Class 12 Chemistry Thermodynamics Notes

CHEMISTRY • CHAPTER 4

Chemical Thermodynamics

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Chemical Thermodynamics

Spontaneous and non-spontaneous process

A natural phenomena which proceed without any external assistance is called spontaneous and tendency of a process to occur naturally is called spontaneity.

A process which occurs by the help of external assistance is called non-spontaneous process or un-natural process.

Examples in spontaneous rxn

Dissolution of salt in water. Flow from high altitude to lower. Rusting of iron when exposed to moist air. Heat flow from hot body to cold body. Rxn bet’n HCl & NaOH to give NaCl & H2O etc.

Characteristics of spontaneous process

  1. It is uni-directional process. It takes place in one direction.
  2. Time has no role whether the rxn is fast or slow.
  3. It will be spontaneous unless it reaches to equilibrium.

Entropy (S)

The thermodynamic parameter which measures the degree of disorderliness or randomness of the molecules of system is called Entropy. It is denoted by S.

It is express in terms of its change & given by:

ΔS = Δq / T = Q / T

It’s unit is J K−1.

where,

  • ΔS = change in entropy
  • Q = Heat supply
  • T = Temperature in kelvin scale

Entropy is state function therefore it’s value depends on initial & final state of a system.

i.e. ΔS = S2 − S1

Entropy of Rxn [ΔSr]

The amount of entropy change when certain molar quantity of reactant are converted into product at given condition temperature & pressure. It is denoted by ΔSr & given by:

ΔSr = ΣΔSp − ΣΔSr

where,

  • ΔSr = Entropy change of rxn
  • ΔSp = Entropy of product
  • ΔSr = Entropy of reactant

Types of Entropy of Physical Transformation

i) Entropy of Fusion [ΔSfus]

The amount of entropy change when one mole of solid change into liquid at its melting point is called Entropy of Fusion. It is denoted by ΔSfus & given by:

ΔSfus = ΔHfus / Tm

where,

  • ΔSfus = Entropy of Fusion
  • ΔHfus = Latent heat of Fusion
  • Tm = melting point

ii) Entropy of vapourization [ΔSvap]

The amount of entropy change when one mole of liquid change into vapour at its boiling point is called entropy of vapourization. It is denoted by ΔSvap & given by:

ΔSvap = ΔHvap / Tb

where,

  • ΔHvap = Latent heat of Vapourization
  • Tb = Boiling point

iii) Entropy of transition [ΔStran]

The amount of entropy change when any one allotrops of the substance change into another allotropic of same substance is called Entropy of transition. It is denoted by ΔStran & given by:

ΔStran = ΔHtran / Tt

where,

  • ΔHtran = latent heat of transition
  • Tt = transition temp

iv) Entropy of sublimation [ΔSsub]

The amount of entropy change when 1 mole of solid change into vapour at its sublimation point is called Entropy of sublimation. It is denoted by ΔSsub & given by:

ΔSsub = ΔHsub / Tsub

where,

  • ΔHsub = Latent heat of sublimation
  • Tsub = sublimation temp

Molar entropy change (ΔSm)

The amount of entropy change by 1 mole of substance is called molar entropy change. Denoted by ΔSm. It’s unit is J K−1 mol−1.

Effect of temp on entropy

Entropy is directly proportional to temp. With increase in temp increases K.E., velocity of molecule as well as arrangement of molecule or disorderness or randomness. Hence entropy also increases.

Physical significance

Entropy is the degree of randomness or disorderness. It is also used to measure the unavailable energy of system which is not used to do useful work.

Entropy = unavailable energy / Temp

The order of entropy in gas, liquid and solid is:

ΔS(gas) > ΔS(liquid) > ΔS(solid)

Features of entropy

  • It is state function and extensive property.
  • It is expressed in terms of its change i.e. ΔS.
  • Entropy change in entropy is zero for cyclic process and at equilibrium.
  • For a spontaneous process there always increase in entropy i.e. ΔS > 0 or ΔS = +ve.

Entropy and Spontaneity

  • If ΔStotal > 0 i.e. ΔStotal = +ve then the process is spontaneous.
  • If ΔStotal < 0 i.e. ΔStotal = −ve then the process is non-spontaneous.
  • If ΔStotal = 0 then the process is cyclic or at an eqm.

Second law of thermodynamics

It states that, the entropy of universe [system + surrounding] continuously increase but total energy of universe remain.

Constant, i.e. ΔS > 0
or, ΔS = +ve
and ΔE = 0 (constant)

Explanation of Second law of thermodynamics

Consider a spontaneous flow of heat from a system higher temperature to lower temperature i.e. surrounding. Temperature of system and temperature of surrounding are Tsys and Tsurr respectively.

Temperature of system > Temperature of surrounding

Let the system evolves a quantity of heat spontaneously to the surrounding.

Now, system decrease the entropy which is given by:

ΔSsys = −Q / Tsys

and surrounding increases the entropy which is given by:

ΔSsurr = Q / Tsurr

Total entropy of universe:

ΔSuniv = ΔSsys + ΔSsurr

ΔSuniv = −Q/Tsys + Q/Tsurr

Since,

Tsys > Tsurr

Therefore:

1/Tsurr > 1/Tsys

ΔSuniv = +ve.

