Planck constant

For the law governing black body radiation, see Planck's law.

Values of h	Units	Ref.
6966662607004000000♠6.626070040(81)×10⁻³⁴	J⋅s	^[1]
6985413566766200000♠4.135667662(25)×10⁻¹⁵	eV⋅s	^[1]
2π	E_P⋅t_P
Values of ħ	Units	Ref.
6966105457179999999♠1.054571800(13)×10⁻³⁴	J⋅s	^[1]
6984658211951400000♠6.582119514(40)×10⁻¹⁶	eV⋅s	^[1]
1	E_P⋅t_P	def
Values of hc	Units	Ref.
6975198644568000000♠1.98644568×10⁻²⁵	J⋅m
7000123984193000000♠1.23984193	eV⋅μm
2π	E_P⋅ℓ_P
Values of ħc	Units	Ref.
6974316152649000000♠3.16152649×10⁻²⁶	J⋅m
6999197326970000000♠0.19732697	eV⋅μm
1	E_P⋅ℓ_P

Plaque at the Humboldt University of Berlin: "Max Planck, discoverer of the elementary quantum of action h, taught in this building from 1889 to 1928."

The Planck constant (denoted $h$ , also called Planck's constant) is a physical constant that is the quantum of action, central in quantum mechanics.

First recognized in 1900 by Max Planck, it was originally the proportionality constant between the minimal increment of energy, $E$ , of a hypothetical electrically charged oscillator in a cavity that contained black body radiation, and the frequency, $f$ , of its associated electromagnetic wave. In 1905 the value $E$ , the minimal energy increment of a hypothetical oscillator, was theoretically associated by Einstein with a "quantum" or minimal element of the energy of the electromagnetic wave itself. The light quantum behaved in some respects as an electrically neutral particle, as opposed to an electromagnetic wave. It was eventually called the photon.

The Planck–Einstein relation connects the particulate photon energy $E$ with its associated wave frequency $f$ :

E = hf

This energy is extremely small in terms of ordinarily perceived everyday objects.

Since the frequency $f$ , wavelength $λ$ , and speed of light $c$ are related by $f= \frac{c}{\lambda}$ , the relation can also be expressed as

E = \frac{hc}{\lambda} .

This leads to another relationship involving the Planck constant. With $p$ denoting the linear momentum of a particle (not only a photon, but other fine particles as well), the de Broglie wavelength $λ$ of the particle is given by

\lambda = \frac{h}{p} .

In applications where it is natural to use the angular frequency (i.e. where the frequency is expressed in terms of radians per second instead of cycles per second or hertz) it is often useful to absorb a factor of $2 π$ into the Planck constant. The resulting constant is called the reduced Planck constant or Dirac constant. It is equal to the Planck constant divided by $2 π$ , and is denoted $ħ$ (pronounced "h-bar"):

\hbar = \frac{h}{2 \pi} .

The energy of a photon with angular frequency $ω$ , where $ω = 2 πν$ , is given by

E = \hbar \omega ,

while its linear momentum relates to

p = \hbar k ,

where k is a wavenumber. In 1923, Louis de Broglie generalized the Planck–Einstein relation by postulating that the Planck constant represents the proportionality between the momentum and the quantum wavelength of not just the photon, but the quantum wavelength of any particle. This was confirmed by experiments soon afterwards. This holds throughout quantum theory, including electrodynamics.

These two relations are the temporal and spatial component parts of the special relativistic expression using 4-Vectors.

P^\mu = \left(\frac{E}{c}, \vec{p}\right) = \hbar K^\mu = \hbar\left(\frac{\omega}{c}, \vec{k}\right)

Classical statistical mechanics requires the existence of $h$ (but does not define its value).^[2] Eventually, following upon Planck's discovery, it was recognized that physical action cannot take on an arbitrary value. Instead, it must be some multiple of a very small quantity, the "quantum of action", now called the Planck constant. Classical physics cannot explain this fact. In many cases, such as for monochromatic light or for atoms, this quantum of action also implies that only certain energy levels are allowed, and values in between are forbidden.^[3]

Value

The Planck constant has dimensions of physical action; these are the same as those of angular momentum, i.e., energy multiplied by time, or momentum multiplied by distance. In SI units, the Planck constant is expressed in joule seconds (J⋅s) or (N⋅m⋅s) or (kg⋅m²⋅s⁻¹).

The value of the Planck constant is:^[1]

h = 6.626\ 070\ 040(81)\times 10^{-34}\text{ J⋅s} = 4.135\ 667\ 662(25)\times 10^{-15}\text{ eV⋅s} .

The value of the reduced Planck constant is:

\hbar = {{h}\over{2\pi}} = 1.054\ 571\ 800(13)\times 10^{-34}\text{ J⋅s} = 6.582\ 119\ 514(40)\times 10^{-16}\text{ eV⋅s} .

The two digits inside the parentheses denote the standard uncertainty in the last two digits of the value. The figures cited here are the 2014 CODATA recommended values for the constants and their uncertainties. The 2014 CODATA results were made available in June 2015^[4] and represent the best-known, internationally accepted values for these constants, based on all data published as of 31 December 2014. New CODATA figures are normally produced every four years.

