View source for Proposed redefinition of SI base units

{{outline|Outline of the metric system}}
[[File:Unit relations in the old SI.svg|thumb|312px| Current (2018) [[International System of Units|SI system]]: Dependence of [[SI base unit|base unit]] definitions on other base units (for example, the [[Metre|metre]] is defined in terms of the distance travelled by light in a specific fraction of a  [[Second|second]]), with the constants of nature and artefacts used to define them (such as the mass of the IPK for the kilogram).]]
[[File:Unit relations in the new SI.svg|thumb|312px|Proposed SI system: Dependence of base unit definitions on physical constants with fixed numerical values and on other base units that are derived from the same set of constants.]]
The [[Organization:International Committee for Weights and Measures|International Committee for Weights and Measures]] (CIPM) has proposed{{r|cipm_106|p=23}} revised definitions of the [[SI base unit]]s, for consideration at the 26th [[General Conference on Weights and Measures]] (CGPM).  It is expected that the formal vote, scheduled for 16 November 2018,<ref name=Milton16>{{cite conference |conference=SIM XXII General Assembly |location=Montevideo, Uruguay |url=http://www.sim-metrologia.org.br/docs/2016Presentations/BIPM%202016.pdf#page=10 |conference-url=http://www.sim-metrologia.org.br/docs/2016Presentations/ |page=10 |title=Highlights in the work of the BIPM in 2016 |first=Martin |last=Milton |date=14 November 2016}}  The conference runs from 13–16 November; the redefinition is scheduled for the morning of the last day.</ref> will be approved<ref name=CODATA2014/><ref name=NIST16/><ref name=Minutes2014/> and that the new definitions will to come into force on 20 May 2019.<ref name=SI-statement>{{citation |url=https://www.bipm.org/utils/common/pdf/SI-statement.pdf |title=BIPM statement: Information for users about the proposed revision of the SI}}</ref><ref>[http://www.bipm.org/en/committees/cipm/meeting/105.html Decision CIPM/105-13 (October 2016)].  The day is the 144th anniversary of the [[Metre Convention]].</ref>  The [[Metric system|metric system]] was originally conceived as a system of measurement that was derivable from unchanging phenomena.<ref>{{cite book|last=Crease|first=Robert P.|title=World in the Balance|date=2011|publisher=W. W. Norton & Company, Inc.|location=New York|isbn=978-0-393-07298-3|pages=83–84|chapter=France: "Realities of Life and Labor"}}</ref> However, when the metric system was first introduced in France in 1799, technical limitations necessitated the use of  artefacts (the [[Prototype metre|prototype metre]] and prototype kilogram) instead.  In 1960 the [[Metre|metre]] was redefined in terms of the [[Wavelength|wavelength]] of [[Physics:Light|light]] from a specified source, making it derivable from natural phenomena, leaving the prototype kilogram as the only artefact upon which the SI unit definitions depend.  If the proposed redefinition is accepted, the metric system (SI) will, for the first time, be wholly derivable from natural phenomena. 

The proposal can be summarised as follows:
{{quote|There will still be the same seven base units (second, metre, kilogram, ampere, kelvin, mole, and candela). Of these, the kilogram, ampere, kelvin and mole will be redefined by choosing exact numerical values for the [[Physics:Planck constant|Planck constant]], the elementary electric charge, the [[Physics:Boltzmann constant|Boltzmann constant]], and the [[Physics:Avogadro constant|Avogadro constant]], respectively. The second, metre and candela are already defined by [[Physics:Physical constant|physical constant]]s and it is only necessary to edit their present definitions. The new definitions will improve the SI without changing the size of any units, thus ensuring continuity with present measurements.<ref name=Kuehne>{{cite web |first=Michael |last=Kühne |title=Redefinition of the SI |url=http://www.its9.org/symposium_program.html#SI_Redefinition_Keynote_Abstract |work=Keynote address, ITS<sup>9</sup> (Ninth International Temperature Symposium) |location=Los Angeles |accessdate=2012-03-01 |date=22 March 2012 |publisher=NIST |archiveurl=https://web.archive.org/web/20130618064512/http://www.its9.org/symposium_program.html |archivedate=2013-06-18 |deadurl=yes}}</ref>}}

Further details are found in the draft chapter of the ''Ninth SI Brochure''.<ref name=Brochure9_2016/>

The last major overhaul of the metric system was in 1960 when the [[International System of Units]] (SI) was formally published as a coherent set of units of measure. SI is structured around seven base units whose definitions are unconstrained by that of any other unit and another twenty-two named units derived from these base units.  Although the set of units forms a coherent system, the definitions do not.{{citation needed|reason=The concept 'coherent set of definitions' needs definition.|date=July 2018}} The proposal before the CIPM seeks to remedy this by using the fundamental quantities of nature as the basis for deriving the base units. This will mean, amongst other things, that the prototype kilogram will cease to be used as ''the'' definitive replica of the kilogram. The [[Second|second]] and the [[Metre|metre]] are already defined in such a manner.

A number of authors have published criticisms of the revised definitions – including that the proposal had failed to address the impact of breaking the link between the definition of the [[Dalton (unit)|dalton]]<ref>The dalton is not defined in the formal proposal to be voted upon by the CGPM, only in the (draft) ''Ninth SI Brochure''.</ref> and the definitions of the [[Kilogram|kilogram]], the [[Mole (unit)|mole]] and the [[Physics:Avogadro constant|Avogadro constant]].

==Background==
The basic structure of SI was developed over a period of about 170 years (1791 to 1960).  Since 1960, technological advances have made it possible to address various weaknesses in SI, such as the dependence on an artefact to define the kilogram.

===Development of SI===
During the early years of the {{wipe|French Revolution}}, the leaders of the French National Constituent Assembly decided to introduce a completely new [[System of measurement|system of measurement]] based on the principles of [[Logic|logic]] and natural phenomena.  Specifically, the metre was defined as one ten-millionth of the distance from the [[Earth:North Pole|North Pole]] to the [[Astronomy:Equator|Equator]], and the kilogram as the mass of one thousandth of a cubic metre of pure [[Chemistry:Water|water]].<!--Additional specifics (Paris meridian, temperature of water) omitted for brevity.-->  Although these definitions were chosen so that nobody would "own" the units, they could not be measured with sufficient convenience or precision for practical use.  Instead, realizations were created in the form of the ''{{lang|fr|mètre des Archives}}'' and ''{{lang|fr|kilogramme des Archives}}'' which were a "best attempt" at fulfilling these principles.<ref>{{cite book
|title=The Measure of all Things – The Seven-Year-Odyssey that Transformed the World
|last=Alder
|first=Ken
|year=2002
|publisher=Abacus
|location=London
|page=1
|isbn=0-349-11507-9}}</ref>

In 1875, by which time the use of the metric system had become widespread in Europe and in Latin America, twenty industrially developed nations met for the [[Convention of the Metre]]. The result was the signing of the Treaty of the Metre under which three bodies were set up to take custody of the international prototype kilogram and metre and to regulate comparisons with national prototypes.<ref>{{cite journal
 |url         = http://lamar.colostate.edu/~hillger/laws/metric-convention.html
 |title       = Metric Convention of 1875 [English translation]
 |publisher   = Office of the President of the United States
 |location    = Washington, D.C.
 |year        = 1876
 |deadurl     = yes
 |archiveurl  = https://web.archive.org/web/20050301093830/http://lamar.colostate.edu/~hillger/laws/metric-convention.html
 |archivedate = 2005-03-01
 |df          = 
}}</ref><ref>{{cite web
|url = http://www.bipm.org/en/convention/
|title = The Metre Convention
|location = Sèvres, France
|publisher = [[Organization:International Bureau of Weights and Measures|International Bureau of Weights and Measures]]
|accessdate = 2013-06-21
}}</ref>  They were:
* CGPM (General Conference on Weights and Measures / ''{{lang|fr|Conférence générale des poids et mesures}}'') – The Conference meets every four to six years and consists of delegates of the nations who had signed the convention. It discusses and examines the arrangements required to ensure the propagation and improvement of the [[International System of Units]] and it endorses the results of new fundamental [[Metrology|metrological]] determinations.
* CIPM (International Committee for Weights and Measures / ''{{lang|fr|Comité international des poids et mesures}}'') – The Committee consists of eighteen eminent scientists, each from a different country, nominated by the CGPM. The CIPM meets annually and is tasked to advise the CGPM. The CIPM has set up a number of sub-committees, each charged with a particular area of interest. One of these, the Consultative Committee for Units (CCU), amongst other things, advises the CIPM on matters concerning units of measurement.<ref>{{cite web
|url = http://www.bipm.org/en/committees/cipm/
|title = CIPM: International Committee for Weights and Measures
|publisher = BIPM
|location = Sèvres, France
|accessdate = 2010-10-03}}</ref>
* BIPM (International Bureau for Weights and Measures / ''{{lang|fr|Bureau international des poids et mesures}}'') – The Bureau provides safe keeping of the international prototype kilogram and metre, provides laboratory facilities for regular comparisons of the national prototypes with the international prototype and is the secretariat for the CIPM and the CGPM.

