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Prentice-Hall General Chemistry: Chapter 7Slide 1 of 50
Chapter 7: Thermochemistry
Philip Dutton
University of Windsor, Canada
Prentice-Hall © 2002
General Chemistry
Principles and Modern Applications
Petrucci • Harwood • Herring
8th
Edition
Prentice-Hall General Chemistry: Chapter 7Slide 2 of 50
Contents
7-1 Getting Started: Some Terminology
7-2 Heat
7-3 Heats of Reaction and Calorimetry
7-4 Work
7-5 The First Law of Thermodynamics
7-6 Heats of Reaction: ∆U and ∆H
7-7 The Indirect Determination of ∆H: Hess’s Law
Prentice-Hall General Chemistry: Chapter 7Slide 3 of 50
Contents
7-7 The Indirect Determination of ∆H, Hess’s Law
7-8 Standard Enthalpies of Formation
7-9 Fuels as Sources of Energy
Focus on Fats, Carbohydrates, and Energy
Storage
Prentice-Hall General Chemistry: Chapter 7Slide 4 of 50
6-1 Getting Started: Some Terminology
• System
• Surroundings
Prentice-Hall General Chemistry: Chapter 7Slide 5 of 50
Terminology
• Energy, U
– The capacity to do work.
• Work
– Force acting through a distance.
• Kinetic Energy
– The energy of motion.
Prentice-Hall General Chemistry: Chapter 7Slide 6 of 50
Energy
• Kinetic Energy
ek =
1
2
mv2
[ek ] =
kg m2
s2 = J
w = Fd [w ] =
kg m
s2 = Jm
• Work
Prentice-Hall General Chemistry: Chapter 7Slide 7 of 50
Energy
• Potential Energy
– Energy due to condition, position, or
composition.
– Associated with forces of attraction or
repulsion between objects.
• Energy can change from potential to
kinetic.
Prentice-Hall General Chemistry: Chapter 7Slide 8 of 50
Energy and Temperature
• Thermal Energy
– Kinetic energy associated with random
molecular motion.
– In general proportional to temperature.
– An intensive property.
• Heat and Work
– q and w.
– Energy changes.
Prentice-Hall General Chemistry: Chapter 7Slide 9 of 50
Heat
Energy transferred between a system and its
surroundings as a result of a temperature
difference.
• Heat flows from hotter to colder.
– Temperature may change.
– Phase may change (an isothermal process).
Prentice-Hall General Chemistry: Chapter 7Slide 10 of 50
Units of Heat
• Calorie (cal)
– The quantity of heat required to change the
temperature of one gram of water by one degree
Celsius.
• Joule (J)
– SI unit for heat
1 cal = 4.184 J
Prentice-Hall General Chemistry: Chapter 7Slide 11 of 50
Heat Capacity
• The quantity of heat required to change the
temperature of a system by one degree.
– Molar heat capacity.
• System is one mole of substance.
– Specific heat capacity, c.
• System is one gram of substance
– Heat capacity
• Mass  specific heat.
q = mc∆T
q = C∆T
Prentice-Hall General Chemistry: Chapter 7Slide 12 of 50
Conservation of Energy
• In interactions between a system and its
surroundings the total energy remains constant—
energy is neither created nor destroyed.
qsystem + qsurroundings = 0
qsystem = -qsurroundings
Prentice-Hall General Chemistry: Chapter 7Slide 13 of 50
Determination of Specific Heat
Prentice-Hall General Chemistry: Chapter 7Slide 14 of 50
Example 7-2
Determining Specific Heat from Experimental Data.
Use the data presented on the last slide to calculate the specific
heat of lead.
qlead = -qwater
qwater = mc∆T = (50.0 g)(4.184 J/g °C)(28.8 - 22.0)°C
qwater = 1.4x103
J
qlead = -1.4x103
J = mc∆T = (150.0 g)(c)(28.8 - 100.0)°C
clead = 0.13 Jg-1
°C-1
Prentice-Hall General Chemistry: Chapter 7Slide 15 of 50
7-3 Heats of Reaction and Calorimetry
• Chemical energy.
– Contributes to the internal energy of a system.
