Download presentation
Presentation is loading. Please wait.
Published byAdele Boyd Modified over 8 years ago
2
1 THERMOCHEMISTRY Thermodynamics The study of Heat and Work and State Functions
3
2 TEKS (A) understand energy and its forms, including kinetic, potential, chemical, and thermal energies; (B) understand the law of conservation of energy and the processes of heat transfer; (C) use thermochemical equations to calculate energy changes that occur in chemical reactions and classify reactions as exothermic or endothermic; (D) perform calculations involving heat, mass, temperature change, and specific heat; and (E) use calorimetry to calculate the heat of a chemical process.
4
3 Energy & Chemistry ENERGY is the capacity to do work or transfer heat. HEAT is the form of energy that flows between 2 objects because of their difference in temperature. Other forms of energy — lightlight electricalelectrical kinetic and potentialkinetic and potential
5
4 Energy & Chemistry peanuts supply sufficient energy to boil a cup of water.Burning peanuts supply sufficient energy to boil a cup of water. Burning sugar (sugar reacts with KClO 3, a strong oxidizing agent)Burning sugar (sugar reacts with KClO 3, a strong oxidizing agent)
6
5 Energy & Chemistry These reactions are PRODUCT FAVOREDThese reactions are PRODUCT FAVORED They proceed almost completely from reactants to products, perhaps with some outside assistance.They proceed almost completely from reactants to products, perhaps with some outside assistance.
7
6 Energy & Chemistry 2 H 2 (g) + O 2 (g) --> 2 H 2 O(g) + heat and light 2 H 2 O(g) + heat and light This can be set up to provide ELECTRIC ENERGY in a fuel cell. Oxidation: 2 H 2 ---> 4 H + + 4 e - Reduction: 4 e - + O 2 + 2 H 2 O ---> 4 OH - CCR, page 845
8
7 Potential & Kinetic Energy Potential energy — energy a motionless body has by virtue of its position.
9
8 Positive and negative particles (ions) attract one another. Two atoms can bond As the particles attract they have a lower potential energy Potential Energy on the Atomic Scale NaCl — composed of Na + and Cl - ions.
10
9 Positive and negative particles (ions) attract one another. Two atoms can bond As the particles attract they have a lower potential energy Potential Energy on the Atomic Scale
11
10 Potential & Kinetic Energy Kinetic energy — energy of motion Translation Translation
12
11 Potential & Kinetic Energy Kinetic energy — energy of motion.
13
12 Internal Energy (E) PE + KE = Internal energy (E or U)PE + KE = Internal energy (E or U) Int. E of a chemical system depends onInt. E of a chemical system depends on number of particlesnumber of particles type of particlestype of particles temperaturetemperature
14
13 Internal Energy (E) PE + KE = Internal energy (E or U)PE + KE = Internal energy (E or U)
15
14 Internal Energy (E) The higher the T the higher the internal energyThe higher the T the higher the internal energy So, use changes in T (∆T) to monitor changes in E (∆E).So, use changes in T (∆T) to monitor changes in E (∆E).
16
15 ThermodynamicsThermodynamics Thermodynamics is the science of heat (energy) transfer. Heat energy is associated with molecular motions. Heat transfers until thermal equilibrium is established.
17
16 Directionality of Heat Transfer Heat always transfer from hotter object to cooler one. EXO thermic: heat transfers from SYSTEM to SURROUNDINGS. T(system) goes down T(surr) goes up
18
17 Directionality of Heat Transfer Heat always transfer from hotter object to cooler one. ENDO thermic: heat transfers from SURROUNDINGS to the SYSTEM. T(system) goes up T (surr) goes down
19
18 Energy & Chemistry All of thermodynamics depends on the law of CONSERVATION OF ENERGY. The total energy is unchanged in a chemical reaction.The total energy is unchanged in a chemical reaction. If PE of products is less than reactants, the difference must be released as KE.If PE of products is less than reactants, the difference must be released as KE.
20
19 Energy Change in Chemical Processes PE of system dropped. KE increased. Therefore, you often feel a T increase.
21
20 UNITS OF ENERGY 1 calorie = heat required to raise temp. of 1.00 g of H 2 O by 1.0 o C. 1000 cal = 1 kilocalorie = 1 kcal 1 kcal = 1 Calorie (a food “calorie”) But we use the unit called the JOULE 1 cal = 4.184 joules James Joule 1818-1889
22
21 HEAT CAPACITY The heat required to raise an object’s T by 1 ˚C. Which has the larger heat capacity?
23
22 Specific Heat Capacity How much energy is transferred due to T difference? The heat (q) “lost” or “gained” is related to a)sample mass b) change in T and c) specific heat capacity
24
23 Specific Heat Capacity SubstanceSpec. Heat (J/gK) H 2 O4.184 Ethylene glycol2.39 Al0.897 glass0.84 Aluminum
25
24 Specific Heat Capacity If 25.0 g of Al cool from 310 o C to 37 o C, how many joules of heat energy are lost by the Al?