Significance of the value

The Planck constant is related to the quantization of light and matter. It can be seen as a subatomic-scale constant. In a unit system adapted to subatomic scales, the electronvolt is the appropriate unit of energy and the petahertz the appropriate unit of frequency. Atomic unit systems are based (in part) on the Planck constant.

The numerical value of the Planck constant depends entirely on the system of units used to measure it. When it is expressed in SI units, it is one of the smallest constants used in physics. This reflects the fact that on a scale adapted to humans, where energies are typically of the order of kilojoules and times are typically of the order of seconds or minutes, the Planck constant (the quantum of action) is very small.

Equivalently, the smallness of the Planck constant reflects the fact that everyday objects and systems are made of a large number of particles. For example, green light with a wavelength of 555 nanometres (the approximate wavelength to which human eyes are most sensitive) has a frequency of 7014540000000000000♠540 THz (7014540000000000000♠540×10¹² Hz). Each photon has an energy E = hf = 6981358000000000000♠3.58×10⁻¹⁹ J. That is a very small amount of energy in terms of everyday experience, but everyday experience is not concerned with individual photons any more than with individual atoms or molecules. An amount of light compatible with everyday experience is the energy of one mole of photons; its energy can be computed by multiplying the photon energy by the Avogadro constant, N_A ≈ 7023602200000000000♠6.022×10²³ mol⁻¹. The result is that green light of wavelength 555 nm has an energy of 7005216000000000000♠216 kJ/mol, a typical energy of everyday life.

Origins

Black-body radiation

Main article: Planck's law

Intensity of light emitted from a black body at any given frequency. Each color is a different temperature. Planck was the first to explain the shape of these curves.

In the last years of the nineteenth century, Planck was investigating the problem of black-body radiation first posed by Kirchhoff some forty years earlier. It is well known that hot objects glow, and that hotter objects glow brighter than cooler ones. The reason is that the electromagnetic field obeys laws of motion just like a mass on a spring, and can come to thermal equilibrium with hot atoms. When a hot object is in equilibrium with light, the amount of light it absorbs is equal to the amount of light it emits. If the object is black, meaning it absorbs all the light that hits it, then it emits the maximum amount of thermal light too.

The assumption that black-body radiation is thermal leads to an accurate prediction: the total amount of emitted energy goes up with the temperature according to a definite rule, the Stefan–Boltzmann law (1879–84). But it was also known that the colour of the light given off by a hot object changes with the temperature, so that "white hot" is hotter than "red hot". Nevertheless, Wilhelm Wien discovered the mathematical relationship between the peaks of the curves at different temperatures, by using the principle of adiabatic invariance. At each different temperature, the curve is moved over by Wien's displacement law (1893). Wien also proposed an approximation for the spectrum of the object, which was correct at high frequencies (short wavelength) but not at low frequencies (long wavelength).^[5] It still was not clear why the spectrum of a hot object had the form that it has (see diagram).

Planck hypothesized that the equations of motion for light describe a set of harmonic oscillators, one for each possible frequency. He examined how the entropy of the oscillators varied with the temperature of the body, trying to match Wien's law, and was able to derive an approximate mathematical function for black-body spectrum.^[6]

However, Planck soon realized that his solution was not unique. There were several different solutions, each of which gave a different value for the entropy of the oscillators.^[6] To save his theory, Planck had to resort to using the then controversial theory of statistical mechanics,^[6] which he described as "an act of despair … I was ready to sacrifice any of my previous convictions about physics."^[7] One of his new boundary conditions was

to interpret U_N [the vibrational energy of N oscillators] not as a continuous, infinitely divisible quantity, but as a discrete quantity composed of an integral number of finite equal parts. Let us call each such part the energy element ε;
— Planck, On the Law of Distribution of Energy in the Normal Spectrum^[6]

With this new condition, Planck had imposed the quantization of the energy of the oscillators, "a purely formal assumption … actually I did not think much about it…" in his own words,^[8] but one which would revolutionize physics. Applying this new approach to Wien's displacement law showed that the "energy element" must be proportional to the frequency of the oscillator, the first version of what is now sometimes termed the "Planck–Einstein relation":

E = hf.

Planck was able to calculate the value of h from experimental data on black-body radiation: his result, 6966655000000000000♠6.55×10⁻³⁴ J⋅s, is within 1.2% of the currently accepted value.^[6] He was also able to make the first determination of the Boltzmann constant k_B from the same data and theory.^[9]

Note that the (black) Rayleigh–Jeans curve never touches the Planck curve.

Prior to Planck's work, it had been assumed that the energy of a body could take on any value whatsoever – that it was a continuous variable. The Rayleigh–Jeans law makes close predictions for a narrow range of values at one limit of temperatures, but the results diverge more and more strongly as temperatures increase. To make Planck's law, which correctly predicts blackbody emissions, it was necessary to multiply the classical expression by a complex factor that involves h in both the numerator and the denominator. The influence of h in this complex factor would not disappear if it were set to zero or to any other value. Making an equation out of Planck's law that would reproduce the Rayleigh–Jeans law could not be done by changing the values of h, of the Boltzmann constant, or of any other constant or variable in the equation. In this case the picture given by classical physics is not duplicated by a range of results in the quantum picture.