The first CGPM (1889) formally approved the use of 40 prototype metres and 40 prototype kilograms from the British firm Johnson Matthey as the standards mandated by the Convention of the Metre.<ref>{{cite web
|url = http://www.bipm.org/en/CGPM/db/1/1/
|title = Resolution of the 1st meeting of the CGPM (1889)
| location = Sèvres, France
|accessdate = 2013-06-21
|publisher = [[Organization:International Bureau of Weights and Measures|International Bureau of Weights and Measures]]
}}</ref> One of each of these was nominated by lot as the international prototypes, other copies were retained by the CGPM as working copies and the rest were distributed to member nations for use as their national prototypes. At regular intervals the national prototypes were compared with and recalibrated against the international prototype.<ref>{{cite journal
 |last1       = Jabbour
 |first1      = Z.J.
 |last2       = Yaniv
 |first2      = S.L.
 |year        = 2001
 |title       = The Kilogram and Measurements of Mass and Force
 |journal     = Journal of Research of the National Institute of Standards and Technology
 |volume      = 106
 |issue       = 1
 |pages       = 25–46
 |publisher   = [[Organization:National Institute of Standards and Technology|National Institute of Standards and Technology]] (NIST)
 |url         = http://nvl.nist.gov/pub/nistpubs/jres/106/1/j61jab.pdf
 |accessdate  = 2011-03-28
 |doi         = 10.6028/jres.106.003
 |deadurl     = yes
 |archiveurl  = https://web.archive.org/web/20110604144310/http://nvl.nist.gov/pub/nistpubs/jres/106/1/j61jab.pdf
 |archivedate = 2011-06-04
 |df          = 
}}</ref>
In 1921 the Convention of the Metre was revised and the mandate of the CGPM was extended to provide standards for all units of measure, not just mass and length. In the ensuing years the CGPM took on responsibility for providing standards of [[Physics:Electric current|electric current]] (1946), [[Astronomy:Luminosity|luminosity]] (1946), [[Physics:Temperature|temperature]] (1948), [[Time|time]] (1956) and [[Physics:Molar mass|molar mass]] (1971).<ref>{{SIbrochure8th|pages=95, 97, 138–140}}</ref>

[[File:Prototype mass drifts.jpg|thumb|right|399px|Mass drift over time of national prototypes {{nowrap|K21–K40}}, plus two of the International Prototype Kilogram's (IPK's) sister copies: K32 and K8(41).<ref group="Note">Prototype No. 8(41) was accidentally stamped with the number 41, but its accessories carry the proper number 8. Since there is no prototype marked 8, this prototype is referred to as 8(41).<sub>{{nbsp}}</sub></ref> All mass changes are relative to the IPK.<ref name="Girard">{{Cite journal |title=The Third Periodic Verification of National Prototypes of the Kilogram (1988–1992) |first=G. |last=Girard |journal=Metrologia |volume=31 |issue=4 |year=1994 |pages=317–336 |doi=10.1088/0026-1394/31/4/007 |bibcode = 1994Metro..31..317G }}</ref>]]

The 9th CGPM (1948) instructed the CIPM "to make recommendations for a single practical system of units of measurement, suitable for adoption by all countries adhering to the Metre Convention".<ref>{{cite web
|url = http://www.bipm.org/en/CGPM/db/9/6/
|title = Resolution 6 of the 9th meeting of the CGPM (1948): Proposal for establishing a practical system of units of measurement
|accessdate = 2011-03-23}}</ref>
The recommendations based on this mandate were presented to the 11th CGPM (1960) where they were formally accepted and given the name "''{{lang|fr|Système International d'Unités}}''" and its abbreviation "SI".<ref>{{cite web
|url = http://www.bipm.org/en/CGPM/db/11/12/
|location = Sèvres, France
|title = Resolution 12 of the 11th meeting of the CGPM (1960): Système International d'Unités
|accessdate = 2011-03-23}}</ref>

===Impetus for change===
Changing the underlying principles behind the definition of the SI base units is not without precedent.  The 11th CGPM (1960) defined the SI metre in terms of the wavelength of [[Physics:Krypton-86|krypton-86]] radiation, replacing the pre-SI metre bar.  The 13th CGPM (1967) replaced the original definition of the [[Second|second]] (which was based on a back-calculation of the [[Earth's rotation]] in the year 1900) with a definition based on the frequency of the radiation emitted between two hyperfine levels of the ground state of the caesium 133 atom.  And the 17th CGPM (1983) replaced the 1960 definition of the metre with one based on the second, by giving an exact definition of the speed of light in units of metres per second.<ref name=BaseDefs>{{SIBrochure8th |pages=112&ndash;116}}</ref>

Over the years, drifts of up to {{val|2|e=-8}} kilograms per annum in the national prototype kilograms relative to the international prototype kilogram have been detected. There was no way of determining whether the national prototypes were gaining mass or whether the IPK was losing mass.<ref>{{cite web
|url = http://physics.vniim.ru/SI50/files/mohr.pdf
|first=Peter
|last=Mohr
|title = Recent progress in fundamental constants and the International System of Units
|work = Third Workshop on Precision Physics and Fundamental Physical Constants
|date = 6 December 2010
|accessdate = 2011-01-02}}</ref> At the 21st meeting of the CGPM (1999), national laboratories were urged to investigate ways of breaking the link between the kilogram and a specific artefact. [[Organization:Newcastle University|Newcastle University]] metrologist Peter Cumpson has since identified [[Chemistry:Mercury (element)|mercury]] vapour absorption or [[Chemistry:Carbon|carbon]]aceous contamination as possible causes of this drift.<ref>{{cite news
|date = 7 January 2013
|url = http://www.thetimes.co.uk/tto/science/physics/article3649580.ece
|newspaper = The Times
|location = London
|title = The dirty secret of why you are not quite as heavy as you think
|first1 = Tom
|last1 = Whipple
|accessdate = 2011-03-23
|page = 15}}</ref><ref>{{cite web
|url =  http://www.livescience.com/26017-kilogram-gained-weight.html
|title = The Kilogram Has Gained Weight
|first1 = Tia
|last1 = Ghose
|publisher = LiveScience
|date = 6 January 2013
|accessdate = 2011-03-23}}</ref>

Independently of this drift having been identified, the [[Physics:Avogadro constant#International Avogadro Coordination|Avogadro project]] and development of the [[Engineering:Kibble balance|Kibble balance]] (known as a "watt balance" before 2016) promised methods of indirectly measuring mass with a very high precision.  These projects provided tools that would enable alternative means of redefining the kilogram.<ref name=Crease>{{cite web
|url = http://physicsworld.com/cws/article/indepth/2011/mar/22/metrology-in-the-balance
|title = Metrology in the balance
|first1 = Robert P.
|last1 = Crease
|accessdate = 2012-06-28
|work = Physics World
|publisher = [[Organization:Institute of Physics|Institute of Physics]]
|date = 22 March 2011}}</ref>

A report published in 2007 by the Consultative Committee for Thermometry (CCT) to the CIPM noted that their current definition of temperature has proved to be unsatisfactory for temperatures below 20 kelvins and for temperatures above 1300 kelvins. The committee was of the view that the [[Physics:Boltzmann constant|Boltzmann constant]] provided a better basis for temperature measurement than did the [[Chemistry:Triple point|triple point]] of water, as it overcame these difficulties.<ref>{{cite web
|url = http://www.bipm.org/wg/CCT/TG-SI/Allowed/Documents/Report_to_CIPM_2.pdf
|title = Report to the CIPM on the implications of changing the definition of the base unit kelvin
|first=J. |last=Fischer |date = 2 May 2007
|accessdate = 2011-01-02 |display-authors=0}}</ref>