• Heat of reaction, qrxn.
– The quantity of heat exchanged between a
system and its surroundings when a chemical
reaction occurs within the system, at constant
temperature.
Prentice-Hall General Chemistry: Chapter 7Slide 16 of 50
Heats of Reaction
• Exothermic reactions.
– Produces heat, qrxn < 0.
• Endothermic reactions.
– Consumes heat, qrxn > 0.
• Calorimeter
– A device for measuring quantities of heat.
Prentice-Hall General Chemistry: Chapter 7Slide 17 of 50
Bomb Calorimeter
qrxn = -qcal
qcal = qbomb + qwater + qwires +…
Define the heat capacity of the
calorimeter:
qcal = mici∆T = C∆T
all i
heat
Prentice-Hall General Chemistry: Chapter 7Slide 18 of 50
Using Bomb Calorimetry Data to Determine a Heat of Reaction.
The combustion of 1.010 g sucrose, in a bomb calorimeter,
causes the temperature to rise from 24.92 to 28.33°C. The
heat capacity of the calorimeter assembly is 4.90 kJ/°C.
(a) What is the heat of combustion of sucrose, expressed in
kJ/mol C12H22O11
(b) Verify the claim of sugar producers that one teaspoon of
sugar (about 4.8 g) contains only 19 calories.
Example 7-3
Prentice-Hall General Chemistry: Chapter 7Slide 19 of 50
Example 7-3
Calculate qcalorimeter:
qcal = C∆T = (4.90 kJ/°C)(28.33-24.92)°C = (4.90)(3.41) kJ
= 16.7 kJ
Calculate qrxn:
qrxn = -qcal = -16.7 kJ per 1.010 g
Example 7-3
Prentice-Hall General Chemistry: Chapter 7Slide 20 of 50
Example 7-3
Calculate qrxn in the required units:
qrxn = -qcal =
-16.7 kJ
1.010 g
= -16.5 kJ/g
343.3 g
1.00 mol
= -16.5 kJ/g
= -5.65  103
kJ/mol
qrxn
(a)
Calculate qrxn for one teaspoon:
4.8 g
1 tsp
= (-16.5 kJ/g)(qrxn (b))( )= -19 cal/tsp
1.00 cal
4.184 J
Example 7-3
Prentice-Hall General Chemistry: Chapter 7Slide 21 of 50
Coffee Cup Calorimeter
• A simple calorimeter.
– Well insulated and therefore isolated.
– Measure temperature change.
qrxn = -qcal
See example 7-4 for a sample calculation.
Prentice-Hall General Chemistry: Chapter 7Slide 22 of 50
7-4 Work
• In addition to heat effects chemical reactions
may also do work.
• Gas formed pushes against
the atmosphere.
• Volume changes.
• Pressure-volume work.
Prentice-Hall General Chemistry: Chapter 7Slide 23 of 50
Pressure Volume Work
w = F  d
= (P  A)  h
= P∆V
w = -Pext∆V
Prentice-Hall General Chemistry: Chapter 7Slide 24 of 50
Example 7-3
Assume an ideal gas and calculate the volume change:
Vi = nRT/P
= (0.100 mol)(0.08201 L atm mol-1
K-1
)(298K)/(2.40 atm)
= 1.02 L
Vf = 1.88 L
Example 7-5
Calculating Pressure-Volume Work.
Suppose the gas in the previous figure is 0.100 mol He at 298 K.
How much work, in Joules, is associated with its expansion at
constant pressure.
∆V = 1.88-1.02 L = 0.86 L
Prentice-Hall General Chemistry: Chapter 7Slide 25 of 50
Example 7-3
Calculate the work done by the system:
w = -P∆V
= -(1.30 atm)(0.86 L)(
= -1.1  102
J
Example 7-5
)
101 J
1 L atm
Where did the conversion factor come from?
Compare two versions of the gas constant and calculate.
8.3145 J/mol K ≡ 0.082057 L atm/mol K
1 ≡ 101.33 J/L atm
Hint: If you use
pressure in kPa you
get Joules directly.
Prentice-Hall General Chemistry: Chapter 7Slide 26 of 50
7-5 The First Law of Thermodynamics
• Internal Energy, U.
