CBSE Class 11 Chemistry Revision Notes Chapter 5 Thermodynamics
Thermodynamics studies energy changes in chemical reactions and physical processes. In CBSE Class 11 Chemistry Chapter 5, students learn how heat, work, internal energy, enthalpy, entropy and Gibbs free energy help explain whether a process can occur.
Chemical reactions involve energy changes. Some reactions release heat, some absorb heat, and some can perform work. Thermodynamics gives a framework to measure these changes and connect them with the direction of a process.
These CBSE class 11 chemistry revision notes chapter 5 follow the chapter in a quick revision format. The chapter begins with system and surroundings, then moves to internal energy, heat, work, first law of thermodynamics, enthalpy, calorimetry, Hess’s law, entropy, Gibbs free energy and equilibrium constant.
Key Takeaways
- Thermodynamics: Study of energy changes in physical and chemical processes.
- System and surroundings: The part under study is the system, and everything else is the surroundings.
- First law: Energy can be transferred as heat or work, but total energy remains conserved.
- Enthalpy: Heat change at constant pressure is measured as enthalpy change.
- Gibbs free energy: It helps predict whether a process is spontaneous.
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Thermodynamics Class 11 Chemistry Notes: Chapter Overview
Thermodynamics explains how energy changes take place during reactions and physical processes. It deals with measurable properties such as pressure, volume, temperature, heat and work.
Class 11 Chemistry Chapter 5 Notes help students understand how energy conservation, heat transfer and entropy decide the feasibility of a process. The chapter also explains why some reactions occur naturally while others need external energy.
| Topic | What Students Learn |
| Thermodynamics | Energy changes in chemical and physical processes |
| System and surroundings | Part under study and everything around it |
| Types of systems | Open system, closed system and isolated system |
| State functions | Properties depending only on state |
| Internal energy | Total energy of a system |
| Heat and work | Modes of energy transfer |
| First law of thermodynamics | Energy conservation |
| Enthalpy | Heat content at constant pressure |
| Heat capacity | Heat required to raise temperature |
| Calorimetry | Measurement of heat change |
| Hess’s law | Enthalpy change through different paths |
| Entropy | Measure of randomness or disorder |
| Gibbs free energy | Criterion for spontaneity |
| Equilibrium constant | Link between Gibbs energy and equilibrium |
What Is Thermodynamics?
Thermodynamics is the branch of Chemistry that studies energy changes during chemical reactions and physical processes. It focuses on macroscopic properties of matter, such as pressure, volume and temperature.
Thermodynamics does not explain the speed of a reaction. It tells whether a process is energetically possible and how much energy change is involved.
| Point | Explanation |
| Main focus | Energy transformation |
| Used for | Heat, work, enthalpy and spontaneity |
| Deals with | Macroscopic systems |
| Helps predict | Direction and feasibility of processes |
System and Surroundings
System and surroundings are the basic terms used in thermodynamics.
A system is the part of the universe selected for study. The surroundings include everything outside the system that can exchange energy or matter with it.
Universe = System + Surroundings
| Term | Meaning | Example |
| System | Part under observation | Reaction mixture in a beaker |
| Surroundings | Everything outside the system | Air and room around the beaker |
| Boundary | Real or imaginary surface separating system and surroundings | Wall of a beaker |
Types of Thermodynamic Systems
Thermodynamic systems are classified based on exchange of matter and energy.
| Type of System | Exchange of Matter | Exchange of Energy | Example |
| Open system | Yes | Yes | Open beaker |
| Closed system | No | Yes | Closed vessel |
| Isolated system | No | No | Thermos flask |
Open System
An open system can exchange both matter and energy with the surroundings. An open beaker containing a reaction mixture is an example.
Closed System
A closed system can exchange energy but does not exchange matter. A closed conducting vessel is an example.
Isolated System
An isolated system exchanges neither matter nor energy with the surroundings. A thermos flask is a common example.
State of a System
The state of a system is described by measurable properties such as pressure, volume, temperature and amount of substance.
These properties define the condition of the system at a given moment.
| Property | Symbol |
| Pressure | p |
| Volume | V |
| Temperature | T |
| Amount of substance | n |
When these properties are fixed, the state of the system is defined.
State Functions
State functions are properties whose values depend only on the present state of the system. They do not depend on the path used to reach that state.
| State Function | Meaning |
| Internal energy | Total energy of the system |
| Enthalpy | Heat content at constant pressure |
| Entropy | Measure of disorder |
| Gibbs free energy | Energy available for useful work |
| Pressure | Force per unit area |
| Volume | Space occupied |
| Temperature | Degree of hotness |
Heat and work are path functions because their values depend on how the process is carried out.