The black-body problem was revisited in 1905, when Rayleigh and Jeans (on the one hand) and Einstein (on the other hand) independently proved that classical electromagnetism could never account for the observed spectrum. These proofs are commonly known as the "ultraviolet catastrophe", a name coined by Paul Ehrenfest in 1911. They contributed greatly (along with Einstein's work on the photoelectric effect) to convincing physicists that Planck's postulate of quantized energy levels was more than a mere mathematical formalism. The very first Solvay Conference in 1911 was devoted to "the theory of radiation and quanta".^[10] Max Planck received the 1918 Nobel Prize in Physics "in recognition of the services he rendered to the advancement of Physics by his discovery of energy quanta".

Photoelectric effect

Main article: Photoelectric effect

The photoelectric effect is the emission of electrons (called "photoelectrons") from a surface when light is shone on it. It was first observed by Alexandre Edmond Becquerel in 1839, although credit is usually reserved for Heinrich Hertz,^[11] who published the first thorough investigation in 1887. Another particularly thorough investigation was published by Philipp Lenard in 1902.^[12] Einstein's 1905 paper^[13] discussing the effect in terms of light quanta would earn him the Nobel Prize in 1921,^[11] when his predictions had been confirmed by the experimental work of Robert Andrews Millikan.^[14] The Nobel committee awarded the prize for his work on the photo-electric effect, rather than relativity, both because of a bias against purely theoretical physics not grounded in discovery or experiment, and dissent amongst its members as to the actual proof that relativity was real.^[15]^[16]

Prior to Einstein's paper, electromagnetic radiation such as visible light was considered to behave as a wave: hence the use of the terms "frequency" and "wavelength" to characterise different types of radiation. The energy transferred by a wave in a given time is called its intensity. The light from a theatre spotlight is more intense than the light from a domestic lightbulb; that is to say that the spotlight gives out more energy per unit time and per unit space(and hence consumes more electricity) than the ordinary bulb, even though the colour of the light might be very similar. Other waves, such as sound or the waves crashing against a seafront, also have their own intensity. However, the energy account of the photoelectric effect didn't seem to agree with the wave description of light.

The "photoelectrons" emitted as a result of the photoelectric effect have a certain kinetic energy, which can be measured. This kinetic energy (for each photoelectron) is independent of the intensity of the light,^[12] but depends linearly on the frequency;^[14] and if the frequency is too low (corresponding to a photon energy that is less than the work function of the material), no photoelectrons are emitted at all, unless a plurality of photons, whose energetic sum is greater than the energy of the photoelectrons, acts virtually simultaneously (multiphoton effect) ^[17] Assuming the frequency is high enough to cause the photoelectric effect, a rise in intensity of the light source causes more photoelectrons to be emitted with the same kinetic energy, rather than the same number of photoelectrons to be emitted with higher kinetic energy.^[12]

Einstein's explanation for these observations was that light itself is quantized; that the energy of light is not transferred continuously as in a classical wave, but only in small "packets" or quanta. The size of these "packets" of energy, which would later be named photons, was to be the same as Planck's "energy element", giving the modern version of the Planck–Einstein relation:

E = hf .

Einstein's postulate was later proven experimentally: the constant of proportionality between the frequency of incident light (f) and the kinetic energy of photoelectrons (E) was shown to be equal to the Planck constant (h).^[14]

Atomic structure

Main article: Bohr model

A schematization of the Bohr model of the hydrogen atom. The transition shown from the n = 3 level to the n = 2 level gives rise to visible light of wavelength 656 nm (red), as the model predicts.

Niels Bohr introduced the first quantized model of the atom in 1913, in an attempt to overcome a major shortcoming of Rutherford's classical model.^[18] In classical electrodynamics, a charge moving in a circle should radiate electromagnetic radiation. If that charge were to be an electron orbiting a nucleus, the radiation would cause it to lose energy and spiral down into the nucleus. Bohr solved this paradox with explicit reference to Planck's work: an electron in a Bohr atom could only have certain defined energies E_n

E_n = -\frac{h c_0 R_{\infty}}{n^2} ,

where c₀ is the speed of light in vacuum, R_∞ is an experimentally determined constant (the Rydberg constant) and n is any integer (n = 1, 2, 3, …). Once the electron reached the lowest energy level (n = 1), it could not get any closer to the nucleus (lower energy). This approach also allowed Bohr to account for the Rydberg formula, an empirical description of the atomic spectrum of hydrogen, and to account for the value of the Rydberg constant R_∞ in terms of other fundamental constants.

