Avogadro constant

From Wikipedia, the free encyclopedia

The Avogadro constant (symbols: L, NA), also called Avogadro's number, is the number of atoms in exactly 12 grams of 12C. A mole is defined as this number of "entities" (usually, atoms or molecules) of any material. The currently accepted value for this number is:

N_A = (6.022 \, 141 \, 79\pm 0.000 \, 000 \, 30)\,\times\,10^{23} \mbox{ mol}^{-1} \,

The value of the Avogadro constant was first indicated by Johann Josef Loschmidt who, in 1865, computed the number of particles in one cubic centimetre of gas held at standard conditions. The term Loschmidt constant is thus more correctly applied for this value, which can be said to be proportional to the Avogadro constant. However, in the German language literature, "Loschmidt constant" refers to both this quantity as well as the number of entities in a mole.

Contents

History and etymology

The Avogadro constant is named after the early nineteenth century Italian scientist Amedeo Avogadro, who is credited (1811) with being the first to realize that the volume of a gas (strictly, of an ideal gas) is proportional to the number of atoms or molecules. The French chemist Jean Baptiste Perrin in 1909 proposed naming the constant in honour of Avogadro.

Loschmidt: Measuring the Avogadro Constant

Avogadro never attempted to measure the constant: the numerical value was first estimated by the Austrian physicist Johann Josef Loschmidt in 1865 using the kinetic theory of gases. In German-speaking countries, the constant is sometimes referred to as the Loschmidt constant or Loschmidt's number, but what Loschmidt actually measured is the number of particles per unit volume of an ideal gas, i.e. the number density of particles in an ideal gas. Thus, the term Loschmidt constant is more appropriate to the number of particles per unit of gas, Symbol: no:

n_\circ = \frac{p}{k_B T} \,

equal to (2.686 7774 ± 0.000 0047) × 1025 m−3 at 273.15 K and 101.325 kPa with kB the Boltzmann constant, T the temperature and p the pressure.

This constant is related to the Avogadro constant by the relation:

 R = N_Ak_B  \,

with kB the Boltzmann constant, and R the gas constant, hence

N_A = \frac{n_\circ R T}{p}  \,

However, in German scientific literature, the term Loschmidt constant is used ambiguously - it often refers to what has come to be known as the Avogadro constant. However, Boltzmann had first used the term for the sense in which Loschmidt had measured it - the number of particles in a unit volume of gas. Thus, its use in referring to the related Avogadro constant leads to confusion and is usually deprecated. For the same reason, sometimes the Avogadro constant is denoted as L as opposed to NA in German texts.

Standardization of the mole

Before 1960, there were conflicting definitions of the mole, and hence of Avogadro's Number (as it was known at the time), based on 16 grams of oxygen: physicists generally used oxygen-16 while chemists generally used the "naturally occurring" isotope ratio.

Switching, in 1960, to 12 grams of carbon-12 as the basis ended this dispute and had other advantages. At this time, Avogadro's Number was defined as the number of atoms in 12 grams of carbon-12, that is as a dimensionless quantity, while a mole was defined as one Avogadro number of atoms, molecules or other entities.

When the mole entered the International System of Units (SI), in 1971, the definitions were interchanged.

In 1971, a mole was defined as the number of atoms in 12 grams of carbon-12, with its own dimension, namely "amount of substance". Avogadro's number became a physical constant with the unit of reciprocal moles (mol−1).

Application

The Avogadro constant can be applied to any substance. It corresponds to the number of atoms or molecules needed to make up a mass equal to the substance's atomic or molecular mass, in grams. For example, the atomic mass of iron is 55.847 g/mol, so NA iron atoms (i.e. one mole of iron atoms) have a mass of 55.847 g. Conversely, 55.847 g of iron contains NA iron atoms. The Avogadro constant also enters into the definition of the unified atomic mass unit, u:

1 \ \mathrm{u} = \frac{1}{N_A} \ \mathrm{g} = (1.660 \, 538\, 86 \pm 0.000\, 000\, 28) 10^{-24} \ \mathrm{g}

Additional physical relations

Because of its role as a scaling factor, the Avogadro constant provides the link between a number of useful physical constants when moving between the atomic scale and the macroscopic scale. For example, it provides the relationship between:

 R = k_BN_A =   8.314 \, 472 \, \pm \, 0.000 \, 015 \, \mbox{J}\cdot\mbox{mol}^{-1}\mbox{K}^{-1}\,
in J mol−1 K−1
 F = N_Ae =   96 \, 485.3383 \, \pm \,0.0083 \,\, \mbox{C}\cdot\mbox{mol}^{-1} \,
in C mol−1

Measurement of the Avogadro constant

Ball-and-stick model of the unit cell of silicon.  X-ray diffraction experiments can determine the length of the cell, a, which can in turn be used to calculate a value for Avogadro's constant Ball-and-stick model of the unit cell of silicon. X-ray diffraction experiments can determine the length of the cell, a, which can in turn be used to calculate a value for Avogadro's constant

A number of methods can be used to measure the Avogadro constant. One modern method is to calculate the Avogadro constant from the density (ρ) of a crystal, the relative atomic mass (M), and the unit cell length (a) determined from x-ray crystallography. Very accurate values of these quantities for silicon have been measured at the National Institute of Standards and Technology (NIST) and used to obtain the value of the Avogadro constant:

 N_A  =  \frac{8M}{a^3\rho} \,
based on silicon (For silicon 8 is the unit cell density. For other types of cubic lattices, this number may vary.)

Trivia

Avogadro's number in binary starts out 11111111000011000011000… and is therefore closely approximated by a power of two, namely 279 = 6.0446 × 1023, about 0.4% high. A random number has about a one-in-a-hundred chance of being that close to a power of two.