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Ohm | |
---|---|

A laboratory one-ohm standard resistor, circa 1917. | |

General information | |

Unit system | SI derived unit |

Unit of | Electrical resistance |

Symbol | Ω |

Named after | Georg Ohm |

In SI base units: | kg⋅m ^{2}⋅s ^{−3}⋅A ^{−2} |

The **ohm** (symbol: Ω) is the SI derived unit of electrical resistance, named after German physicist Georg Simon Ohm. Although several empirically derived standard units for expressing electrical resistance were developed in connection with early telegraphy practice, the British Association for the Advancement of Science proposed a unit derived from existing units of mass, length and time and of a convenient size for practical work as early as 1861. The definition of the ohm was revised several times. Today, the definition of the ohm is expressed from the quantum Hall effect.

**Omega** is the 24th and last letter of the Greek alphabet. In the Greek numeric system/Isopsephy (Gematria), it has a value of 800. The word literally means "great O", as opposed to omicron, which means "little O".

**SI derived units** are units of measurement derived from the seven base units specified by the International System of Units (SI). They are either dimensionless or can be expressed as a product of one or more of the base units, possibly scaled by an appropriate power of exponentiation.

The **quantum Hall effect** is a quantum-mechanical version of the Hall effect, observed in two-dimensional electron systems subjected to low temperatures and strong magnetic fields, in which the Hall conductance *σ* undergoes quantum Hall transitions to take on the quantized values

The ohm is defined as an electrical resistance between two points of a conductor when a constant potential difference of one volt, applied to these points, produces in the conductor a current of one ampere, the conductor not being the seat of any electromotive force.^{ [1] }

The **volt** is the derived unit for electric potential, electric potential difference (voltage), and electromotive force. It is named after the Italian physicist Alessandro Volta (1745–1827).

The **ampere**, often shortened to "amp", is the base unit of electric current in the International System of Units (SI). It is named after André-Marie Ampère (1775–1836), French mathematician and physicist, considered the father of electrodynamics.

**Electromotive force**, abbreviated **emf**, is the electrical action produced by a non-electrical source. A device that converts other forms of energy into electrical energy, such as a battery or generator, provides an emf as its output. Sometimes an analogy to water "pressure" is used to describe electromotive force.

in which the following units appear: volt (V), ampere (A), siemens (S), watt (W), second (s), farad (F), henry (H), joule (J), kilogram (kg), metre (m), and coulomb (C).

The **siemens** is the derived unit of electric conductance, electric susceptance, and electric admittance in the International System of Units (SI). Conductance, susceptance, and admittance are the reciprocals of resistance, reactance, and impedance respectively; hence one siemens is redundantly equal to the reciprocal of one ohm, and is also referred to as the *mho*. The 14th General Conference on Weights and Measures approved the addition of the siemens as a derived unit in 1971.

The **watt** is a unit of power. In the International System of Units (SI) it is defined as a derived unit of 1 joule per second, and is used to quantify the rate of energy transfer. In dimensional analysis, power is described by .

The **second** is the base unit of time in the International System of Units (SI), commonly understood and historically defined as ^{1}⁄_{86400} of a day – this factor derived from the division of the day first into 24 hours, then to 60 minutes and finally to 60 seconds each. Analog clocks and watches often have sixty tick marks on their faces, representing seconds, and a "second hand" to mark the passage of time in seconds. Digital clocks and watches often have a two-digit seconds counter. The second is also part of several other units of measurement like meters per second for velocity, meters per second per second for acceleration, and per second for frequency.

In many cases the resistance of a conductor in ohms is approximately constant within a certain range of voltages, temperatures, and other parameters. These are called linear resistors. In other cases resistance varies (e.g., thermistors).

A **resistor** is a passive two-terminal electrical component that implements electrical resistance as a circuit element. In electronic circuits, resistors are used to reduce current flow, adjust signal levels, to divide voltages, bias active elements, and terminate transmission lines, among other uses. High-power resistors that can dissipate many watts of electrical power as heat, may be used as part of motor controls, in power distribution systems, or as test loads for generators. Fixed resistors have resistances that only change slightly with temperature, time or operating voltage. Variable resistors can be used to adjust circuit elements, or as sensing devices for heat, light, humidity, force, or chemical activity.

A **thermistor** is a type of resistor whose resistance is dependent on temperature, more so than in standard resistors. The word is a portmanteau of *thermal* and *resistor*. Thermistors are widely used as inrush current limiters, temperature sensors, self-resetting overcurrent protectors, and self-regulating heating elements.

