# Proposed redefinition of SI base units

For a topical guide to this subject, see Outline of the metric system.
Current (2013) SI System: Dependence of base unit definitions on other base units (for example, the metre is defined in terms of the distance traveled by light in a specific fraction of a second)
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.

A committee of the International Committee for Weights and Measures (CIPM) has proposed revised formal definitions of the SI base units, which are being examined by the CIPM and which will probably be introduced at the 26th 'General Conference on Weights and Measures' in 2018. The metric system was originally conceived as a system of measurement that was derivable from nature. When the metric system was first introduced in France in 1799 technical problems necessitated the use of artifacts as the prototype metre and kilogram. In 1960 the metre was redefined in terms of the wavelength of light from a specified source, making it derivable from nature, but the kilogram is still being defined by an artifact since its introduction. If the proposed redefinition is accepted, the metric system (SI) will, for the first time, be wholly derivable from nature.

The proposal can be summarised as follows:

"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 Planck constant, the elementary electric charge, the Boltzmann constant, and the Avogadro constant, respectively. The second, metre and candela are already defined by physical constants 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."[1]

Further details are found in the draft chapter of the Ninth SI Units Brochure.[2]

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 that have apparently "arbitrary" definitions and another twenty units that are derived from these base units. Although the units themselves form a coherent system, the definitions do not. 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 and the metre are already defined in such a manner.

A number of authors have published criticisms of the revised definitions — in particular that proposal had failed to address the impact of breaking the link between the mole and the kilogram, the dalton and the unified atomic mass unit, and the Avogadro constant and Avogadro's number.

## BackgroundEdit

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, notably the dependence on an artifact to define the kilogram.

### Development of SIEdit

During the early years of the French Revolution, the leaders of the French National Constituent Assembly decided to introduce a completely new system of measurement based on the principles of logic and natural phenomena. The resulting mètre des archives and kilogramme des archives were defined in terms of artefacts that were a "best attempt" at fulfilling these principles.[3]

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.[4][5] They were:

• CGPM (General Conference on Weights and Measures / 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 metrological determinations.
• CIPM (International Committee for Weights and Measures / 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 CCU (Consultative Committee for Units), amongst other things, advises the CIPM on matters concerning units of measurement.[6]
• BIPM (International Bureau for Weights and Measures / 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.[7] 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.[8] 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 electric current (1946), luminosity (1946), temperature (1948), time (1956) and molar mass (1971).[9]

Mass drift over time of national prototypes K21–K40, plus two of the International Prototype Kilogram's (IPK's) sister copies: K32 and K8(41).[Note 1] All mass changes are relative to the IPK.[10]

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".[11] The recommendations based on this mandate were presented to the 11th CGPM (1960) where they were formally accepted and given the name "Système International d'Unités" and its abbreviation "SI".[12]

### Impetus for changeEdit

Changing the underlying principles behind the definition of the SI base units is not without precedent. The 13th CGPM (1967) replaced the original definition of the 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. Similarly, the 17th CGPM (1983) replaced the 1960 definition of the metre[Note 2] with one where the metre is derived from the speed of light where the speed of light had been defined exactly in terms of metres per second.[13]

Over the years, drifts of up to 2×10−8 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.[14] 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. Newcastle University metrologist Peter Cumpson has since identified mercury vapour absorption or carbonaceous contamination as possible causes of this drift.[15][16]

Independently of this drift having been identified, the Avogadro project and development of the Watt balance promised methods of indirectly measuring mass with a very high precision. These projects provided tools that would enable alternative means of redefining the kilogram.[17]

A report published in 2007 by the Consultative Committee for Thermometry 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 Boltzmann constant provided a better basis for temperature measurement than did the triple point of water, as it overcame these difficulties.[18]

At its 23rd meeting (2007), the GCPM 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 International Union of Pure and Applied Physics (IUPAP).[19] At a meeting of the CCU held in Reading, United Kingdom, in September 2010, a resolution[20] 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.[21] 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.[Note 3] For this reason the CIPM does not propose a revision of the SI at the present time";[23] however, the CIPM presented a resolution for consideration at the 24th CGPM (17–21 October 2011) to agree the new definitions in principle, but not to implement them until the details have been finalised.[24] This resolution was accepted by the conference,[25] and in addition the CGPM moved the date of the 25th meeting forward from 2015 to 2014.[26][27] 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",[28] thus postponing the revision to the next meeting in 2018.

## The proposalEdit

In this section, an "X" at the end of a number means one or more final digits yet to be agreed upon.

