Thermodynamic State Variables And Equation Of State

Thermodynamic State Variables And Equation Of State

Vishal kumarUpdated on 02 Jul 2025, 06:28 PM IST

Thermodynamic variables such as temperature, pressure, volume and internal energy are what define the state of a thermodynamic system whose importance cannot be overemphasized. However, the quartet is crucial in deploying the attributes of the state. As such, the equation of state seeks to harmonize them all.

This Story also Contains

  1. Definition of Thermodynamic Variables
  2. What are the Extensive and Intensive properties/variables
  3. What is the Equation of state?
  4. What is the Thermodynamic process?
  5. What is the State and Path function?
  6. Solved Examples Based on Thermodynamic Variables and Equation of State
  7. Summary

In this article, we will cover the concept of the 'Thermodynamic variables and equation of state’. This topic falls under the broader category of Thermodynamics, which is a crucial chapter in Class 11 physics. It is not only essential for board exams but also for competitive exams like the Joint Entrance Examination (JEE Main), National Eligibility Entrance Test (NEET), and other entrance exams such as SRMJEE, BITSAT, WBJEE, BCECE and more. Over the last ten years of the JEE Main exam (from 2013 to 2023), two questions have been asked on this concept. And for NEET one question was asked from this concept.

Let's read this entire article to gain an in-depth understanding of thermodynamic variables and the equation of state.

Definition of Thermodynamic Variables

Thermodynamic variables: Any thermodynamic system can be described by specifying some of the variables i.e. its pressure(P), volume(V), temperature(T), internal energy(U) and the number of moles(n). These parameters are called thermodynamic variables.

What are the Extensive and Intensive properties/variables

Intensive properties do not depend on the amount of matter that is present. These are bulk properties. Examples of intensive properties are - Density, Temperature etc. and the Extensive properties are those properties which depend on the amount of matter that is present. Examples of extensive properties are - Volume, Weight etc.

What is the Equation of state?

The relation between the thermodynamic variables (P, V, T) of the system is called the equation of state.

For n moles of an ideal gas, the equation of state is PV = nRT

For n moles of a real gas equation of state is $(P + \frac{an^{2}}{V^{2}})(V- nb) = nRT$

What is the Thermodynamic process?

The process of change of state of a system involves the change of thermodynamic variables such as pressure P, volume V and temperature T of the system. The process is known as the thermodynamic process.

Some important processes are

(i) Isothermal process (ii) Adiabatic process (iii) Isobaric process (iv) Isochoric process

(v) Cyclic and non-cyclic process (vi) Reversible and irreversible process

Later, we will study all these processes one by one in detail.

What is the State and Path function?

State or Point function does not depend on the path followed by the thermodynamic process but it depends on the final and initial position of the process. The Path function depends on the path followed by a thermodynamic process and not on the initial and final states of the system. An example of a point function is Internal energy and an example of a path function is Heat and work.

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Solved Examples Based on Thermodynamic Variables and Equation of State

Example 1: One mole of an ideal gas passes through a process where pressure and volume obey the relation $P = P_0 [ 1- \frac{1}{2}\left ( \frac{V_0}{V} \right )^2]$ .Here $P_0$ and $V_0$ are constant. Calculate the change in temperature of gas if its volume changes from $V_0 \: \: to \: \: 2 V_0$ :

1) $\frac{1P_0 V_0 }{2R}$

2) $\frac{5 P_0 V_0 }{4 R}$

3) $\frac{3 P_0 V_0 }{4 R}$

4) $\frac{ P_{0} V_{0}}{4 R}$

Solution:

$PV=nRT$

$\frac{nRT }{V} = P_0 [ 1- \frac{1}{2}\left ( \frac{V_0}{V} \right )^2] \\\\ \\T = \frac{P_0 V }{nR} [ 1- \frac{1}{2}\left ( \frac{V_0}{V} \right )^2] \\\\ T_i = \frac{P_0 V_0 }{R} [ 1- \frac{1}{2}\left ( \frac{V_0^2}{V_0^2} \right )].... at \ V = V_0 \\\\ T_f = \frac{P_0 2V_0 }{R} [ 1- \frac{1}{8}\left ( \frac{V_0^2}{V_0^2} \right )].... \ at \ V = 2 V_0$

$\delta T = T_f - T_i = \frac{7 P_0 V_0 }{4 R } - \frac{P_0 V_0 }{2 R } = \frac{5 P_0 V_0 }{4 R }$

Hence, the answer is the option (2).

Example 2: Which of the following is not a thermodynamic variable?

1) Pressure

2) Temperature

3) Momentum

4) Volume

Solution:

Thermodynamics Variable

Parameters which define the Thermodynamics system.

e.g. pressure, volume, temperature

Hence, the answer is the option 3.

Example 3: Which of the following parameters does not characterize the thermodynamic state of matter?

1) Temperature

2) Pressure

3) Work

4) Volume

Solution:

Equation of state

The relation between the Thermodynamics variable (P, V, T) of the system is called an equation of state.

PV=nRT

(P, V, T) represent the Thermodynamic state of matter.

Work does not represent the thermodynamic state of matter.

Hence, the answer is the option (3).

Example 4: Which one of the following statements is false?

1) Work is a state function

2) Temperature is a state function

3) Change in the state is completely defined when the initial and final states are specified.

4) Work appears at the boundary of the system.

Solution:

As we have learnt,
Path functions are properties or quantities whose values depend on the transition of a system from the initial state to the final state.
E.g.: Work, heat, loss of energy due to friction, etc. are some common examples of a path function.
Hence, the answer is the option 1.