Total heat energy change = Q − Q = 0.

Hence, total energy of universe is unchanged whereas the total entropy of universe remain constant which is second law of thermodynamics.

Gibbs free energy change [ΔG]

It is the thermodynamic parameter which measures amount of energy available for doing useful work at constant temp and pressure. It is denoted by G and given by:

G = H − TS

where, H, T and S are enthalpy, temperature in kelvin scale and S is entropy respectively. H, T and S are state functions then G is also state function.

G1 = H1 − TS1   (initial state)

G2 = H2 − TS2   (final state)

Subtracting (2) from eqn (1):

G2 − G1 = (H2 − H1) − T(S2 − S1)

ΔG = ΔH − TΔS

This is the relation bet’n change in Gibbs free energy both change in enthalpy and change in entropy at constant temp and pressure called Gibbs-Helmholtz eqn.

Standard Gibbs free energy of formation (ΔG°f)

The amount of free energy change when one mole of compound is formed from its elements in given condition of temperature and pressure.

Standard Gibbs free energy change (ΔG°r)

The amount of Gibbs free energy change when certain molar quantities of reactant are converted into product at given condition of temp and pressure. It is denoted by ΔG°r and given by:

ΔG°r = Σ ΔG°f(product) − Σ ΔG°f(reactant)

where, ΣΔG°f(product) = Sum of standard free energy change of formation of product.

ΔG°f(reactant) = sum of standard free energy change of formation of reactant.

Relation bet’n standard free energy change and equilibrium constant

From eqn:

ΔG = ΔG° + RT ln Q   …(1)

where,

  • ΔG = Gibbs free energy change
  • ΔG° = Standard Gibbs free energy change
  • R = Universal gas constant
  • T = Temp in kelvin scale
  • Q = Rxn quotient

At eqm:

ΔG = 0 and Q is replaced by K where K is eqm constant.

0 = ΔG° + RT ln K

ΔG° = −RT ln K

ΔG° = −2.303 RT log K

This is the relation between standard Gibbs energy and eqm constant.

Relation bet’n Gibbs free energy change with total entropy

Let us consider a system which release heat energy to the surrounding spontaneously then total entropy change of universe is:

ΔSuniverse = ΔSsys + ΔSsurr

ΔSsurr = −Q/T + ΔSsys [as written in source]

When system and surrounding is carried at same T:

ΔSuniverse = −Q/T + ΔS

TΔSuniverse = −Q + TΔS

TΔSuniv = −ΔH + TΔS

TΔSuniv = −(ΔH − TΔS)

TΔSuniv = −ΔG

Gibbs free energy change and criteria for spontaneity

  1. If TΔSuniv > 0 then ΔG = −ve and the process is spontaneous.
  2. If TΔSuniv < 0 then ΔG = +ve and the process is non-spontaneous.
  3. If TΔSuniv = 0 then ΔG = 0 and the process is in equilibrium or cyclic process.
Process ΔG ΔS
Spontaneous−ve+ve
Non-spontaneous+ve−ve

Relation bet’n free energy change and useful work

Let w be the total work done which is the sum of useful work (net work) and mechanical (experimental work).

i.e. w = wuseful + PΔV

from 1st law of thermodynamics:

ΔQ = ΔE + PΔV

TΔS = ΔE + PΔV

TΔS = ΔE + wuseful + PΔV

TΔS = ΔH + wuseful

wuseful = TΔS − ΔH

wuseful = −(ΔH − TΔS)

wuseful = −ΔG

Gibbs-Helmholtz eqn of direct chemical change for exothermic and endothermic Rxn

We know Gibbs Helmholtz eqn:

ΔG = ΔH − TΔS

Given,

  • ΔG = Gibbs free energy
  • ΔH = enthalpy change
  • T = Temp in kelvin scale
  • ΔS = Entropy change

1) For exothermic Rxn [ΔH = −ve]

  1. If ΔS = +ve then ΔG = −ve and the process is spontaneous.
  2. If ΔS = −ve then ΔG = −ve or +ve and depends on temp:
    1. If temp is low, ΔG = −ve and process is spontaneous in given direction.
    2. If temp is high, ΔG = +ve and the process is non-spontaneous in the given direction.

2) For endothermic Rxn [ΔH = +ve]

  1. If ΔS = −ve then ΔG = +ve and the process is non-spontaneous.
  2. If temp is low, ΔG = +ve and the process is non-spontaneous in given direction.
  3. If temperature is high, ΔG = −ve and the process is spontaneous in given direction.

Hence, exothermic rxn is favoured at low temperature but endothermic rxn is favoured on high temperature.

Copper

Uses

  • It is used as an electrolytic soln in electroplating.
  • It is used as preservative for timber.
  • It is used as weedicide in water reservoirs and swimming pool.

Write the molecular formula of green-vitriol and mohr’s salt and also write its uses

Green-vitriol / hepta-hydrated ferrous sulphate: FeSO4·7H2O

  • It is used as reducing agent.

Mohr’s salt: [FeSO4·(NH4)2SO4·6H2O]

  • It is used as reducing agent.
  • It is used in volumetric analysis for standardization of KMnO4 soln.
This “Copper” page appears as page 11 of the supplied Chapter 4 PDF, so it has been preserved in the typed notes in the same source sequence.

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