Bohr also introduced the quantity $\frac{h}{2\pi}$ , now known as the reduced Planck constant, as the quantum of angular momentum. At first, Bohr thought that this was the angular momentum of each electron in an atom: this proved incorrect and, despite developments by Sommerfeld and others, an accurate description of the electron angular momentum proved beyond the Bohr model. The correct quantization rules for electrons – in which the energy reduces to the Bohr model equation in the case of the hydrogen atom – were given by Heisenberg's matrix mechanics in 1925 and the Schrödinger wave equation in 1926: the reduced Planck constant remains the fundamental quantum of angular momentum. In modern terms, if J is the total angular momentum of a system with rotational invariance, and J_z the angular momentum measured along any given direction, these quantities can only take on the values

\begin{align} J^2 = j(j+1) \hbar^2,\qquad & j = 0, \tfrac{1}{2}, 1, \tfrac{3}{2}, \ldots, \\ J_z = m \hbar, \qquad\qquad\quad & m = -j, -j+1, \ldots, j. \end{align}

Uncertainty principle

Main article: Uncertainty principle

The Planck constant also occurs in statements of Werner Heisenberg's uncertainty principle. Given a large number of particles prepared in the same state, the uncertainty in their position, Δx, and the uncertainty in their momentum (in the same direction), Δp, obey

\Delta x\, \Delta p \ge \frac{\hbar}{2} ,

where the uncertainty is given as the standard deviation of the measured value from its expected value. There are a number of other such pairs of physically measurable values which obey a similar rule. One example is time vs. energy. The either-or nature of uncertainty forces measurement attempts to choose between trade offs, and given that they are quanta, the trade offs often take the form of either-or (as in Fourier analysis), rather than the compromises and gray areas of time series analysis.

In addition to some assumptions underlying the interpretation of certain values in the quantum mechanical formulation, one of the fundamental cornerstones to the entire theory lies in the commutator relationship between the position operator $\hat{x}$ and the momentum operator $\hat{p}$ :

[\hat{p}_i, \hat{x}_j] = -i \hbar \delta_{ij} ,

where δ_ij is the Kronecker delta.

Dependent physical constants

There are several related constants for which more than 99% of the uncertainty in the 2014 CODATA values^[19] is due to the uncertainty in the value of the Planck constant, as indicated by the square of the correlation coefficient (r² > 0.99, r > 0.995). The Planck constant is (with one or two exceptions)^[20] the fundamental physical constant which is known to the lowest level of precision, with a 1σ relative uncertainty u_r of 6992120000000000000♠1.2×10⁻⁸.

Rest mass of the electron

The normal textbook derivation of the Rydberg constant R_∞ defines it in terms of the electron mass m_e and a variety of other physical constants.

R_\infty = \frac{m_{\rm e} e^4}{8 \varepsilon_0^2 h^3 c_0} = \frac{m_{\rm e} c_0 \alpha^2}{2 h} .

However, the Rydberg constant can be determined very accurately (u_r = 6988590000000000000♠5.9×10⁻¹²) from the atomic spectrum of hydrogen, whereas there is no direct method to measure the mass of a stationary electron in SI units. Hence the equation for the computation of m_e becomes

m_{\rm e} = \frac{2 R_{\infty} h}{c_0 \alpha^2} ,

where c₀ is the speed of light and α is the fine-structure constant. The speed of light has an exactly defined value in SI units, and the fine-structure constant can be determined more accurately (u_r = 6990229999999999999♠2.3×10⁻¹⁰) than the Planck constant. Thus, the uncertainty in the value of the electron rest mass is due entirely to the uncertainty in the value of the Planck constant (r² > 0.999).

Avogadro constant

Main article: Avogadro constant

The Avogadro constant N_A is determined as the ratio of the mass of one mole of electrons to the mass of a single electron; the mass of one mole of electrons is the "relative atomic mass" of an electron A_r(e), which can be measured in a Penning trap (u_r = 6989290000000000000♠2.9×10⁻¹¹), multiplied by the molar mass constant M_u, which is defined as 6997100000000000000♠0.001 M.

N_{\rm A} = \frac{M_{\rm u} A_{\rm r}({\rm e})}{m_{\rm e}} = \frac{M_{\rm u} A_{\rm r}({\rm e}) c_0 \alpha^2}{2 R_{\infty} h} .

The dependence of the Avogadro constant on the Planck constant (r² > 0.999) also holds for the physical constants which are related to amount of substance, such as the atomic mass constant. The uncertainty in the value of the Planck constant limits the knowledge of the masses of atoms and subatomic particles when expressed in SI units. It is possible to measure the masses more precisely in atomic mass units, but not to convert them more precisely into kilograms.

Elementary charge

Main article: Elementary charge

Sommerfeld originally defined the fine-structure constant α as:

\alpha\ =\ \frac{e^2}{\hbar c_0 \ 4 \pi \varepsilon_0}\ =\ \frac{e^2 c_0 \mu_0}{2 h} ,

where e is the elementary charge, ε₀ is the electric constant (also called the permittivity of free space), and μ₀ is the magnetic constant (also called the permeability of free space). The latter two constants have fixed values in the International System of Units. However, α can also be determined experimentally, notably by measuring the electron spin g-factor g_e, then comparing the result with the value predicted by quantum electrodynamics.

