Insulation Resistance Theory - doc00030
Insulation resistance is a very complex parameter, but it is very
important to study it in the field of electrical & electronic
engineering. The I.R. value, of a specimen changes with time on
continuous application of D.C.voltage, the IR value changes with change
in magnitude of the applied DC voltage and IR value also varies with
Temperature, Humidity and contamination. When measurement is made, the
IR value slightly increases after each measurement cycle. This is due
to residual polarization of the previous application of voltage due to
all the above factors, IR measurement becomes both difficult and
complicated. The DRT101 overcomes most of the conventional problems
and makes Insulation resistance analysis more scientific &
practical.
The problem of residual polarization can be overcome by :
- The terminals of the insulation shorted for a
few minutes.
- The terminals are reversed after each
measurement.
The DRT101 shorts the specimen terminals automatically when it does
not apply voltage. But most accurate results are obtained only on the
1st measurement on a specimen or by giving a gap of 30 mts for
depolarization between each measurement.
When a steady DC voltage is applied to an insulation, the observed
behavior is a analogous to that of changing a leaky capacitance through
a series high resistance. The resultant current comprises of these
components.
- A charging current due to the natural capacitance.
This
is large in the beginning and becomes negligible in a few seconds.
- The absorption current flows in the body of the
dielectric and
decays with time. The time may run to many minutes, this absorption
current gives rise to polarization residue effect.
- The actual conduction current through the insulation.
This is
constant with time. But can vary with voltage & temperature.
- The surface leakage current depends much on Humidity
contamination.
Insulation may fail due to the following reasons:
- Mechanical vibrations may rupture insulation.
- Temperature decreases thermal strength.
- Dust & moisture cause contamination & decay.
- Corrosive material & electrochemical reactions.
Mode of insulation failure :
- Intrinsic breakdown.
- Thermal effects.
- Ionization.
Methods of measuring high resistance and IR :
- High voltage bridge.
- Leakage current measurement method.
- Loss of charge method.


High Resistance Materials Tables
Liquids
| 20 C
|
OHM
|
-M
|
| |
min
|
max
|
| Benzene |
1011
|
1012
|
| Transformer
oil |
1010
|
1013
|
| Gasoline |
1010
|
1013
|
| Castor oil |
108
|
1010
|
| Acetone |
104
|
105
|
| Ethanol |
104
|
105
|
| Distilled
water |
103
|
104
|
Glass At High Temperature
| 200 C |
OHM
-M |
| Sodium Pyrex |
2 * 106
|
| Potassium Pyrex |
8 * 109
|
| Lead glass |
2 * 1011 |
Effect Of Contamination On Surface Resistivity
| 70%
RH |
CONTAMINATED |
CLEAN |
| Window
glass |
2
* 108 |
1012
|
| Fused
quartz |
2
* 108 |
1013
|
Relation Of Resistivity With RH % And Temp
| MATERIAL |
70%
RH 20
deg C |
0%
RH 100
deg C |
0%
RH 20
deg C |
| Marble |
106 - 108
|
1010 - 1012
|
1012
- 1014 |
| Wood |
106 - 107
|
1010 - 1012
|
1011 - 1013
|
| Vulcanized
fibers fibers |
106 - 109
|
108 - 109
|
1011 - 1012
|
| MATERIALS |
SOLIDS
OHM -M |
Solids
| MATERIALS |
OHM -M |
| Polyethylene |
1017 |
| Poly propylene |
1017 |
| PVC |
1018 |
| Polyurethane |
1015 |
| Asbestos fiber +
phenol |
108 |
| Mica + phenol |
1012 |
| Glass-fiber +
polyester |
1012 |
| Glass-fiber +
epoxy |
1014 |
Pages 1, 2, 3, 41, 42, 43 of DRT101 Insulation Tester
and Tera Ohm Meter
Operating Manual, A product that i used to make-n-sell. - Ananth
|
|