In 2011 the CCU published a draft of the proposed change in the form of an amendment that should be made to the 8th edition of the SI Brochure.[2] In it they proposed that in addition to the speed of light, four further constants of nature should be defined to have exact values:

These constants were described in the 2006 version of the SI manual; the latter three were defined as "constants to be obtained by experiment".

The CCU also proposed that the numerical values associated with the following constants of nature be retained unchanged:

The seven definitions above are rewritten below after converting the derived units (joule, coulomb, hertz, lumen and watt) into the seven base units (second, metre, kilogram, ampere, kelvin, mole and candela). In the list that follows, the symbol sr stands for the dimensionless unit steradian.

• Δν(133Cs)hfs = 9192631770s−1
• c = 299792458m·s−1
• h = 6.62606X×10−34kg·m2·s−1
• e = 1.60217X×10−19A·s
• k = 1.38065X×10−23kg·m2·K−1·s−2
• NA = 6.02214X×1023mol−1
• Kcd = 683 cd·sr·s3·kg−1·m−2

In addition the CCU proposed that

• the international prototype kilogram be retired and that the current definition of the kilogram be abrogated,
• the current definition of the ampere be abrogated,
• the current definition of the kelvin be abrogated and
• the current definition of the mole be revised.

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

## Impact on base unit definitionsEdit

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.[29] 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 as being the length of three barleycorns[30] and since 1889 the 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 speed of light was defined to be exactly 299,792,458 metres per second and as long as the second has already been defined, the length of the metre can be defined.

The current (2008)[13] and proposed (2011)[21] definitions are given below. In many cases the final digit of any constant is yet to be agreed, so it has been represented by an "X"

### SecondEdit

The proposed definition of the second is effectively the same as the current definition, the only difference being that the conditions under which the measurements are made are more rigorously defined.

Current definition: The second is the duration of 9192631770 periods of the radiation corresponding to the transition between the two hyperfine levels of the ground state of the caesium-133 atom.
Proposed definition: The second, s, is the unit of time; its magnitude is set by fixing the numerical value of the ground state hyperfine splitting frequency of the caesium-133 atom, at rest and at a temperature of 0 K, to be equal to exactly 9192631770 when it is expressed in the unit s−1, which is equal to Hz.

### MetreEdit

The proposed definition of the 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 1/299792458 of a second.
Proposed definition: The metre, m, is the unit of length; its magnitude is set by fixing the numerical value of the speed of light in vacuum to be equal to exactly 299792458 when it is expressed in the unit m·s−1.

### KilogramEdit

The watt balance which will measure the ratio of the Planck constant to the international prototype kilogram.[31]

The definition of the kilogram is undergoing a fundamental change - the current definition defines the kilogram as being the mass of the international prototype kilogram which is an artifact, not a constant of nature[32] while the new definition relates it to the equivalent energy of a photon 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, kg, is the unit of mass; its magnitude is set by fixing the numerical value of the Planck constant to be equal to exactly 6.62606X×10−34 when it is expressed in the unit s−1·m2·kg, which is equal to J·s.

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

### AmpereEdit

The definition of the ampere is undergoing a major overhaul—the current definition, which is difficult to realise with high precision in practice, is being replaced by a definition that is more intuitive and that is easier to realise.

Current definition: The ampere is that constant current which, if maintained in two straight parallel conductors of infinite length, of negligible circular cross-section, and placed 1 m apart in vacuum, would produce between these conductors a force equal to 2×10−7 newton per metre of length.
Proposed definition: The ampere, A, is the unit of electric current; its magnitude is set by fixing the numerical value of the elementary charge to be equal to exactly 1.60217X×10−19 when it is expressed in the unit A·s, which is equal to C.

Since the current definition contains a reference to force which has the dimensions MLT−2 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 this definition are that in SI the value of vacuum permeability0) is fixed at exactly ×10−7 H⋅m−1.[33] Since the speed of light in vacuum (c) is also fixed, it follows from the relationship

$c^2 = \frac{1}{\mu_0\varepsilon_0}$

that the vacuum permittivity0) has a fixed value and from

$Z_0 = \sqrt{\frac{\mu_0}{\varepsilon_0}}$

that the impedance of free space (Z0) likewise has a fixed value.[34]

One consequence of the proposed changes to the definition of the ampere is that the definition will no longer be dependent on the definitions of the kilogram and the metre, but will still be dependent on the definition of the second. In addition the vacuum permeability, vacuum permittivity and impedance of free space, which, in the current definition have exact values will, in the future, be subject to experimental error.[35]

### KelvinEdit

The definition of the kelvin will undergo a fundamental change if the proposal is accepted. 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 thermodynamic temperature, is the fraction 1/273.16 of the thermodynamic temperature of the triple point of water.
Proposed definition: The kelvin, K, is the unit of thermodynamic temperature; its magnitude is set by fixing the numerical value of the Boltzmann constant to be equal to exactly 1.38065X×10−23 when it is expressed in the unit s−2·m2·kg·K−1, which is equal to J·K−1.