– Total energy (potential and kinetic) in a system.
•Translational kinetic energy.
•Molecular rotation.
•Bond vibration.
•Intermolecular attractions.
•Chemical bonds.
•Electrons.
Prentice-Hall General Chemistry: Chapter 7Slide 27 of 50
First Law of Thermodynamics
• A system contains only internal energy.
– A system does not contain heat or work.
– These only occur during a change in the system.
• Law of Conservation of Energy
– The energy of an isolated system is constant
∆U = q + w
Prentice-Hall General Chemistry: Chapter 7Slide 28 of 50
First Law of Thermodynamics
Prentice-Hall General Chemistry: Chapter 7Slide 29 of 50
State Functions
• Any property that has a unique value for a
specified state of a system is said to be a
State Function.
• Water at 293.15 K and 1.00 atm is in a specified state.
• d = 0.99820 g/mL
• This density is a unique function of the state.
• It does not matter how the state was established.
Prentice-Hall General Chemistry: Chapter 7Slide 30 of 50
Functions of State
• U is a function of state.
– Not easily measured.
∀∆U has a unique value between two states.
– Is easily measured.
Prentice-Hall General Chemistry: Chapter 7Slide 31 of 50
Path Dependent Functions
• Changes in heat and work are not functions of
state.
– Remember example 7-5, w = -1.1  102
J in a one step
expansion of gas:
– Consider 2.40 atm to 1.80 atm and finally to 1.30 atm.
w = (-1.80 atm)(1.30-1.02)L – (1.30 atm)(1.88-1.36)L
= -0.61 L atm – 0.68 L atm = -1.3 L atm
= 1.3  102
J
Prentice-Hall General Chemistry: Chapter 7Slide 32 of 50
7-6 Heats of Reaction: ∆U and ∆H
Reactants → Products
Ui Uf
∆U = Uf - Ui
∆U = qrxn + w
In a system at constant volume:
∆U = qrxn + 0 = qrxn = qv
But we live in a constant pressure world!
How does qp relate to qv?
Prentice-Hall General Chemistry: Chapter 7Slide 33 of 50
Heats of Reaction
Prentice-Hall General Chemistry: Chapter 7Slide 34 of 50
Heats of Reaction
qV = qP + w
We know that w = - P∆V and ∆U = qP, therefore:
∆U = qP - P∆V
qP = ∆U + P∆V
These are all state functions, so define a new function.
Let H = U + PV
Then ∆H = Hf – Hi = ∆U + ∆PV
If we work at constant pressure and temperature:
∆H = ∆U + P∆V = qP
Prentice-Hall General Chemistry: Chapter 7Slide 35 of 50
Comparing Heats of Reaction
qP = -566 kJ/mol
= ∆H
P∆V = P(Vf – Vi)
= RT(nf – ni)
= -2.5 kJ
∆U = ∆H - P∆V
= -563.5 kJ/mol
= qV
Prentice-Hall General Chemistry: Chapter 7Slide 36 of 50
Changes of State of Matter
H2O (l) → H2O(g) ∆H = 44.0 kJ at 298 K
Molar enthalpy of vaporization:
Molar enthalpy of fusion:
H2O (s) → H2O(l) ∆H = 6.01 kJ at 273.15 K
Prentice-Hall General Chemistry: Chapter 7Slide 37 of 50
Example 7-3Example 7-8
Break the problem into two steps: Raise the temperature of
the liquid first then completely vaporize it. The total enthalpy
change is the sum of the changes in each step.
Enthalpy Changes Accompanying Changes in States of Matter.
Calculate ∆H for the process in which 50.0 g of water is
converted from liquid at 10.0°C to vapor at 25.0°C.
= (50.0 g)(4.184 J/g °C)(25.0-10.0)°C +
50.0 g
18.0 g/mol
44.0 kJ/mol
Set up the equation and calculate:
qP = mcH2O∆T + n∆Hvap
= 3.14 kJ + 122 kJ = 125 kJ
Prentice-Hall General Chemistry: Chapter 7Slide 38 of 50
Standard States and Standard Enthalpy
Changes
• Define a particular state as a standard state.
