Conductors

Conductors

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Electrical conductor

Overhead conductors carry electric power from generating stations to customers.

In physics and electrical engineering, aconductor is an object or type of material that allows the flow of an electrical current in one or more directions. Materials made of metal are common electrical conductors. Electrical current is generated by the flow of negatively charged electrons, positively charged holes, and positive or negative ions in some cases.

In order for current to flow, it is not necessary for one charged particle to travel from the machine producing the current to that consuming it. Instead, the charged particle simply needs to nudge its neighbor a finite amount who will nudge its neighbor and on and on until a particle is nudged into the consumer, thus powering the machine. Essentially what is occurring here is a long chain of momentum transfer between mobile charge carriers; the Drude model of conduction describes this process more rigorously. This momentum transfer model makes metal an ideal choice for a conductor as metals, characteristically, possess a delocalized sea of electrons which gives the electrons enough mobility to collide and thus effect a momentum transfer.

As discussed above, electrons are the primary mover in metals; however, other devices such as the cationic electrolyte(s) of a battery, or the mobile protons of the proton conductor of a fuel cell rely on positive charge carriers.Insulators are non-conducting materials with few mobile charges that support only insignificant electric currents.

Resistance and conductanceEdit

A piece of resistive material with electrical contacts on both ends.

Main article: Electrical resistance and conductance

The resistance of a given conductor depends on the material it is made of, and on its dimensions. For a given material, the resistance is inversely proportional to the cross-sectional area. For example, a thick copper wire has lower resistance than an otherwise-identical thin copper wire. Also, for a given material, the resistance is proportional to the length; for example, a long copper wire has higher resistance than an otherwise-identical short copper wire. The resistance Rand conductance G of a conductor of uniform cross section, therefore, can be computed as

${\displaystyle {\begin{aligned}R&=\rho {\frac {\ell }{A}},\\[6pt]G&=\sigma {\frac {A}{\ell }}.\end{aligned}}}$

where ${\displaystyle \ell }$ is the length of the conductor, measured in metres [m], A is the cross-section area of the conductor measured in square metres [m²], σ (sigma) is the electrical conductivity measured in siemens per meter (S·m⁻¹), and ρ (rho) is the electrical resistivity(also called specific electrical resistance) of the material, measured in ohm-metres (Ω·m). The resistivity and conductivity are proportionality constants, and therefore depend only on the material the wire is made of, not the geometry of the wire. Resistivity and conductivity are reciprocals: ${\displaystyle \rho =1/\sigma }$. Resistivity is a measure of the material's ability to oppose electric current.

This formula is not exact: It assumes thecurrent density is totally uniform in the conductor, which is not always true in practical situations. However, this formula still provides a good approximation for long thin conductors such as wires.

Another situation this formula is not exact for is with alternating current (AC), because theskin effect inhibits current flow near the center of the conductor. Then, the geometricalcross-section is different from the effectivecross-section in which current actually flows, so the resistance is higher than expected. Similarly, if two conductors are near each other carrying AC current, their resistances increase due to the proximity effect. Atcommercial power frequency, these effects are significant for large conductors carrying large currents, such as busbars in anelectrical substation,^[1] or large power cables carrying more than a few hundred amperes.

Aside from the geometry of the wire, temperature also has a significant effect on the efficacy of conductors. Temperature affects conductors in two main ways, the first is that materials may expand under the application of heat. The amount that the material will expand is governed by thethermal expansion coefficient specific to the material. Such an expansion (or contraction) will change the geometry of the conductor and therefore its characteristic resistance. However, this effect is generally small, on the order of 10⁻⁶. An increase in temperature will also increase the number of phonons generated within the material. A phonon is essentially a lattice vibration, or rather a small, harmonic kinetic movement of the atoms of the material. Much like the shaking of a pinball machine, phonons serve to disrupt the path of electrons, causing them to scatter. This electron scattering will decrease the number of electron collisions and therefore will decrease the total amount of current transferred.

Conductor materialsEdit

Main article: Electrical resistivity and conductivity § Resistivity of various materials

Further information: Copper wire and cable andAluminum wire

Material	ρ [Ω·m] at 20°C	σ [S/m] at 20°C
Silver, Ag	1.59 × 10−8	6.30 × 107
Copper, Cu	1.68 × 10−8	5.96 × 107
Aluminum, Al	2.82 × 10−8	3.50 × 107

Conduction materials include metals,electrolytes, superconductors,semiconductors, plasmas and some nonmetallic conductors such as graphite andConductive polymers.