At present, the most precise value for the elementary charge is obtained by rearranging the definition of α to obtain the following definition of e in terms of α and h:

e = \sqrt{\frac{2\alpha h}{\mu_0 c_0}} = \sqrt{{2\alpha h \varepsilon_0 c_0}} .

Bohr magneton and nuclear magneton

Main articles: Bohr magneton and Nuclear magneton

The Bohr magneton and the nuclear magneton are units which are used to describe the magnetic properties of the electron and atomic nuclei respectively. The Bohr magneton is the magnetic moment which would be expected for an electron if it behaved as a spinning charge according to classical electrodynamics. It is defined in terms of the reduced Planck constant, the elementary charge and the electron mass, all of which depend on the Planck constant: the final dependence on h^1/2 (r² > 0.995) can be found by expanding the variables.

\mu_{\rm B} = \frac{e \hbar}{2 m_{\rm e}} = \sqrt{\frac{c_0 \alpha^5 h}{32 \pi^2 \mu_0 R_{\infty}^2}}

The nuclear magneton has a similar definition, but corrected for the fact that the proton is much more massive than the electron. The ratio of the electron relative atomic mass to the proton relative atomic mass can be determined experimentally to a high level of precision (u_r = 6989950000000000000♠9.5×10⁻¹¹).

\mu_{\rm N} = \mu_{\rm B} \frac{A_{\rm r}({\rm e})}{A_{\rm r}({\rm p})}

Determination

Method	Value of h (6966100000000000000♠10⁻³⁴ J⋅s)	Relative uncertainty	Ref.
Watt balance	7000662606889000000♠6.62606889(23)	6992340000000000000♠3.4×10⁻⁸	^[21]^[22]^[23]
X-ray crystal density	7000662607450000000♠6.6260745(19)	6993290000000000000♠2.9×10⁻⁷	^[24]
Josephson constant	7000662606780000000♠6.6260678(27)	6993409999999999999♠4.1×10⁻⁷	^[25]^[26]
Magnetic resonance	7000662607240000000♠6.6260724(57)	6993859999999999999♠8.6×10⁻⁷	^[27]^[28]
Faraday constant	7000662606570000000♠6.6260657(88)	1.3×10⁻⁶	^[29]
CODATA 2010 recommended value	7000662606957000000♠6.62606957(29)	4.4×10⁻⁸	^[30]
The nine recent determinations of the Planck constant cover five separate methods. Where there is more than one recent determination for a given method, the value of h given here is a weighted mean of the results, as calculated by CODATA.

In principle, the Planck constant could be determined by examining the spectrum of a black-body radiator or the kinetic energy of photoelectrons, and this is how its value was first calculated in the early twentieth century. In practice, these are no longer the most accurate methods. The CODATA value quoted here is based on three watt-balance measurements of K_J²R_K and one inter-laboratory determination of the molar volume of silicon,^[31] but is mostly determined by a 2007 watt-balance measurement made at the U.S. National Institute of Standards and Technology (NIST).^[23] Five other measurements by three different methods were initially considered, but not included in the final refinement as they were too imprecise to affect the result.

There are both practical and theoretical difficulties in determining h. The practical difficulties can be illustrated by the fact that the two most accurate methods, the watt balance and the X-ray crystal density method, do not appear to agree with one another. The most likely reason is that the measurement uncertainty for one (or both) of the methods has been estimated too low – it is (or they are) not as precise as is currently believed – but for the time being there is no indication which method is at fault.

The theoretical difficulties arise from the fact that all of the methods except the X-ray crystal density method rely on the theoretical basis of the Josephson effect and the quantum Hall effect. If these theories are slightly inaccurate – though there is no evidence at present to suggest they are – the methods would not give accurate values for the Planck constant. More importantly, the values of the Planck constant obtained in this way cannot be used as tests of the theories without falling into a circular argument. Fortunately, there are other statistical ways of testing the theories, and the theories have yet to be refuted.^[31]

Josephson constant

The Josephson constant K_J relates the potential difference U generated by the Josephson effect at a "Josephson junction" with the frequency ν of the microwave radiation. The theoretical treatment of Josephson effect suggests very strongly that K_J = 2e/h.

K_{\rm J} = \frac{\nu}{U} = \frac{2e}{h}\,

The Josephson constant may be measured by comparing the potential difference generated by an array of Josephson junctions with a potential difference which is known in SI volts. The measurement of the potential difference in SI units is done by allowing an electrostatic force to cancel out a measurable gravitational force. Assuming the validity of the theoretical treatment of the Josephson effect, K_J is related to the Planck constant by

h = \frac{8\alpha}{\mu_0 c_0 K_{\rm J}^2}.

Watt balance

Main article: Watt balance

A watt balance is an instrument for comparing two powers, one of which is measured in SI watts and the other of which is measured in conventional electrical units. From the definition of the conventional watt W₉₀, this gives a measure of the product K_J²R_K in SI units, where R_K is the von Klitzing constant which appears in the quantum Hall effect. If the theoretical treatments of the Josephson effect and the quantum Hall effect are valid, and in particular assuming that R_K = h/e², the measurement of K_J²R_K is a direct determination of the Planck constant.

h = \frac{4}{K_{\rm J}^2 R_{\rm K}} .