• Standard enthalpy of reaction, ∆H°
– The enthalpy change of a reaction in which all
reactants and products are in their standard states.
• Standard State
– The pure element or compound at a pressure of 1
bar and at the temperature of interest.
Prentice-Hall General Chemistry: Chapter 7Slide 39 of 50
Enthalpy Diagrams
Prentice-Hall General Chemistry: Chapter 7Slide 40 of 50
7-7 Indirect Determination of ∆H:
Hess’s Law
∀ ∆H is an extensive property.
– Enthalpy change is directly proportional to the amount of
substance in a system.
N2(g) + O2(g) → 2 NO(g) ∆H = +180.50 kJ
½N2(g) + ½O2(g) → NO(g) ∆H = +90.25 kJ
∀ ∆H changes sign when a process is reversed
NO(g) → ½N2(g) + ½O2(g) ∆H = -90.25 kJ
Prentice-Hall General Chemistry: Chapter 7Slide 41 of 50
Hess’s Law
• Hess’s law of constant heat summation
– If a process occurs in stages or steps (even hypothetically),
the enthalpy change for the overall process is the sum of the
enthalpy changes for the individual steps.
½N2(g) + O2(g) → NO2(g) ∆H = +33.18 kJ
½N2(g) + ½O2(g) → NO(g) ∆H = +90.25 kJ
NO(g) + ½O2(g) → NO2(g) ∆H = -57.07 kJ
Prentice-Hall General Chemistry: Chapter 7Slide 42 of 50
Hess’s Law Schematically
Prentice-Hall General Chemistry: Chapter 7Slide 43 of 50
• The enthalpy change that occurs in the
formation of one mole of a substance in the
standard state from the reference forms of
the elements in their standard states.
• The standard enthalpy of formation of a
pure element in its reference state is 0.
∆Hf
°
7-8 Standard Enthalpies of Formation
Prentice-Hall General Chemistry: Chapter 7Slide 44 of 50
Standard Enthalpies of Formation
Prentice-Hall General Chemistry: Chapter 7Slide 45 of 50
Standard Enthalpies of Formation
Prentice-Hall General Chemistry: Chapter 7Slide 46 of 50
Standard Enthalpies of Reaction
∆Hoverall = -2∆Hf
°
NaHCO3
+ ∆Hf
°
Na2CO3
+∆Hf
°
CO2
+ ∆Hf
°
H2O
Prentice-Hall General Chemistry: Chapter 7Slide 47 of 50
Enthalpy of Reaction
∆Hrxn = ∆Hf
°
products- ∆Hf
°
reactants
Prentice-Hall General Chemistry: Chapter 7Slide 48 of 50
Table 7.3 Enthalpies of Formation of Ions
in Aqueous Solutions
Prentice-Hall General Chemistry: Chapter 7Slide 49 of 50
7-9 Fuels as Sources
of Energy
• Fossil fuels.
– Combustion is exothermic.
– Non-renewable resource.
– Environmental impact.
Prentice-Hall General Chemistry: Chapter 7Slide 50 of 50
Chapter 7 Questions
1, 2, 3, 11, 14, 16,
22, 24, 29, 37, 49,
52, 63, 67, 73, 81

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  • 1. Prentice-Hall General Chemistry: Chapter 7Slide 1 of 50 Chapter 7: Thermochemistry Philip Dutton University of Windsor, Canada Prentice-Hall © 2002 General Chemistry Principles and Modern Applications Petrucci • Harwood • Herring 8th Edition
  • 2. Prentice-Hall General Chemistry: Chapter 7Slide 2 of 50 Contents 7-1 Getting Started: Some Terminology 7-2 Heat 7-3 Heats of Reaction and Calorimetry 7-4 Work 7-5 The First Law of Thermodynamics 7-6 Heats of Reaction: ∆U and ∆H 7-7 The Indirect Determination of ∆H: Hess’s Law
  • 3. Prentice-Hall General Chemistry: Chapter 7Slide 3 of 50 Contents 7-7 The Indirect Determination of ∆H, Hess’s Law 7-8 Standard Enthalpies of Formation 7-9 Fuels as Sources of Energy Focus on Fats, Carbohydrates, and Energy Storage
  • 4. Prentice-Hall General Chemistry: Chapter 7Slide 4 of 50 6-1 Getting Started: Some Terminology • System • Surroundings
  • 5. Prentice-Hall General Chemistry: Chapter 7Slide 5 of 50 Terminology • Energy, U – The capacity to do work. • Work – Force acting through a distance. • Kinetic Energy – The energy of motion.