At its 23rd meeting (2007), the CGPM mandated the CIPM to investigate the use of natural constants as the basis for all units of measure rather than the artefacts that were then in use. The following year this was endorsed by the [[Organization:International Union of Pure and Applied Physics|International Union of Pure and Applied Physics]] (IUPAP).<ref>{{cite web
|url = http://iupap.org/wp-content/uploads/2013/08/file_50095.pdf
|title = Resolution proposal submitted to the IUPAP Assembly by Commission C2 (SUNAMCO)
|publisher = International Union of Pure and Applied Physics
|year = 2008
|accessdate = 2015-09-06}}</ref> At a meeting of the CCU held in Reading, United Kingdom, in September 2010, a resolution<ref>{{cite web
|url = http://www.bipm.org/utils/en/pdf/24_CGPM_Convocation_Draft_Resolution_A.pdf
|title = On the possible future revision of the International System of Units, the SI
|first=Ian |last=Mills
|publisher = CCU
|date = 29 September 2010
|accessdate = 2011-01-01}}</ref> and draft changes to the SI brochure that were to be presented to the next meeting of the CIPM in October 2010 were agreed to in principle.<ref name="draft">{{cite web
|url = http://www.bipm.org/utils/en/pdf/si_brochure_draft_ch2.pdf
|title = Draft Chapter 2 for SI Brochure, following redefinitions of the base units
|first=Ian |last=Mills
|publisher = CCU
|date = 29 September 2010
|accessdate = 2011-01-01}}</ref> The CIPM meeting of October 2010 found that "the conditions set by the General Conference at its 23rd meeting have not yet been fully met.{{#tag:ref|In particular the CIPM was to prepare a detailed ''mise en pratique'' for each the new definitions of the kilogram, ampere, kelvin and mole set by the 23rd CGPM<ref>{{cite web
|url = http://www.bipm.org/en/CGPM/db/23/12/
|title = Resolution 12 of the 23rd meeting of the CGPM (2007)
| location = Sèvres, France
|publisher = [[General Conference on Weights and Measures]]
|accessdate = 2013-06-21}}</ref>|group = Note}} For this reason the CIPM does not propose a revision of the SI at the present time";<ref>{{cite web
|url = http://www.bipm.org/en/si/new_si/
|title = Towards the "new SI"
|publisher = [[Organization:International Bureau of Weights and Measures|International Bureau of Weights and Measures]] (BIPM)
|accessdate = 2011-02-20}}</ref> however, the CIPM presented a resolution for consideration at the 24th CGPM (17–21 October 2011) to agree to the new definitions in principle, but not to implement them until the details have been finalised.<ref>{{cite web
|url = http://www.bipm.org/utils/common/pdf/24_CGPM_Convocation_Draft_Resolution_A.pdf
|title = On the possible future revision of the International System of Units, the SI – Draft Resolution A
|publisher = [[Organization:International Committee for Weights and Measures|International Committee for Weights and Measures]] (CIPM)
|accessdate = 2011-07-14}}</ref> This resolution was accepted by the conference,<ref name=Resolution>{{Citation
| title = 24th meeting of the General Conference on Weights and Measures
| contribution = Resolution 1: On the possible future revision of the International System of Units, the SI
| contribution-url = http://www.bipm.org/utils/en/pdf/24_CGPM_Resolution_1.pdf
| publisher = International Bureau for Weights and Measures
| location = Sèvres, France
| date = 21 Oct 2011 
| mode = cs1}} It is not expected to be adopted until some prerequisite conditions are met, and in any case not before 2014. See {{cite journal |title=Possible changes to the international system of units
|journal=IUPAC Wire
|volume=34 |issue=1 |date=January–February 2012 |publisher=[[Organization:International Union of Pure and Applied Chemistry|International Union of Pure and Applied Chemistry]]}}
</ref> and in addition the CGPM moved the date of the 25th meeting forward from 2015 to 2014.<ref>{{cite press release
| url = http://www.bipm.org/utils/en/pdf/Press_release_resolution_1_CGPM.pdf
| title = General Conference on Weights and Measures approves possible changes to the International System of Units, including redefinition of the kilogram.
| publisher = [[General Conference on Weights and Measures]]
| location = Sèvres, France
| date = 23 October 2011
| accessdate = 2011-10-25}}</ref><ref name=Mohr>
{{cite web |title=Redefining the SI base units |first=Peter |last=Mohr |date=2 November 2011 |work=NIST Newsletter |url=https://www.nist.gov/pml/newsletter/siredef.cfm |publisher=NIST |accessdate=2012-03-01}}</ref> At the 25th meeting (18–20 November 2014), it was found that "despite [the progress in the necessary requirements] the data do not yet appear to be sufficiently robust for the CGPM to adopt the revised SI at its 25th meeting",<ref>{{cite web
|title = Resolutions adopted by the CGPM at its 25th meeting (18–20 November 2014)
| url = http://www.bipm.org/utils/common/pdf/CGPM-2014/25th-CGPM-Resolutions.pdf
| publisher = International Bureau for Weights and Measures
|location = Sèvres, France
|date=21 November 2014}}</ref> thus postponing the revision to the next meeting in 2018.  A revised Draft Resolution A for consideration at the 26th meeting of the CGPM is available.<ref name=draft-resolution-A/>

==Proposal==
{{hatnote|The numerical values given in this section are the values proposed by the CIPM{{r|cipm_106|p=23}} in its Draft Resolution A,<ref name=draft-resolution-A>
{{citation
 |title=Draft Resolution A "On the revision of the International System of units (SI)" to be submitted to the CGPM at its 26th meeting (2018)
 |url=https://www.bipm.org/utils/en/pdf/CGPM/Draft-Resolution-A-EN.pdf
}}</ref> which correspond to the published CODATA 2017 values.<ref name=codata_2017>
{{cite journal
 |title=The CODATA 2017 Values of ''h'', ''e'', ''k'', and ''N''<sub>A</sub> for the Revision of the SI
 |first1=David B. |last1=Newell  |first2=F. |last2=Cabiati  |first3=J. |last3=Fischer
 |first4=K. |last4=Fujii  |first5=S. G. |last5=Karshenboim  |first6=H. S. |last6=Margolis
 |first7=E. |last7=de Mirandés  |first8=P. J. |last8=Mohr  |first9=F. |last9=Nez
 |first10=K. |last10=Pachucki  |first11=T. J. |last11=Quinn  |first12=B. N. |last12=Taylor
 |first13=M. |last13=Wang  |first14=B. M. |last14=Wood  |first15=Z. |last15=Zhang
 |collaboration=Committee on Data for Science and Technology (CODATA) Task Group on Fundamental Constants (TGFC)
 |url=http://iopscience.iop.org/article/10.1088/1681-7575/aa950a/pdf
 |doi=10.1088/1681-7575/aa950a |doi-access=free
 |publisher=[[Organization:Institute of Physics|Institute of Physics]]
 |journal=Metrologia (in press)
 |date=20 October 2017|bibcode=2018Metro..55L..13N}}</ref>}}
Following a recommendation from its Consultative Committee for Units (CCU), the BIPM has proposed that, in addition to the speed of light, four further constants of nature should be defined to have exact values.  Using the values recommended for standardization in the CODATA 2017 adjustment,{{r|codata_2017}} these would be:
:* The [[Physics:Planck constant|Planck constant]] '''''h''''' is exactly {{val|6.62607015|e=-34|u=joule-second (J⋅s)}}.
:* The [[Physics:Elementary charge|elementary charge]] '''''e''''' is exactly {{val|1.602176634|e=-19|u=coulomb (C)}}.
:* The [[Physics:Boltzmann constant|Boltzmann constant]] '''''k''''' is exactly {{val|1.380649|e=-23|u=joule per kelvin (J⋅K<sup>−1</sup>)}}.
:* The [[Physics:Avogadro constant|Avogadro constant]] '''''N''<sub>A</sub>''' is exactly {{val|6.02214076|e=23|u=reciprocal mole (mol<sup>−1</sup>)}}.
These constants were described in the 2006 version of the SI manual, but in that version the latter three were defined as "constants to be obtained by experiment" rather than as "defining constants".

The CCU also proposed that the numerical values associated with the following constants of nature be retained unchanged:
:* The [[Physics:Speed of light|speed of light]] '''''c''''' is exactly  {{val|299792458|u=metres per second (m⋅s<sup>−1</sup>)}}.
:* The ground state hyperfine splitting [[Physics:Frequency|frequency]] of the [[Chemistry:Caesium|caesium]]-133 atom '''Δ''ν''(<sup>133</sup>Cs)<sub>hfs</sub>''' is exactly {{val|9192631770|u=hertz (Hz)}}.
:* The [[Physics:Luminous efficacy|luminous efficacy]] '''''K''<sub>cd</sub>''' of monochromatic radiation of frequency {{val|540|e=12|u=Hz}} is exactly {{val|683|u=lumens per watt (lm⋅W<sup>−1</sup>)}}.

The seven definitions above are rewritten below after converting the [[SI derived unit|derived unit]]s ([[Joule|joule]], [[Coulomb|coulomb]], [[Hertz|hertz]], [[Lumen (unit)|lumen]] and [[Watt|watt]]) into the seven [[SI base unit|base unit]]s (second, metre, kilogram, ampere, kelvin, mole and candela), according to the updated draft of the 9th edition of the SI Brochure (2016).<ref name=Brochure9_2016>
{{cite web
 |title=Draft of the ninth SI Brochure
 |publisher=BIPM
 |url=http://www.bipm.org/utils/common/pdf/si-brochure-draft-2016b.pdf
 |pages=2–9
 |date=10 November 2016
 |accessdate=2017-01-12
}}</ref>  In the list that follows, the symbol sr stands for the dimensionless unit [[Steradian|steradian]].

:* Δ''ν''<sub>Cs</sub> = Δ''ν''(<sup>133</sup>Cs)<sub>hfs</sub> = {{val|9192631770|u=s<sup>−1</sup>}}
:* ''c'' = {{val|299792458|u=m⋅s<sup>−1</sup>}}
:* ''h'' = {{val|6.62607015|e=-34|u=kg⋅m<sup>2</sup>⋅s<sup>−1</sup>|s=<ref group=Note name=DraftNote>These are the final values proposed for standardization, but have not been formally accepted yet.</ref>}}
:* ''e'' = {{val|1.602176634|e=-19|u=A⋅s|s=<ref group=Note name=DraftNote/>}}
:* ''k'' = {{val|1.380649|e=-23|u=kg⋅m<sup>2</sup>⋅K<sup>−1</sup>⋅s<sup>−2</sup>|s=<ref group=Note name=DraftNote/>}}
:* ''N''<sub>A</sub> = {{val|6.02214076|e=23|u=mol<sup>−1</sup>|s=<ref group=Note name=DraftNote/>}}
:* ''K''<sub>cd</sub> = {{val|683|u=cd⋅sr⋅s<sup>3</sup>⋅kg<sup>−1</sup>⋅m<sup>−2</sup>}}

In addition the CIPM proposes that
:* The international prototype kilogram be retired and that the current definition of the kilogram be abrogated,
:* The current definition of the [[Ampere|ampere]] be abrogated,
:* The current definition of the [[Kelvin|kelvin]] be abrogated and
:* The current definition of the [[Mole (unit)|mole]] be revised.