A vowel of the prefixed units kiloohm and megaohm is commonly omitted, producing kilohm and megohm.^{ [2] }

In alternating current circuits, electrical impedance is also measured in ohms.

**Electrical impedance** is the measure of the opposition that a circuit presents to a current when a voltage is applied. The term *complex impedance* may be used interchangeably.

Following the 2019 redefinition of the SI base units, in which the ampere and the kilogram were redefined in terms of fundamental constants, the ohm is now also defined in terms of these constants.

The siemens (symbol: S) is the SI derived unit of electric conductance and admittance, also known as the mho (ohm spelled backwards, symbol is ℧); it is the reciprocal of resistance in ohms (Ω).

The power dissipated by a resistor may be calculated from its resistance, and the voltage or current involved. The formula is a combination of Ohm's law and Joule's law:

where:

*P*is the power*R*is the resistance*V*is the voltage across the resistor*I*is the current through the resistor

A linear resistor has a constant resistance value over all applied voltages or currents; many practical resistors are linear over a useful range of currents. Non-linear resistors have a value that may vary depending on the applied voltage (or current). Where alternating current is applied to the circuit (or where the resistance value is a function of time), the relation above is true at any instant but calculation of average power over an interval of time requires integration of "instantaneous" power over that interval.

Since the ohm belongs to a coherent system of units, when each of these quantities has its corresponding SI unit (watt for *P*, ohm for *R*, volt for *V* and ampere for *I*, which are related as in § Definition, this formula remains valid numerically when these units are used (and thought of as being cancelled or omitted).

The rapid rise of electrotechnology in the last half of the 19th century created a demand for a rational, coherent, consistent, and international system of units for electrical quantities. Telegraphers and other early users of electricity in the 19th century needed a practical standard unit of measurement for resistance. Resistance was often expressed as a multiple of the resistance of a standard length of telegraph wires; different agencies used different bases for a standard, so units were not readily interchangeable. Electrical units so defined were not a coherent system with the units for energy, mass, length, and time, requiring conversion factors to be used in calculations relating energy or power to resistance.^{ [3] }

Two different methods of establishing a system of electrical units can be chosen. Various artifacts, such as a length of wire or a standard electrochemical cell, could be specified as producing defined quantities for resistance, voltage, and so on. Alternatively, the electrical units can be related to the mechanical units by defining, for example, a unit of current that gives a specified force between two wires, or a unit of charge that gives a unit of force between two unit charges. This latter method ensures coherence with the units of energy. Defining a unit for resistance that is coherent with units of energy and time in effect also requires defining units for potential and current. It is desirable that one unit of electrical potential will force one unit of electric current through one unit of electrical resistance, doing one unit of work in one unit of time, otherwise all electrical calculations will require conversion factors.

Since so-called "absolute" units of charge and current are expressed as combinations of units of mass, length, and time, dimensional analysis of the relations between potential, current, and resistance show that resistance is expressed in units of length per time — a velocity. Some early definitions of a unit of resistance, for example, defined a unit resistance as one quadrant of the Earth per second.

The absolute-units system related magnetic and electrostatic quantities to metric base units of mass, time, and length. These units had the great advantage of simplifying the equations used in the solution of electromagnetic problems, and eliminated conversion factors in calculations about electrical quantities. However, the centimeter-gram-second, CGS, units turned out to have impractical sizes for practical measurements.

Various artifact standards were proposed as the definition of the unit of resistance. In 1860 Werner Siemens (1816–1892) published a suggestion for a reproducible resistance standard in Poggendorffs * Annalen der Physik und Chemie *.^{ [4] } He proposed a column of pure mercury, of one square millimeter cross section, one metre long: Siemens mercury unit. However, this unit was not coherent with other units. One proposal was to devise a unit based on a mercury column that would be coherent – in effect, adjusting the length to make the resistance one ohm. Not all users of units had the resources to carry out metrology experiments to the required precision, so working standards notionally based on the physical definition were required.

In 1861, Latimer Clark (1822–1898) and Sir Charles Bright (1832–1888) presented a paper at the British Association for the Advancement of Science meeting ^{ [5] } suggesting that standards for electrical units be established and suggesting names for these units derived from eminent philosophers, 'Ohma', 'Farad' and 'Volt'. The BAAS in 1861 appointed a committee including Maxwell and Thomson to report upon standards of electrical resistance.^{ [6] } Their objectives were to devise a unit that was of convenient size, part of a complete system for electrical measurements, coherent with the units for energy, stable, reproducible and based on the French metrical system.^{ [7] } In the third report of the committee, 1864, the resistance unit is referred to as "B.A. unit, or Ohmad".^{ [8] } By 1867 the unit is referred to as simply *ohm*.^{ [9] }

The B.A. ohm was intended to be 10^{9} CGS units but owing to an error in calculations the definition was 1.3% too small. The error was significant for preparation of working standards.

