The Ideal Gas Law relates pressure, volume, molecular quantity, and temperature of an ideal gas together in one neat mathematical expression:
P
V = nRT
Where,
P = Absolute pressure
(atmospheres)
V = Volume (liters)
n = Gas quantity (moles)
R = Universal gas
constant (0.0821 L · atm / mol · K)
T = Absolute temperature
(K)
An alternative form of
the Ideal Gas Law uses the number of actual gas molecules (N) instead of the
number of moles of molecules (n):
P
V = NkT
Where,
P = Absolute pressure
(atmospheres)
V = Volume (liters)
N = Gas quantity (moles)
k = Boltzmann’s constant
(1.38 × 10−23 J / K)
T = Absolute temperature
(K)
Although no gas in real
life is ideal, the Ideal Gas Law is a close approximation for conditions of
modest gas density, and no phase changes (gas turning into liquid or
visa-versa).
Since the molecular
quantity of an enclosed gas is constant, and the universal gas constant must be
constant, the Ideal Gas Law may be written as a proportionality instead of an
equation:
P
V ∝ T
Several “gas laws” are
derived from this Ideal Gas Law. They are as follows:
P V = Constant Boyle’s
Law (assuming constant temperature T)
V ∝ T Charles’s Law
(assuming constant pressure P)
P ∝ T Gay-Lussac’s Law
(assuming constant volume V )
You will see these laws
referenced in explanations where the specified quantity is constant (or very
nearly constant).
For non-ideal conditions,
the “Real” Gas Law formula incorporates a corrected term for the
compressibility of the
gas:
P
V = ZnRT
Where,
P = Absolute pressure
(atmospheres)
V = Volume (liters)
Z = Gas compressibility
factor (unitless)
n = Gas quantity (moles)
R = Universal gas
constant (0.0821 L · atm / mol · K)
T = Absolute temperature
(K)
The compressibility
factor for an ideal gas is unity (Z = 1), making the Ideal Gas Law a limiting
case of the Real Gas Law. Real gases have compressibility factors less than
unity (< 1). What this means is real gases tend to compress more than the
Ideal Gas Law would predict (i.e. occupies less volume for a given amount of
pressure than predicted, and/or exerts less pressure for a given volume than
predicted).
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