1 Thermochemistry Chapter 6

2 Overview Introduce the nature of energy and the general topics related to energy problems. Familiarize with the experimental procedures for measuring heats of reactions. Hess’s law and its applications based on enthalpies. Read the present and new sources of energy.

3 Energy is the capacity to do work or produce heat Thermal energy is the energy associated with the random motion of atoms and molecules Chemical energy is the energy stored within the bonds of chemical substances Nuclear energy is the energy stored within the collection of neutrons and protons in the atom Electrical energy is the energy associated with the flow of electrons Potential energy is the energy available by virtue of an object’s position

4 Law of Conservation of Energy Energy can be converted from one form to another but can neither be created nor destroyed. (E universe is constant)

5 The Two Types of Energy Potential: due to position or composition - can be converted to work (water before falling from dam, gasoline, etc.) Kinetic: due to motion of the object (water falling and doing work, gasoline burning and driving engine, etc.) KE = 1 / 2 mv 2 (m = mass, v = velocity)

6 Figure 6.1: (a) In the initial positions, ball A has a higher potential energy than ball B. (b) After A has rolled down the hill, the potential energy lost by A has been converted to random motions of the components of the hill (frictional heating) and to the increase in the potential energy of B.

7 Total Energy = (PE) A + (KE) B + frictional heat

8 Energy is a State Function Depends only on the present state of the system - not how it arrived there. It is independent of pathway. Internal Energy or Total Energy  E, Enthalpy  H, V, P, T are State Functions Heat and Work are not state functions

9 Thermodynamics State functions are properties that are determined by the state of the system, regardless of how that condition was achieved. Potential energy of hiker 1 and hiker 2 is the same even though they took different paths. energy, pressure, volume, temperature

10 Temperature v. Heat Temperature reflects random motions of particles, therefore related to kinetic energy of the system. Heat involves a transfer of energy between 2 objects due to a temperature difference

11 Heat is the transfer of thermal energy between two bodies that are at different temperatures. Energy Changes in Chemical Reactions Temperature is a measure of the thermal energy. Temperature = Thermal Energy 90 0 C 40 0 C greater thermal energy

12 Thermochemistry is the study of heat change in chemical reactions. The system is the specific part of the universe that is of interest in the study. open mass & energyExchange: closed energy isolated nothing SYSTEM SURROUNDINGS

13 System and Surroundings System: That on which we focus attention Surroundings: Everything else in the universe Universe = System + Surroundings

14 Exo and Endothermic Heat exchange accompanies chemical reactions. Exothermic: Heat flows out of the system (to the surroundings). Endothermic: Heat flows into the system (from the surroundings).

15 Exothermic process is any process that gives off heat – transfers thermal energy from the system to the surroundings. PE stored in chemical bonds are the source of chemical energy. Endothermic process is any process in which heat has to be supplied to the system from the surroundings. 2H 2 (g) + O 2 (g) 2H 2 O (l) + energy H 2 O (g) H 2 O (l) + energy energy + 2HgO (s) 2Hg (l) + O 2 (g) energy + H 2 O (s) H 2 O (l) Energy lost by system = Energy gained by surrounding

16 Exothermic versus endothermic.

17 The study of energy and its conversion is called thermodynamics. The law of conservation of energy is called First Law of Thermodynamics.

18 First Law First Law of Thermodynamics: The energy of the universe is constant.

19 Mathematical Definition of the First Law  E = q + w  E = change in system’s internal energy q = heat w = work

20 Figure 6.4: (a) The piston, moving a distance ∆h against a pressure P, does work on the surroundings. (b) Since the volume of a cylinder is the area of the base times its height, the change in volume of the gas is given by ∆h x A = V. Expansion

21 Work work = force  distance since pressure = force / area, work = pressure  volume w system =  P  V

22 Enthalpy Enthalpy = H = E + PV  E =  H  P  V  H =  E + P  V At constant pressure, q P =  E + P  V, where q P =  H at constant pressure  H = energy flow as heat (at constant pressure) E, H, P, V are state functions

23 At constant pressure where PV work is allowed the change in enthalpy  H is equal to the energy flow as heat (q or Q).

24 Signs Convention H eat Flowing to the system from surrounding (heating) :  E < 0, q or  H <0 H eat Flowing from the system to the surrounding (cooling) :  E > 0, q or  H >0 W ork done by the system on the surrounding : W > 0 (-) W ork done on the system by the surrounding : W < 0 (+)

25 Thermochemical Equations CH 4 (g) + 2O 2 (g) CO 2 (g) + 2H 2 O (l)  H = kJ Is  H negative or positive? System gives off heat Exothermic  H < kJ are released for every 1 mole of methane that is combusted at 25 0 C and 1 atm.

