constant

avogadro constant

Number of constituent particles per mole
Value
\(N_{A} = 6.02214076 \times 10^{23}\)per mole
5 related articles · 1 formulas

Description

The Avogadro constant is the number of atoms, molecules, or other particles in one mole of a substance. Its value is approximately 6.022 × 10^23 per mole. This constant bridges the microscopic world of individual particles and the macroscopic world of grams and liters, allowing chemists and physicists to count particles by weighing bulk material.

History

The concept was introduced by Amedeo Avogadro in 1811, though he did not determine the number itself. The first accurate estimate came from Johann Josef Loschmidt in 1865, and the constant was later named in Avogadro's honor. The modern value was precisely determined in the 20th century through X-ray crystallography and other techniques.

How it works

The constant is defined so that the mass of one mole of a substance in grams equals its atomic or molecular mass in atomic mass units. For example, one mole of carbon-12 atoms has a mass of exactly 12 grams and contains Avogadro's number of atoms. This works because the atomic mass unit is defined as one-twelfth the mass of a carbon-12 atom, and the mole is defined as the amount of substance containing as many elementary entities as there are atoms in 12 grams of carbon-12.

In practice

The Avogadro constant is essential in chemistry for stoichiometry, in physics for defining the mole and the kilogram (until 2019, when the kilogram was redefined using the Planck constant), and in biology for calculating concentrations of solutions.

Fun fact

If you had Avogadro's number of pennies, they would cover the entire Earth's surface to a depth of about 1.6 kilometers.

Concept graph →

Formulas

$$-\frac{dE}{dx} = \frac{4\pi N_A r_e^2 m_e c^2 \rho z^2}{A \beta^2} \left[ \ln\left(\frac{2m_e \gamma^2 v^2 W_{\text{max}}}{I^2}\right) - 2\beta^2 - \delta - 2\frac{C}{Z} \right]$$
Energy loss of charged particles due to ionization in matter.
What is in the formula
EvariableKinetic energy of the charged particle — energy joule
xvariablePath length in the material — length metre
\rhovariableDensity of the absorbing material — density kilogram per cubic metre
zvariableCharge number of the incident particle — charge number
AvariableAtomic mass number of the absorber — atomic mass number
\betavariableSpeed of the particle relative to the speed of light — velocity ratio
\gammavariableLorentz factor of the particle — lorentz factor
vvariableSpeed of the particle — velocity metre per second
W_{\text{max}}variableMaximum energy transfer in a single collision — energy joule
IvariableMean excitation potential of the absorber — energy joule
\deltavariableDensity correction factor — density correction
CvariableShell correction factor — shell correction
ZvariableAtomic number of the absorber — atomic number
N_AconstantNumber of constituent particles per mole — avogadro constant = 6.02214076e23 per mole
r_econstantRadius of a classical electron — classical electron radius = 2.8179403262e-15 metre
m_econstantRest mass of the electron — electron mass = 9.1093837015e-31 kilogram
cconstantSpeed of light in vacuum — speed of light = 299792458 metre per second
-\frac{d}{dx}operatorNegative derivative with respect to path length — negative derivative
\lnoperatorNatural logarithm — natural logarithm

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