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Chemical Thermodynamics & Energetics Sontakke S.A.

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Presentation on theme: "Chemical Thermodynamics & Energetics Sontakke S.A."— Presentation transcript:

1 Chemical Thermodynamics & Energetics Sontakke S.A.

2 Chemical Thermodynamic s & Energetics First law of thermodynamics & its limitations

3 Statements Energy can neither be created nor be destroyed. One form of energy disappears exactly equivalent amount of some other form of energy reappears. Total energy of universe is constant. Total energy of an isolated system is constant. It is merely the law of conservation of energy

4 Limitations Limitations of the first law of thermodynamics are discussed below: 1. No restriction on the direction of the flow of heat: the first law establishes definite relationship between the heat absorbed and the work performed by a system. The first law does not indicate whether heat can flow from a cold end to a hot end or not. For example: we cannot extract heat from the ice or cold water by cooling it to a low temperature and use it to make the tea hot. This is possible by first law of thermodynamics.

5 . 2. Does not specify the feasibility of the reaction: first law does not specify that process is feasible or not for example: when a rod is heated at one end then equilibrium has to be obtained which is possible only by some expenditure of energy. 3. Practically it is not possible to convert the heat energy into an equivalent amount of work. To overcome this limitations, another law is needed which is known as second law of thermodynamics

6 Second law of thermodynamics The spontaneous flow of heat is always unidirectional, from higher temperature to lower temperature. Heat can not be converted into exactly equivalent amount of work without producing permanent changes either in system or surrounding. No machine yet to have unit efficiency.

7 Spontaneous and nonspontaneous process Definition:-It is the process that takes place of its own without the external influence.

8 Some examples are- 1. Flow of water from higher level to lower level. 2. Flow of heat from hot end to cold end. 3. Neutralization of acid by base. 4. Flow of gas from high pressure to low pressure.

9 Spontaneous Processes The gas in vessel B will spontaneously effuse into vessel A, but once the gas is in both vessels, it will not spontaneously

10 Characteristics of spontaneous process All spontaneous processes have a tendency to take place in particular direction on their own. Spontaneous process may be fast or slow Some spontaneous reaction may needs initiation.

11 All spontaneous processes proceed until a state of equilibrium is attained.

12 Processes that are spontaneous in one direction are nonspontane ous in the reverse direction.

13 Spontaneous Processes  Processes that are spontaneous at one temperature may be nonspontaneous at other temperatures.  Above 0  C it is spontaneous for ice to melt.  Below 0  C the reverse process is spontaneous.

14 Driving force that makes the process spontaneous 1. Energy and spontaneity All spontaneous process are exothermic, that it tend to have lowest potential energy and maximum stability.

15 Examples 1) combustion of 1 mol of carbon ΔH = -394 kJ/mol Formation of two mol of ammonia from nitrogen and hydrogen ΔH = 92.4 kJ Formation of 1 mol of water from hydrogen and oxygen Δ H =-285.7 kJ/mol

16 Limitation to criterion of decrease in enthalpy 1) Some endothermic reactions are also known to occur spontaneously. Such as Evaporation of water from open container or sea water ΔH =+44.0 kJ Dissolution of NH4Cl in water ΔH=+15.1 kJ

17 Reaction do not goes to completion even ΔH value is negative Reversible reaction also occurs. Forward reaction is exothermic while backward reaction is endothermic

18 2. Randomness or disorder & Spontaneity The process proceeds spontaneously in a direction in which the randomness or disorder of system increases.  Dissolution of solid:

19 Entropy Is this your room/ Then you already know about entropy

20 Definition :- It is measure of molecular disorder or randomness.

21 In general Gases have higher entropies than liquids. Liquids have higher entropies than solids. Entropy is greater for larger atoms. Entropy is greater for molecules with more atoms. S solid S liquid S gas 

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23 Examples Ar has higher entropy than Ne as Ar molecules are larger. C 8 H 18(l) has higher entropy than C 5 H 12(l) as complex molecules have higher entropy than simple ones. Br 2(g) has higher entropy than Br 2(l) as gases have higher entropies than liquids since gases have more ways of being arranged

24 By this criteria for any spontaneous process the entropy of system increases i.e ΔS system value is +ve E.g Iodine dissolve in water ΔS= +ve Hydrogen molecule into hydrogen atom ΔS= +ve Evaporation of water ΔS= +ve Ammonium chloride dissolved into water ΔS= +ve

25 Quantitative definition of entropy Instead of absolute entropy(S), entropy change(ΔS) is measured.

26 Entropy change of system in a process is amount of heat absorbed isothermally and reversibly divided by absolute temperature Mathematically it is expressed as  Unit of entropy change Since q is expressed in joule and temperature in kelvin ΔS is expressed in J /K

27 Entropy and second law of thermodynamics Entropy of system increases in spontaneous process However only entropy of system is not sufficient to talk about the spontaneity of process. Though ΔS value –ve,reaction is spontaneous, thus total entropy i.e system and surrounding is considered.