For a physical interpretation of this new definition, consider an ideal gas concentrated such that the average volume per molecule is 1.38065X×10−23 m3. That is the volume of a cube with a side length of about 24 nm. The ratio of the gas's temperature and pressure would be defined exactly equal to 1 K/Pa.

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.

### MoleEdit

A near-perfect sphere of ultra-pure silicon - part of the Avogadro project, an International Avogadro Coordination project to determine the Avogadro number[31]

The current definition of the 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 amount of substance of a system that contains as many elementary entities as there are atoms in 0.012 kilogram of carbon-12. When the mole is used, the elementary entities must be specified and may be atoms, molecules, ions, electrons, other particles, or specified groups of such particles.
Proposed definition: The mole, mol, is the unit of amount of substance of a specified elementary entity, which may be an atom, molecule, ion, electron, any other particle or a specified group of such particles; its magnitude is set by fixing the numerical value of the Avogadro constant to be equal to exactly 6.02214X×1023 when it is expressed in the unit mol−1.

One consequence of this change is that the current defined relationship between the mass of the 12C atom, the dalton, the kilogram, and Avogadro's number will no longer be valid. One of the following must change:

• the mass of a 12C atom is exactly 12 dalton
• the number of dalton in a gram is exactly the numerical value of Avogadro's constant

The draft SI brochure assumes the first will remain true, which would mean that the second will no longer be true. The molar mass constant, while still with great accuracy remaining equal to 1 g/mol, will no longer be exactly equal to that.

### CandelaEdit

The proposed definition of the candela is effectively the same as the current definition, but has been rephrased.

Current definition: The candela is the luminous intensity, in a given direction, of a source that emits monochromatic radiation of frequency 540×1012 Hz and that has a radiant intensity in that direction of 1/683 watt per steradian.
Proposed definition: The candela, cd, is the unit of luminous intensity in a given direction; its magnitude is set by fixing the numerical value of the luminous efficacy of monochromatic radiation of frequency 540×1012 Hz to be equal to exactly 683 when it is expressed in the unit s3·m−2·kg−1·cd·sr, or cd·sr·W−1, which is equal to lm·W−1.

## Impact on reproducibilityEdit

Apart from the candela,[Note 4][36] all the base units will be defined in terms of universal physical constants, but without an explicit 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 universal gravitational constant G could, from a dimensional point of view, be used to define mass.[Note 5] It should be noted that in practice G can only be measured with a relative uncertainty of 10−4[Note 6] which would have resulted in upper limit of the kilogram's reproducibility being 10−4 whereas the current international prototype kilogram can be measured with a relative uncertainty of 5 × 10−8.[35] 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)[37] 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.

### Physical constants used in the new definitions and other physical constantsEdit

There are four types of physical constants:

• Fixed constants, whose value is set a fixed number, from which units can be determined. For example, the speed of light has the fixed value of 299792458 metres per second (m·s−1).
• Constants as a combination of fixed constants. For example, the vacuum permittivity is determined by the reciprocal of the product of the speed of light squared and the magnetic constant: ε0 = c−2 μ0−18.854187817620... × 10−12 A2·s4·kg−1·m−3.
• Constants that are directly measured, usually measured in units determined by the fixed constants (for example the Josephson constant), or are dimensionless (for example the fine-structure constant).
• Constants that are a combination of directly measured constants and also fixed constants. These constants have a (relative) uncertainty depending on the uncertainties of the directly measured constants.

The Committee on Data for Science and Technology (CODATA) periodically publishes values of physical constants with the best (least) consistent uncertainty. Constants that can't be directly determined with the best accuracy are determined by a combination of direct measurements of other constants. The following table catalogues the changes in the relative uncertainty of the physical constants, as of the data of CODATA of 2010, and of base units that are directly affected by the proposal to change the units. Constants that don't change values are not mentioned. Also, the source of the relative uncertainty has been given, depending on the relative uncertainty of the direct measurements.