On September 21, 1881 the * Congrès internationale des électriciens * (international conference of electricians) defined a *practical* unit of ohm for the resistance, based on CGS units, using a mercury column 1 sq. mm. in cross-section, approximately 104.9 cm in length at 0 °C,^{ [10] } similar to the apparatus suggested by Siemens.

A *legal* ohm, a reproducible standard, was defined by the international conference of electricians at Paris in 1884^{[ citation needed ]} as the resistance of a mercury column of specified weight and 106 cm long; this was a compromise value between the B. A. unit (equivalent to 104.7 cm), the Siemens unit (100 cm by definition), and the CGS unit. Although called "legal", this standard was not adopted by any national legislation. The "international" ohm was recommended by unanimous resolution at the International Electrical Congress 1893 in Chicago.^{ [11] } The unit was based upon the ohm equal to 10^{9} units of resistance of the C.G.S. system of electromagnetic units. The international ohm is represented by the resistance offered to an unvarying electric current in a mercury column of constant cross-sectional area 106.3 cm long of mass 14.4521 grams and 0 °C. This definition became the basis for the legal definition of the ohm in several countries. In 1908, this definition was adopted by scientific representatives from several countries at the International Conference on Electric Units and Standards in London.^{ [11] } The mercury column standard was maintained until the 1948 General Conference on Weights and Measures, at which the ohm was redefined in absolute terms instead of as an artifact standard.

By the end of the 19th century, units were well understood and consistent. Definitions would change with little effect on commercial uses of the units. Advances in metrology allowed definitions to be formulated with a high degree of precision and repeatability.

Unit^{ [12] } | Definition | Value in B.A. ohms | Remarks |
---|---|---|---|

Absolute foot/second × 10^{7} | using imperial units | 0.3048 | considered obsolete even in 1884 |

Thomson's unit | using imperial units | 0.3202 | 100 million feet/second, considered obsolete even in 1884 |

Jacobi copper unit | A specified copper wire 25 feet long weighing 345 grains | 0.6367 | Used in 1850s |

Weber's absolute unit × 10^{7} | Based on the metre and the second | 0.9191 | |

Siemens mercury unit | 1860. A column of pure mercury | 0.9537 | 100 cm and 1 mm^{2} cross section at 0 °C |

British Association (B.A.) "ohm" | 1863 | 1.000 | Standard coils deposited at Kew Observatory in 1863^{ [13] } |

Digney, Breguet, Swiss | 9.266–10.420 | Iron wire 1 km long and 4 square mm cross section | |

Matthiessen | 13.59 | One mile of 1/16 inch diameter pure annealed copper wire at 15.5 °C | |

Varley | 25.61 | One mile of special 1/16 inch diameter copper wire | |

German mile | 57.44 | A German mile (8,238 yard) of iron wire 1/6th inch diameter | |

Abohm | 10^{−9} | Electromagnetic absolute unit in centimeter–gram–second units | |

Statohm | 8.987551787 × 10^{11} | Electrostatic absolute unit in centimeter–gram–second units |

The mercury column method of realizing a physical standard ohm turned out to be difficult to reproduce, owing to the effects of non-constant cross section of the glass tubing. Various resistance coils were constructed by the British Association and others, to serve as physical artifact standards for the unit of resistance. The long-term stability and reproducibility of these artifacts was an ongoing field of research, as the effects of temperature, air pressure, humidity, and time on the standards were detected and analyzed.

Artifact standards are still used, but metrology experiments relating accurately-dimensioned inductors and capacitors provided a more fundamental basis for the definition of the ohm. Since 1990 the quantum Hall effect has been used to define the ohm with high precision and repeatability. The quantum Hall experiments are used to check the stability of working standards that have convenient values for comparison.^{ [14] }

Following the 2019 redefinition of the SI base units, in which the ampere and the kilogram were redefined in terms of fundamental constants, the ohm is now also defined in terms of these constants.

The symbol Ω was suggested, because of the similar sound of ohm and omega, by William Henry Preece in 1867.^{ [15] } In documents printed before WWII the unit symbol often consisted of the raised lowercase omega (ω), such that 56 Ω was written as 56^{ω}.

Historically, some document editing software applications have used the Symbol typeface to render the character Ω.^{ [16] } Where the font is not supported, a W is displayed instead ("10 W" instead of "10 Ω", for instance). As W represents the watt, the SI unit of power, this can lead to confusion, making the use of the correct Unicode code point preferable.