  • 6. Prentice-Hall General Chemistry: Chapter 7Slide 6 of 50 Energy • Kinetic Energy ek = 1 2 mv2 [ek ] = kg m2 s2 = J w = Fd [w ] = kg m s2 = Jm • Work
  • 7. Prentice-Hall General Chemistry: Chapter 7Slide 7 of 50 Energy • Potential Energy – Energy due to condition, position, or composition. – Associated with forces of attraction or repulsion between objects. • Energy can change from potential to kinetic.
  • 8. Prentice-Hall General Chemistry: Chapter 7Slide 8 of 50 Energy and Temperature • Thermal Energy – Kinetic energy associated with random molecular motion. – In general proportional to temperature. – An intensive property. • Heat and Work – q and w. – Energy changes.
  • 9. Prentice-Hall General Chemistry: Chapter 7Slide 9 of 50 Heat Energy transferred between a system and its surroundings as a result of a temperature difference. • Heat flows from hotter to colder. – Temperature may change. – Phase may change (an isothermal process).
  • 10. Prentice-Hall General Chemistry: Chapter 7Slide 10 of 50 Units of Heat • Calorie (cal) – The quantity of heat required to change the temperature of one gram of water by one degree Celsius. • Joule (J) – SI unit for heat 1 cal = 4.184 J
  • 11. Prentice-Hall General Chemistry: Chapter 7Slide 11 of 50 Heat Capacity • The quantity of heat required to change the temperature of a system by one degree. – Molar heat capacity. • System is one mole of substance. – Specific heat capacity, c. • System is one gram of substance – Heat capacity • Mass  specific heat. q = mc∆T q = C∆T
  • 12. Prentice-Hall General Chemistry: Chapter 7Slide 12 of 50 Conservation of Energy • In interactions between a system and its surroundings the total energy remains constant— energy is neither created nor destroyed. qsystem + qsurroundings = 0 qsystem = -qsurroundings
  • 13. Prentice-Hall General Chemistry: Chapter 7Slide 13 of 50 Determination of Specific Heat
  • 14. Prentice-Hall General Chemistry: Chapter 7Slide 14 of 50 Example 7-2 Determining Specific Heat from Experimental Data. Use the data presented on the last slide to calculate the specific heat of lead. qlead = -qwater qwater = mc∆T = (50.0 g)(4.184 J/g °C)(28.8 - 22.0)°C qwater = 1.4x103 J qlead = -1.4x103 J = mc∆T = (150.0 g)(c)(28.8 - 100.0)°C clead = 0.13 Jg-1 °C-1
  • 15. Prentice-Hall General Chemistry: Chapter 7Slide 15 of 50 7-3 Heats of Reaction and Calorimetry • Chemical energy. – Contributes to the internal energy of a system. • Heat of reaction, qrxn. – The quantity of heat exchanged between a system and its surroundings when a chemical reaction occurs within the system, at constant temperature.
  • 16. Prentice-Hall General Chemistry: Chapter 7Slide 16 of 50 Heats of Reaction • Exothermic reactions. – Produces heat, qrxn < 0. • Endothermic reactions. – Consumes heat, qrxn > 0. • Calorimeter – A device for measuring quantities of heat.