Magnetic resonance

Main article: Gyromagnetic ratio

The gyromagnetic ratio γ is the constant of proportionality between the frequency ν of nuclear magnetic resonance (or electron paramagnetic resonance for electrons) and the applied magnetic field B: ν = γB. It is difficult to measure gyromagnetic ratios precisely because of the difficulties in precisely measuring B, but the value for protons in water at 7002298150000000000♠25 °C is known to better than one part per million. The protons are said to be "shielded" from the applied magnetic field by the electrons in the water molecule, the same effect that gives rise to chemical shift in NMR spectroscopy, and this is indicated by a prime on the symbol for the gyromagnetic ratio, γ′_p. The gyromagnetic ratio is related to the shielded proton magnetic moment μ′_p, the spin number I (I = ¹⁄₂ for protons) and the reduced Planck constant.

\gamma^{\prime}_{\rm p} = \frac{\mu^{\prime}_{\rm p}}{I \hbar} = \frac{2 \mu^{\prime}_{\rm p}}{\hbar}

The ratio of the shielded proton magnetic moment μ′_p to the electron magnetic moment μ_e can be measured separately and to high precision, as the imprecisely known value of the applied magnetic field cancels itself out in taking the ratio. The value of μ_e in Bohr magnetons is also known: it is half the electron g-factor g_e. Hence

\mu^{\prime}_{\rm p} = \frac{\mu^{\prime}_{\rm p}}{\mu_{\rm e}} \frac{g_{\rm e} \mu_{\rm B}}{2}

\gamma^{\prime}_{\rm p} = \frac{\mu^{\prime}_{\rm p}}{\mu_{\rm e}} \frac{g_{\rm e} \mu_{\rm B}}{\hbar}.

A further complication is that the measurement of γ′_p involves the measurement of an electric current: this is invariably measured in conventional amperes rather than in SI amperes, so a conversion factor is required. The symbol Γ′_p-90 is used for the measured gyromagnetic ratio using conventional electrical units. In addition, there are two methods of measuring the value, a "low-field" method and a "high-field" method, and the conversion factors are different in the two cases. Only the high-field value Γ′_p-90(hi) is of interest in determining the Planck constant.

\gamma^{\prime}_{\rm p} = \frac{K_{\rm J-90} R_{\rm K-90}}{K_{\rm J} R_{\rm K}} \Gamma^{\prime}_{\rm p-90}({\rm hi}) = \frac{K_{\rm J-90} R_{\rm K-90} e}{2} \Gamma^{\prime}_{\rm p-90}({\rm hi})

Substitution gives the expression for the Planck constant in terms of Γ′_p-90(hi):

h = \frac{c_0 \alpha^2 g_{\rm e}}{2 K_{\rm J-90} R_{\rm K-90} R_{\infty} \Gamma^{\prime}_{\rm p-90}({\rm hi})} \frac{\mu_{\rm p}^{\prime}}{\mu_{\rm e}} .

Faraday constant

Main article: Faraday constant

The Faraday constant F is the charge of one mole of electrons, equal to the Avogadro constant N_A multiplied by the elementary charge e. It can be determined by careful electrolysis experiments, measuring the amount of silver dissolved from an electrode in a given time and for a given electric current. In practice, it is measured in conventional electrical units, and so given the symbol F₉₀. Substituting the definitions of N_A and e, and converting from conventional electrical units to SI units, gives the relation to the Planck constant.

h = \frac{c_0 M_{\rm u} A_{\rm r}({\rm e})\alpha^2}{R_{\infty}} \frac{1}{K_{\rm J-90} R_{\rm K-90} F_{90}}

X-ray crystal density

The X-ray crystal density method is primarily a method for determining the Avogadro constant N_A but as the Avogadro constant is related to the Planck constant it also determines a value for h. The principle behind the method is to determine N_A as the ratio between the volume of the unit cell of a crystal, measured by X-ray crystallography, and the molar volume of the substance. Crystals of silicon are used, as they are available in high quality and purity by the technology developed for the semiconductor industry. The unit cell volume is calculated from the spacing between two crystal planes referred to as d₂₂₀. The molar volume V_m(Si) requires a knowledge of the density of the crystal and the atomic weight of the silicon used. The Planck constant is given by

h = \frac{M_{\rm u} A_{\rm r}({\rm e}) c_0 \alpha^2}{R_{\infty}} \frac{\sqrt{2}d^3_{220}}{V_{\rm m}({\rm Si})} .

Particle accelerator

The experimental measurement of the Planck constant in the Large Hadron Collider laboratory was carried out in 2011. The study called PCC using a giant particle accelerator helped to better understand the relationships between the Planck constant and measuring distances in space.