These changes will have the effect of redefining the SI base units, though the definitions of the derived SI units in terms of the base units will remain the same.

==Impact on base unit definitions==
The CCU proposal recommended that the text of the definitions of all the base units be either refined or rewritten changing the emphasis from explicit-unit to explicit-constant type definitions.<ref name=Explicit>{{cite journal
|url = http://www.iupac.org/publications/ci/2011/3305/4_mills.html
|journal = Chemistry International
|volume = 33
|number = 5
|date = September–October 2011
|title = Part II – Explicit-Constant Definitions for the Kilogram and for the Mole
|first1 = Ian
|last1 = Mills
|issn = 0193-6484
|pages = 12–15}}</ref> Explicit-unit type definitions define a unit in terms of a specific example of that unit – for example in 1324 Edward II defined the [[Inch|inch]] as being the length of three [[Barleycorn (unit)|barleycorn]]s<ref name=Smoot>{{cite book
|title = Smoot's Ear – The Measure of Humanity
|first1 = Robert
|last1 = Travenor
|year = 2007
|isbn = 978-0-300-14334-8
|pages = 35–36
|publisher = Yale University Press}}</ref> and since 1889 the [[Kilogram|kilogram]] has been defined as being the mass of the International Prototype Kilogram. In explicit-constant definitions, a constant of nature is given a specified value and the definition of the unit emerges as a consequence. For example, in 1983, the [[Physics:Speed of light|speed of light]] was defined to be exactly {{val|299792458}} metres per second and, since the second had been independently defined, the length of the metre could thus be derived.

The current{{r|BaseDefs}} ({{as of|2018||lc=y}}) and proposed{{r|Brochure9_2016|codata_2017}} (expected 2019) definitions are given below.

===Second===
The proposed definition of the [[Second|second]] is effectively the same as the current definition, the only difference being that the conditions under which the definition applies are more rigorously defined.
:'''Current definition:''' The second is the duration of {{val|9192631770}} periods of the radiation corresponding to the transition between the two [[Physics:Hyperfine structure|hyperfine level]]s of the [[Physics:Ground state|ground state]] of the [[Physics:Caesium-133|caesium-133]] atom. 
:'''Proposed definition:''' The second, symbol s, is the SI unit of time. It is defined by taking the fixed numerical value of the caesium frequency Δ''ν''<sub>Cs</sub>, the unperturbed ground-state hyperfine transition frequency of the caesium 133 atom, to be {{val|9192631770}} when expressed in the unit Hz, which is equal to s<sup>−1</sup>.

===Metre===
The proposed definition of the [[Metre|metre]] is effectively the same as the current definition, the only difference being that the additional rigour in the definition of the second will propagate to the metre.
:'''Current definition:''' The metre is the length of the path travelled by light in vacuum during a time interval of {{sfrac|{{val|299792458}}}} of a second.
:'''Proposed definition:''' The metre, symbol m, is the SI unit of length. It is defined by taking the fixed numerical value of the speed of light in vacuum ''c'' to be {{val|299792458}} when expressed in the unit m⋅s<sup>−1</sup>, where the second is defined in terms of the caesium frequency Δ''ν''<sub>Cs</sub>.

===Kilogram===
[[File:Watt balance, large view.jpg|thumb|A Kibble balance, which is being used to measure the [[Physics:Planck constant|Planck constant]] in terms of the international prototype kilogram.<ref name=BIPMwatt>{{cite web
|url = http://www.bipm.org/en/scientific/elec/watt_balance/
|title = The BIPM watt balance
|publisher = International Bureau of Weights and Measures
|accessdate = 2013-03-28
|year = 2012}}</ref>]]
The definition of the [[Kilogram|kilogram]] is due to change fundamentally – the current definition defines the kilogram as being the mass of the international prototype kilogram, which is an artefact and not a constant of nature,<ref name = Barry>{{cite journal
|title = The Current SI Seen From the Perspective of the Proposed New SI
|first1 = Barry N
|last1 = Taylor
|journal = Journal of Research of the National Institute of Standards and Technology
|publisher = [[Organization:National Institute of Standards and Technology|National Institute of Standards and Technology]] (NIST)
|number = 6
|volume = 116
|date = November–December 2011
|pages = 797–80.
|doi=10.6028/jres.116.022
}}</ref> whereas the new definition relates it to the [[Mass–energy equivalence|equivalent mass]] of the energy of a [[Physics:Photon|photon]] given its frequency, via the Planck constant.
:'''Current definition:''' The kilogram is the unit of mass; it is equal to the mass of the international prototype of the kilogram.
:'''Proposed definition:''' The kilogram, symbol kg, is the SI unit of mass. It is defined by taking the fixed numerical value of the [[Physics:Planck constant|Planck constant]] ''h'' to be {{val|6.62607015|e=-34}} when expressed in the unit J⋅s, which is equal to kg⋅m<sup>2</sup>⋅s<sup>−1</sup>, where the metre and the second are defined in terms of ''c'' and Δ''ν''<sub>Cs</sub>.
 
A consequence of this change is that the new definition of the kilogram is dependent on the definitions of the second and the metre.

===Ampere===
The definition of the [[Ampere|ampere]] is due to undergo a major revision – the current definition, which is difficult to realise with high precision in practice, will be replaced by a definition that is more intuitive and easier to realise.
:'''Current definition:''' The ampere is that constant [[Physics:Electric current|current]] which, if maintained in two straight parallel conductors of infinite length, of negligible circular cross-section, and placed 1&nbsp;m apart in vacuum, would produce between these conductors a force equal to {{val|2|e=-7}} newton per metre of length.
:'''Proposed definition:''' The ampere, symbol A, is the SI unit of electric current. It is defined by taking the fixed numerical value of the [[Physics:Elementary charge|elementary charge]] ''e'' to be {{val|1.602176634|e=-19}} when expressed in the unit [[Coulomb|C]], which is equal to A⋅s, where the second is defined in terms of Δ''ν''<sub>Cs</sub>.

Since the current definition contains a reference to [[Physics:Force|force]], which has the [[Dimensional analysis|dimension]]s MLT<sup>−2</sup>, it follows that in SI the kilogram, metre and second, the base units representing these dimensions, must be defined before the ampere can be defined.  Other consequences of the current definition are that in SI the value of [[Physics:Vacuum permeability|vacuum permeability]] (''μ''<sub>0</sub>) is fixed at exactly {{val|4|end=''π''|e=-7|u=H.m-1}}.<ref>{{cite web
|url=http://physics.nist.gov/cuu/Units/ampere.html
|title=Unit of electric current (ampere)
|accessdate=2015-09-07
|work=Historical context of the SI
|publisher=NIST }}</ref> Since the [[Physics:Speed of light|speed of light]] in vacuum (''c'') is also fixed, it follows from the relationship
:<math>c^2 = \frac{1}{\mu_0\varepsilon_0} </math>
that the [[Physics:Vacuum permittivity|vacuum permittivity]] (''ε''<sub>0</sub>) has a fixed value, and from
:<math>Z_0 = \sqrt{\frac{\mu_0}{\varepsilon_0}} ,</math>
that the [[Physics:Impedance of free space|impedance of free space]] (''Z''<sub>0</sub>) likewise has a fixed value.<ref>{{cite book
|url = http://www.ece.rutgers.edu/~orfanidi/ewa/ch01.pdf
|at = 1.3 Constitutive Relations
|title = Electromagnetic Waves and Antennas
|first = Sophocles J.
|last = Orfanidis
|publisher = ECE Department, [[Organization:Rutgers University|Rutgers University]]
|accessdate = 2013-06-24
|date = 31 August 2010}}</ref>

A consequence of the proposed changes to the definition of the ampere is that the definition will no longer depend on the definitions of the kilogram and the metre, but will still depend on the definition of the second.  In addition, the numerical values of the [[Physics:Vacuum permeability|vacuum permeability]], [[Physics:Vacuum permittivity|vacuum permittivity]] and [[Physics:Impedance of free space|impedance of free space]], which, in the current definition are exact, will be subject to experimental error.<ref name=Chyla/>

===Kelvin===
The definition of the [[Kelvin|kelvin]] is due to undergo a fundamental change. Rather than using the triple point of water to fix the temperature scale, the proposal recommends that the energy equivalent as given by Boltzmann's equation be used.
:'''Current definition:''' The kelvin, unit of [[Physics:Thermodynamic temperature|thermodynamic temperature]], is {{sfrac|273.16}} of the thermodynamic temperature of the [[Chemistry:Triple point|triple point]] of [[Chemistry:Water|water]].
:'''Proposed definition:''' The kelvin, symbol K, is the SI unit of thermodynamic temperature. It is defined by taking the fixed numerical value of the [[Physics:Boltzmann constant|Boltzmann constant]] ''k'' to be {{val|1.380649|e=-23}} when expressed in the unit J⋅K<sup>−1</sup>, which is equal to kg⋅m<sup>2</sup>⋅s<sup>−2</sup>⋅K<sup>−1</sup>, where the kilogram, metre and second are defined in terms of ''h'', ''c'' and Δ''ν''<sub>Cs</sub>.

One consequence of this change is that the new definition makes the definition of the kelvin depend on the definitions of the second, the metre, and the kilogram.