  • 17. Prentice-Hall General Chemistry: Chapter 7Slide 17 of 50 Bomb Calorimeter qrxn = -qcal qcal = qbomb + qwater + qwires +… Define the heat capacity of the calorimeter: qcal = mici∆T = C∆T all i heat
  • 18. Prentice-Hall General Chemistry: Chapter 7Slide 18 of 50 Using Bomb Calorimetry Data to Determine a Heat of Reaction. The combustion of 1.010 g sucrose, in a bomb calorimeter, causes the temperature to rise from 24.92 to 28.33°C. The heat capacity of the calorimeter assembly is 4.90 kJ/°C. (a) What is the heat of combustion of sucrose, expressed in kJ/mol C12H22O11 (b) Verify the claim of sugar producers that one teaspoon of sugar (about 4.8 g) contains only 19 calories. Example 7-3
  • 19. Prentice-Hall General Chemistry: Chapter 7Slide 19 of 50 Example 7-3 Calculate qcalorimeter: qcal = C∆T = (4.90 kJ/°C)(28.33-24.92)°C = (4.90)(3.41) kJ = 16.7 kJ Calculate qrxn: qrxn = -qcal = -16.7 kJ per 1.010 g Example 7-3
  • 20. Prentice-Hall General Chemistry: Chapter 7Slide 20 of 50 Example 7-3 Calculate qrxn in the required units: qrxn = -qcal = -16.7 kJ 1.010 g = -16.5 kJ/g 343.3 g 1.00 mol = -16.5 kJ/g = -5.65  103 kJ/mol qrxn (a) Calculate qrxn for one teaspoon: 4.8 g 1 tsp = (-16.5 kJ/g)(qrxn (b))( )= -19 cal/tsp 1.00 cal 4.184 J Example 7-3
  • 21. Prentice-Hall General Chemistry: Chapter 7Slide 21 of 50 Coffee Cup Calorimeter • A simple calorimeter. – Well insulated and therefore isolated. – Measure temperature change. qrxn = -qcal See example 7-4 for a sample calculation.
  • 22. Prentice-Hall General Chemistry: Chapter 7Slide 22 of 50 7-4 Work • In addition to heat effects chemical reactions may also do work. • Gas formed pushes against the atmosphere. • Volume changes. • Pressure-volume work.
  • 23. Prentice-Hall General Chemistry: Chapter 7Slide 23 of 50 Pressure Volume Work w = F  d = (P  A)  h = P∆V w = -Pext∆V
  • 24. Prentice-Hall General Chemistry: Chapter 7Slide 24 of 50 Example 7-3 Assume an ideal gas and calculate the volume change: Vi = nRT/P = (0.100 mol)(0.08201 L atm mol-1 K-1 )(298K)/(2.40 atm) = 1.02 L Vf = 1.88 L Example 7-5 Calculating Pressure-Volume Work. Suppose the gas in the previous figure is 0.100 mol He at 298 K. How much work, in Joules, is associated with its expansion at constant pressure. ∆V = 1.88-1.02 L = 0.86 L
  • 25. Prentice-Hall General Chemistry: Chapter 7Slide 25 of 50 Example 7-3 Calculate the work done by the system: w = -P∆V = -(1.30 atm)(0.86 L)( = -1.1  102 J Example 7-5 ) 101 J 1 L atm Where did the conversion factor come from? Compare two versions of the gas constant and calculate. 8.3145 J/mol K ≡ 0.082057 L atm/mol K 1 ≡ 101.33 J/L atm Hint: If you use pressure in kPa you get Joules directly.
  • 26. Prentice-Hall General Chemistry: Chapter 7Slide 26 of 50 7-5 The First Law of Thermodynamics • Internal Energy, U. – Total energy (potential and kinetic) in a system. •Translational kinetic energy. •Molecular rotation. •Bond vibration. •Intermolecular attractions. •Chemical bonds. •Electrons.
  • 27. Prentice-Hall General Chemistry: Chapter 7Slide 27 of 50 First Law of Thermodynamics • A system contains only internal energy. – A system does not contain heat or work. – These only occur during a change in the system. • Law of Conservation of Energy – The energy of an isolated system is constant ∆U = q + w
  • 28. Prentice-Hall General Chemistry: Chapter 7Slide 28 of 50 First Law of Thermodynamics
  • 29. Prentice-Hall General Chemistry: Chapter 7Slide 29 of 50 State Functions • Any property that has a unique value for a specified state of a system is said to be a State Function. • Water at 293.15 K and 1.00 atm is in a specified state. • d = 0.99820 g/mL • This density is a unique function of the state. • It does not matter how the state was established.