Because values of fundamental constants are highly dependent upon each other, the constants expressed in direct measurements can be more complex than the formal definition of that constant. The mass of the electron, for example, has an expression depending on the Rydberg constant, and, together with the molar mass of the electron, determines a whole array of constants. The constants are only expressed in direct measurements and fixed constants, because that way the source of the uncertainty can be traced down and the uncertainty in the calculation might be reduced. For example, the Faraday constant is in the current definition the product of the elementary charge and the Avogadro constant, each having an uncertainty depending on the uncertainty of the Josephson constant. One would suspect, by calculating the propagation of uncertainty, that the uncertainty in the Faraday constant would be, in total, approximately three times that of the Josephson constant (equal to 6.6×10−8), but in the expression of the Faraday constant two factors cancel, so the uncertainty would be only approximately that of the Josephson constant. It is often so that, by calculating the (relative) uncertainty, the uncertainty of very well known constants doesn't result in a different value of the uncertainty. That's why only the factors which are significant to the uncertainty are also mentioned. A tilde (~) is noted if the value of the uncertainty is only approximately that of other constants. The relative uncertainty of such other constant is noted as ur(constant).

Constant Symbol Current definition 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 International prototype kilogram $m(\mathcal{K})$ 1 kg N/A exact $m(\mathcal{K})$ $m(\mathcal{K})$ $u_\text{r}(m(\mathcal{K})) = 4.4 \times 10^{-8}$
Planck constant $h$ $\frac{8 \alpha}{c \mu_0 K_\text{J}^2}$ $K_\text{J}^2$ $\sim 2 u_\text{r}(K_\text{J}) = 4.4 \times 10^{-8}$ 6.62606X×10−34kg·m2·s−1 N/A exact
Josephson constant $K_\text{J}$ $K_\text{J}$ $K_\text{J}$ $u_\text{r}(K_\text{J}) = 2.2 \times 10^{-8}$ $\frac{2 e}{h}$ N/A exact
von Klitzing constant $R_\text{K}$ $\frac{c \mu_0}{2 \alpha}$ $\alpha$ $u_\text{r}(\alpha) = 3.2 \times 10^{-10}$ $\frac{h}{e^2}$ N/A exact
Elementary charge $e$ $\frac{4 \alpha}{c \mu_0 K_\text{J}}$ $K_\text{J}$ $\sim u_\text{r}(K_\text{J}) = 2.2 \times 10^{-8}$ 1.60217X×10−19A·s N/A exact
Magnetic constant $\mu_0$ ×10−7 m·kg·s−2·A−2 N/A exact $\frac{2 h \alpha}{c e^2}$ $\alpha$ $u_\text{r}(\alpha) = 3.2 \times 10^{-10}$
vacuum permittivity $\epsilon_0$ $\frac{1}{c^2 \mu_0}$ N/A exact $\frac{e^2}{2 h c \alpha}$ $\alpha$ $u_\text{r}(\alpha) = 3.2 \times 10^{-10}$
impedance of free space $Z_0$ $c \mu_0$ N/A exact $\frac{2 h \alpha}{e^2}$ $\alpha$ $u_\text{r}(\alpha) = 3.2 \times 10^{-10}$
Molar mass constant $M_\text{u}$ 1 g mol−1 = 0.001 kg mol−1 N/A exact $\frac{2 h N_\text{a} R_{\infty}}{c \alpha^2 A_\text{r}(\text{e})}$ $\alpha^2, A_\text{r}(\text{e})$ $\sim \sqrt{(2 u_\text{r}(\alpha))^2 + u_\text{r}(A_\text{r}(\text{e}))^2} \approx 7.5 \times 10^{-10}$
Molar mass of carbon-12 $M(^{12}\text{C})$ 12 g mol−1 = 0.012 kg mol−1 N/A exact $\frac{24 h N_\text{a} R_{\infty}}{c \alpha^2 A_\text{r}(\text{e})}$ $\alpha^2, A_\text{r}(\text{e})$ $\sim \sqrt{(2 u_\text{r}(\alpha))^2 + u_\text{r}(A_\text{r}(\text{e}))^2} \approx 7.5 \times 10^{-10}$
Avogadro constant $N_\text{A}$ $\frac{c^2 \alpha \mu_0 A_\text{r}(\text{e}) K_\text{J}^2 M_\text{u}}{16 R_{\infty}}$ $K_\text{J}^2$ $\sim 2 u_\text{r}(K_\text{J}) = 4.4 \times 10^{-8}$ 6.02214X×1023mol−1 N/A exact
unified atomic mass unit or dalton $m_\text{u}$ $\frac{16 R_{\infty}}{c^2 \alpha \mu_0 A_\text{r}(\text{e}) K_\text{J}^2}$ $K_\text{J}^2$ $\sim 2 u_\text{r}(K_\text{J}) = 4.4 \times 10^{-8}$ $\frac{2 h R_{\infty}}{c \alpha^2 A_\text{r}(\text{e})}$ $\alpha^2, A_\text{r}(\text{e})$ $\sim \sqrt{(2 u_\text{r}(\alpha))^2 + u_\text{r}(A_\text{r}(\text{e}))^2} \approx 7.5 \times 10^{-10}$
electron mass $m_\text{e}$ $\frac{16 R_{\infty}}{c^2 \alpha \mu_0 K_\text{J}^2}$ $K_\text{J}^2$ $\sim 2 u_\text{r}(K_\text{J}) = 4.4 \times 10^{-8}$ $\frac{2 h R_{\infty}}{c \alpha^2}$ $\alpha^2$ $\sim 2 u_\text{r}(\alpha) = 6.4 \times 10^{-10}$
Atomic mass of carbon-12 $m(^{12}\text{C})$ $\frac{192 R_{\infty}}{c^2 \alpha \mu_0 A_\text{r}(\text{e}) K_\text{J}^2}$ $K_\text{J}^2$ $\sim 2 u_\text{r}(K_\text{J}) = 4.4 \times 10^{-8}$ $\frac{24 h R_{\infty}}{c \alpha^2 A_\text{r}(\text{e})}$ $\alpha^2, A_\text{r}(\text{e})$ $\sim \sqrt{(2 u_\text{r}(\alpha))^2 + u_\text{r}(A_\text{r}(\text{e}))^2} \approx 7.5 \times 10^{-10}$
Faraday constant $F$ $\frac{c \alpha^2 A_\text{r}(\text{e}) K_\text{J} M_\text{u}}{4 R_{\infty}}$ $K_\text{J}$ $\sim u_\text{r}(K_\text{J}) = 2.2 \times 10^{-8}$ $e N_\text{A}$ N/A exact
Temperature of triple point of water $T_\text{TPW}$ 273.16 K N/A exact $T_\text{TPW}$ $T_\text{TPW}$ $u_\text{r}(T_\text{TPW}) = 9.1 \times 10^{-7}$
Molar gas constant $R$ $R$ $R$ $u_\text{r}(R) = 9.1 \times 10^{-7}$ $k N_\text{A}$ N/A exact
Boltzmann constant $k$ $\frac{c^2 \alpha \mu_0 A_\text{r}(\text{e}) K_\text{J}^2 M_\text{u} R}{16 R_{\infty}}$ $R$ $\sim u_\text{r}(R) = 9.1 \times 10^{-7}$ 1.38065X×10−23kg·m2·K−1·s−2 N/A exact
Stefan–Boltzmann constant $\sigma$ $\frac{256 \pi^5 R^4 R_{\infty}^4}{15 c^7 \alpha^7 \mu_0 A_\text{r}(\text{e})^4 M_\text{u}^4 K_\text{J}^2}$ $R^4$ $\sim 4 u_\text{r}(R) \approx 3.6 \times 10^{-6}$ $\frac{2 \pi^5 k^4}{15 h^3 c^2}$ N/A exact