Internal Energy
Internal energy is the total energy stored in a system. It includes all forms of molecular energy, such as translational, rotational, vibrational, electronic and chemical energy.
It is represented by U.
A system’s absolute internal energy cannot be measured directly, but the change in internal energy can be measured.
ΔU = U₂ - U₁
| Situation | Internal Energy Change |
| System absorbs energy | Internal energy increases |
| System releases energy | Internal energy decreases |
| Work done on system | Internal energy increases |
| Work done by system | Internal energy decreases |
Heat
Heat is energy transferred between system and surroundings because of temperature difference.
It is represented by q.
| Sign of q | Meaning |
| q is positive | Heat is absorbed by the system |
| q is negative | Heat is released by the system |
Heat is measured in joule or kilojoule.
Work
Work is another mode of energy transfer. In Chemistry, pressure-volume work is commonly studied.
When a gas expands or compresses, work is done.
w = -pΔV
| Situation | Work Sign |
| Work done on the system | Positive |
| Work done by the system | Negative |
| Expansion | Work is done by the system |
| Compression | Work is done on the system |
First Law of Thermodynamics
First law of thermodynamics states that energy can neither be created nor destroyed. It can only be transferred from one form to another.
Mathematically:
ΔU = q + w
| Term | Meaning |
| ΔU | Change in internal energy |
| q | Heat exchanged |
| w | Work done |
This law is also called the law of conservation of energy.
First Law for Different Conditions
| Condition | Equation | Meaning |
| Constant volume | ΔU = qᵥ | Heat absorbed equals change in internal energy |
| Adiabatic process | q = 0, ΔU = w | Energy change happens through work |
| Free expansion | w = 0 | No work is done |
| Isolated system | q = 0 and w = 0 | ΔU = 0 |
Thermodynamic Processes
Thermodynamic processes are changes that take a system from one state to another.
| Process | Constant Quantity | Main Feature |
| Isothermal process | Temperature | ΔT = 0 |
| Adiabatic process | Heat exchange | q = 0 |
| Isobaric process | Pressure | p remains constant |
| Isochoric process | Volume | ΔV = 0 |
Isothermal Process
In an isothermal process, temperature remains constant. For an ideal gas, internal energy depends only on temperature, so ΔU is zero.
Adiabatic Process
In an adiabatic process, no heat is exchanged between the system and surroundings.
Isobaric Process
In an isobaric process, pressure remains constant.
Isochoric Process
In an isochoric process, volume remains constant. Since ΔV = 0, no pressure-volume work is done.
Enthalpy
Enthalpy is a thermodynamic state function represented by H.
H = U + pV
At constant pressure, heat absorbed or released is equal to enthalpy change.
ΔH = qₚ
| Sign of ΔH | Meaning |
| ΔH is positive | Endothermic process |
| ΔH is negative | Exothermic process |
Relation Between ΔH and ΔU
For reactions involving gases:
ΔH = ΔU + ΔnᵍRT
| Term | Meaning |
| ΔH | Enthalpy change |
| ΔU | Internal energy change |
| Δnᵍ | Moles of gaseous products minus moles of gaseous reactants |
| R | Gas constant |
| T | Temperature in kelvin |
The difference between ΔH and ΔU is more important when gases are involved.
Extensive and Intensive Properties
Extensive and intensive properties help describe thermodynamic systems.
| Property Type | Meaning | Examples |
| Extensive properties | Depend on amount of substance | Mass, volume, internal energy, enthalpy |
| Intensive properties | Do not depend on amount of substance | Temperature, pressure, density |
If a system is divided into two equal parts, extensive properties are divided, but intensive properties remain the same.
Heat Capacity
Heat capacity is the amount of heat required to raise the temperature of a system by one degree Celsius or one kelvin.
q = CΔT
| Term | Meaning |
| q | Heat supplied |
| C | Heat capacity |
| ΔT | Change in temperature |
Molar Heat Capacity
Molar heat capacity is the heat required to raise the temperature of one mole of a substance by one degree.
Specific Heat Capacity
Specific heat capacity is the heat required to raise the temperature of unit mass of a substance by one degree.
Relationship Between Cp and Cv
For one mole of an ideal gas:
Cp - Cv = R
| Term | Meaning |
| Cp | Heat capacity at constant pressure |
| Cv | Heat capacity at constant volume |
| R | Universal gas constant |
This relation is useful for ideal gases.
Calorimetry
Calorimetry is the experimental method used to measure heat changes in physical and chemical processes.