28 - The entropy of the universe always increases in a spontaneous process and remains unchanged in an equilibrium process ΔS> 0 “But ma, it’s not my fault… the universe wants my room like this!”>

29 Statement:-Total entropy of system and its surrounding(universe) increases in the spontaneous process. Entropy Change in the Universe The universe is composed of the system and the surroundings. Therefore,  S universe =  S system +  S surroundings For spontaneous processes  S universe > 0

30 Figure 20.10 Components of  S 0 universe for spontaneous reactions system becomes more disordered system becomes more ordered system becomes more disordered  S universe =  S system +  S surroundings

31 If entropy always increases, how can we account for the fact that water spontaneously freezes when placed in the freezer? Movement of compressor + Evaporation and condensation of refrigerant + Warming of air around container Net increase in the entropy of the universe

32 Gibbs energy and Gibbs energy change & spontaneity. Most of chemical reaction takes place either in closed system or open system, there is change of enthalpy as well as entropy takes place. It is not possible to achieve both factor [minimum energy and maximum stability] simultaneously,so new thermodynamic function is introduced called as Gibbs energy(G)

33 Definition:-It is the maximum amount of energy available to a system during a process that can be converted into useful work. Mathematical expression- G = H -TS Gibbs energy change is ΔG =ΔH -TΔS

34 Gibbs energy change:- = – Gibbs Free Energy

35 Make this equation nicer:

36 Practical uses: surroundings & system …Gibbs Free Energy  T  S universe is defined as the Gibbs free energy,  G. For spontaneous processes:  S universe > 0 And therefore:  G < 0  G is easier to determine than  S universe. So: Use  G to decide if a process is spontaneous.

37 1. If  G is negative, the forward reaction is spontaneous. 2. If  G is 0, the system is at equilibrium. 3. If  G is positive, the reaction is spontaneous in the reverse direction.  G as a criteria for spontaneity.

38 Free Energy and TemperatureFree Energy and Temperature

39 Temperature of equilibrium At equilibrium process is neither spontaneous nor nonspontaneous. So at equilbrium ΔG = 0,therefore the equation ΔG = ΔH –TΔS Can be written as 0 = ΔH –TΔS T= ΔH /ΔS

40 Gibbs energy change & equilibrium constant Q is the reaction quotiant Note: at equilibrium:  G = 0. and Q =K sign of  G tells which way reaction goes spontaneously.

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42 Third law of thermodynamics Entropy of a perfectly ordered crystalline substance is zero at absolute zero temperature.0 K Importance of this law is to determine absolute entropy of any substance. When substance at T=0 with S=0 is heated from 0 K to T K,the increase in entropy ΔS = S T - So= At T=0,S=0,thus ΔS = S T =

43 Calculating the Entropy Change  S o rxn =  n S o (products) -  m S o (reactants)

44 Sample Problem 20.1: Predicting Relative Entropy Values PROBLEM:Choose the member with the higher entropy in each of the following pairs, and justify your choice [assume constant temperature, except in part (e)]: (a) 1mol of SO 2 ( g ) or 1mol of SO 3 ( g ) (b) 1mol of CO 2 ( s ) or 1mol of CO 2 ( g ) (c) 3mol of oxygen gas (O 2 ) or 2mol of ozone gas (O 3 ) (d) 1mol of KBr( s ) or 1mol of KBr( aq ) (e) Seawater in midwinter at 2 0 C or in midsummer at 23 0 C (f) 1mol of CF 4 ( g ) or 1mol of CCl 4 ( g )

45 PLAN: In general less ordered systems have higher entropy than ordered systems and entropy increases with an increase in temperature. SOLUTION: (a) 1mol of SO 3 ( g ) - more atoms (b) 1mol of CO 2 ( g ) - gas > solid (c) 3mol of O 2 ( g ) - larger #mols (d) 1mol of KBr( aq ) - solution > solid (e) 23 0 C - higher temperature (f) CCl 4 - larger mass

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