Fixation

Notes

1 2 3 4 5 Barry N. Taylor of the Data Center in close collaboration with Peter J. Mohr of the Physical Measurement Laboratory's Atomic Physics Division, Termed the "2014 CODATA recommended values," they are generally recognized worldwide for use in all fields of science and technology. The values became available on 25 June 2015 and replaced the 2010 CODATA set. They are based on all of the data available through 31 December 2014. Available: http://physics.nist.gov
↑ Giuseppe Morandi, F. Napoli, E. Ercolessi (2001), Statistical mechanics: an intermediate course, p. 84, ISBN 978-981-02-4477-4
↑ Einstein, Albert (2003), "Physics and Reality" (PDF), Daedalus 132 (4): 24, doi:10.1162/001152603771338742, The question is first: How can one assign a discrete succession of energy value $H σ$ to a system specified in the sense of classical mechanics (the energy function is a given function of the coordinates $q r$ and the corresponding momenta $p r$ )? The Planck constant $h$ relates the frequency $H σ /h$ to the energy values $H σ$ . It is therefore sufficient to give to the system a succession of discrete frequency values.
↑ "CODATA recommended values".
↑ R. Bowley, M. Sánchez (1999), Introductory Statistical Mechanics (2nd ed.), Oxford: Clarendon Press, ISBN 0-19-850576-0
1 2 3 4 5 Planck, Max (1901), "Ueber das Gesetz der Energieverteilung im Normalspectrum" (PDF), Ann. Phys. 309 (3): 553–63, Bibcode:1901AnP...309..553P, doi:10.1002/andp.19013090310 . English translation: "On the Law of Distribution of Energy in the Normal Spectrum".
↑ Kragh, Helge (1 December 2000), Max Planck: the reluctant revolutionary, PhysicsWorld.com
↑ Kragh, Helge (1999), Quantum Generations: A History of Physics in the Twentieth Century, Princeton University Press, p. 62, ISBN 0-691-09552-3
↑ Planck, Max (2 June 1920), The Genesis and Present State of Development of the Quantum Theory (Nobel Lecture)
↑ Previous Solvay Conferences on Physics, International Solvay Institutes, retrieved 12 December 2008
1 2 See, e.g., Arrhenius, Svante (10 December 1922), Presentation speech of the 1921 Nobel Prize for Physics
1 2 3 Lenard, P. (1902), "Ueber die lichtelektrische Wirkung", Ann. Phys. 313 (5): 149–98, Bibcode:1902AnP...313..149L, doi:10.1002/andp.19023130510
↑ Einstein, Albert (1905), "Über einen die Erzeugung und Verwandlung des Lichtes betreffenden heuristischen Gesichtspunkt" (PDF), Ann. Phys. 17 (6): 132–48, Bibcode:1905AnP...322..132E, doi:10.1002/andp.19053220607
1 2 3 Millikan, R. A. (1916), "A Direct Photoelectric Determination of Planck's h", Phys. Rev. 7 (3): 355–88, Bibcode:1916PhRv....7..355M, doi:10.1103/PhysRev.7.355
↑ Isaacson, Walter (2007-04-10), Einstein: His Life and Universe, ISBN 1-4165-3932-8 , pp. 309–314.
↑ "The Nobel Prize in Physics 1921". Nobelprize.org. Retrieved 2014-04-23.
↑ Smith, Richard (1962), "Two Photon Photoelectric Effect", Physical Review 128 (5): 2225, Bibcode:1962PhRv..128.2225S, doi:10.1103/PhysRev.128.2225. Smith, Richard (1963), "Two-Photon Photoelectric Effect", Physical Review 130 (6): 2599, Bibcode:1963PhRv..130.2599S, doi:10.1103/PhysRev.130.2599.4.
↑ Bohr, Niels (1913), "On the Constitution of Atoms and Molecules", Phil. Mag., Ser. 6 26 (153): 1–25, doi:10.1080/14786441308634993
↑ Mohr, Peter J.; Newell, David B.; Taylor, Barry N. (2015). "CODATA recommended values of the fundamental physical constants: 2014". Zenodo. arXiv:1507.07956. doi:10.5281/zenodo.22826.
↑ The main exceptions are the Newtonian constant of gravitation G (u_r = 6995470000000000000♠4.7×10⁻⁵) and the gas constant R (u_r = 6993570000000000000♠5.7×10⁻⁷). The uncertainty in the value of the gas constant also affects those physical constants which are related to it, such as the Boltzmann constant and the Loschmidt constant.
↑ Kibble, B P; Robinson, I A; Belliss, J H (1990), "A Realization of the SI Watt by the NPL Moving-coil Balance", Metrologia 27 (4): 173–92, Bibcode:1990Metro..27..173K, doi:10.1088/0026-1394/27/4/002
↑ Steiner, R.; Newell, D.; Williams, E. (2005), "Details of the 1998 Watt Balance Experiment Determining the Planck Constant" (PDF), Journal of Research (National Institute of Standards and Technology) 110 (1): 1–26
