**Electrical resistivity** (also known as *specific electrical resistance*) is a measure indicating how strongly a material opposes the flow of electric current; if the resistivity of the material is small, that means that material is effective to carry electrons.

The resistivity of a material is usually denoted by the lower-case Greek letter rho (ρ) and is given by *RS/l*, where *R* is the resistance of a uniform specimen of the material, having a length *l* and a cross-section area *S*. The units of ρ are ohm meters. Its reciprocal quantity is electrical conductivity.

Also the resistivity is the magnitude of the electric field divided by the magnitude of the current density.

In general, electrical resistivity of metals increases with temperature, while the resistivity of semiconductors decreases with temperature.

As the temperature of a metal is reduced, the resistance usually reduces until it reaches a constant value, known as the residual resistivity. This value depends not only on the type of metal, but on its purity and thermal history.

Some materials lose all electrical resistivity at sufficiently low temperatures; this effect is known as superconductivity.

The table of resistivity for various materials (at 20 degree):

Material | Resistivity (Ohm-meters) |

Silver | 1.59 x 10^{-8} |

Copper | 1.7 x 10^{-8} |

Gold | 2.44 x 10^{-8} |

Aluminum | 2.82 x 10^{-8} |

Tungsten | 5.6 x 10^{-8} |

Iron | 10 x 10^{-8} |

Platinum | 11 x 10^{-8} |

Lead | 22 x 10^{-8} |

Nichrome (A nickel-chromium alloy commonly used in heating elements) | 1.50 x 10^{-6} |

Carbon | 3.5 x 10^{-5} |

Germanium | 0.46 |

Silicon | 640 |

Glass | 10^{10} to 10^{14} |

Hard rubber | approximately 10^{13} |

Sulfur | 10^{15} |

Quartz (fused) | 75 x ^{16} |