basic types, which are:
(a)  Attraction type
(b) Repulsion type
For both type of these instruments, the necessary magnetic field is produced by the ampere turns of a current carrying coil. As we are talking about ammeter; the coil has comparatively fewer turns of thick wire so that the ammeter has low resistance because it is to be connected in series with the circuit.

ATTRACTION TYPE INSTRUMENT –

The figure below shows the constructional details of an attraction type moving iron instrument.
ATTRACTION TYPE MOVING IRON INSTRUMENT
The coil is flat disc or a sector eccentrically mounted. When the current flows through the coil, a magnetic field is set up and the moving iron moves from a region of weaker field to region of stronger magnetic field, thereby deflecting the pointer over a calibrated scale.
The controlling torque is provided by springs but can also be gravity controlled. Damping is provided by air friction usually by a vane moving in a sector shaped chamber.

REPULSION TYPE INSTRUMENT –
REPULSION TYPE MOVING IRON ONSTRUMENT

In repulsion type, there are two iron vanes inside the coil; one fixed and other movable. When the current flows through the coil, these vanes get similarly magnetized and there is force of repulsion between the two vanes resulting in the movement of moving vane, and therefore the pointer.

Why moving iron can be used in both AC and DC?

The function of moving iron instruments depends on the attraction or repulsion of iron vanes. Thus, they are unpolarised i.e. they are independent of the direction in which the current flows. Therefore, they can be used both in AC as well as DC.

DEFLECTION PRODUCED –

The deflection in a moving iron instrument is given by
                        \[\theta =\frac{1}{2}\frac{{{I}^{2}}}{K}\frac{dl}{d\theta }\]
Thus, $\theta \propto {{I}^{2}}$
As, the deflection is proportional to the square of the current, it is evident that the scale of such an instrument is non-uniform.
If there is no saturation, the change of inductance with the angle of deflection is uniform i.e. $\frac{dl}{d\theta }$ is constant. Thus, the scale can be easily laid as the measured quantity is proportional to the square root of deflection.

SOURCES OF ERROR –                                                                      

     (a)  Errors with both AC and DC work –

          (i)  Errors due to hysteresis -  
             Because of hysteresis in the iron parts of the moving system, readings are higher            for descending values and lower for ascending values. This can be completely              eliminated by using Mu metal or Perm-alloy, which has negligible hysteresis loss. 
         (ii)  Errors due to stray fields –
               Unless shielding is not done from external fields, the results obtained may be                  wrong. Thus, the instrument is shielded with cast iron.                              

     (b) Errors with AC work –

     Changes of frequency produce change in the impedance of the coil and change in          the magnitude of AC currents.

ADVANTAGES - 

  • Cheap and robust.
  • Can be used both in AC and DC.

DISADVANTAGE –

  • They cannot be calibrated with DC because of the effect of hysteresis in the iron      vanes. Hence, they are usually calibrated by comparison with AC standard.
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