26
25 Specific Heat Capacity If 25.0 g of Al cool from 310 o C to 37 o C, how many joules of heat energy are lost by the Al? heat gain/lose = q = (sp. ht.)(mass)(∆T) where ∆T = T final - T initial q = (0.897 J/gK)(25.0 g)(37 - 310)K q = - 6120 J Notice that the negative sign on q signals heat “lost by” or transferred OUT of Al.
27
26 Heat Transfer No Change in State q transferred = (sp. ht.)(mass)(∆T)
28
27 Heat Transfer with Change of State Changes of state involve energy (at constant T) Ice + 333 J/g (heat of fusion) -----> Liquid water q = (heat of fusion)(mass)
29
28 Heat Transfer and Changes of State Requires energy (heat). This is the reason a)you cool down after swimming b)you use water to put out a fire. + energy Liquid ---> Vapor
30
29 Heat water Evaporate water Melt ice Heating/Cooling Curve for Water Note that T is constant as ice melts
31
30 Heat of fusion of ice = 333 J/g Specific heat of water = 4.2 J/gK Heat of vaporization = 2260 J/g Heat of fusion of ice = 333 J/g Specific heat of water = 4.2 J/gK Heat of vaporization = 2260 J/g What quantity of heat is required to melt 500. g of ice and heat the water to steam at 100 o C? Heat & Changes of State +333 J/g +2260 J/g
32
31 How much heat is required to melt 500. g of ice and heat the water to steam at 100 o C? 1. To melt ice q = (500. g)(333 J/g) = 1.67 x 10 5 J q = (500. g)(333 J/g) = 1.67 x 10 5 J 2.To raise water from 0 o C to 100 o C q = (500. g)(4.2 J/gK)(100 - 0)K = 2.1 x 10 5 J q = (500. g)(4.2 J/gK)(100 - 0)K = 2.1 x 10 5 J 3.To evaporate water at 100 o C q = (500. g)(2260 J/g) = 1.13 x 10 6 J q = (500. g)(2260 J/g) = 1.13 x 10 6 J 4. Total heat energy = 1.51 x 10 6 J = 1510 kJ Heat & Changes of State
33
32 Chemical Reactivity What drives chemical reactions? How do they occur? The first is answered by THERMODYNAMICS and the second by KINETICS. Have already seen a number of “driving forces” for reactions that are PRODUCT-FAVORED. formation of a precipitateformation of a precipitate gas formationgas formation H 2 O formation (acid-base reaction)H 2 O formation (acid-base reaction) electron transfer in a batteryelectron transfer in a battery
34
33 Chemical Reactivity But energy transfer also allows us to predict reactivity. In general, reactions that transfer energy to their surroundings are product- favored. So, let us consider heat transfer in chemical processes.
35
34 Heat Energy Transfer in a Physical Process CO 2 (s, -78 o C) ---> CO 2 (g, -78 o C) Heat transfers from surroundings to system in endothermic process.
36
35 Heat Energy Transfer in a Physical Process CO 2 (s, -78 o C) ---> CO 2 (g, -78 o C)CO 2 (s, -78 o C) ---> CO 2 (g, -78 o C) A regular array of molecules in a solid -----> gas phase molecules.A regular array of molecules in a solid -----> gas phase molecules. Gas molecules have higher kinetic energy.Gas molecules have higher kinetic energy.
37
36 Energy Level Diagram for Heat Energy Transfer Transfer ∆E = E(final) - E(initial) = E(gas) - E(solid) CO 2 solid CO 2 gas
38
37 Heat Energy Transfer in Physical Change Gas molecules have higher kinetic energy.Gas molecules have higher kinetic energy. Also, WORK is done by the system in pushing aside the atmosphere.Also, WORK is done by the system in pushing aside the atmosphere. CO 2 (s, -78 o C) ---> CO 2 (g, -78 o C) Two things have happened!
39
38 FIRST LAW OF THERMODYNAMICS ∆E = q + w heat energy transferred energychange work done by the system Energy is conserved!