===Mole===
[[File:Silicon sphere for Avogadro project.jpg|thumb|upright|A near-perfect sphere of ultra-pure silicon – part of the Avogadro project, an International Avogadro Coordination project to determine the Avogadro number<ref name=BIPMwatt/>]]
The current definition of the [[Mole (unit)|mole]] links it to the kilogram. The proposed definition will break that link by making a mole a specific number of entities of the substance in question.
:'''Current definition:''' The mole is the [[Physics:Amount of substance|amount of substance]] of a system that contains as many elementary entities as there are atoms in 0.012 kilogram of [[Physics:Carbon-12|carbon-12]]. When the mole is used, the [[Physics:Elementary particle|elementary entities]] must be specified and may be [[Physics:Atom|atom]]s, [[Physics:Molecule|molecule]]s, [[Physics:Ion|ion]]s, [[Physics:Electron|electron]]s, other particles, or specified groups of such particles.
:'''Proposed definition:'''{{r|cipm_106|p=22}} The mole, symbol mol, is the SI unit of amount of substance. One mole contains exactly {{val|6.02214076|e=23}} elementary entities. This number is the fixed numerical value of the [[Physics:Avogadro constant|Avogadro constant]], ''N''<sub>A</sub>, when expressed in the unit mol<sup>−1</sup> and is called the Avogadro number.
:The amount of substance, symbol ''n'', of a system is a measure of the number of specified elementary entities. An elementary entity may be an atom, a molecule, an ion, an electron, any other particle or specified group of particles.

One consequence of this change is that the current defined relationship between the mass of the <sup>12</sup>C atom, the dalton, the kilogram, and the Avogadro number will no longer be valid. One of the following must change:
* The mass of a <sup>12</sup>C atom is exactly 12 dalton.
* The number of dalton in a gram is exactly the numerical value of the Avogadro number.
The wording of the Draft of the ninth SI Brochure implies the first, which would mean that the second will no longer be true. The [[Physics:Molar mass constant|molar mass constant]], while still with great accuracy remaining equal to 1 g/mol, will no longer be exactly equal to that.

===Candela===
The proposed definition of the [[Candela|candela]] is effectively the same as the current definition, with the only difference being that the additional rigour in the definition of the second and metre will propagate to the candela.
:'''Current definition:''' The candela is the [[Physics:Luminous intensity|luminous intensity]], in a given direction, of a source that emits monochromatic radiation of frequency {{val|540|e=12|u=Hz}} and that has a radiant intensity in that direction of {{sfrac|683}} watt per [[Steradian|steradian]].
:'''Proposed definition:''' The candela, symbol cd, is the SI unit of luminous intensity in a given direction. It is defined by taking the fixed numerical value of the [[Physics:Luminous efficacy|luminous efficacy]] of monochromatic radiation of frequency {{val|540|e=12|u=Hz}}, ''K''<sub>cd</sub>, to be 683 when expressed in the unit lm⋅W<sup>−1</sup>, which is equal to cd⋅sr⋅W<sup>−1</sup>, or cd⋅sr⋅kg<sup>−1</sup>⋅m<sup>−2</sup>⋅s<sup>3</sup>, where the kilogram, metre and second are defined in terms of ''h'', ''c'' and Δ''ν''<sub>Cs</sub>.

==Impact on reproducibility==
Apart from the candela,<ref group="Note" name="CandelaNote">Translating physical measurements of spectral intensity into units of candela also requires a model of the response of the human eye to different wavelengths of light known as the [[Physics:Luminosity function|luminosity function]] and denoted by ''V''(''λ''), a function that is determined by the International Commission on Illumination (CIE).</ref><ref>{{cite book
|url = http://www.bipm.org/utils/en/pdf/Monographie1983-1.pdf
|title = Principles covering Photometry
|publisher = Conférence général des poids et mesures (CGPM)
|location = Sevres
|first1 = G
|last1 = Wyszecki
|first2 = WR
|last2 = Blevin
|first3 = KG
|last3 = Kessler
|first4 = KD
|last4 = Mielenz
|year = 1983}}</ref> all the base units will be defined in terms of universal physical constants, but without a direct [[Bijection|one-to-one correspondence]] between the constants and the base units. Thus six physical constants will be needed to define the six base units.

When the New SI was first designed, there were more than six suitable physical constants from which the designers could choose. For example, once length and time had been established, the [[Physics:Gravitational constant|universal gravitational constant]] ''G'' could, from a dimensional point of view, be used to define mass.<ref group="Note">The dimensions of ''G'' are L<sup>3</sup>M<sup>−1</sup>T<sup>−2</sup>, so once standards have been established for length and for time, mass can in theory be deduced from ''G''. Also, when fundamental constants as relations between these three units are set, the units can be deduced by a combination of these constants, for example as a linear combination of [[Planck units]].</ref>  It should be noted that in practice ''G'' can only be measured with a [[Measurement uncertainty|relative uncertainty]] of the order of 10<sup>−5</sup>,<ref group = "Note" name="VIM">The following terms are defined in [http://www.bipm.org/utils/common/documents/jcgm/JCGM_200_2012.pdf ''International vocabulary of metrology – Basic and general concepts and associated terms'']:
*measurement reproducibility – definition 2.25
*standard measurement uncertainty – definition 2.30
*relative standard measurement uncertainty – definition 2.32</ref> which would have resulted in upper limit of the kilogram's [[Reproducibility|reproducibility]] being around 10<sup>−5</sup> whereas the current international prototype kilogram can be measured with a reproducibility of 1.2&nbsp;×&nbsp;10<sup>−8</sup>.<ref name=Chyla>{{cite journal
|url = http://przyrbwn.icm.edu.pl/APP/PDF/120/a120z6p04.pdf
|title = Evolution of the International Metric System of Units SI
|first1 = W.T.
|last1 = Chyla
|date = December 2011
|accessdate = 2013-06-22
|journal = Acta Physica Polonica A
|number = 6
|volume = 120
|pages = 998–1011}}</ref> The choice of physical constants was made on the basis of minimal uncertainty associated with measuring the constant and the degree of independence of the constant in respect of other constants that were being used. Although the BIPM has developed a standard ''mise en pratique'' (practical technique)<ref>{{cite web
|url = http://www.bipm.org/en/measurement-units/new-si/mise-en-pratique.html
|title = What is a ''mise en pratique''?
|publisher = BIPM
|year = 2011
|quote = is a set of instructions that allows the definition to be realized in practice at the highest level.
|accessdate = 2015-09-06}}</ref> for each type of measurement, the ''mise en pratique'' used to make the measurement is not part of the measurement's definition – it is merely an assurance that the measurement can be done without exceeding the specified maximum uncertainty.

===Uncertainty of fundamental physical constants===
Fundamental physical constants are often highly dependent upon each other. This implies that the best value of a fundamental physical constant, one with the least uncertainty, often can be determined by directly measuring other fundamental physical constants, from which the value can be calculated. The uncertainty in these constants is then determined from the uncertainty of the others by the [[Propagation of uncertainty|propagation of uncertainty]]. Constants whose value is fixed, for determining the units in which they are expressed, don't have an uncertainty associated with them, so they do not account for any extra uncertainty in the value of the calculated constant. One of the reasons the SI unit system will be changed is that determination of values can often be greatly improved if expressed in these new units. This is due to the dependence of these values on physical constants.

The following table catalogues the notable changes in determination of fundamental physical constants. The constants are expressed in direct measurements and fixed constants to minimize and determine the uncertainty. Some constants in that expression do not contribute significantly to the uncertainty; only the significant factors are noted. The value of the relative uncertainty by the data of CODATA of 2014 is given, and is expressed in the relative uncertainty of the significant factors, noted with ''u''<sub>r</sub>(''constant''). An approximately equals sign (≈) is used if an uncertainty is only approximated by the expression. This is due to unsignificant factors or rounding errors.

