Electrical Properties of Engineering Materials
The Electrical properties of a material are those which determine ability of material to be suitable for a particular Electrical Engineering Application. Some of the typical Electrical properties of engineering materials are listed below-
- Resistivity
- Conductivity
- Temperature coefficient of Resistance
- Permittivity
- Thermoelectricity
Resistivity
It the property of material which resists the flow of electric current through material. It is the reciprocal of conductivity.
It is dented by ‘ρ’. Resistivity of a material of a conductor can be determined as below
ρ = RA/l
Where, ‘R’ is the resistance of conductor in Ω.
‘A’ is the cross sectional area of conductor in m2
‘l’ is the length of the conductor in meter SI unit of resistivity of is Ω¦-meter. Resistivity of some materials is listed below
| Sl. No. | Element | Resistivity at 20oC in Ω – m |
| 1 | Silver | 1.59 × 10-8 |
| 2 | Copper | 1.7 × 10-8 |
| 3 | Gold | 2.44 × 10-8 |
| 4 | Aluminum | 2.82 × 10-8 |
| 5 | Tungsten | 5.6 × 10-8 |
| 6 | Iron | 1.0 × 10-7 |
| 7 | Platinum | 1.1 × 10-7 |
| 8 | Lead | 2.2 × 10-7 |
| 9 | Manganin | 4.82 × 10-7 |
| 10 | Constantan | 4.9 × 10-7 |
| 11 | Mercury | 9.8 × 10-7 |
| 12 | Carbon (Graphite) | 3.5 × 10-5 |
| 13 | Germanium | 4.6 × 10-1 |
| 14 | Silicon | 6.4 × 102 |
| 15 | Glass | 1010 to 1014 |
| 16 | Quartz (fused) | 7.5 × 1017 |
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Dielectric Strength
It is the property of material which indicates the ability of material to withstand at high voltages. Generally it is specified for insulating material to represent their operating voltage. A material having high Dielectric strength can withstand at high voltages. Generally, it is represented in the unit of KV/cm. Dielectric strength of some insulating materials are listed below-
| Sl. No. | Material | Dielectric Strength [KV(max.)/cm] |
| 1 | Air | 30 |
| 2 | Porcelain | 80 |
| 3 | Paraffin Wax | 120 |
| 4 | Transformer oil | 160 |
| 5 | Bakelite | 220 |
| 6 | Rubber | 280 |
| 7 | Paper | 500 |
| 8 | Teflon | 600 |
| 9 | Glass | 1200 |
| 10 | Mica | 2000 |
Conductivity
Thermoelectricity
If the junction, formed by joining to two metals, is heated, a small voltage in the range of millivolt is produced. This effect is called thermoelectricity or thermoelectric effect. This effect forms the basis of operation of thermocouples and some temperature based transducers. This effect can be used to generate electricity, to measure the temperature and to measure the change is temperature of objects.
Temperature Coefficient of Resistance
The temperature coefficient of resistance of a material indicates the change in resistance of material with change in temperature. Resistance of conductor changes with change of temperature.
The rise in resistance of a material with rise in temperature depends on following things,
- R2 – R1 ∝ R1
- R2 – R1 ∝ t2 – t1
- Property of material of conductor.
Where, R1 is the resistance of conductor at temperature of t1oC and R2 is the resistance of conductor at temperature of t2oC.
Hence, from above, R2 – R1 ∝ R1 (t2 – t1)
Or, R2 – R1 = α1 R1 (t2 – t1) ⇒ R2 = R1 [1 + α1 (t2 – t1)]
Where, α1 is temperature coefficient of resistance of material at temperature of t1oC. Its unit is /oC. Temperature coefficient of resistance of material is also depends on temperature. temperature coefficient of some materials are listed below,
| Sl. No. | Element | Temperature Coefficient of Resistance in /oC |
| 1 | Manganin | 0.00002 |
| 2 | Constantan | 0.00017 |
| 3 | Nichrome | 0.0004 |
| 4 | Mercury | 0.0009 |
| 5 | Silver | 0.0038 |
| 6 | Copper | 0.00386 |
| 7 | Annealed copper | 0.000393 |
| 8 | Platinum | 0.003927 |
| 9 | Aluminum | 0.00429 |
| 10 | Carbon (Graphite) | – 0.0005 |
| 11 | Germanium | – 0.05 |
| 12 | Silicon | – 0.07 |
Read article – Mechanical Properties of Engineering Materials
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