Where the character set is limited to ASCII, the IEEE 260.1 standard recommends substituting the symbol *ohm* for Ω.

In the electronics industry it is common to use the character *R* instead of the Ω symbol, thus, a 10 Ω resistor may be represented as 10R. This is the British standard BS 1852 code. It is used in many instances where the value has a decimal place. For example, 5.6 Ω is listed as 5R6. This method avoids overlooking the decimal point, which may not be rendered reliably on components or when duplicating documents.

Unicode encodes the symbol as U+2126ΩOHM SIGN, distinct from Greek omega among letterlike symbols, but it is only included for backwards compatibility and the Greek uppercase omega character U+03A9ΩGREEK CAPITAL LETTER OMEGA (HTML `Ω`

**·**`Ω`

) is preferred.^{ [17] } In DOS and Windows, the alt code ALT 234 may produce the Ω symbol. In Mac OS, `⌥ Opt`+`Z` does the same.

- ↑ BIPM SI Brochure: Appendix 1, p. 144
- ↑ The
*NIST Guide to the SI: 9.3 Spelling unit names with prefixes*reports that IEEE/ASTM SI 10-2002*IEEE/ASTM Standard for Use of the International System of Units (SI): The Modern Metric System*states that there are three cases in which the final vowel of an SI prefix is commonly omitted: megohm, kilohm, and hectare, but that in all other cases in which the unit name begins with a vowel, both the final vowel of the prefix and the vowel of the unit name are retained and both are pronounced. - ↑ Hunt, Bruce J (1994). "The Ohm Is Where the Art Is: British Telegraph Engineers and the Development of Electrical Standards" (PDF).
*Osiris*. 2nd.**9**: 48–63. doi:10.1086/368729. Archived from the original (PDF) on 8 March 2014. Retrieved 27 February 2014. - ↑ Werner Siemens (1860), "Vorschlag eines reproducirbaren Widerstandsmaaßes",
*Annalen der Physik und Chemie*(in German),**186**(5), pp. 1–20, Bibcode:1860AnP...186....1S, doi:10.1002/andp.18601860502 - ↑ Clark, Latimer; Bright, Sir Charles (1861-11-09). "Measurement of Electrical Quantities and Resistance".
*The Electrician*.**1**(1): 3–4. Retrieved 27 February 2014. - ↑
*Report of the Thirty-First Meeting of the British Association for the Advancement of Science; held at Manchester in September 1861*. September 1861. pp. xxxix–xl. - ↑ Williamson, Professor A; Wheatstone, Professor C; Thomson, Professor W; Miller, Professor WH; Matthiessen, Dr. A; Jenkin, Mr. Fleeming (September 1862).
*Provisional Report of the Committee appointed by the British Association on Standards of Electrical Resistance*. Thirty-second Meeting of the British Association for the Advancement of Science. London: John Murray. pp. 125–163. Retrieved 2014-02-27. - ↑ Williamson, Professor A; Wheatstone, Professor C; Thomson, Professor W; Miller, Professor WH; Matthiessen, Dr. A; Jenkin, Mr. Fleeming; Bright, Sir Charles; Maxwell, Professor; Siemens, Mr. CW; Stewart, Mr. Balfour; Joule, Dr.; Varley, Mr. CF (September 1864).
*Report of the Committee on Standards of Electrical Resistance*. Thirty-fourth Meeting of the British Association for the Advancement of Science. London: John Murray. p. Foldout facing page 349. Retrieved 2014-02-27. - ↑ Williamson, Professor A; Wheatstone, Professor C; Thomson, Professor W; Miller, Professor WH; Matthiessen, Dr. A; Jenkin, Mr. Fleeming; Bright, Sir Charles; Maxwell, Professor; Siemens, Mr. CW; Stewart, Mr. Balfour; Varley, Mr. CF; Foster, Professor GC; Clark, Mr. Latimer; Forbes, Mr. D.; Hockin, Mr. Charles; Joule, Dr. (September 1867).
*Report of the Committee on Standards of Electrical Resistance*. Thirty-seventh Meeting of the British Association for the Advancement of Science. London: John Murray. p. 488. Retrieved 2014-02-27. - ↑ "System of measurement units".
*Engineering and Technology History Wiki*. Retrieved 13 April 2018. - 1 2 "Units, Physical".
*Encyclopædia Britannica*.**27**(11th ed.). 1911. p. 742. - ↑ Gordon Wigan (trans. and ed.),
*Electrician's Pocket Book*, Cassel and Company, London, 1884 - ↑ Historical Studies in International Corporate Business. Teich p34
- ↑ R. Dzuiba and others,
*Stability of Double-Walled Maganin Resistors*in*NIST Special Publication Proceedings of SPIE--the International Society for Optical Engineering*, The Institute, 1988 pages 63-64 - ↑ Preece, William Henry (1867), "The B.A. unit for electrical measurements",
*Philosophical Magazine*,**33**, p. 397, retrieved 26 February 2017 - ↑ E.g. recommended in HTML 4.01: "HTML 4.01 Specification".
*W3C*. 1998. Section 24.1 "Introduction to character entity references". Retrieved 2018-11-22. - ↑ Excerpts from
*The Unicode Standard, Version 4.0*, accessed 11 October 2006