<div style="overflow:auto">
{| class="wikitable"
|-
!rowspan="2"| Constant !!rowspan="2"| Symbol !!colspan="3"| Current definition  !!colspan="3"| Proposed definition
|-
! Relation to directly measured and fixed constants !! Significant factor(s) in uncertainty !! Relative uncertainty !! Relation to directly measured and fixed constants !! Significant factor(s) in uncertainty !! Relative uncertainty
|-
| Mass of IPK<ref group="Note">Technically, the mass of International Prototype Kilogram would no longer be a "fundamental physical constant" when the artefact is abandoned in the new SI.</ref> || <math>m(\mathcal{K})</math> || 1&nbsp;kg || none || exact || <math>m(\mathcal{K})</math> || <math>m(\mathcal{K})</math> || <math>1.2 \times 10^{-8} = u_\text{r}(m(\mathcal{K}))</math>
|-
| [[Physics:Planck constant|Planck constant]] || <math>h</math> || <math>\frac{8 \alpha}{c \mu_0 K_\text{J}^2}</math> || <math>K_\text{J}^2</math> || <math>1.2 \times 10^{-8} \approx 2 u_\text{r}(K_\text{J})</math> || {{val|6.62607015|e=-34}}<br/>&emsp;kg⋅m<sup>2</sup>⋅s<sup>−1</sup> || none || exact
|-
| Josephson constant || <math>K_\text{J}</math> || <math>K_\text{J}</math> || <math>K_\text{J}</math> || <math>6.1 \times 10^{-9} = u_\text{r}(K_\text{J})</math> || <math>\frac{2 e}{h}</math> || none || exact
|-
| Von Klitzing constant || <math>R_\text{K}</math> || <math>\frac{c \mu_0}{2 \alpha}</math> || <math>\alpha</math> || <math>2.3 \times 10^{-10} = u_\text{r}(\alpha)</math> || <math>\frac{h}{e^2}</math> || none || exact
|-
| [[Physics:Elementary charge|Elementary charge]] || <math>e</math> || <math>\frac{4 \alpha}{c \mu_0 K_\text{J}}</math> || <math>K_\text{J}</math> || <math>6.1 \times 10^{-9} \approx u_\text{r}(K_\text{J})</math> || {{val|1.602176634|e=-19}}<br/>&emsp;A⋅s || none || exact
|-
| Magnetic constant || <math>\mu_0</math> || {{val|4|end=''π''|e=-7}} m⋅kg⋅s<sup>−2</sup>⋅A<sup>−2</sup> || none || exact || <math>\frac{2 h \alpha}{c e^2}</math> || <math>\alpha</math> || <math>2.3 \times 10^{-10} = u_\text{r}(\alpha)</math>
|-
| [[Physics:Vacuum permittivity|Vacuum permittivity]] || <math>\varepsilon_0</math> || <math>\frac{1}{c^2 \mu_0}</math> || none || exact || <math>\frac{e^2}{2 h c \alpha}</math> || <math>\alpha</math> || <math>2.3 \times 10^{-10} = u_\text{r}(\alpha)</math>
|-
| [[Physics:Impedance of free space|Impedance of free space]] || <math>Z_0</math> || <math>c \mu_0</math> || none || exact || <math>\frac{2 h \alpha}{e^2}</math> || <math>\alpha</math> || <math>2.3 \times 10^{-10} = u_\text{r}(\alpha)</math>
|-
| [[Physics:Electron mass|Electron mass]] || <math>m_\text{e}</math> || <math>\frac{16 R_{\infty}}{c^2 \alpha \mu_0 K_\text{J}^2}</math> || <math>K_\text{J}^2</math> || <math>1.2 \times 10^{-8} \approx 2 u_\text{r}(K_\text{J})</math> || <math>\frac{2 h R_{\infty}}{c \alpha^2}</math> || <math>\alpha^2</math> || <math>4.7 \times 10^{-10} \approx 2 u_\text{r}(\alpha)</math>
|-
| Electron molar mass || <math>M(\text{e})</math> || <math>A_\text{r}(\text{e}) M_\text{u}</math> || <math>A_\text{r}(\text{e})</math> || <math>2.9 \times 10^{-11} = u_\text{r}(A_\text{r}(\text{e}))</math> || <math>\frac{2 h R_{\infty} N_\text{A}}{c \alpha^2}</math> || <math>\alpha^2</math> || <math>4.7 \times 10^{-10} \approx 2 u_\text{r}(\alpha)</math>
|-
| [[Physics:Unified atomic mass unit|Unified atomic mass unit]] or dalton || <math>\begin{align}m_\text{u} & = 1 \text{ u} \\ & = 1 \text{ Da}\end{align}</math> || <math>\frac{16 R_{\infty}}{c^2 \alpha \mu_0 K_\text{J}^2 A_\text{r}(\text{e})}</math> || <math>K_\text{J}^2</math> || <math>1.2 \times 10^{-8} \approx 2 u_\text{r}(K_\text{J})</math>
|| <math>\frac{2 h R_{\infty}}{c \alpha^2 A_\text{r}(\text{e})}</math> || <math>\alpha^2</math> || <math>4.7 \times 10^{-10} \approx 2 u_\text{r}(\alpha)</math>
|-
| [[Physics:Molar mass constant|Molar mass constant]] || <math>M_\text{u}</math> || 0.001&nbsp;kg⋅mol<sup>−1</sup> || none || exact
|| <math>\frac{2 h R_{\infty} N_\text{A}}{c \alpha^2 A_\text{r}(\text{e})}</math> || <math>\alpha^2</math> || <math>4.7 \times 10^{-10} \approx 2 u_\text{r}(\alpha)</math>
|-
| [[Physics:Avogadro constant|Avogadro constant]] || <math>N_\text{A}</math> || <math>\frac{c^2 \alpha \mu_0 K_\text{J}^2 A_\text{r}(\text{e}) M_\text{u}}{16 R_{\infty}}</math> || <math>K_\text{J}^2</math> || <math>1.2 \times 10^{-8} \approx 2 u_\text{r}(K_\text{J})</math> || {{val|6.02214076|e=23}}<br/>&emsp;mol<sup>−1</sup> || none || exact
|-
| Atomic mass of carbon-12 || <math>m(^{12}\text{C})</math> || <math>\frac{192 R_{\infty}}{c^2 \alpha \mu_0 K_\text{J}^2 A_\text{r}(\text{e})}</math> || <math>K_\text{J}^2</math> || <math>1.2 \times 10^{-8} \approx 2 u_\text{r}(K_\text{J})</math> || <math>\frac{24 h R_{\infty}}{c \alpha^2 A_\text{r}(\text{e})}</math> || <math>\alpha^2</math> || <math>4.7 \times 10^{-10} \approx 2 u_\text{r}(\alpha)</math>
|-
| Molar mass of carbon-12 || <math>M(^{12}\text{C})</math> || 0.012&nbsp;kg⋅mol<sup>−1</sup> || none || exact || <math>\frac{24 h R_{\infty} N_\text{A}}{c \alpha^2 A_\text{r}(\text{e})}</math> || <math>\alpha^2</math> || <math>4.7 \times 10^{-10} \approx 2 u_\text{r}(\alpha)</math>
|-
| [[Physics:Faraday constant|Faraday constant]] || <math>F</math> || <math>\frac{c \alpha^2 K_\text{J} A_\text{r}(\text{e}) M_\text{u}}{4 R_{\infty}}</math> || <math>K_\text{J}, \alpha^2</math> || <math>6.2 \times 10^{-9} \approx u_\text{r}(K_\text{J})</math><ref group="Note">Although the calculation of the uncertainty implies that the fine structure constant isn't a significant factor, because of rounding errors, the uncertainty in fine structure constant does have an effect on the determined value.</ref> || <math>e N_\text{A}</math> || none || exact
|-
| Temperature of triple point of water || <math>T_\text{TPW}</math> || 273.16 K || none || exact || <math>T_\text{TPW}</math> || <math>T_\text{TPW}</math> || <math>5.7 \times 10^{-7} = u_\text{r}(T_\text{TPW})</math>
|-
| [[Physics:Gas constant|Molar gas constant]] || <math>R</math> || <math>R</math> || <math>R</math> || <math>5.7 \times 10^{-7} = u_\text{r}(R)</math> || <math>k N_\text{A}</math> || none || exact
|-
| [[Physics:Boltzmann constant|Boltzmann constant]] || <math>k</math> || <math>\frac{16 R R_{\infty}}{c^2 \alpha \mu_0 K_\text{J}^2 A_\text{r}(\text{e}) M_\text{u}}</math> || <math>R</math> || <math>5.7 \times 10^{-7} \approx u_\text{r}(R)</math> || {{val|1.380649|e=-23}}<br/>&emsp;kg⋅m<sup>2</sup>⋅K<sup>−1</sup>⋅s<sup>−2</sup> || none || exact
|-
| [[Physics:Stefan–Boltzmann constant|Stefan–Boltzmann constant]] || <math>\sigma</math> || <math>\frac{256 \pi^5 R^4 R_{\infty}^4}{15 c^7 \alpha^7 \mu_0 K_\text{J}^2 A_\text{r}(\text{e})^4 M_\text{u}^4}</math> || <math>R^4</math> || <math>2.3 \times 10^{-6} \approx 4 u_\text{r}(R)</math> || <math>\frac{2 \pi^5 k^4}{15 h^3 c^2}</math> || none || exact
|}
</div>

(<math>c</math> = [[Physics:Speed of light|speed of light]], <math>\alpha</math> = [[Physics:Fine-structure constant|fine-structure constant]], <math>R_\infty</math> = [[Physics:Rydberg constant|Rydberg constant]].)