The instrument used is called a calorimeter.
| Measurement | Condition |
| ΔU | Constant volume |
| ΔH | Constant pressure |
Bomb Calorimeter
A bomb calorimeter measures heat change at constant volume. It is commonly used for combustion reactions.
Coffee Cup Calorimeter
A coffee cup calorimeter measures heat change at constant pressure. It is commonly used for reactions in solution.
Enthalpy Change
Enthalpy change is the heat absorbed or released during a process at constant pressure.
| Type of Enthalpy Change | Meaning |
| Enthalpy of reaction | Heat change during a chemical reaction |
| Enthalpy of formation | Heat change when one mole of compound forms from elements |
| Enthalpy of combustion | Heat change when one mole of substance burns completely |
| Enthalpy of atomisation | Heat change when one mole of gaseous atoms forms |
| Enthalpy of neutralisation | Heat change when acid and base react to form water |
| Enthalpy of solution | Heat change when solute dissolves in solvent |
Standard Enthalpy Change
Standard enthalpy change is the enthalpy change measured under standard conditions.
| Standard Condition | Value |
| Pressure | 1 bar |
| Temperature | Usually 298 K |
| Concentration for solutions | 1 mol L⁻¹ |
It is represented by ΔH°.
Hess’s Law
Hess’s law states that the total enthalpy change for a reaction remains the same whether the reaction takes place in one step or several steps.
This is because enthalpy is a state function.
| Use of Hess’s Law | Explanation |
| Calculate unknown enthalpy changes | Uses known reactions |
| Find enthalpy of formation | Uses formation equations |
| Calculate combustion enthalpy | Uses combustion data |
| Support energy conservation | Total heat change remains fixed |
Hess’s Law Example
If a reaction can be written as the sum of two or more reactions, the enthalpy change of the main reaction equals the sum of the enthalpy changes of those reactions.
ΔH = ΔH₁ + ΔH₂ + ΔH₃
Bond Enthalpy and Reaction Enthalpy
Bond enthalpy is the energy required to break one mole of bonds in gaseous molecules.
For a reaction:
ΔH = Bond enthalpy of bonds broken - Bond enthalpy of bonds formed
| Step | Energy Change |
| Breaking bonds | Requires energy |
| Forming bonds | Releases energy |
| Overall reaction | Difference between the two |
Spontaneous Process
A spontaneous process is a process that can take place on its own under given conditions.
A spontaneous process may be slow or fast. Thermodynamics only tells whether the process is possible, not the rate of the process.
| Example | Why It Is Spontaneous |
| Heat flows from hot body to cold body | Natural direction of heat flow |
| Gas expands into vacuum | Greater freedom of movement |
| Ice melts above 0°C | Favoured at that temperature |
Non Spontaneous Process
A non spontaneous process does not occur on its own under given conditions. It needs continuous external help.
| Process | Reason |
| Heat flowing from cold body to hot body | Needs external work |
| Water moving uphill | Needs external energy |
| Gas compressing by itself | Needs external pressure |
Entropy
Entropy is a thermodynamic state function that measures the randomness or disorder of a system. It is represented by S.
Higher disorder means higher entropy.
| Change | Entropy Effect |
| Solid to liquid | Entropy increases |
| Liquid to gas | Entropy increases |
| Gas to liquid | Entropy decreases |
| More gas molecules formed | Entropy increases |
| Fewer gas molecules formed | Entropy decreases |
Entropy helps explain the direction of natural processes.
Entropy Change
Entropy change is represented as ΔS.
For a reversible process:
ΔS = qrev / T
| Term | Meaning |
| ΔS | Entropy change |
| qrev | Heat absorbed reversibly |
| T | Temperature in kelvin |
A process is favoured when total entropy of the universe increases.
Gibbs Free Energy
Gibbs free energy is a thermodynamic function that helps predict spontaneity at constant temperature and pressure.
It is represented by G.
ΔG = ΔH - TΔS
| Term | Meaning |
| ΔG | Gibbs free energy change |
| ΔH | Enthalpy change |
| T | Temperature in kelvin |
| ΔS | Entropy change |
Gibbs Free Energy and Spontaneity
| Value of ΔG | Meaning |
| ΔG < 0 | Process is spontaneous |
| ΔG > 0 | Process is non spontaneous |
| ΔG = 0 | System is at equilibrium |
Gibbs free energy connects enthalpy and entropy in one equation.