40
39 heat transfer out (exothermic), -q heat transfer in (endothermic), +q SYSTEMSYSTEM ∆E = q + w w transfer in (+w) w transfer out (-w)
41
40 ENTHALPYENTHALPY Most chemical reactions occur at constant P, so and so ∆E = ∆H + w (and w is usually small) ∆H = heat transferred at constant P ≈ ∆E ∆H = change in heat content of the system ∆H = H final - H initial and so ∆E = ∆H + w (and w is usually small) ∆H = heat transferred at constant P ≈ ∆E ∆H = change in heat content of the system ∆H = H final - H initial Heat transferred at constant P = q p q p = ∆H where H = enthalpy Heat transferred at constant P = q p q p = ∆H where H = enthalpy
42
41 If H final < H initial then ∆H is negative Process is EXOTHERMIC If H final < H initial then ∆H is negative Process is EXOTHERMIC If H final > H initial then ∆H is positive Process is ENDOTHERMIC If H final > H initial then ∆H is positive Process is ENDOTHERMIC ENTHALPYENTHALPY ∆H = H final - H initial
43
42 Consider the formation of water H 2 (g) + 1/2 O 2 (g) --> H 2 O(g) + 241.8 kJ USING ENTHALPY Exothermic reaction — heat is a “product” and ∆H = – 241.8 kJ
44
43 Making liquid H 2 O from H 2 + O 2 involves two exothermic steps. USING ENTHALPY H 2 + O 2 gas Liquid H 2 OH 2 O vapor
45
44 Making H 2 O from H 2 involves two steps. H 2 (g) + 1/2 O 2 (g) ---> H 2 O(g) + 242 kJ H 2 O(g) ---> H 2 O(liq) + 44 kJ ----------------------------------------------------------------------- H 2 (g) + 1/2 O 2 (g) --> H 2 O(liq) + 286 kJ Example of HESS’S LAW — If a rxn. is the sum of 2 or more others, the net ∆H is the sum of the ∆H’s of the other rxns. USING ENTHALPY
46
45 Hess’s Law & Energy Level Diagrams Forming H 2 O can occur in a single step or in a two steps. ∆H total is the same no matter which path is followed.
47
46 Hess’s Law & Energy Level Diagrams Forming CO 2 can occur in a single step or in a two steps. ∆H total is the same no matter which path is followed.
48
47 This equation is valid because ∆H is a STATE FUNCTIONThis equation is valid because ∆H is a STATE FUNCTION These depend only on the state of the system and not on how the system got there.These depend only on the state of the system and not on how the system got there. V, T, P, energy — and your bank account!V, T, P, energy — and your bank account! Unlike V, T, and P, one cannot measure absolute H. Can only measure ∆H.Unlike V, T, and P, one cannot measure absolute H. Can only measure ∆H. ∆H along one path = ∆H along another path ∆H along another path ∆H along one path = ∆H along another path ∆H along another path
49
48 Standard Enthalpy Values Most ∆H values are labeled ∆H o Measured under standard conditions P = 1 bar = 10 5 Pa = 1 atm /1.01325 Concentration = 1 mol/L T = usually 25 o C with all species in standard states e.g., C = graphite and O 2 = gas
50
49 Enthalpy Values H 2 (g) + 1/2 O 2 (g) --> H 2 O(g) ∆H˚ = -242 kJ 2 H 2 (g) + O 2 (g) --> 2 H 2 O(g) ∆H˚ = -484 kJ H 2 O(g) ---> H 2 (g) + 1/2 O 2 (g) ∆H˚ = +242 kJ H 2 (g) + 1/2 O 2 (g) --> H 2 O(liquid) ∆H˚ = -286 kJ Depend on how the reaction is written and on phases of reactants and products
51
50 Standard Enthalpy Values NIST (Nat’l Institute for Standards and Technology) gives values of ∆H f o = standard molar enthalpy of formation ∆H f o = standard molar enthalpy of formation — the enthalpy change when 1 mol of compound is formed from elements under standard conditions. See Table 6.2
52
51 ∆H f o, standard molar enthalpy of formation Enthalpy change when 1 mol of compound is formed from the corresponding elements under standard conditions H 2 (g) + 1/2 O 2 (g) --> H 2 O(g) ∆H f o (H 2 O, g)= -241.8 kJ/mol By definition, ∆H f o = 0 for elements in their standard states.