It should be noted that the relative atomic mass of the electron ''A''<sub>r</sub>(e) is measured relative to the mass of a carbon-12 atom (divided by 12). When the Avogadro constant is set in the new SI, atomic masses might be measured in dalton (by fixing the Avogadro constant), instead of atomic mass units (by fixing the mass of carbon-12), thus resulting in a difference between the values of the relative atomic mass and the atomic mass in units of dalton.{{citation needed|reason=This should to be reworded, since it is evident from the Ninth SI Brochure draft that the units Da and u will be defined identically as 1/12 of the mass of a carbon-12 atom.|date=May 2018}}

===Dalton===
In 1993, the [[Organization:International Union of Pure and Applied Chemistry|International Union of Pure and Applied Chemistry]] (IUPAC) approved the use of the [[Dalton (unit)|dalton]] as an alternative to the [[Physics:Unified atomic mass unit|unified atomic mass unit]] with the qualification that the CGPM had not given its approval.<ref>{{cite book
|title=Quantities, Units and Symbols in Physical Chemistry International Union of Pure and Applied Chemistry; Physical Chemistry Division
|publisher=[[Organization:International Union of Pure and Applied Chemistry|International Union of Pure and Applied Chemistry]], Blackwell Science Ltd
|edition=2nd
|year=1993
|first=Ian|last=Mills
|first2=Tomislav|last2= Cvitaš
|first3=Klaus|last3=Homann
|first4= Nikola|last4= Kallay
|first5= Kozo |last5=Kuchitsu
|ISBN=0-632-03583-8}}</ref> This approval has since been given.<ref>{{SIBrochure8th|pages = 114, 115}}</ref> Following the proposal to redefine the mole by fixing the value of the Avogadro constant, Brian Leonard of the [[Organization:University of Akron|University of Akron]], writing in ''[[Metrologia]]'' proposed that the dalton (Da) be redefined such that ''N''<sub>A</sub> = (g/Da)&nbsp;mol{{sup|−1}}, but that the unified atomic mass unit (''m''<sub>u</sub>) retain its current definition based on the mass of <sup>12</sup>C, ceasing to exactly equal to the dalton.  This would result in the dalton and the atomic mass unit potentially differing from each other with a relative uncertainty of the order of 10<sup>−10</sup>.<ref>{{cite journal
|url = https://www.researchgate.net/profile/Brian_Leonard4/publication/231073122_Why_the_dalton_should_be_redefined_exactly_in_terms_of_the_kilogram/links/56c48b6608aea564e304ba50.pdf
|title = Why the dalton should be redefined exactly in terms of the kilogram
|first = Brian Phillip |last = Leonard
|date = May 2012
|journal = Metrologia |volume = 49 |issue = 4 |pages = 487–491
|doi = 10.1088/0026-1394/49/4/487|bibcode = 2012Metro..49..487L }}</ref>

==Acceptance==
Much of the work done by the CIPM is delegated to consultative committees. The CIPM Consultative Committee for Units (CCU) has made the proposed changes while other committees have examined the proposal in detail and have made recommendations regarding their acceptance by the CGPM in 2014. The various consultative committees have laid down a number of criteria that must be met before they will support the CCU's proposal, including:
* For the redefinition of the kilogram, at least three separate experiments be carried out yielding values for the Planck constant having a relative expanded (95%) [[Measurement uncertainty|uncertainty]] of no more than {{val|5|e=-8}} and at least one of these values should be better than {{val|2|e=-8}}.  Both the [[Engineering:Kibble balance|Kibble balance]] and the [[Physics:Avogadro constant#International Avogadro Coordination|Avogadro project]] should be included in the experiments and any differences between these be reconciled.<ref>{{cite web
|url = http://www.bipm.org/utils/common/pdf/CCM12.pdf#page=23
|title = Recommendations of the Consultative Committee for Mass and Related Quantities to the International Committee for Weights and Measures.
|work = 12th Meeting of the CCM
|date = 26 March 2010
|publisher = Bureau International des Poids et Mesures
|location = Sèvres
|accessdate = 2012-06-27}}</ref><ref>{{cite web
|url = http://www.bipm.org/utils/common/pdf/CCQM16.pdf#page=40
|title = Recommendations of the Consultative Committee for Amount of Substance: Metrology in Chemistry to the International Committee for Weights and Measures.
|work = 16th Meeting of the CCQM
|date = 15–16 April 2010
|publisher = Bureau International des Poids et Mesures
|location = Sèvres
|accessdate = 2012-06-27}}</ref>
* For the redefinition of the kelvin, the relative uncertainty of Boltzmann constant derived from two fundamentally different methods such as acoustic gas thermometry and dielectric constant gas thermometry be better than one part in 10<sup>−6</sup> and that these values be corroborated by other measurements.<ref>{{cite web
|url = http://www.bipm.org/utils/common/pdf/CCT25.pdf#page=53
|title = Recommendations of the Consultative Committee for Thermometry to the International Committee for Weights and Measures.
|work = 25th Meeting of the Consultative Committee for Thermometry
|date = 6–7 May 2010
|publisher = Bureau International des Poids et Mesures
|location = Sèvres
|accessdate = 2012-06-27}}</ref>

As at March 2011, the International Avogadro Coordination (IAC) group had obtained an uncertainty of {{val|3.0|e=-8}} and [[Organization:National Institute of Standards and Technology|NIST]] had obtained an uncertainty of {{val|3.6|e=-8}} in their measurements.<ref name=Crease/><!--Is this standard (1 sigma) or expanded (2 sigma) uncertainty?-->

On 1 September 2012 the European Association of National Metrology Institutes (EURAMET) launched a formal project to reduce the relative difference between the Kibble balance and the silicon sphere approach to measuring the kilogram from {{val|17|5|e=-8}} to within {{val|2|e=-8}}.<ref>{{cite web
|url = http://www.inrim.it/luc/know/index.htm
|title = kilogram NOW – Realization of the awaited definition of the kilogram
|publisher = European Association of National Metrology Institutes
|accessdate = 2012-10-08}}</ref>

{{As of|2013|3}} the proposed redefinition is known as the "New SI",<ref name=Kuehne/> but Mohr, in a paper following the CGPM proposal but predating the formal CCU proposal, suggested that since the proposed system makes use of [[Quantum realm|atomic scale]] phenomena rather than [[Physics:Macroscopic scale|macroscopic]] phenomena, it should be called the "Quantum SI System".<ref>{{cite journal
|journal = Advances in Quantum Chemistry
|url = https://books.google.com/books?id=Wsk36wNstDEC&pg=PA34&lpg=PA34&dq=si+definitions+boltzmann+planck&source=bl&ots=tD8hy3Q9GA&sig=O4zWn7Zxp4x9M-PvIWKH9jQxizY&hl=de&sa=X&ei=u7F6T5OSJfP54QS988GIBA&sqi=2&ved=0CE4Q6AEwBg#v=onepage&q=si%20definitions%20boltzmann%20planck&f=false
|year = 2008
|title = The Quantum SI: A Possible New International System of Units
|first = Peter J. |last = Mohr
|volume = 53 |page = 34
|isbn = 978-0-12-373925-4
|publisher = Academic Press
|accessdate = 2012-04-02
|doi=10.1016/s0065-3276(07)53003-0 |bibcode = 2008AdQC...53...27M }}</ref>

As of the 2014 CODATA recommended values of the fundamental physical constants (published in 2016, using data collected through the end of 2014), all measurements meet the CGPM's requirements and the way is clear to proceed with the redefinition and the next CGPM quadrennial  meeting in late 2018.<ref name=NIST16>{{cite press release |title=Universe’s Constants Now Known with Sufficient Certainty to Completely Redefine the International System of Units |url=https://www.nist.gov/news-events/news/2016/11/universes-constants-now-known-sufficient-certainty-completely-redefine |accessdate=31 December 2016 |publisher=NIST |date=22 November 2016}}</ref><ref name=CODATA2014>{{cite journal |title=CODATA recommended values of the fundamental physical constants: 2014 |journal=[[Physics:Reviews of Modern Physics|Reviews of Modern Physics]] |volume=88 |issue=3 |page=035009-1–73 |date=26 September 2016 |first1=Peter J. |last1=Mohr |first2=David B. |last2=Newell |first3=Barry N. |last3=Taylor |doi=10.1103/RevModPhys.88.035009 |quote=This is a truly major development, because these uncertainties are now sufficiently small that the adoption of the new SI by the 26th CGPM is expected.|arxiv=1507.07956 |bibcode=2016RvMP...88c5009M }}</ref>

On 20 October 2017, the 106th meeting of the International Committee for Weights and Measures (CIPM) formally accepted a revised Draft Resolution A calling for the redefinition of the SI, to be voted on at the 26th CGPM,<ref name=cipm_106>{{cite conference
 |title=Proceedings of the 106th meeting
 |conference=International Committee for Weights and Measures
 |date=16–20 October 2017
 |url=https://www.bipm.org/utils/en/pdf/CIPM/CIPM2017-EN.pdf?page=23
 |conference-url=https://www.bipm.org/en/committees/cipm/meeting/106.html
 |location=Sèvres
}}</ref>{{Rp|17–23}}  The same day, in response to the CIPM's endorsement of the final values{{r|cipm_106|p=22}}, the CODATA Task Group on Fundamental Constants published its 2017 recommended values for the four constants (with uncertainties) and proposed numerical values for the redefinition (without uncertainty).{{r|codata_2017}}


==Comment==

In 2010 Marcus Foster of the Commonwealth Scientific and Industrial Research Organisation published a wide-ranging critique of SI in which he raised numerous issues ranging from basic issues such as the absence of the symbol "[[Ohm|Ω]]" from most Western [[Computer keyboard|keyboards]] to the abstract issues such as inadequate formalism in the [[Metrology|metrological]] concepts on which SI is based. The changes proposed in the New SI only addressed issues regarding the definition of the base units including new definitions of the [[Candela|candela]] and the [[Mole (unit)|mole]] – units that Foster argued were not true base units. Other issues raised by Foster fell outside the scope of the proposal.<ref name=Foster/>