### DaltonEdit

In 1993, the International Union of Pure and Applied Chemistry approved the use of the dalton as an alternative to the unified atomic mass unit with the qualification that the GCPM had not given its approval.[38] This approval has since been given.[39] Following the proposal to redefine the mole by fixing the value of the Avogadro number, Brian Leonard of the University of Akron, writing in Metrologia proposed that the dalton (Da) be redefined as an SI derived unit exactly equal to (1/1000NA) kg; but that the unified atomic mass unit (mu) retain its current definition based on the mass of 12C, ceasing to be SI. This would result in the dalton and the atomic mass unit potentially differing from each other by a factor of the order of 10−9 (now 10−10).[40]

## AcceptanceEdit

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 GCPM 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:

• At least three separate experiments be carried out yielding values having a relative expanded (95%) uncertainty of no more than 5 × 10−8 and at least one of these values should be better than 2 × 10−8. Both the Watt balance and the Avogadro project should be included in the experiments and any differences between these be reconciled.[41][42]
• 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 10−6 and that these values be corroborated by other measurements.[43]

As at March 2011, the International Avogadro Coordination (IAC) group had obtained an uncertainty of 3.0 × 10−8 and NIST had obtained an uncertainty of 3.6 × 10−8 in their measurements.[17]

On 1 September 2012 the European Association of National Metrology Institutes (Euramet) launched a formal project to reduce the relative difference between the watt-balance and the silicon sphere approach to measuring the kilogram from 17 ± 5 × 10−8 to within 2 × 10−8.[44]

As of March 2013 the proposed redefinition is known as the "New SI",[1] but Mohr, in a paper following the CGPM proposal but predating the formal CCU proposal, suggested that since the proposed system makes use of atomic scale phenomena rather than macroscopic phenomena, it should be called the "Quantum SI System".[45]