  • 30. Prentice-Hall General Chemistry: Chapter 7Slide 30 of 50 Functions of State • U is a function of state. – Not easily measured. ∀∆U has a unique value between two states. – Is easily measured.
  • 31. Prentice-Hall General Chemistry: Chapter 7Slide 31 of 50 Path Dependent Functions • Changes in heat and work are not functions of state. – Remember example 7-5, w = -1.1  102 J in a one step expansion of gas: – Consider 2.40 atm to 1.80 atm and finally to 1.30 atm. w = (-1.80 atm)(1.30-1.02)L – (1.30 atm)(1.88-1.36)L = -0.61 L atm – 0.68 L atm = -1.3 L atm = 1.3  102 J
  • 32. Prentice-Hall General Chemistry: Chapter 7Slide 32 of 50 7-6 Heats of Reaction: ∆U and ∆H Reactants → Products Ui Uf ∆U = Uf - Ui ∆U = qrxn + w In a system at constant volume: ∆U = qrxn + 0 = qrxn = qv But we live in a constant pressure world! How does qp relate to qv?
  • 33. Prentice-Hall General Chemistry: Chapter 7Slide 33 of 50 Heats of Reaction
  • 34. Prentice-Hall General Chemistry: Chapter 7Slide 34 of 50 Heats of Reaction qV = qP + w We know that w = - P∆V and ∆U = qP, therefore: ∆U = qP - P∆V qP = ∆U + P∆V These are all state functions, so define a new function. Let H = U + PV Then ∆H = Hf – Hi = ∆U + ∆PV If we work at constant pressure and temperature: ∆H = ∆U + P∆V = qP
  • 35. Prentice-Hall General Chemistry: Chapter 7Slide 35 of 50 Comparing Heats of Reaction qP = -566 kJ/mol = ∆H P∆V = P(Vf – Vi) = RT(nf – ni) = -2.5 kJ ∆U = ∆H - P∆V = -563.5 kJ/mol = qV
  • 36. Prentice-Hall General Chemistry: Chapter 7Slide 36 of 50 Changes of State of Matter H2O (l) → H2O(g) ∆H = 44.0 kJ at 298 K Molar enthalpy of vaporization: Molar enthalpy of fusion: H2O (s) → H2O(l) ∆H = 6.01 kJ at 273.15 K
  • 37. Prentice-Hall General Chemistry: Chapter 7Slide 37 of 50 Example 7-3Example 7-8 Break the problem into two steps: Raise the temperature of the liquid first then completely vaporize it. The total enthalpy change is the sum of the changes in each step. Enthalpy Changes Accompanying Changes in States of Matter. Calculate ∆H for the process in which 50.0 g of water is converted from liquid at 10.0°C to vapor at 25.0°C. = (50.0 g)(4.184 J/g °C)(25.0-10.0)°C + 50.0 g 18.0 g/mol 44.0 kJ/mol Set up the equation and calculate: qP = mcH2O∆T + n∆Hvap = 3.14 kJ + 122 kJ = 125 kJ
  • 38. Prentice-Hall General Chemistry: Chapter 7Slide 38 of 50 Standard States and Standard Enthalpy Changes • Define a particular state as a standard state. • Standard enthalpy of reaction, ∆H° – The enthalpy change of a reaction in which all reactants and products are in their standard states. • Standard State – The pure element or compound at a pressure of 1 bar and at the temperature of interest.
