According to van der Waals, the theorem of corresponding states, it tells that all fluids, when compared at the same reduced temperature and reduced pressure, have approximately the same compressibility factor and all deviate from ideal gas behaviour to about the same degree.
The Van der Waals equation is an equation of state that describes the behavior of real gases by accounting for the finite size of molecules and the intermolecular forces (attractive and repulsive) between them. It is a modification of the Ideal Gas Law to provide a more accurate description of real gases, especially under conditions of high pressure and low temperature, where ideal gas behavior breaks down.
The Van der Waals equation is given by:
Where:
1. P+ a/V2: This term accounts for the attractive forces between gas molecules. In real gases, molecules attract each other, which reduces the pressure exerted by the gas on the container walls. The term V2a adjusts for the intermolecular attraction (where "a" is a constant specific to the gas).
2. (V−b): This term corrects for the volume occupied by gas molecules. In the Ideal Gas Law, gas molecules are considered point masses, but real molecules have finite size and occupy a certain volume. The volume term b accounts for the effective volume occupied by the molecules themselves (where "b" is a constant specific to the gas).
3. RT: This represents the ideal gas contribution, where the gas behaves ideally and obeys the Ideal Gas Law.
This leads to the general form of the Van der Waals equation for real gases:
When the molar volume Vm is large, the term b becomes negligible, and the intermolecular forces term a/Vm2 becomes insignificant compared to the pressure. In such conditions, the Van der Waals equation simplifies to the Ideal Gas Law:
Thus, the Van der Waals equation provides a more accurate description of real gases by correcting for the finite size of molecules and their intermolecular interactions, while the Ideal Gas Law holds for gases that behave nearly ideally under conditions of low pressure and high temperature.
The principle of Corresponding States (PCS) was stated by van der Waals and reads: “Substances behave alike at the same reduced states. Substances at same reduced states are at corresponding states.” That is,
“Substances at corresponding states behave alike.”
Reduced properties are used to define corresponding states. Reduced properties provide a measure of the “departure” of the conditions of the substance from its own critical conditions and are defined as follows:
If Pr = Tr = vr = 1, the substance is at its critical condition. If we are beyond critical conditions, Tr > 1, Pr > 1 and vr > 1. By the same token, if all the conditions are subcritical, Tr < 1, Pr < 1 and vr < 1. Critical conditions become the scaling factor by which substances can be compared among each other in terms of their “departure from criticality” or reduced properties.
The PCS says that all gases behave alike at the same reduced conditions. That is, if two gases have the same “relative departure” from criticality (i.e., they are at the same reduced conditions), the corresponding state principle demands that they behave alike. In this case, the two conditions “correspond” to one another, and we are to expect those gases to have the same properties.
The Corresponding State Principle can be derived from vdW EOS. If we recall,
By substitution into the van der Waals equation we find:
The compressibility factor (Z) is a measure of how much a real gas deviates from ideal gas behavior. It is defined as:Where:
For ideal gases, the compressibility factor Z is always equal to 1. However, for real gases, Z varies depending on the conditions of pressure, temperature, and the specific gas.
The critical point refers to the temperature and pressure at which the liquid and gas phases of a substance become indistinguishable. It is characterized by:
At the critical point, the compressibility factor (Z) of a real gas is typically found to be close to 0.3 to 0.4, depending on the substance. This value is less than 1, indicating that the gas is more compressible than an ideal gas under the same conditions.
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