## CommentEdit

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 "Ω" from most Western keyboards to the abstract issues such as inadequate formalism in the 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 and the mole—units that Foster argued were not true base units. Other issues raised by Foster fell outside the scope of the proposal.[46]

### Explicit-unit and explicit-constant definitionsEdit

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.[47] 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[48] 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.[49] 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 quantum electrodynamics level is somewhat different from the nature at classical electrodynamic levels, it is considered inappropriate to use classical electrodynamics to define quantities that exist at quantum electrodynamic levels.[35]

### Mass and the Avogadro constantEdit

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 silicon-28 atom or should it be determined using the watt 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.[50]

Concern has also been expressed that the authors of the proposal had failed to address the impact of breaking the link between the mole, kilogram, the dalton (Da), the Avogadro constant (NA) and Avogadro's number (NN).[Note 7] 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".[46][51]

The SI Brochure (8th edition) implicitly defines the dalton as 0.001÷NN kg where the value of NN is determined by experiment. The proposal fixes NA, so if the Avogadro constant and Avogadro's number are to be numerically identical, the dalton must be related to either the mass of a single carbon atom or to the kilogram — it cannot be related to both.[52][53]

### TemperatureEdit

Temperature is somewhat of an enigma - room temperature can be measured by means of expansion and contraction of a liquid in a thermometer, but high temperatures are often associated with a colour. Wojciech T. Chyla, approaching the structure of SI from a philosophical point of view in the Journal of the Polish Physical Society, argued that temperature is not a real base unit but is rather an average of the thermal energies of the individual particles that make up the body concerned.[35] He noted that in many theoretical papers, temperature is represented by the quantities Θ or β where

$\Theta = k_b T; \beta = {1 \over k_b T}$

and kb 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 thermodynamics is based on temperature. Foster,[46] writing from the point of view of quality control argued that the introduction of the Boltzmann constant into the definition of temperature was an unnecessary complication.

The Consultative Committee for Thermometry, part of the 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.[54][55]

### Luminous intensityEdit

Foster argued that "luminous intensity [the candela] is not a physical quantity, but a photobiological quantity that exists in human perception" thereby questioning whether or not the candela should be a base unit.[46]

## NotesEdit

1. ^ 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).
2. ^ Since the adoption of SI in 1960, the metre had been defined in terms of the wavelength of krypton 86 radiation.
3. ^ 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[22]
4. ^ Measurement of the candela also requires a knowledge of the response of the human eye to different wavelengths of light known as the (luminosity function) and denoted by V(λ), a function computed by the International Commission on Illumination (CIE) to different wavelengths of light.
5. ^ The dimensions of G are L3M−1T−2, 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.
6. ^ The following terms are defined in 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
7. ^ The two quantities of the Avogadro constant and Avogadro's number are numerically the same, but while NA has the units of mole−1, NN is a pure number.