The **centimetre–gram–second system of units** is a variant of the metric system based on the centimetre as the unit of length, the gram as the unit of mass, and the second as the unit of time. All CGS mechanical units are unambiguously derived from these three base units, but there are several different ways of extending the CGS system to cover electromagnetism.

The **International System of Units** is the modern form of the metric system, and is the most widely used system of measurement. It comprises a coherent system of units of measurement built on seven base units, which are the second, metre, kilogram, ampere, kelvin, mole, candela, and a set of twenty prefixes to the unit names and unit symbols that may be used when specifying multiples and fractions of the units. The system also specifies names for 22 derived units, such as lumen and watt, for other common physical quantities.

**Voltage**, **electric potential difference**, **electric pressure **or **electric tension** is the difference in electric potential between two points. The difference in electric potential between two points in a static electric field is defined as the work needed per unit of charge to move a test charge between the two points. In the International System of Units, the derived unit for voltage is named *volt*. In SI units, work per unit charge is expressed as joules per coulomb, where 1 volt = 1 joule per 1 coulomb. The official SI definition for *volt* uses power and current, where 1 volt = 1 watt per 1 ampere. This definition is equivalent to the more commonly used 'joules per coulomb'. Voltage or electric potential difference is denoted symbolically by ∆*V*, but more often simply as *V*, for instance in the context of Ohm's or Kirchhoff's circuit laws.

The **coulomb** is the International System of Units (SI) unit of electric charge. It is the charge transported by a constant current of one ampere in one second:

**Ohm's law** states that the current through a conductor between two points is directly proportional to the voltage across the two points. Introducing the constant of proportionality, the resistance, one arrives at the usual mathematical equation that describes this relationship:

The **electrical resistance** of an object is a measure of its opposition to the flow of electric current. The inverse quantity is **electrical conductance**, and is the ease with which an electric current passes. Electrical resistance shares some conceptual parallels with the notion of mechanical friction. The SI unit of electrical resistance is the ohm (Ω), while electrical conductance is measured in siemens (S).

The **henry** is the SI derived unit of electrical inductance. If a current of 1 ampere flowing through the coil produces flux linkage of 1 weber turn, the coil has a self inductance of 1 henry. The unit is named after Joseph Henry (1797–1878), the American scientist who discovered electromagnetic induction independently of and at about the same time as Michael Faraday (1791–1867) in England.

The **farad** is the SI derived unit of electrical capacitance, the ability of a body to store an electrical charge. It is named after the English physicist Michael Faraday.

As originally stated in terms of DC resistive circuits only, **Thévenin's theorem** holds that:

**Transconductance**, also infrequently called **mutual conductance**, is the electrical characteristic relating the current through the output of a device to the voltage across the input of a device. Conductance is the reciprocal of resistance.

In physics, the **weber** is the SI derived unit of magnetic flux. A *flux density* of one Wb/m^{2} is one tesla.

A **conventional electrical unit** is a unit of measurement in the field of electricity which is based on the so-called "conventional values" of the Josephson constant and the von Klitzing constant agreed by the International Committee for Weights and Measures (CIPM) in 1988. These units are very similar in scale to their corresponding SI units, but are not identical because of their different definition. They are distinguished from the corresponding SI units by setting the symbol in italic typeface and adding a subscript "90" – e.g., the conventional volt has the symbol *V*_{90} – as they came into international use on 1 January 1990.

The **International System of Electrical and Magnetic Units** is an obsolete system of units used for measuring electrical and magnetic quantities. It was proposed as a system of practical international units by unanimous recommendation at the International Electrical Congress, discussed at other Congresses, and finally adopted at the International Conference on Electric Units and Standards in London in 1908. It was rendered obsolete by the inclusion of electromagnetic units in the International System of Units (SI) at the 9th General Conference on Weights and Measures in 1948.

The constants **K _{M}** and

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