Copper has a high conductivity. Annealedcopper is the international standard to which all other electrical conductors are compared. The main grade of copper used for electrical applications, such as building wire, motorwindings, cables and busbars, is electrolytic-tough pitch (ETP) copper (CW004A or ASTMdesignation C100140). This copper has an electrical conductivity of at least 100% IACS (International Annealed Copper Standard). If high conductivity copper must be welded orbrazed or used in a reducing atmosphere, then oxygen-free high conductivity copper(CW008A or ASTM designation C10100) may be used.^[2] Because of its ease of connection by soldering or clamping, copper is still the most common choice for most light-gauge wires.

Silver is more 'conductive' than copper, but due to cost it is not practical in most cases. However, it is used in specialized equipment, such as satellites, and as a thin plating to mitigate skin effect losses at high frequencies.

Aluminum wire, which has 61% of the conductivity of copper, has been used in building wiring for its lower cost. By weight, aluminum has higher conductivity than copper, but it has properties that cause problems when used for building wiring. It can form a resistive oxide within connections that makes wiring terminals heat. Aluminum can "creep", slowly deforming under load, eventually causing device connections to loosen, and also has a different coefficient of thermal expansion compared to materials used for connections. This accelerates the loosening of connections. These effects can be minimized by using wiring devices approved for use with aluminum.

Aluminum wires used for low voltage distribution, such as buried cables and service drops, require use of compatible connectors and installation methods to prevent heating at joints. Aluminum is also the most common metal used in high-voltage transmission lines, in combination with steel as structural reinforcement. Anodized aluminum surfaces are not conductive. This affects the design of electrical enclosures that require the enclosure to be electrically connected.

Organic compounds such as octane, which has 8 carbon atoms and 18 hydrogen atoms, cannot conduct electricity. Oils are hydrocarbons, since carbon has the property of tetracovalency and forms covalent bonds with other elements such as hydrogen, since it does not lose or gain electrons, thus does not form ions. Covalent bonds are simply the sharing of electrons. Hence, there is no separation of ions when electricity is passed through it. So the liquid (oil or any organic compound) cannot conduct electricity.

While pure water is not an electrical conductor, even a small portion of impurities, such as salt, can rapidly transform it into a conductor.

Wire sizeEdit

Wires are measured by their cross sectional area. In many countries, the size is expressed in square millimetres. In North America, conductors are measured by American wire gauge for smaller ones, and circular mils for larger ones. The size of a wire contributes to its ampacity. The American wire gauge article contains a table showing allowable ampacities for a variety of copper wire sizes.

Conductor ampacityEdit

The ampacity of a conductor, that is, the amount of current it can carry, is related to its electrical resistance: a lower-resistance conductor can carry a larger value of current. The resistance, in turn, is determined by the material the conductor is made from (as described above) and the conductor's size. For a given material, conductors with a larger cross-sectional area have less resistance than conductors with a smaller cross-sectional area.

For bare conductors, the ultimate limit is the point at which power lost to resistance causes the conductor to melt. Aside fromfuses, most conductors in the real world are operated far below this limit, however. For example, household wiring is usually insulated with PVC insulation that is only rated to operate to about 60 °C, therefore, the current in such wires must be limited so that it never heats the copper conductor above 60 °C, causing a risk of fire. Other, more expensive insulation such as Teflon or fiberglass may allow operation at much higher temperatures.

IsotropyEdit

If an electric field is applied to a material, and the resulting induced electric current is in the same direction, the material is said to be anisotropic electrical conductor. If the resulting electric current is in a different direction from the applied electric field, the material is said to be an anisotropic electrical conductor.

See alsoEdit

Classification of materials based on permittivity

εr″/εr′	Current conduction	Field propagation
0		perfect dielectric lossless medium
≪ 1	low-conductivity material poor conductor	low-loss medium good dielectric
≈ 1	lossy conducting material	lossy propagation medium
≫ 1	high-conductivity material good conductor	high-loss medium poor dielectric
∞	perfect conductor

• Stephen Gray, first to identify electrical conductors and insulators
• Resistivity
• Charge transfer complex
• Bundle conductor
• Superconductivity