Microscopic Reversibility
Microscopic reversibility is concerned with the behaviour of matter at the molecular level. To understand this concept clearly,…
The concept of fugacity is one of the most important concepts in chemical thermodynamics. It was introduced by Gilbert Newton Lewis in 1901 to explain the behavior of real gases. In thermodynamics, many equations such as those for chemical potential, equilibrium constant, and phase equilibrium are derived assuming that gases behave ideally. However, under practical conditions, especially at high pressures and low temperatures, gases deviate from ideal behavior. Therefore, pressure alone is not sufficient to describe the thermodynamic state of a real gas. To overcome this limitation, Lewis introduced the concept of fugacity, which replaces pressure in thermodynamic equations for real gases.
According to the kinetic theory of gases, an ideal gas satisfies the following assumptions:
Hence, an ideal gas obeys
$$
PV=nRT
$$
where
However, no gas is perfectly ideal. At high pressure, gas molecules come closer together and their finite size as well as intermolecular forces become important. Consequently, the observed pressure is no longer a true measure of the tendency of gas molecules to escape from the system. This deviation from ideal behavior necessitates the introduction of a corrected pressure known as fugacity.
The word fugacity is derived from the Latin word fugere, meaning “to flee” or “to escape”. Therefore, fugacity represents the tendency of molecules to escape from one phase into another.
For example, molecules of a compressed gas have a greater tendency to escape than molecules of a gas at low pressure. Thus, higher fugacity indicates a greater escaping tendency.
Fugacity is defined as the effective pressure or corrected pressure of a real gas that replaces the actual pressure in thermodynamic equations so that the equations become applicable to real gases.
In simple words, fugacity is the pressure that a real gas would have if it behaved ideally while possessing the same chemical potential.
It is denoted by the symbol
$$
\boxed{f}
$$
The SI unit of fugacity is Pascal (Pa), although bar and atmosphere are also commonly used.
Pressure measures the mechanical force exerted by gas molecules on the walls of a container. Fugacity, on the other hand, measures the escaping tendency of molecules from a phase.
If the escaping tendency increases, fugacity also increases. Therefore, fugacity is a thermodynamic quantity rather than merely a mechanical quantity.
For example:
For an ideal gas,
$$
\boxed{f=P}
$$
Thus, pressure itself represents the escaping tendency of an ideal gas.
For a real gas,
$$
\boxed{f\neq P}
$$
because intermolecular attractive and repulsive forces alter the effective escaping tendency of gas molecules.
At extremely low pressure,
$$
\boxed{\lim_{P\rightarrow0}\frac{f}{P}=1}
$$
This shows that every real gas approaches ideal behavior as the pressure approaches zero.
Fugacity is an effective or corrected pressure introduced by G. N. Lewis to describe the behavior of real gases. It represents the escaping tendency of gas molecules and replaces pressure in thermodynamic equations whenever real gases deviate from ideal behavior. At low pressure, fugacity becomes equal to pressure, whereas at high pressure it differs because of intermolecular interactions. Thus, fugacity provides a more accurate thermodynamic description of real gases than pressure alone.
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