26 Enthalpy (H) is used to quantify the heat flow into or out of a system in a process that occurs at constant pressure.  H = H (products) – H (reactants)  H = heat given off or absorbed during a reaction at constant pressure H products < H reactants  H < 0 H products > H reactants  H > 0

27 Heat Capacity

28 The specific heat (s) of a substance is the amount of heat (q) required to raise the temperature of one gram of the substance by one degree Celsius. The heat capacity (C) of a substance is the amount of heat (q) required to raise the temperature of a given quantity (m) of the substance by one degree Celsius. C = ms Heat (q) absorbed or released: q = ms  t q = C  t  t = t final - t initial

29

30 How much heat is given off when an 869 g iron bar cools from 94 0 C to 5 0 C? s of Fe = J/g 0 C  t = t final – t initial = 5 0 C – 94 0 C = C q = ms  t = 869 g x J/g 0 C x –89 0 C= -34,000 J

31 Some Heat Exchange Terms specific heat capacity heat capacity per gram = J/°C g or J/K g molar heat capacity heat capacity per mole = J/°C mol or J/K mol

32 Calorimetry The device used experimentally to determine the heat from chemical reaction is called a calorimeter. Calorimetry is the science to measure heat changes and it is based on the temperature change. Heat capacity is a measure of the body or system ability to absorb heat.

33 Two Types of Calorimeters 1.Constant Volume Calorimeter 2.Constant Pressure Calorimeter

34 Constant-Pressure or Coffee Cup Calorimetry q lost = - q gained q rxn = - (q water + q calorimeter ) q water = ms  t q cal = C cal  t Reaction at Constant P  H = q rxn May be used to determine many Heats such as heat of solution, neutralization (acid-base), etc.

35 Constant-Volume Calorimetry No heat enters or leaves! q sys = q water + q bomb + q rxn q sys = 0 q rxn = - (q water + q bomb ) q water = ms  t q bomb = C bomb  t Reaction at Constant V  H ~ q rxn  H = q rxn W = -p  V = 0  E = q + W  E = q V

36 The enthalpy of solution (  H soln ) is the heat generated or absorbed when a certain amount of solute dissolves in a certain amount of solvent.  H soln = H soln - H components Which substance(s) could be used for melting ice? Which substance(s) could be used for a cold pack?

37 The Solution Process for NaCl  H soln = Step 1 + Step 2 = 788 – 784 = 4 kJ/mol

38

39 Sample Exercise Calculate the energy per gram for burning 1.50g of CH 4 in a constant-volume calorimeter (S=11.3 KJ/ 0 C) where  t = C.. Energy released = m x s x  t = 1.50 x 11.3x10 3 x 7.3 = 83 KJ per 1.50g of CH 4 83 Energy released per g = = KJ/g

40 H 2 O (s) H 2 O (l)  H = 6.01 kJ The stoichiometric coefficients always refer to the number of moles of a substance Thermochemical Equations If you reverse a reaction, the sign of  H changes H 2 O (l) H 2 O (s)  H = kJ If you multiply both sides of the equation by a factor n, then  H must change by the same factor n. 2H 2 O (s) 2H 2 O (l)  H = 2 x 6.01 = 12.0 kJ

41 H 2 O (s) H 2 O (l)  H = 6.01 kJ The physical states of all reactants and products must be specified in thermochemical equations. Thermochemical Equations H 2 O (l) H 2 O (g)  H = 44.0 kJ How much heat is evolved when 266 g of white phosphorus (P 4 ) burn in air? P 4 (s) + 5O 2 (g) P 4 O 10 (s)  H = kJ Q Q = kJ 1 mol P g kJ 266gQ

42 Hess’s Law Reactants  Products The change in enthalpy is the same whether the reaction takes place in one step or a series of steps.

43 Because there is no way to measure the absolute value of the enthalpy of a substance, must I measure the enthalpy change for every reaction of interest? Establish an arbitrary scale with the standard enthalpy of formation (  H 0 ) as a reference point for all enthalpy expressions. f

44 Standard enthalpy of formation (  H 0 f ) is the heat change that results when one mole of a compound is formed from its elements at a pressure of 1 atm. Example CO 2(g) is formed from C (s) and O 2(g) C (s) + O 2(g) CO 2(g) H0fH0f

45 The standard enthalpy of formation of any element in its most stable form is zero.  H 0 (O 2 ) = 0 f  H 0 (O 3 ) = 142 kJ/mol f  H 0 (C, graphite) = 0 f  H 0 (C, diamond) = 1.90 kJ/mol f

46 Then Apply Hess’s Law

47 Standard States Compound 4 For a gas, pressure is exactly 1 atmosphere. 4 For a solution, concentration is exactly 1 molar. 4 Pure substance (liquid or solid), it is the pure liquid or solid. Element 4 The form [N 2 (g), K(s)] in which it exists at 1 atm and 25°C.

