JEE Chemistry Thermodynamics Notes Set 06

Chemistry Concept Notes for JEE: Thermodynamics

Explore reliable concept summaries and revision materials through the JEE Chemistry Thermodynamics Notes Set 06. Tailored for JEE learners, utilizing these notes for Chemistry Thermodynamics ensures thorough preparation and strengthens core academic definitions before final evaluations.

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Access the complete concept summary PDF for Thermodynamics below. Regular review of these targeted notes builds familiarity with complex JEE Chemistry themes and helps secure higher marks in final school evaluations.

Basic Terms

System is the part of the universe under study; everything else is the surroundings. An open system exchanges matter and energy, a closed system exchanges only energy, and an isolated system exchanges neither.
State functions (P, V, T, E, H, S, G) depend only on the present state; path functions (heat q and work w) depend on how the change is carried out. Extensive properties (mass, volume, E, H, S, G) depend on the amount of matter; intensive properties (T, P, density, molar quantities) do not.
Process types: isothermal (T constant), isobaric (P constant), isochoric (V constant), adiabatic (q = 0), cyclic (initial = final state, so all state functions change by zero).

First Law of Thermodynamics

Energy can be neither created nor destroyed: \( \Delta E = q + w \), where w is work done on the system. With work done by the system written as w, \( \Delta E = q - w \).
Expansion work against constant external pressure: \( w = -P\Delta V \). Free expansion into vacuum: w = 0. Reversible isothermal work: \( w = -2.303\,nRT\log\dfrac{V_2}{V_1} \).
Isothermal ideal gas: \( \Delta E = 0 \) so q = -w. Adiabatic: q = 0 so \( \Delta E = w \). Isochoric: \( \Delta E = q_v \).

Enthalpy and Heat Capacity

\( H = E + PV \). At constant pressure \( q_p = \Delta H \); at constant volume \( q_v = \Delta E \). For reactions involving gases: \( \Delta H = \Delta E + \Delta n_g RT \), where \( \Delta n_g \) is moles of gaseous products minus moles of gaseous reactants.
\( C_p - C_v = R \) for one mole of an ideal gas. \( C_v = \tfrac32R \) for a monatomic gas and \( \tfrac52R \) for a diatomic gas (ignoring vibration). For an adiabatic reversible change \( TV^{\gamma-1} \) is constant, with \( \gamma = C_p/C_v \).

Thermochemistry

Exothermic reactions have \( \Delta H < 0 \); endothermic reactions have \( \Delta H > 0 \). Standard state: pure substance at 1 bar (about 1 atm) and the stated temperature, usually 298 K; the enthalpy of formation of an element in its standard state is zero.
Types: enthalpy of formation, combustion, neutralisation (about -57.3 kJ/mol for a strong acid and strong base; less negative for weak acids or bases because some energy is used in ionisation), fusion, vaporisation, sublimation, atomisation and bond dissociation.
Hess's law: the total enthalpy change of a reaction is the same whether it takes place in one step or several. \( \Delta H_{reaction} = \sum \Delta H_f(products) - \sum \Delta H_f(reactants) \). With bond energies: \( \Delta H = \sum (bonds\ broken) - \sum (bonds\ formed) \).
Kirchhoff's equation: \( \Delta H_2 - \Delta H_1 = \Delta C_p\,(T_2 - T_1) \).

Second and Third Laws, Entropy

Entropy S measures the randomness of a system. For a reversible process \( \Delta S = q_{rev}/T \). At a phase change \( \Delta S = \Delta H/T \). The entropy of a gas is much greater than that of a liquid, which is greater than that of a solid.
Second law: in a spontaneous process the total entropy of the system plus surroundings increases, \( \Delta S_{total} > 0 \); the entropy of the universe tends to a maximum. Third law: the entropy of a perfectly crystalline substance is zero at absolute zero.
Efficiency of a Carnot engine: \( \eta = 1 - T_2/T_1 = (T_1 - T_2)/T_1 \).

Gibbs Free Energy

\( \Delta G = \Delta H - T\Delta S \). A process is spontaneous if \( \Delta G < 0 \), at equilibrium if \( \Delta G = 0 \), and non-spontaneous if \( \Delta G > 0 \).
Cases: \( \Delta H<0, \Delta S>0 \) spontaneous at all temperatures; \( \Delta H>0, \Delta S<0 \) never spontaneous; \( \Delta H<0, \Delta S<0 \) spontaneous at low T; \( \Delta H>0, \Delta S>0 \) spontaneous at high T. The changeover temperature is \( T = \Delta H/\Delta S \).
\( \Delta G^\circ = -RT\ln K = -2.303\,RT\log K \). Maximum non-expansion (useful) work equals \( -\Delta G \).

Worked Examples

Example 1. Find \( \Delta E \) for \( 2NH_3(g)\rightarrow N_2(g)+3H_2(g) \) at 300 K if \( \Delta H = 92.4 \) kJ.
Answer:
\( \Delta n_g = 4-2 = 2 \).
\( \Delta E = \Delta H - \Delta n_gRT = 92.4 - 2(8.314\times10^{-3})(300) = 87.4 \) kJ.

Example 2. Above what temperature is a reaction with \( \Delta H = +30.56 \) kJ and \( \Delta S = 66 \) J/K spontaneous?
Answer:
\( T = \Delta H/\Delta S = 30560/66 = 463 \) K.
Above 463 K, \( \Delta G \) is negative.

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