Checking the voltage/current (V/I) ratio of conductors at various temperatures shows that the resistance of most conducting materials increases linearly with temperature except at very hot or very cold temperatures.

Temperature has little effect on the resistance of some alloys, such as **constantan**. For a few materials, including carbon and other semiconductors, the **resistance decreases as the temperature increases**.

**Figure 1** shows the resistance of a conductor increases with temperature. R_{1} is the resistance at temperature T_{1}, and R_{2} is the resistance at temperature T. The line segment **CF** shows how the resistance varies for temperatures between T_{1} and T_{2}. The steeper the slope of segment **CF,** the more the resistance increases with temperature.

**Figure 1** Effect of temperature on resistance

Extending CF to the temperature axis produces triangles ABC and ADF. Since these triangles are similar,

\[\frac{DF}{BC}=\frac{AD}{AB}=\frac{AO+OD}{AO+OB}\]

Substituting the quantities that the sides of the triangles represent gives

\[\begin{matrix} \frac{{{R}_{2}}}{{{R}_{1}}}=\frac{x+{{T}_{2}}}{x+{{T}_{1}}} & {} & \left( 1 \right) \\\end{matrix}\]

Where R_{1} is the resistance of the conductor at temperature T_{1}, R_{2} is the resistance at temperature T_{2}, and x is the difference between 0°C and the temperature at which the resistance would be zero if it continued to decrease linearly at very low temperatures.

- You May Also Read: Electrical Resistance: Definition, Unit, Formula, Examples

Table 1 lists values for x for some metals commonly used for conductors. The values for Nichrome II and constantan show that x is not the actual temperature at which the resistance becomes zero ohms. However, we can use x to calculate resistances within the range of temperatures where the resistance varies linearly with temperature.

Material |
x(^{o}C) |

Silver | 243 |

Copper | 234.5 |

Aluminum | 236 |

Tungsten | 202 |

Nickel | 147 |

Iron | 180 |

Nichrome | 6 250 |

Constantan | 125 000 |

**Table 1** Values of x for common conductors

**Example**

A copper conductor has a resistance of 12.0 V at 20°C. Find the resistance at 100°C.

**Solution**

Since,

\[\frac{{{R}_{2}}}{{{R}_{1}}}=\frac{x+{{T}_{2}}}{x+{{T}_{1}}}\]

So,

\[{{R}_{2}}={{R}_{1}}\times \frac{x+{{T}_{2}}}{x+{{T}_{1}}}=12\Omega \times \frac{234.5+100}{234.5+20}=15.8\Omega \]

Note that the temperature units, °C, cancel out in this calculation.

In addition to being able to calculate the effect that temperature has on resistance, we can use the change in resistance of a certain material to calculate the temperature in locations where it is difficult to place a thermometer.

**Example**

The copper winding of an electric motor that has been standing for several hours in a room at 20°C has a resistance of 0.20 V. When the motor has been in use for some hours, the resistance of the winding is found to be 0.22 V. Calculate the temperature rise in the winding.

**Solution**

$\begin{align} & \frac{{{R}_{2}}}{{{R}_{1}}}=\frac{x+{{T}_{2}}}{x+{{T}_{1}}} \\ & \frac{0.22}{0.20}=\frac{234.5+{{T}_{2}}}{234.5+20} \\ & {{T}_{2}}=\frac{0.22}{0.20}\times \left( 234.5+20 \right)={{45.45}^{o}}C \\\end{align}$

**Temperature rise** = T_{2} – T_{1} = 45.45^{o}C – 20^{o}C = 25^{o}C

Substituting $R=\rho \frac{l}{A}$ for R_{1} in Equation 1 gives

\[\begin{matrix} R=\rho \frac{l}{A}\left( \frac{x+T}{x+20} \right) & {} & \left( 2 \right) \\\end{matrix}\]

With values for ρ and x, we can use Equation 2 to estimate the resistance of any metallic conductor at any temperature.

**Temperature Coefficient of Resistance**

Now we shall derive an alternative method of showing the effect of temperature on the resistance of a conductor. In Figure 1, line segment CE is parallel to the temperature axis. Since resistivity is usually stated for a temperature of 20°C, we shall let T_{1} represent 20°C.

Triangle ABC is similar to triangle CEF, so

\[\frac{FE}{BC}=\frac{CE}{AB}\]

Substituting the quantities that the sides of the triangles represent gives

\[\frac{FE}{{{R}_{1}}}=\frac{\Delta T}{x+20}\]

Where ΔT is the difference between T_{2} and 20°C.

Therefore,

\[FE={{R}_{1}}\times \frac{\Delta T}{x+20}\]

Since **CE** and **BD** are parallel,

\[{{R}_{2}}=ED+FE={{R}_{1}}+{{R}_{1}}\times \frac{\Delta T}{x+20}={{R}_{1}}\left( 1+\frac{\Delta T}{x+20} \right)\]

The quantity $\frac{1}{x+20}$ is the temperature coefficient of resistance at 20°C, the proportion by which the resistance changes per degree of change in temperature from 20°C. We represent this coefficient by the Greek letter α (alpha).

$\begin{matrix} {{R}_{2}}={{R}_{1}}\left( 1+\alpha \Delta T \right) & {} & \left( 3 \right) \\\end{matrix}$

Where R_{2} is the resistance of a conductor at any specified temperature, R_{1} is its resistance at 20°C, α is the temperature coefficient of resistance at 20°C for the conductor, and ΔT is the difference between the specified temperature and 20°C.

Substituting ${{R}_{1}}=\rho \frac{l}{A}$ gives a general equation for the resistance of a conductor:

\[R=\rho \frac{l}{A}\begin{matrix} \left( 1+\alpha \Delta T \right) & {} & \left( 4 \right) \\\end{matrix}\]

where R is the resistance of the conductor in ohms, ρ is the resistivity of the material in ohmmeters at 20°C, l is the length in meters, A is the cross-sectional area in square meters, a is the temperature coefficient of resistance of the material at 20°C, and DT is the difference between the temperature of the conductor and 20°C.

**Table 2** lists temperature coefficients for some materials commonly used for conductors and resistors.

Conductor material |
α(K^{-1}) |

Silver | 0.003 8 |

Copper | 0.003 93 |

Aluminum | 0.003 9 |

Tungsten | 0.004 5 |

Nickel | 0.006 |

Iron | 0.005 5 |

Nichrome | 0.000 16 |

Constantan | 0.000 008 |

Carbon | -0.000 5 |

**Table 2** Temperature coefficients of resistance at 20°C

**Example**

A heating element made from Nichrome II has a resistance of 16.0 V at 1500°C. Find the resistance at normal room temperature.

**Solution **

In this example, R_{2} in Equation 3 is given and R_{1} is unknown. Hence,

\[{{R}_{1}}=\frac{{{R}_{2}}}{1+\alpha \Delta T}=\frac{16}{1+0.00016\times 1480}=12.9\Omega \]

If the required temperature is below 20°C, ΔT will be a negative quantity and the resulting resistance is less than the resistance at 20°C.