48 Keep in mind the following concepts.

49 Change in Enthalpy Can be calculated from enthalpies of formation of reactants and products.  H rxn ° =  n p  H f  (products)   n r  H f  (reactants)

50 The standard enthalpy of reaction (  H 0 ) is the enthalpy of a reaction carried out at 1 atm. rxn aA + bB cC + dD H0H0 rxn d  H 0 (D) f c  H 0 (C) f = [+] - b  H 0 (B) f a  H 0 (A) f [+] H0H0 rxn n  H 0 (products) f =  m  H 0 (reactants) f  - Hess’s Law: When reactants are converted to products, the change in enthalpy is the same whether the reaction takes place in one step or in a series of steps. (Enthalpy is a state function. It doesn’t matter how you get there, only where you start and end.)

51 Calculations via Hess’s Law 1. If a reaction is reversed,  H is also reversed. N 2 (g) + O 2 (g)  2NO(g)  H = 180 kJ 2NO(g)  N 2 (g) + O 2 (g)  H =  180 kJ 2. If the coefficients of a reaction are multiplied by an integer,  H is multiplied by that same integer. 6NO(g)  3N 2 (g) + 3O 2 (g)  H =  540 kJ

52 Calculate the standard enthalpy of formation of CS 2 (l) given that: C (graphite) + O 2 (g) CO 2 (g)  H 0 = kJ rxn S (rhombic) + O 2 (g) SO 2 (g)  H 0 = kJ rxn CS 2 (l) + 3O 2 (g) CO 2 (g) + 2SO 2 (g)  H 0 = kJ rxn 1. Write the enthalpy of formation reaction for CS 2 C (graphite) + 2S (rhombic) CS 2 (l) 2. Add the given rxns so that the result is the desired rxn. rxn C (graphite) + O 2 (g) CO 2 (g)  H 0 = kJ 2S (rhombic) + 2O 2 (g) 2SO 2 (g)  H 0 = x2 kJ rxn CO 2 (g) + 2SO 2 (g) CS 2 (l) + 3O 2 (g)  H 0 = kJ rxn + C (graphite) + 2S (rhombic) CS 2 (l)  H 0 = (2x-296.1) = 86.3 kJ rxn

53 Benzene (C 6 H 6 ) burns in air to produce carbon dioxide and liquid water. How much heat is released per mole of benzene combusted? The standard enthalpy of formation of benzene is kJ/mol. 2C 6 H 6 (l) + 15O 2 (g) 12CO 2 (g) + 6H 2 O (l) H0H0 rxn n  H 0 (products) f =  m  H 0 (reactants) f  - H0H0 rxn 6  H 0 (H 2 O) f 12  H 0 (CO 2 ) f = [+] - 2  H 0 (C 6 H 6 ) f [] H0H0 rxn = [ 12x– x–187.6 ] – [ 2x49.04 ] = kJ kJ 2 mol = kJ/mol C 6 H 6

54

55

56 Sample Exercise Calculate the work done when 50.0 g of magnesium (Mg) dissolve in excess acid at 1.00 atm and C.

57 Sample Exercise Determine the heat of reaction at 298 K for the reaction which occurs in a welder's acetylene torch: H 2 (g) + 1/2 O 2 (g) H 2 O(l)H o /kJ = C(s) + H 2 (g) C 2 H 2 (g)H o /kJ = C(s) + O 2 (g) CO 2 (g)H o /kJ = C 2 H 2 (g) + 5 O 2 (g) 4 CO 2 (g) + 2 H 2 O(l) Given the following equations and H o values

58 Sample Exercise A 15.0g nickel is heated to C and dropped into 55.0g of water initially at 23 0 C. Assuming an isolated system, calculate the final temperature of the nickel and water. S nickel = J/ 0 Cg. Q lost by nickel = - Q gained by water (mst) nickel = - (ms  t) water t = tf - ti t f is the same. t i is different.

59 QUESTION

60 ANSWER

61 QUESTION

62 ANSWER

63 QUESTION

64 ANSWER

65 QUESTION

66 ANSWER

67 ANSWER (continued)

68 QUESTION

69 ANSWER

70 QUESTION

71 ANSWER

72 QUESTION

73 ANSWER

74 QUESTION

75 ANSWER

76 QUESTION

77 ANSWER

78 QUESTION

79 ANSWER

80 QUESTION

81 QUESTION (continued)

82 ANSWER

83 QUESTION

84 ANSWER

85 QUESTION

86 ANSWER

87 QUESTION

88 ANSWER

89 ANSWER (continued)

90 QUESTION

91 QUESTION (continued)

92 ANSWER

93 QUESTION

94 QUESTION

95 ANSWER

96 QUESTION

97 ANSWER

98 QUESTION

99 ANSWER