## ReferencesEdit

1. ^ a b Michael Kuehne (22 March 2012). "Redefinition of the SI". Keynote address, ITS9 (Ninth International Temperature Symposium). Los Angeles: NIST. Retrieved 2012-03-01.
2. ^ a b Ian Mills (27 September 2010). "Draft Chapter 2 for SI Brochure, following redefinitions of the base units". BIPM. Retrieved 2012-03-01.
3. ^ Alder, Ken (2002). The Measure of all Things - The Seven-Year-Odyssey that Transformed the World. London: Abacus. p. 1. ISBN 0349115079.
4. ^ "Metric Convention of 1875 [English translation]". Washington, D.C.: Office of the President of the United States. 1876.
5. ^ "The Metre Convention". Sèvres, France: International Bureau of Weights and Measures. Retrieved 2013-06-21.
6. ^ "CIPM: International Committee for Weights and Measures". Sèvres, France: BIPM. Retrieved 2010-10-03.
7. ^ "Resolution of the 1st meeting of the CGPM (1889)". Sèvres, France: International Bureau of Weights and Measures. Retrieved 2013-06-21.
8. ^ Jabbour, Z.J.; Yaniv, S.L. (2001). "The Kilogram and Measurements of Mass and Force". J. Res. Natl. Inst. Stand. Technol. (National Institute of Standards and Technology (NIST) 106 (1): 25–46. doi:10.6028/jres.106.003. Retrieved 2011-03-28.
9. ^ International Bureau of Weights and Measures (2006), The International System of Units (SI) (8th ed.), pp. 95, 97, 138–140, ISBN 92-822-2213-6
10. ^ G. Girard (1994). "The Third Periodic Verification of National Prototypes of the Kilogram (1988–1992)". Metrologia 31 (4): 317–336. Bibcode:1994Metro..31..317G. doi:10.1088/0026-1394/31/4/007.
11. ^
12. ^ "Resolution 12 of the 11th meeting of the CGPM (1960): Système International d'Unités". Sèvres, France. Retrieved 2011-03-23.
13. ^ a b International Bureau of Weights and Measures (2006), The International System of Units (SI) (8th ed.), pp. 112–116, ISBN 92-822-2213-6
14. ^ Peter Mohr (6 December 2010). "Recent progress in fundamental constants and the International System of Units". Third Workshop on Precision Physics and Fundamental Physical Constants. Retrieved 2011-01-02.
15. ^ Whipple, Tom (7 January 2013). "The dirty secret of why you are not quite as heavy as you think". The Times (London). p. 15. Retrieved 2011-03-23.
16. ^ Ghose, Tia (6 January 2013). "The Kilogram Has Gained Weight". LiveScience. Retrieved 2011-03-23.
17. ^ a b Crease, Robert P (22 March 2011). "Metrology in the balance". Physics World. Institute of Physics. Retrieved 2012-06-28.
18. ^ Fischer, J. et al (2 May 2007). "Report to the CIPM on the implications of changing the definition of the base unit kelvin". Retrieved 2011-01-02.
19. ^ "Resolution proposal submitted to the IUPAP Assembly by Commission C2 (SUNAMCO)". International Union of Pure and Applied Physics. 2008. Retrieved 2011-05-08.
20. ^ Ian Mills (29 September 2010). "On the possible future revision of the International System of Units, the SI". CCU. Retrieved 2011-01-01.
21. ^ a b Ian Mills (29 September 2010). "Draft Chapter 2 for SI Brochure, following redefinitions of the base units". CCU. Retrieved 2011-01-01.
22. ^ "Resolution 12 of the 23rd meeting of the CGPM (2007)". Sèvres, France: General Conference on Weights and Measures. Retrieved 2013-06-21.
23. ^ "Towards the "new SI"". International Bureau of Weights and Measures (BIPM). Retrieved 2011-02-20.
24. ^
25. ^ "On the possible future revision of the International System of Units, the SI". Sèvres, France: International Bureau for Weights and Measures. 21 Oct 2011. |chapter= ignored (help) It is not expected to be adopted until some prerequisite conditions are met, and in any case not before 2014. See "Possible changes to the international system of units". IUPAC Wire (International Union of Pure and Applied Chemistry) 34 (1). January–February 2012.
26. ^ "General Conference on Weights and Measures approves possible changes to the International System of Units, including redefinition of the kilogram." (Press release). Sèvres, France: General Conference on Weights and Measures. 23 October 2011. Retrieved 2011-10-25.
27. ^ Peter Mohr (November 2, 2011). "Redefining the SI base units". NIST Newsletter. NIST. Retrieved 2012-03-01.
28. ^ "Resolutions adopted by the CGPM at its 25th meeting (18‐20 November 2014)". Sèvres, France: International Bureau for Weights and Measures. 21 Nov 2014.
29. ^ Mills, Ian (September–October 2011). "Part II—Explicit-Constant Definitions for the Kilogram and for the Mole". Chemistry International 33 (5): 12–15. ISSN 0193-6484.
30. ^ Travenor, Robert (2007). Smoot's Ear - The Measure of Humanity. Yale University Press. pp. 35–36. ISBN 978-0-300-14334-8.
31. ^ a b "The BIPM watt balance". International Bureau of Weights and Measures. 2012. Retrieved 2013-03-28.
32. ^ Taylor, Barry N (November–December 2011). "The Current SI Seen From the Perspective of the Proposed New SI". Journal of Research of the National Institute of Standards and Technology (National Institute of Standards and Technology (NIST)) 116 (6): 797–807. doi:10.6028/jres.116.022.
