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Electrical conductance is a measure of how easily electricity flows along a certain path through an electrical element. The SI derived unit of conductance is the siemens (also called the mho, because it is the reciprocal of electrical resistance, measured in ohms). Oliver Heaviside coined the term in September 1885.## Relation to other quantities

As mentioned, conductance is related to resistance by:
## Combining conductances

## Small-signal device conductances

The term conductance is applied to electronic devices such as transistors and diodes, where it usually refers to a small-signal model that is a linearization of the underlying device equations about a selected DC operating point or Q-point. This conductance is the reciprocal of the small-signal device resistance. See Early effect and channel length modulation.
## References

## See also

Electrical conductance is related to but should not be confused with conduction, which is the mechanism by which charge flows, or with conductivity, which is a property of a material.

- $G\; =\; frac\{1\}\{R\}\; =\; frac\{I\}\{V\}\; ,$

where:

- G is the electrical conductance,

- R is the electrical resistance,

- I is the electric current,

- V is the voltage.

(Note: this is not true where the impedance is complex)

Furthermore, conductance is related to susceptance and admittance by the equation:

- $Y\; =\; G\; +\; j\; B\; ,$

or

- $G\; =\; Re(Y)\; ,$

where:

- Y is the admittance,

- $j$ is the imaginary unit,

- B is the susceptance.

The conductance G of an object of cross-sectional area A and length $ell$ can be determined from the material's conductivity σ by the formula,

- $G=frac\{sigma\; ,\; A\}\{ell\}$

From Kirchhoff's circuit laws we can deduce the rules for combining conductances. For two conductances $G\_1$ and $G\_2$ in parallel the voltage across them is the same and from Kirchoff's Current Law the total current is

- $I\_\{Eq\}\; =\; I\_1\; +\; I\_2\; ,$.

Substituting Ohm's law for conductances gives

- $G\_\{Eq\}\; V\; =\; G\_1\; V\; +\; G\_2\; V\; ,$

and the equivalent conductance will be,

- $G\_\{Eq\}\; =\; G\_1\; +\; G\_2\; ,$.

For two conductances $G\_1$ and $G\_2$ in series the current through them will be the same and Kirchhoff's Voltage Law tells us that the voltage across them is the sum of the voltages across each conductance, that is,

- $V\_\{Eq\}\; =\; V\_1\; +\; V\_2\; ,$.

Substituting Ohm's law for conductance then gives,

- $frac\; \{I\}\{G\_\{Eq\}\}\; =\; frac\; \{I\}\{G\_1\}\; +\; frac\; \{I\}\{G\_2\}$

which in turn gives the formula for the equivalent conductance,

- $frac\; \{1\}\{G\_\{Eq\}\}\; =\; frac\; \{1\}\{G\_1\}\; +\; frac\; \{1\}\{G\_2\}$

This equation can be rearranged slightly,

- $G\_\{Eq\}\; =\; frac\{G\_1\; G\_2\}\{G\_1+G\_2\}$.

- Halliday, David (1960).
*Physics Part II*. John Wiley and Sons.

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Last updated on Thursday September 25, 2008 at 17:18:15 PDT (GMT -0700)

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This article is licensed under the GNU Free Documentation License.

Last updated on Thursday September 25, 2008 at 17:18:15 PDT (GMT -0700)

View this article at Wikipedia.org - Edit this article at Wikipedia.org - Donate to the Wikimedia Foundation

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