Example 5: $\left(\mathrm{P}+\frac{\mathrm{a}}{\mathrm{V}^2}\right)(\mathrm{V}-\mathrm{b})=\mathrm{RT}$ represents the equation of the state of some gases. Where P is the pressure, V is the volume, T is the temperature, and a, b, and R are the constants. The physical quantity, which has a dimensional formula as that of $\frac{b^{2}}{a}$ will be :

1) Compressibility

2) Energy density

3) Modulus of rigidity

4) Bulk modulus

Solution:

$\begin{aligned} & {[\mathrm{b}]=\left[\mathrm{L}^3\right]} \\ & \begin{aligned} {[\mathrm{a}] } & =\left[\mathrm{PV}^2\right] \\ & =\left[\mathrm{ML}^{-1} \mathrm{~T}^{-2}\right]\left[\mathrm{L}^6\right] \\ & =\left[\mathrm{ML}^5 \mathrm{~T}^{-2}\right] \end{aligned} \\ & \frac{\left[\mathrm{b}^2\right]}{[\mathrm{a}]}=\frac{\left[\mathrm{L}^6\right]}{\left[\mathrm{ML}^5 \mathrm{~T}^{-2}\right]}=\left[\mathrm{M}^{-1} \mathrm{~L}^1 \mathrm{~T}^2\right] \end{aligned}$

Hence, the answer is the Option (1).

Summary

Temperature, pressure, and volume are examples of thermodynamic variables while internal energy is another important one. The state of a thermodynamic system is described in terms of temperature, pressure, volume, and internal energy, and these properties are called the thermodynamic variables. Formulated as an equation, this equation describes how the system behaves under different circumstances as the arrangement that connects these variables altogether. Such relationships enable us to know how the system will behave under various conditions.

Frequently Asked Questions (FAQs)

Q: What is the relationship between state variables and thermodynamic cycles?
A:
Thermodynamic cycles, such as the Carnot cycle or refrigeration cycle, are described by a series of processes that eventually return the system to its initial state. State variables are crucial for analyzing these cycles because the change in any state variable over a complete cycle must be zero. This property allows us to calculate efficiencies and work outputs of cycles, which is fundamental in the design of heat engines, refrigerators, and power plants.
Q: How do state variables behave in systems with long-range interactions, like plasmas or gravitational systems?
A:
In systems with long-range interactions, the behavior of state variables can deviate significantly from that in conventional thermodynamic systems. For example, the concept of extensivity may break down, and the system may exhibit negative heat capacities or other counterintuitive properties. Understanding these behaviors is crucial in fields like astrophysics and plasma physics, where long-range forces dominate system behavior.
Q: What is the significance of the triple point in terms of state variables?
A:
The triple point is a unique set of conditions (specific values of state variables like temperature and pressure) where three phases of a substance coexist in equilibrium. It's a fixed point on a substance's phase diagram and is often used as a reference point. For example, the triple point of water is used to define the Kelvin temperature scale. Understanding the triple point is crucial in fields like cryogenics and in calibrating thermometers.
Q: How do state variables relate to the concept of fugacity in thermodynamics?
A:
Fugacity is a state variable that replaces pressure in chemical potential expressions for real gases. It's a measure of the tendency of a substance to escape from a phase. Fugacity is related to other state variables through equations of state and is crucial for accurately describing phase equilibria and chemical equilibria in non-ideal systems. This concept is particularly important in chemical engineering and petroleum engineering for modeling complex mixtures and processes.
Q: What is the significance of the virial equation of state?
A:
The virial equation of state is a series expansion that describes deviations from
Q: How do equations of state help in predicting phase behavior?
A:
Equations of state help predict phase behavior by relating state variables like pressure, volume, and temperature. They can be used to construct phase diagrams, which show how a substance behaves under different conditions. For instance, the van der Waals equation can predict the existence of a liquid phase and critical point, which the ideal gas law cannot. This predictive power is crucial in fields like petroleum engineering and chemical processing, where understanding phase behavior is essential.
Q: Why is it important to distinguish between state functions and path functions in thermodynamics?
A:
Distinguishing between state functions (which depend only on the current state) and path functions (which depend on the path taken between states) is crucial in thermodynamics. State functions, like internal energy or entropy, allow us to analyze systems without knowing their history. Path functions, like heat or work, are important for understanding specific processes. This distinction is key to applying the First Law of Thermodynamics and calculating changes in system properties correctly.
Q: Why is it important to understand the behavior of state variables near phase transitions?
A:
Near phase transitions, many state variables exhibit unusual behavior. For example, heat capacity often spikes, and compressibility can become very large. Understanding these behaviors is crucial for accurately predicting system properties and behavior during processes involving phase changes. This knowledge is applied in diverse fields, from designing efficient heat exchangers to understanding geological processes like volcanic eruptions.
Q: How do equations of state account for intermolecular forces?
A:
Real gas equations of state, unlike the ideal gas law, incorporate terms to account for intermolecular forces. For example, the van der Waals equation includes a term (a/V^2) to account for attractive forces and another (b) for the volume occupied by molecules. More sophisticated equations like the Peng-Robinson or Redlich-Kwong equations provide even better approximations for real gas behavior. Understanding these modifications is crucial for accurately predicting gas behavior in high-pressure or low-temperature conditions.
Q: What is the significance of partial molar quantities in thermodynamics?
A:
Partial molar quantities describe how an extensive property of a mixture changes when the amount of one component is varied while keeping pressure, temperature, and the amounts of other components constant. They are crucial for understanding the behavior of mixtures and solutions. For example, the partial molar volume explains why the total volume of a mixture might not be the sum of the volumes of its components. This concept is essential in fields like solution thermodynamics and chemical engineering.