Second law of thermodynamics. It is known from everyday life that nature does the most probable thing when nothing prevents that For example it rains.

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Presentation transcript:

Second law of thermodynamics

It is known from everyday life that nature does the most probable thing when nothing prevents that For example it rains at cool weather because the liquid phase has less energy and the reaction is exothermic ΔH o H2O(g) = kJ/mole, ΔH o H2O(l) = kJ/mole Enthalpy considerations explain only a part of the way nature behaves as water also evaporates at certain conditions although it is an endothermic reaction The other part of the spontaneity discussions involve entropy, the degree of energy dispersion during a process Enthalpy and entropy are extensive properties of matter that simultaneously determine the direction of a change in its energy, similar to the way electric and magnetic forces affect matter at the same time

The first law of thermodynamics states that total energy of the universe is constant and all processes that involve transfer of energy from one form to other can happen The second law of thermodynamics restricts the processes that is considered possible by the first law to the most probable one that will happen under certain conditions set by the intensive properties of matter: The total entropy of any system plus that of its environment increases as a result of all natural processes The entropy of universe increases In all natural processes it has been found that the total entropy increases so natural processes tend to move toward a state of greater disorder. In short, the entropy of the universe should increase as a result of a spontaneous process just happened

Alternative statements of the second law The entropy of a given system can increase or decrease but the change in entropy of the system  S, plus the change in entropy of the environment  S env must be greater than or equal to zero It is impossible for an engine working in a cycle to transform a given amount of heat from a reservoir completely into work It is impossible to make a cyclic engine whose only effect is to transfer thermal energy from a colder body to a hotter body Heat can be completely converted into work in a single reversible process, but continuous conversion of heat into work requires a cyclic process ( a heat engine)

The total internal energy of the universe remains constant  U sys +  U surr =  U univ = 0 The total heat energy of the universe increases as a result of irreversible processes The total entropy of the universe increases  S univ =  S sys +  S surr > 0 Therefore the total energy available in the universe to do work decreases as a result of irreversible processes  H sys +  H surr =  H univ > 0 Comparing energy, enthalpy and entropy

Enthalpy of a system is the energy of the system at constant temperature and pressure However not all of that energy is available for the system to do work or contribute to a chemical reaction Recall that Entropy times temperature is not an energy but it controls the availability of energy to do work Consider the change in energy content of a process with temperature: The process will happen irreversibly when temperature exceeds T 6 where the process is in equilibrium Equilibrium condition

Example – Consider the combustion of propane to form CO 2 and H 2 O at 298 K: C 3 H 8 (g) +5O 2 (g)  3CO 2 (g) + 4H 2 O(l) At what temperature does the reverse reaction become spontaneous?  H = kJ; and  S = J/K at 298 K

Spontaneous dispersion of heat energy and the resultant increase in entropy The energy transfer between an open system and the surroundings Time

Spontaneous diffusion of molecules in the system and the resultant increase in entropy Time

Salt dissolving in water Solutions of comparable concentrations of species are complex such that the components interact with each other Entropy has dual effect upon salt dissolution in water: 1- Entropy is increased by the additional space occupied by the salt ions 2- Entropy is decreased by the orientation of water molecules around salt ions Time

Gibbs free energy and reaction spontaneity  G =  H - T  S If  S for a reaction is (+), reaction is favored due to higher freedom of the products If  H is (–), reaction is favored due to lower energy of the products so  G = (-) - (+) (+) = (-) since both entropy and enthalpy drive the reaction forward, the reaction must be spontaneous forward Thus a negative  G indicates a spontaneous forward reaction  G = - Forward reaction is spontaneous  G = + Reverse reaction is spontaneous  G = 0 Reaction is at equilibrium  G = Gibbs free energy (kJ/mole)  H = Enthalpy change (kJ/mole)  S = Entropy change (J/mole.K) T = Kelvin temperature (always +)

ΔH o H2O(g) = kJ/mole ΔH o H2O(l) = kJ/mole

-ΔS-ΔS

The effect of temperature on spontaneity is most strongly observed when enthalpy and entropy are of the same sign In this case when enthalpy and entropy factors affect Gibbs free energy oppositely, entropy factor TΔS dominates at high temperatures enthalpy factor ΔH dominates at low temperatures

Example - Oxidation of SO 2 (g) to SO 3 (g) happens during the production of sulfuric acid according to the reaction 2SO 2 (g) + O 2 (g) → 2SO 3 (g)  G = kJ;  H = kJ; and  S = J/K at 298 K Find out if this reaction is spontaneous at 25°C, and predict how  G will change with increasing T

Deciding on reaction spontaneity without calculation The signs of  H,  S and  G can be used to decide on the spontaneity of reactions as well as the temperature dependence of a reaction  H T K  S  G Reaction Direction SPONTANEOUS AT ALL TEMPERATURES NON SPONTANEOUS AT ALL TEMPERATURES / - SPONTANEOUS AT LOW TEMPERATURES / - SPONTANEOUS AT HIGH TEMPERATURES Example: If  H = Kcal for the reaction: 2 H 2 O 2 (l)  2 H 2 O (l) + O 2 (g) is the reaction spontaneous? Since  H is temperature independent, the reaction is exothermic at all temperatures and is favored by lower energy Two liquid molecules convert to two liquid and a gas molecule and is therefore favored by increasing entropy Both lower enthalpy (  H is negative) and increasing entropy (  S is positive) favor the forward reaction and the reaction is sure to be spontaneous at all temperatures

The standard Gibbs free energy of formation is the free energy change that occurs when 1 mole of substance is formed from its elements in their standard states at 1 atm and at 298 K The corresponding reaction for the standard Gibbs free energy of formation is the same as that for standard enthalpy of formation,    G o =  n  G o products -  m  G o reactants Example - Calculate the change in Gibbs free energy,  G° for the oxidation of ethyl alcohol to acetic acid using standard free energies of formation CH 3 CH 2 OH(l) + O 2 (g)  CH 3 COOH(l) + H 2 O(l)  G°, kJ/mol – –392.5 –237.2 n, mol n  G°, kJ– –392.5 –237.2  G° = –629.7 – (–174.8) = kJ

Example - Will this reaction occur spontaneously at 298 K? Mo 2 S 3 + 6Cu  3Cu 2 S + 2Mo DataΔH o 298 S o 298 abc Cu(s) Cu 2 S(s) Mo(s) Mo 2 S 3 (s)

The relationship between  G o and K at 298 K Example - Estimate  G o for the decomposition of NO 2 at 25 o C At 25 o C and 1.00 atmosphere pressure, K =4.3x FORWARD REACTION REVERSE REACTION

Example -The equilibrium constant at different temperatures for the following reaction is given: SO 3 (g) = SO 2 (g) + ½ O 2 (g) K= 900K K= 1000K K= 1100K Estimate the enthalpy change of the reaction at 1000K and the equilibrium composition at the same temperature