===Explicit-unit and explicit-constant definitions===
Concerns have been expressed that the use of explicit-constant definitions of the unit being defined that are not related to an example of its quantity will have many adverse effects.<ref>{{cite journal
|title = A sceptic’s review of the New SI
|first=Gary |last=Price
|year = 2011
|journal = Accreditation and Quality Assurance
|volume=16
|issue=3
|pages=121–132
|doi=10.1007/s00769-010-0738-x}}</ref> Although this criticism applies to the proposed linking of the kilogram to the Planck constant via a route that requires a knowledge of both special relativity and quantum mechanics,<ref>{{cite journal
|url = http://www.iupac.org/publications/ci/2011/3305/4_mills.html
|journal = Chemistry International
|volume = 33
|number = 5
|date = September–October 2011
|title = Part I – From the Current "Kilogram Problem" to a Proposed Definition
|first1 = Albert C
|last1 = Censullo
|issn = 0193-6484
|pages = 9–12}}</ref> it does not apply to the proposed definition of the ampere, which is closer to an example of its quantity than is the current definition.<ref>{{cite journal
|url = http://www.apajournal.org.uk/2013_0028-0044.pdf
|journal = Journal of the Association of Public Analysts (Online)
|year = 2013
|number = 41 2
|pages = 28–44
|title = The Background and Implications of the "New SI" for Analytical Chemists
|first1 = D Thorburn
|last1 = Burns
|first2 = EH
|last2 = Korte
|accessdate = 2013-06-25
|publisher = Association of Public Analysts
|location = London}}</ref> Some observers have welcomed the proposal to base the definition of electric current on the charge of the electron rather than the current definition of a force between two parallel current-carrying wires – since the nature of the electromagnetic interaction between two bodies at the [[Physics:Quantum electrodynamics|quantum electrodynamics level]] is somewhat different from the nature at [[Physics:Classical electromagnetism|classical electrodynamic levels]], it is considered inappropriate to use classical electrodynamics to define quantities that exist at quantum electrodynamic levels.<ref name=Chyla/>

===Mass and the Avogadro constant===
When the scale of the divergence between the IPK and national kilogram prototypes was reported in 2005, a debate arose on how best to redefine the kilogram – should the kilogram be defined in terms of the mass of the [[Physics:Isotopes of silicon|silicon-28]] atom or should it be determined using the [[Engineering:Kibble balance|Kibble balance]]? The mass of a silicon atom could be determined using the Avogadro project and using the Avogadro number be linked directly to the kilogram.<ref>{{cite journal
|url = http://kcdb.bipm.org/NL/16/OIML_Davis_2011.pdf
|journal = OIML Bulletin
|volume = LII
|number = 4
|date = October 2011
|title = Proposed change to the definition of the kilogram: Consequences for legal metrology
|first1 = Richard
|last1 = Davis}}</ref>

Concern has also been expressed that the authors of the proposal had failed to address the impact of breaking the link between the [[Mole (unit)|mole]], [[Kilogram|kilogram]], the [[Dalton (unit)|dalton]] (Da) and the [[Physics:Avogadro constant|Avogadro constant]] (''N''<sub>A</sub>).<Ref group = Note>The two quantities of the Avogadro constant ''N''<sub>A</sub> and the Avogadro number ''N''<sub>N</sub> are numerically the same, but while ''N''<sub>A</sub> has the unit mol<sup>−1</sup>, ''N''<sub>N</sub> is a pure number.</ref> This direct link has caused many to argue that the mole is not a true physical unit, but, in the words of the Swedish philosopher Johansson, the mole is a "scaling factor".<ref name=Foster/><ref>{{cite journal
|title = The Mole is Not an Ordinary Measurement Unit
|first1 = Ingvar
|last1 = Johansson
|journal = Accreditation and Quality Assurance
|year = 2011
|number = 16
|pages = 467–470
|doi = 10.1007/s00769-011-0804-z}}</ref>

The [http://www.bipm.org/utils/common/pdf/si_brochure_8_en.pdf SI Brochure (8th edition)] defines the dalton in terms of the mass of an atom of <sup>12</sup>C.  It defines the Avogadro constant in terms of this mass and the kilogram, making it determined by experiment. The proposal fixes the Avogadro constant, and the draft of the Ninth SI Brochure{{r|Brochure9_2016}} retains the definition of dalton in terms of <sup>12</sup>C, with the effect that the link between the dalton and the kilogram will be broken.<ref>{{cite journal
|title = Comments on recent proposals for redefining the mole and kilogram
|first=B.P. |last=Leonard
|url = http://iopscience.iop.org/0026-1394/47/3/L01/
|year = 2010
|volume = 47
|accessdate=2013-09-15
|issue = 3
|pages = L5–L8
|journal = [[Metrologia]]
|doi = 10.1088/0026-1394/47/3/L01|bibcode = 2010Metro..47L...5L }}</ref><ref>{{cite journal
|title = Some reflections on the proposed redefinition of the unit for the amount of substance and of other SI units
|last1 = Pavese
|first1 =  Franco
|year = 2011
|journal = Accreditation and Quality Assurance
|volume=16
|issue=3
|pages=161–165
|doi=10.1007/s00769-010-0700-y}}</ref>

===Temperature===
Temperature is somewhat of an enigma – [[Physics:Room temperature|room temperature]] can be measured by means of expansion and contraction of a liquid in a [[Physics:Thermometer|thermometer]], but high temperatures are often associated with a [[Earth:Color temperature|colour]].  Wojciech T. Chyla,  approaching the structure of SI from a philosophical point of view in the [[Physics:Acta Physica Polonica|Journal of the Polish Physical Society]], argued that temperature is not a real base unit but is rather an [[Average|average]] of the [[Physics:Thermal energy|thermal energies]] of the individual particles that make up the body concerned.<ref name=Chyla/> He noted that in many theoretical papers, temperature is represented by the quantities Θ or ''β'' where
:<math>\Theta = k T; \ \ \ \beta = {1 \over k T}</math>
and ''k'' is the Boltzmann constant.

Chyla acknowledged however that in the macroscopic world temperature plays the role of a base unit as much of the theory of [[Physics:Thermodynamics|thermodynamics]] is based on temperature.

The Consultative Committee for Thermometry, part of the [[Organization:International Committee for Weights and Measures|International Committee for Weights and Measures]] publishes a ''mise en pratique'' (practical technique), last updated in 1990, for measuring temperature which, at very low and at very high temperatures, makes great use of linking energy to temperature via the Boltzmann constant.<ref>{{cite web
|title = ''Mise en pratique'' for the definition of the kelvin
|year = 2011
|url = http://www.bipm.org/utils/en/pdf/MeP_K.pdf
|publisher = Consultative Committee for Thermometry (CCT), [[Organization:International Committee for Weights and Measures|International Committee for Weights and Measures]] (CIPM)
|location = Sèvres, France
|accessdate = 2013-06-25}}</ref><ref>{{cite journal
|journal = Procès-verbaux du Comité International des Poids et Mesures, 78th meeting
|url = http://www.bipm.org/utils/en/pdf/ITS-90.pdf
|title = The International Temperature Scale of 1990 (ITS-90)
|year = 1989
|author = Consultative Committee for Thermometry (CCT)
|publisher = [[Organization:International Committee for Weights and Measures|International Committee for Weights and Measures]] (CIPM)
|location = Sèvres, France
|accessdate = 2013-06-25}}</ref>

===Luminous intensity===
Foster argued that "luminous intensity [the candela] is not a [[Physics:Physical quantity|physical quantity]], but a [[Biology:Photobiology|photobiological]] quantity that exists in human perception", thereby questioning whether the candela should be a base unit.<ref name=Foster>{{cite journal
|url = http://publications.csiro.au/rpr/download?pid=csiro:EP11794&dsid=DS4
|last1 = Foster
|first1 =  Marcus P
|journal = Metrologia
|volume = 47
|number = 6
|date = 5 October 2010
|accessdate = 2013-06-24
|doi = 10.1088/0026-1394/47/6/R01
|title = The next 50 years of the SI: a review of the opportunities for the e-Science age|bibcode = 2010Metro..47R..41F }}</ref>

==See also==
* [[International System of Units]]
* International Vocabulary of Metrology
* [[Physics:Physical constant|Physical constant]]
* [[SI base unit]]

==Notes==
{{Reflist|60em|group="Note"}}

==References==
{{Reflist|30em|refs=
<ref name=Minutes2014>{{Cite web
 |url=http://www.bipm.org/cc/TGFC/Allowed/Minutes/CODATA_Minutes_14-BIPM-public.pdf
 |title=Report on the Meeting of the CODATA Task Group on Fundamental Constants
 |date=3–4 November 2014
 |place=BIPM
 |first=B. |last=Wood
 |page=7
 |quote=[BIPM director Martin] Milton responded to a question about what would happen if ... the CIPM or the CGPM voted not to move forward with the redefinition of the SI. He responded that he felt that by that time the decision to move forward should be seen as a foregone conclusion.
}}</ref>}}

==Further reading==
* {{SIbrochure9th}}
* {{cite web |work=[[Metrologia]] |author=[[Organization:International Bureau of Weights and Measures|International Bureau of Weights and Measures]] (BIPM) |title=Input data for the special CODATA-2017 adjustment |edition=Updated |date=2017-08-10 |url=http://iopscience.iop.org/journal/0026-1394/page/CODATA-2017_adjustment |access-date=2017-08-14 }}

==External links==
* [http://www.bipm.org/en/si/new_si/ BIPM website on the New SI], including a [http://www.bipm.org/en/si/new_si/faqs.html FAQ page].

{{SI units}}


[[Category:SI units]]

de:Internationales Einheitensystem#Zukünftige Entwicklungen

{{Sourceattribution|Proposed redefinition of SI base units|1}}