Skip to main content

Mega Ohm Bridge

Methods for Measurement of High Resistance:

The different methods employed are :
1. Direct deflection method.
2. Loss of charge method:
3. Megohm bridge.
4. Meggar

Megohm bridge

Figure (a) shows very high resistance R with its two main terminals A and B, and a guard terminal, which is put on the insulation. This high resistance may be diagrammatically represented as in Figure(b). The resistance R is between main terminals A and B and the leakage resistances RAr. and Rnr between the A and B of the main terminal from a "Three terminal resistance".
Let us consider the hypothetical case of a 100 M Ohm resistance. We assume that each of the leakage
resistances is 100 M Ohm 
i.e., RAG = RBG = 100 M Ohm. Let this resistance be measured by an ordinary
Wheatstone bridge as shown in Figure (a) below It is clear that the Wheatstone bridge will measure the resistance of (100 x 200) / (100 +200)= 67M Ohm instead of 100 M Ohm thus giving an error of 33 per cent.




However, if the same resistance is measured by a modified Wheatstone bridge as shown in Figure (b) above with the guard connection G connected as indicated, the error in measurement is considerably reduced. For the arrangement shown in Figure(b) resistance RBG is put in parallel with the galvanometer and thus it has no effect on the balance and only effects the sensitivity of the galvanometer slightly. The resistance Rag =100M Ohm is put in parallel with a resistance P = 100 k Ohm and therefore for the arrangement shown 
the measured value has an error of only 0.01 percent and this error is entirely negligible for measurements of this type.

The arrangement of the Figure illustrates the operation of a Megohm bridge. The above Figure shows the circuit of a completely self-contained Megohm bridge which includes power supplies, bridge members, amplifiers, and indicating, instruments. It has a range from 0.1 M Ohm to 106 M Ohm. The accuracy is within 3% for the lower part of the range to possibly 10% above 10,000 M Ohm.

Sensitivity for balancing against high resistance is obtained by the use of adjustable high voltage supplies of 500 V or 1000 V and the use of a sensitive null indicating arrangements such as a high gain amplifier with an electronic voltmeter or a C.R.O. The dial on Ohm is calibrated 1 - 10 - 100 - 1000 M Ohm, with main decade 1 - 10 occupying the greater part of the dial space. Since unknown resistance R = PS/ Q the arm Q is made, tapered, so that the dial calibration is approximately logarithmic in the main decade, 1 — 10. Arm S gives five multipliers, 0.1, 1, 10, 100 and 1000. The junction of ratio arms P and Q is brought on the main panel and is designated as the 'Guard' terminal.




Comments

Popular posts from this blog

Concepts and types of Digital voltmeter

Digital Voltmeter (DVM) Definition : Digital Voltmeter is a  voltage-sensitive device . It  measures AC  or  DC voltage  and  displays  the value directly in  numeric form  instead of pointer deflection.  DVM  is an acronym for  Digital Voltmeter . DVM was first invented in  1954  by  Andrew Kay . There exist many factors that affect the measurement accuracy of a digital voltmeter(DVM). These are basically temperature, input impedance, variation in power supply voltage etc. As we know that an  analogue instrument  provides results by  pointer deflection  on a continuous scale. On contrary, a  digital instrument  provides results as  discrete numerals . Thus providing accuracy and versatility together. The input range of DVM may vary from  ±1 V  to  1000 V . Precision DVM offers  input resistance  of  1 GΩ  or high for a voltage range of less th...

DSO & MSO (Block Diagram)

DIGITAL STORAGE OSCILLOSCOPE (DSO) The digital storage oscilloscope eliminates the disadvantages of the analog storage oscilloscope. It replaces the unreliable storage method used in analog storage scopes with digital storage with the help of memory. The memory can store data as long as required without degradation. It also allows the complex processing of the signal by the high-speed digital signal processing circuits.  In this digital storage oscilloscope, the waveform to be stored is digitised and then stored in digital memory. The conventional cathode ray tube is used in this oscilloscope hence the cost is less. The power to be applied to memory is small and can be supplied by small battery. Due to this the stored image can be displayed indefinitely as long as power is supplied to memory. Once the waveform is digitised then it can be further loaded into the computer and can be analysed in detail. Block Diagram As done in all the oscilloscopes, the input signal is applied to the...

Maxwell’s inductance bridge

 Maxwell's Bridge Maxwell's bridge can be used to measure inductance by comparison either with variable standard self-inductance or with a standard variable capacitance. These measurements can be done by using Maxwell's Bridge in two different forms. Maxwell's Inductance Bridge Using this bridge, We can measure inductance by comparing it with a Standard variable self-inductance arranged in a bridge circuit as shown in Fig.  (a). Consider Maxwell's inductance bridge as shown in Fig  (a). Two branches consist of non-inductive resistances R1 and R2. One of the arms consists of Variable inductance with series resistance r. The remaining arm consists of unknown inductance Lx. Maxwell's Inductance Capacitance Bridge Using this bridge, we can measure inductance by comparing it with a variable standard capacitor. The bridge circuit diagram is shown in Fig. One of the ratio arms consists of resistance and capacitance in parallel. Hence it is simple to write the bridge eq...