Avogadro's law is a gas law saying that "Equal volumes of ideal gases, at the same temperature and pressure, contain the same number of particles, or molecules." Thus, the number of molecules in a specific volume of gas is independent of the size or mass of the gas molecules.
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Avogadro's law is one of the gas laws. The law is named after Amedeo Avogadro, who in 1811 hypothesized that equal volumes of gases, at the same temperature and pressure, contain the same number of particles, or molecules. Thus, the number of molecules in a specific volume of gas is independent of the size or mass of the gas molecules.
The minor aspect of the law can be stated mathematically as:
- V is the volume of the gas.
- n is the number of moles in the gas.
- a is a constant.
However, this above equation is just a trivial one, which is valid
for all homogeneous substances, including homogeneous liquids and
solids. This relation is easy to deduce, its validity was assumed
before Avogadro's work.
The most important consequence of Avogadro's law is the following: The ideal gas constant has the same value for all gases. This means that the constant const of
has the same value for all gases, independent of the size or mass of the gas molecules. This statement is nontrivial, and it containts Avogadro's ingenious insight in the nature of ideal gases. It took decades to prove Avogadro's law based on the kinetic theory of gases.
One mole of an ideal gas occupies 22.4 liters (dm3) at STP (Standard conditions for temperature and pressure). This is often referred to as the molar volume of an ideal gas. Real gases may deviate from this value.
The number of molecules in one mole is called Avogadro's number: approximately 6.022×1023 particles per mole.
Avogadro's law, together with the combined gas law, forms the ideal gas law.
The Ideal gas law is the equation of state of a hypothetical ideal gas. It is a good approximation to the behavior of many gases under many conditions, although it has several limitations. It was first stated by Émile Clapeyron in 1834 as a combination of Boyle's law and Charles's law. It can also be derived from kinetic theory, as was achieved (apparently independently) by August Krönig in 1856 and Rudolf Clausius in 1857.
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