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This review explores the energy flow within a system and its surroundings, focusing on the first law of thermodynamics and the exchange of energy as heat and work. It also discusses the state functions, thermochemistry, and the stability of products compared to reactants in endothermic and exothermic reactions. The review provides examples and calculations to illustrate these concepts.
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Review • system + surroundings Universe = • into system = • + • - • out of system = internal energy E = kinetic energy • + potential energy E = • K.E. - energy of motion P.E. - energy of position
Euniverse = 1st Law of Thermodynamics Energy can not be created or destroyed Euniverse= 0 Esystem + Esurroundings = 0 - Esurroundings Esystem = heat = q Energy is exchanged as : work = w E = q + w
heat flow of energy along a T gradient If T1 > T2 System at T1 Surroundings at T2 • q system Exothermic reaction • q surroundings
heat flow of energy along a T gradient If T1 < T2 System at T1 Surroundings at T2 > 0 • q system Endothermic reaction • q surroundings • < 0
work Electrical work Mechanical work = force x distance force = pressure x area = P x m2 distance = m work = = P x V P x m2 x m Pext V - Wsystem=
State Functions Property that depends only on the initial and final states Temperature, T : raise T from 298 300 K path 1 T = Tfinal - Tinitial= 300 - 298 = 2 K : raise T 298 500 K path 2 lower T from 500 300 K T = Tfinal - Tinitial = 300 - 298 = 2 K
Extensive v.s. Intensive Extensive: Proportional to the mass of the system Intensive: Independent of the mass of the system Temperature: Intensive or Extensive Volume : Intensive or Extensive Pressure: Intensive or Extensive Internal Energy: Intensive or Extensive
System 1 How much work will be done as the gas expands against the piston? Pext = 1.5 atm, T = 298 K P1 = 6.0 atm V1 = 0.4 L V2 = 1.6 L P2 = 1.5 atm P1 V1 = P2 V2 PV = nRT (6.0 atm) (0.4 L) = (1.5 atm) (V2) w = -PextV -(1.5 atm) -1.8 L atm w = (1.6 - 0.4)L = (-1.8 L atm) (101.3 J/L atm) = -182 J
System 2 How much work is done when the stopcock is opened? ideal gas vacuum 0.4 L 1.2 L 6.0 atm P1 = 6 atm P2 = 1.5 atm V1 = 0.4 L V2 = 1.2 + 0.4 L = 1.6 L T1 = 298 K = T2 P1 V1 = P2 V2 w = -PextV = -(0 atm) (1.6 L - 0.4 L) w = 0
System 1 System 2 P1 = P2 = V1 = V2 = T1 = T2 = 6.0 atm 1.5 atm P1 = P2 = V1 = V2 = T1 = T2 = 6.0 atm 1.5 atm 0.4 L 1.6 L 0.4 L 1.6 L 298 K 298 K w = -182 J q = +182 J w = 0 q = 0 Same initial and final conditions all State functions are the same E will be the same if T = 0, E = 0 Ideal gases : E = q + w = 0
Thermochemistry State 1 = State 2 = reactants products E = Eproducts - Ereactants Endothermicreaction 2NH3(g) + Ba(SCN)2(l) + 10H2O(l) + 2NH4SCN (s) Ba(OH)2•8H2O (s) reaction lowered T of system
EndothermicReaction Tprod< Treact K.E.prod < K.E.react P.E.prod> P.E.react productsless stable than reactants
Exothermic Reaction Tprod> Treact K.E.prod > K.E.react P.E.prod< P.E.react mix of gases C12H24O12 (s) + KClO3(s) products more stable than reactants