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statcoulomb | |
---|---|

Unit system | Gaussian, cgs-esu |

Unit of | electrical charge |

Symbol | Fr, statC, esu |

Derivation | dyn^{1/2}⋅cm |

Conversions | |

1 Fr in ... | ... is equal to ... |

CGS base units | cm^{3/2}⋅g^{1/2}⋅s^{−1} |

SI (charge) | ≘ ~3.33564×10^{−10} C |

SI (flux) | ≘ ~2.65×10^{−11} C |

The **franklin** (**Fr**) or **statcoulomb** (**statC**) **electrostatic unit of charge** (**esu**) is the physical unit for electrical charge used in the centimetre–gram–second electrostatic units variant (CGS-ESU) and Gaussian systems of units. It is a derived unit given by

- 1 statC = 1 dyn
^{1/2}⋅cm = 1 cm^{3/2}⋅g^{1/2}⋅s^{−1}.

That is, it is defined so that the Coulomb constant becomes a dimensionless quantity equal to 1.

It can be converted using

- 1 newton = 10
^{5}dyne - 1 cm = 10
^{−2}m

The SI system of units uses the coulomb (C) instead. The conversion between C and statC is different in different contexts. The most common contexts are:

- For electric charge:
- 1 C ≘ 2997924580 statC ≈ 3.00×10
^{9}statC - ⇒ 1 statC ≘ ~3.33564×10
^{−10}C.

- 1 C ≘ 2997924580 statC ≈ 3.00×10
- For electric flux (Φ
_{D}):- 1 C ≘ 4π × 2997924580 statC ≈ 3.77×10
^{10}statC - ⇒ 1 statC ≘ ~2.65×10
^{−11}C.

- 1 C ≘ 4π × 2997924580 statC ≈ 3.77×10

The symbol "≘" ('corresponds to') is used instead of "=" because the two sides are not interchangeable, as discussed below. The number 2997924580 is 10 times the numeric value of the speed of light expressed in meters/second, and the conversions are *exact* except where indicated. The second context implies that the SI and cgs units for an electric displacement field (D) are related by:

- 1 C/m
^{2}≘ 4π × 2997924580×10^{−4}statC/cm^{2}≈ 3.77×10^{6}statC/cm^{2} - ⇒ 1 statC/cm
^{2}≘ ~2.65×10^{−7}C/m^{2}

due to the relation between the metre and the centimetre. The coulomb is an extremely large charge rarely encountered in electrostatics, while the statcoulomb is closer to everyday charges.

The statcoulomb is defined as follows: if two stationary objects each carry a charge of 1 statC and are 1 cm apart, they will electrically repel each other with a force of 1 dyne. This repulsion is governed by Coulomb's law, which in the Gaussian-cgs system states:

where *F* is the force, *q*^{G}_{1} and *q*^{G}_{2} are the two charges, and *r* is the distance between the charges. Performing dimensional analysis on Coulomb's law, the dimension of electrical charge in cgs must be [mass]^{1/2} [length]^{3/2} [time]^{−1}. (This statement is *not* true in SI units; see below.) We can be more specific in light of the definition above: Substituting *F* = 1 dyn, *q*^{G}_{1} = *q*^{G}_{2} = 1 statC, and *r* = 1 cm, we get:

- 1 statC = g
^{1/2}⋅cm^{3/2}⋅s^{−1}

as expected.

This section may contain material unrelated or insufficiently related to the topic of the article; the off-topic material is the topic of another article, Gaussian units#Major differences between Gaussian and SI units. Please help improve this section or discuss this issue on the talk page. (February 2013) (Learn how and when to remove this template message)

Coulomb's law in the Gaussian unit system and the SI are respectively:

- (Gaussian)
- (SI)

Since *ε*_{0}, the vacuum permittivity, is *not* dimensionless, the coulomb is **not** dimensionally equivalent to [mass]^{1/2} [length]^{3/2} [time]^{−1}, unlike the statcoulomb. In fact, it is impossible to express the coulomb in terms of mass, length, and time alone.

Consequently, a conversion equation like "1 C = *n* statC" is misleading: the units on the two sides are not consistent. One *cannot* freely switch between coulombs and statcoulombs within a formula or equation, as one would freely switch between centimeters and meters. One can, however, find a *correspondence* between coulombs and statcoulombs in different contexts. As described below, "1 C *corresponds to* 3.00×10^{9} statC" when describing the charge of objects. In other words, if a physical object has a charge of 1 C, it also has a charge of 3.00×10^{9} statC. Likewise, "1 C *corresponds to* 3.77×10^{10} statC" when describing an electric displacement field flux.

The statcoulomb is defined as follows: If two stationary objects each carry a charge of 1 statC and are 1 cm apart in vacuum, they will electrically repel each other with a force of 1 dyne. From this definition, it is straightforward to find an equivalent charge in coulombs. Using the SI equation

- (SI),

and plugging in F = 1 dyn = 10^{−5} N, and r = 1 cm = 10^{−2} m, and then solving for *q* = *q*^{SI}_{1} = *q*^{SI}_{2}, the result is q = (1/2997924580) C ≈ 3.34×10^{−10} C. Therefore, an object with a charge of 1 statC has a charge of 3.34×10^{−10} C.

This can also be expressed by the following conversion, which is fully dimensionally consistent, and often useful for switching between SI and cgs formulae:

An electric flux (specifically, a flux of the electric displacement field **D**) has units of charge: statC in cgs and coulombs in SI. The conversion factor can be derived from Gauss's law:

where

Therefore, the conversion factor for flux is 4π different from the conversion factor for charge:

- (as unit of Φ
_{D}).

The dimensionally consistent version is:

- (as unit of Φ
_{D})