Effect of Temperature on Spontaneity
The spontaneity of a process depends on ΔH, ΔS and temperature.
| ΔH | ΔS | Spontaneity |
| Negative | Positive | Spontaneous at all temperatures |
| Positive | Negative | Non spontaneous at all temperatures |
| Negative | Negative | Spontaneous at low temperature |
| Positive | Positive | Spontaneous at high temperature |
Gibbs Free Energy and Equilibrium Constant
Gibbs free energy is related to equilibrium constant.
ΔG° = -RT ln K
| Term | Meaning |
| ΔG° | Standard Gibbs free energy change |
| R | Gas constant |
| T | Temperature |
| K | Equilibrium constant |
| Value of K | Meaning |
| K > 1 | Products are favoured |
| K < 1 | Reactants are favoured |
| K = 1 | Reactants and products are comparable |
When ΔG° is negative, K is greater than 1 and products are favoured.
Thermodynamics Class 11 Chemistry Chapter 5 CBSE Notes: Quick Revision Tables
Important Formulae
| Concept | Formula |
| Universe | System + Surroundings |
| Change in internal energy | ΔU = q + w |
| Pressure-volume work | w = -pΔV |
| Enthalpy | H = U + pV |
| Enthalpy change at constant pressure | ΔH = qₚ |
| Relation between ΔH and ΔU | ΔH = ΔU + ΔnᵍRT |
| Heat supplied | q = CΔT |
| Heat with specific heat | q = mcΔT |
| Ideal gas heat capacities | Cp - Cv = R |
| Entropy change | ΔS = qrev / T |
| Gibbs free energy | ΔG = ΔH - TΔS |
| Gibbs energy and equilibrium | ΔG° = -RT ln K |
System Types Summary
| Type | Matter Exchange | Energy Exchange |
| Open system | Yes | Yes |
| Closed system | No | Yes |
| Isolated system | No | No |
State and Path Functions
| State Functions | Path Functions |
| Internal energy | Heat |
| Enthalpy | Work |
| Entropy | |
| Gibbs free energy | |
| Pressure | |
| Volume | |
| Temperature |
Thermodynamic Processes
| Process | Constant Quantity | Key Point |
| Isothermal | Temperature | ΔT = 0 |
| Adiabatic | Heat exchange | q = 0 |
| Isobaric | Pressure | Pressure remains fixed |
| Isochoric | Volume | Work is zero |
Key Terms from CBSE Class 11 Chemistry Revision Notes Chapter 5
| Key Term | Meaning |
| Thermodynamics | Study of energy changes |
| System | Part of universe under study |
| Surroundings | Everything outside the system |
| Boundary | Surface separating system and surroundings |
| Open System | Exchanges matter and energy |
| Closed System | Exchanges energy but not matter |
| Isolated System | Exchanges neither matter nor energy |
| State Function | Property depending only on state |
| Internal Energy | Total energy of a system |
| Heat | Energy transfer due to temperature difference |
| Work | Energy transfer due to force or volume change |
| First Law of Thermodynamics | Energy conservation law |
| Enthalpy | Heat content at constant pressure |
| Heat Capacity | Heat needed to raise temperature |
| Calorimetry | Measurement of heat change |
| Hess’s Law | Total enthalpy change is path independent |
| Entropy | Measure of disorder |
| Gibbs Free Energy | Energy function used to predict spontaneity |
| Spontaneous Process | Process that can occur on its own |
| Non Spontaneous Process | Process that needs external help |
| Equilibrium Constant | Ratio showing extent of reaction at equilibrium |
Useful Links for CBSE Class 11 Chemistry
| Section | Useful Links |
| Syllabus | CBSE Class 11 Chemistry Syllabus |
| Revision Notes | CBSE Class 11 Chemistry Revision Notes |
| NCERT Solutions | NCERT Solutions Class 11 Chemistry |
| Sample Papers | CBSE Sample Papers for Class 11 Chemistry |
| Important Questions | Important Questions Class 11 Chemistry |
| NCERT Books | NCERT Books for Class 11 Chemistry |
| Class 11 Support | CBSE Class 11 Syllabus |
| NCERT Solutions | NCERT Solutions for Class 11 |
FAQs (Frequently Asked Questions)
The first law of thermodynamics states that energy can neither be created nor destroyed. It is expressed as ΔU = q + w.
Heat is energy transfer due to temperature difference. Work is energy transfer caused by force, movement or volume change.
Enthalpy helps measure heat change at constant pressure. Since many chemical reactions occur at constant pressure, ΔH becomes useful for reaction heat calculations.
Entropy tells us about disorder or randomness in a system. A process is favoured when the total entropy of the universe increases.
Gibbs free energy uses the equation ΔG = ΔH – TΔS. If ΔG is negative, the process is spontaneous. If ΔG is positive, the process is non spontaneous.