1 2 Steiner, Richard L.; Williams, Edwin R.; Liu, Ruimin; Newell, David B. (2007), "Uncertainty Improvements of the NIST Electronic Kilogram", IEEE Transactions on Instrumentation and Measurement 56 (2): 592–96, doi:10.1109/TIM.2007.890590
↑ Fujii, K.; Waseda, A.; Kuramoto, N.; Mizushima, S.; Becker, P.; Bettin, H.; Nicolaus, A.; Kuetgens, U.; Valkiers, S.; Taylor, P.; Debievre, P.; Mana, G.; Massa, E.; Matyi, R.; Kessler, E.G.; Hanke, M. (2005), "Present state of the Avogadro constant determination from silicon crystals with natural isotopic compositions", IEEE Transactions on Instrumentation and Measurement 54 (2): 854–59, doi:10.1109/TIM.2004.843101
↑ Sienknecht, Volkmar; Funck, Torsten (1985), "Determination of the SI Volt at the PTB", IEEE Transactions on Instrumentation and Measurement 34 (2): 195–98, doi:10.1109/TIM.1985.4315300 . Sienknecht, V.; Funck, T. (1986), "Realization of the SI Unit Volt by Means of a Voltage Balance", Metrologia 22 (3): 209–12, Bibcode:1986Metro..22..209S, doi:10.1088/0026-1394/22/3/018 . Funck, T.; Sienknecht, V. (1991), "Determination of the volt with the improved PTB voltage balance", IEEE Transactions on Instrumentation and Measurement 40 (2): 158–61, doi:10.1109/TIM.1990.1032905
↑ Clothier, W. K.; Sloggett, G. J.; Bairnsfather, H.; Currey, M. F.; Benjamin, D. J. (1989), "A Determination of the Volt", Metrologia 26 (1): 9–46, Bibcode:1989Metro..26....9C, doi:10.1088/0026-1394/26/1/003
↑ Kibble, B P; Hunt, G J (1979), "A Measurement of the Gyromagnetic Ratio of the Proton in a Strong Magnetic Field", Metrologia 15 (1): 5–30, Bibcode:1979Metro..15....5K, doi:10.1088/0026-1394/15/1/002
↑ Liu Ruimin; Liu Hengji; Jin Tiruo; Lu Zhirong; Du Xianhe; Xue Shouqing; Kong Jingwen; Yu Baijiang; Zhou Xianan; Liu Tiebin; Zhang Wei (1995), "A Recent Determination for the SI Values of γ′_p and 2e/h at NIM", Acta Metrologica Sinica 16 (3): 161–68
↑ Bower, V. E.; Davis, R. S. (1980), "The Electrochemical Equivalent of Pure Silver: A Value of the Faraday Constant", Journal of Research (National Bureau Standards) 85 (3): 175–91, doi:10.6028/jres.085.009
↑ P.J. Mohr, B.N. Taylor, and D.B. Newell (2011), "The 2010 CODATA Recommended Values of the Fundamental Physical Constants" (Web Version 6.0). This database was developed by J. Baker, M. Douma, and S. Kotochigova. Available: http://physics.nist.gov [Thursday, 02-Jun-2011 21:00:12 EDT]. National Institute of Standards and Technology, Gaithersburg, MD 20899.
1 2 Mohr, Peter J.; Taylor, Barry N.; Newell, David B. (2008). "CODATA Recommended Values of the Fundamental Physical Constants: 2006". Rev. Mod. Phys. 80 (2): 633–730. arXiv:0801.0028. Bibcode:2008RvMP...80..633M. doi:10.1103/RevModPhys.80.633. Direct link to value.
1 2 94th Meeting of the International Committee for Weights and Measures (2005). Recommendation 1: Preparative steps towards new definitions of the kilogram, the ampere, the kelvin and the mole in terms of fundamental constants
1 2 23rd General Conference on Weights and Measures (2007). Resolution 12: On the possible redefinition of certain base units of the International System of Units (SI).
↑ Taylor, B. N.; Mohr, P. J. (1999), "On the redefinition of the kilogram" (PDF), Metrologia 36 (1): 63–64, Bibcode:1999Metro..36...63T, doi:10.1088/0026-1394/36/1/11
↑ Draft Resolution A: On the possible future revision of the International System of Units, the SI (PDF)

References

Barrow, John D. (2002), The Constants of Nature; From Alpha to Omega – The Numbers that Encode the Deepest Secrets of the Universe, Pantheon Books, ISBN 0-375-42221-8

External links

Quantum of Action and Quantum of Spin – Numericana
Moriarty, Philip; Eaves, Laurence; Merrifield, Michael (2009). "h Planck's Constant". Sixty Symbols. Brady Haran for the University of Nottingham. Cite uses deprecated parameter |coauthors= (help)

Planck's natural units

Planck's constant Planck units

Base Planck units	Planck time Planck length Planck mass Planck charge Planck temperature

Derived Planck units	Planck energy Planck force Planck power Planck density Planck angular frequency Planck pressure Planck current Planck voltage Planck impedance Planck momentum Planck area Planck volume

This article is issued from Wikipedia - version of the Saturday, February 13, 2016. The text is available under the Creative Commons Attribution/Share Alike but additional terms may apply for the media files.