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The resistance of a conductor is determined by the length, cross-sectional area, and resistivityof the conductor. Since temperature affects resistivity, resistance is indirectly affected by temperature.

Resistance is directly-proportional to the length of the conductor and inversely-proportional to its cross-sectional area, and resistivity is its constant of proportionality. If the length of the conductor is expressed in metres, and the cross-sectional area is expressed in square metres, then resistivity is expressed in ohm metres. Using American units of measurements, however, where length is expressed in feet and cross-sectional area in circular mils, resistivity is normally expressed in 'ohm circular mill per foot' (not, as often seen in textbooks: 'ohms per circular mil foot'!).

In the case of d.c. current, the charge carriers distribute themselves across the entire cross-sectional area of the conductor. In the case of a.c. current, however, due to what is known as the 'skin effect', there is a tendency for the charge carriers to move closer to the surface of the conductor -this acts to reduce the effective cross-sectional area of the conductor and, thus, raise its resistance. So a conductor's resistance to a.c. is somewhat higher than it is to d.c., and is generally termed its 'a.c. resistance'. A.C. resistance increases with frequency (and should not be confused with 'reactance' or 'impedance').

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