53
52 Using Standard Enthalpy Values Use ∆H˚’s to calculate enthalpy change for H 2 O(g) + C(graphite) --> H 2 (g) + CO(g) (product is called “water gas”)
54
53 Using Standard Enthalpy Values H 2 O(g) + C(graphite) --> H 2 (g) + CO(g) From reference books we find H 2 (g) + 1/2 O 2 (g) --> H 2 O(g) ∆H f ˚ = - 242 kJ/molH 2 (g) + 1/2 O 2 (g) --> H 2 O(g) ∆H f ˚ = - 242 kJ/mol C(s) + 1/2 O 2 (g) --> CO(g) ∆H f ˚ = - 111 kJ/molC(s) + 1/2 O 2 (g) --> CO(g) ∆H f ˚ = - 111 kJ/mol
55
54 Using Standard Enthalpy Values H 2 O(g) --> H 2 (g) + 1/2 O 2 (g) ∆H o = +242 kJ C(s) + 1/2 O 2 (g) --> CO(g)∆H o = -111 kJ C(s) + 1/2 O 2 (g) --> CO(g) ∆H o = -111 kJ -------------------------------------------------------------------------------- To convert 1 mol of water to 1 mol each of H 2 and CO requires 131 kJ of energy. The “water gas” reaction is ENDOthermic. H 2 O(g) + C(graphite) --> H 2 (g) + CO(g) ∆H o net = +131 kJ ∆H o net = +131 kJ H 2 O(g) + C(graphite) --> H 2 (g) + CO(g) ∆H o net = +131 kJ ∆H o net = +131 kJ
56
55 Using Standard Enthalpy Values In general, when ALL enthalpies of formation are known: Calculate ∆H of reaction? ∆H o rxn = ∆H f o (products) - ∆H f o (reactants) Remember that ∆ always = final – initial
57
56 Using Standard Enthalpy Values Calculate the heat of combustion of methanol, i.e., ∆H o rxn for CH 3 OH(g) + 3/2 O 2 (g) --> CO 2 (g) + 2 H 2 O(g) ∆H o rxn = ∆H f o (prod) - ∆H f o (react) ∆H o rxn = ∆H f o (prod) - ∆H f o (react)
58
57 Using Standard Enthalpy Values ∆H o rxn = ∆H f o (CO 2 ) + 2 ∆H f o (H 2 O) - {3/2 ∆H f o (O 2 ) + ∆H f o (CH 3 OH)} - {3/2 ∆H f o (O 2 ) + ∆H f o (CH 3 OH)} = (-393.5 kJ) + 2 (-241.8 kJ) = (-393.5 kJ) + 2 (-241.8 kJ) - {0 + (-201.5 kJ)} - {0 + (-201.5 kJ)} ∆H o rxn = -675.6 kJ per mol of methanol CH 3 OH(g) + 3/2 O 2 (g) --> CO 2 (g) + 2 H 2 O(g) ∆H o rxn = ∆H f o (prod) - ∆H f o (react) ∆H o rxn = ∆H f o (prod) - ∆H f o (react)
59
58 Measuring Heats of Reaction CALORIMETRYCALORIMETRY Constant Volume “Bomb” Calorimeter Burn combustible sample. Measure heat evolved in a reaction. Derive ∆E for reaction.
60
59 Calorimetry Some heat from reaction warms water q water = (sp. ht.)(water mass)(∆T) Some heat from reaction warms “bomb” q bomb = (heat capacity, J/K)(∆T) Total heat evolved = q total = q water + q bomb
61
60 Calculate heat of combustion of octane. C 8 H 18 + 25/2 O 2 --> 8 CO 2 + 9 H 2 O Burn 1.00 g of octaneBurn 1.00 g of octane Temp rises from 25.00 to 33.20 o CTemp rises from 25.00 to 33.20 o C Calorimeter contains 1200 g waterCalorimeter contains 1200 g water Heat capacity of bomb = 837 J/KHeat capacity of bomb = 837 J/K Measuring Heats of Reaction CALORIMETRY
62
61 Step 1Calc. heat transferred from reaction to water. q = (4.184 J/gK)(1200 g)(8.20 K) = 41,170 J Step 2Calc. heat transferred from reaction to bomb. q = (bomb heat capacity)(∆T) = (837 J/K)(8.20 K) = 6860 J = (837 J/K)(8.20 K) = 6860 J Step 3Total heat evolved 41,170 J + 6860 J = 48,030 J 41,170 J + 6860 J = 48,030 J Heat of combustion of 1.00 g of octane = - 48.0 kJ Measuring Heats of Reaction CALORIMETRY
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.