33. ^ "Unit of electric current (ampere)". Historical context of the SI. NIST. Retrieved 2013-06-124. Check date values in: |accessdate= (help)
34. ^ Orfanidis, Sophocles J. (31 August 2010). Electromagnetic Waves and Antennas. ECE Department, Rutgers University. 1.3 Constitutive Relations. Retrieved 24 June 2013.
35. ^ a b c d Chyla, W.T. (December 2011). "Evolution of the International Metric System of Units SI". Acta Physica Polonica A 120 (6): 998–1011. Retrieved 22 June 2013.
36. ^ Wyszecki, G; Blevin, WR; Kessler, KG; Mielenz, KD (1983). Principles covering Photometry. Sevres: Conférence général des poids et mesures (CGPM).
37. ^ "What is a mise en pratique?". BIPM. 2011. Retrieved 2011-03-11.
38. ^ Mills, Ian; Cvitaš, Tomislav; Homann, Klaus; Kallay, Nikola; Kuchitsu, Kozo (1993). Quantities, Units and Symbols in Physical Chemistry International Union of Pure and Applied Chemistry; Physical Chemistry Division (2nd ed.). International Union of Pure and Applied Chemistry and published for them by Blackwell Science Ltd. ISBN 0-632-03583-8.
39. ^ International Bureau of Weights and Measures (2006), The International System of Units (SI) (8th ed.), pp. 114, 115, ISBN 92-822-2213-6
40. ^ Leonard, B P (2012). "Why the dalton should be redefined exactly in terms of the kilogram". Metrologia (49): 487. Bibcode:2012Metro..49..487L. doi:10.1088/0026-1394/49/4/487.
41. ^ "Recommendations of the Consultative Committee for Mass and Related Quantities to the International Committee for Weights and Measures.". 12th Meeting of the CCM. Sèvres: Bureau International des Poids et Mesures. 26 March 2010. Retrieved 2012-06-27.
42. ^ "Recommendations of the Consultative Committee for Amount of Substance: Metrology in Chemistry to the International Committee for Weights and Measures.". 16th Meeting of the CCQM. Sèvres: Bureau International des Poids et Mesures. 15–16 April 2010. Retrieved 2012-06-27.
43. ^ "Recommendations of the Consultative Committee for Thermometry to the International Committee for Weights and Measures.". 25th Meeting of the CCT. Sèvres: Bureau International des Poids et Mesures. 6–7 May 2010. Retrieved 2012-06-27.
44. ^ "kilogram NOW - Realization of the awaited definition of the kilogram". European Association of National Metrology Institutes. Retrieved 2012-10-08.
45. ^ Mohr, Peter J (2008). "The Quantum SI: A Possible New International System of Units". Advances in Quantum Chemistry (Academic Press) 53: 34. Bibcode:2008AdQC...53...27M. doi:10.1016/s0065-3276(07)53003-0. ISBN 978-0-12-373925-4. Retrieved 2012-04-02.
46. ^ a b c d Foster, Marcus P (5 October 2010). "The next 50 years of the SI: a review of the opportunities for the e-Science age". Metrologia 47 (6). Bibcode:2010Metro..47R..41F. doi:10.1088/0026-1394/47/6/R01. Retrieved 24 June 2013.
47. ^ Price, Gary (2011). "A sceptic’s review of the New SI". Accreditation and Quality Assurance: Journal for Quality, Comparability and Reliability in Chemical Measurement 16 (3): 121–132. doi:10.1007/s00769-010-0738-x.
48. ^ Censullo, Albert C (September–October 2011). "Part I—From the Current "Kilogram Problem" to a Proposed Definition". Chemistry International 33 (5): 9–12. ISSN 0193-6484.
49. ^ Burns, D Thorburn; Korte, EH (2013). "The Background and Implications of the "New SI" for Analytical Chemists". Journal of the Association of Public Analysts (Online) (London: Association of Public Analysts) (41 2): 28–44. Retrieved 25 June 2013.
50. ^ Davis, Richard (October 2011). "Proposed change to the definition of the kilogram: Consequences for legal metrology". OIML Buletin LII (4).
51. ^ Johansson, Ingvar (2011). "The Mole is Not an Ordinary Measurement Unit". Accreditation and Quality assurance (16): 467–470. doi:10.1007/s00769-011-0804-z.
52. ^ Leonard, B. P. (2010). "Comments on recent proposals for redefining the mole and kilogram". Metrologia 47 (3): L5–L8. Bibcode:2010Metro..47L...5L. doi:10.1088/0026-1394/47/3/L01. Retrieved 2013-09-15.
53. ^ Pavese, Franco (2011). "Some reflections on the proposed redefinition of the unit for the amount of substance and of other SI units". Accreditation and Quality Assurance: Journal for Quality, Comparability and Reliability in Chemical Measurement 16 (3): 161–165. doi:10.1007/s00769-010-0700-y.
54. ^ "Mise en pratique for the definition of the kelvin". Sèvres, France: Consultative Committee for Thermometry (CCT), International Committee for Weights and Measures (CIPM). 2011. Retrieved 25 June 2013.
55. ^ Consultative Committee for Thermometry (CCT) (1989). "The International Temperature Scale of 1990 (ITS-90)". Procès-verbaux du Comité International des Poids et Mesures, 78th meeting (Sèvres, France: International Committee for Weights and Measures (CIPM)). Retrieved 25 June 2013.