  • 39. Prentice-Hall General Chemistry: Chapter 7Slide 39 of 50 Enthalpy Diagrams
  • 40. Prentice-Hall General Chemistry: Chapter 7Slide 40 of 50 7-7 Indirect Determination of ∆H: Hess’s Law ∀ ∆H is an extensive property. – Enthalpy change is directly proportional to the amount of substance in a system. N2(g) + O2(g) → 2 NO(g) ∆H = +180.50 kJ ½N2(g) + ½O2(g) → NO(g) ∆H = +90.25 kJ ∀ ∆H changes sign when a process is reversed NO(g) → ½N2(g) + ½O2(g) ∆H = -90.25 kJ
  • 41. Prentice-Hall General Chemistry: Chapter 7Slide 41 of 50 Hess’s Law • Hess’s law of constant heat summation – If a process occurs in stages or steps (even hypothetically), the enthalpy change for the overall process is the sum of the enthalpy changes for the individual steps. ½N2(g) + O2(g) → NO2(g) ∆H = +33.18 kJ ½N2(g) + ½O2(g) → NO(g) ∆H = +90.25 kJ NO(g) + ½O2(g) → NO2(g) ∆H = -57.07 kJ
  • 42. Prentice-Hall General Chemistry: Chapter 7Slide 42 of 50 Hess’s Law Schematically
  • 43. Prentice-Hall General Chemistry: Chapter 7Slide 43 of 50 • The enthalpy change that occurs in the formation of one mole of a substance in the standard state from the reference forms of the elements in their standard states. • The standard enthalpy of formation of a pure element in its reference state is 0. ∆Hf ° 7-8 Standard Enthalpies of Formation
  • 44. Prentice-Hall General Chemistry: Chapter 7Slide 44 of 50 Standard Enthalpies of Formation
  • 45. Prentice-Hall General Chemistry: Chapter 7Slide 45 of 50 Standard Enthalpies of Formation
  • 46. Prentice-Hall General Chemistry: Chapter 7Slide 46 of 50 Standard Enthalpies of Reaction ∆Hoverall = -2∆Hf ° NaHCO3 + ∆Hf ° Na2CO3 +∆Hf ° CO2 + ∆Hf ° H2O
  • 47. Prentice-Hall General Chemistry: Chapter 7Slide 47 of 50 Enthalpy of Reaction ∆Hrxn = ∆Hf ° products- ∆Hf ° reactants
  • 48. Prentice-Hall General Chemistry: Chapter 7Slide 48 of 50 Table 7.3 Enthalpies of Formation of Ions in Aqueous Solutions
  • 49. Prentice-Hall General Chemistry: Chapter 7Slide 49 of 50 7-9 Fuels as Sources of Energy • Fossil fuels. – Combustion is exothermic. – Non-renewable resource. – Environmental impact.
  • 50. Prentice-Hall General Chemistry: Chapter 7Slide 50 of 50 Chapter 7 Questions 1, 2, 3, 11, 14, 16, 22, 24, 29, 37, 49, 52, 63, 67, 73, 81

Editor's Notes

  1. Thermochemistry branch of chemistry concerned with heat effects accompanying chemical reactions. Direct and indirect measurement of heat. Answer practical questions: why is natural gas a better fuel than coal, and why do fats have higher energy value than carbohydrates and protiens.
  2. Energy is from the Greek “work within”. Moving objects do work when they slow down or are stopped. Kinetic means “motion” in greek.
  3. [w] means UNITS OF WORK, not concentration in this case.
  4. Energy changes continuously from potential to kinetic. Energy is lost to the surroundings.
  5. Heat is transfer of energy. Bodies do NOT contain heat.
  6. In practice, the temperature is allowed to change and the heat that is lost or needed as the system returns to its original temperature is calculated.
  7. Heat of reaction in an isolated system produces a change in the thermal energy of the system. The causes a temperature change. In an non-isolated system the temperature remains constant and the heat is transferred to the surroundings. Top picture is CaO(s) + H2O(l) → Ca(OH)2 Bottome picture is Ba(OH)2·8H2O + 2NH4Cl(s)→BaCl2(s) + 2 NH3(aq) + 8 H2O(l)
  8. System includes everything inside the double walled container. All the water, wires, stirrer, thermometer, and the reaction chamber. Bomb is filled with sample and assembled. Then pressurized witih O2. A short pulse of electric current heats the sample and ignites it. The final temperature of the calorimeter assembly is determined after the combustion reaction. Because the reaction is carried out at a fixed volume we say that this is at constant volume.
  9. Negative sign is introduced for Pext because the system does work ON the surroundings. When a gas expands V is positive and w is negative. When a gas is compressed V is negative and w is positive, indicating that energy (as work) enters the system. In many cases the external pressure is the same as the internal pressure of the system, so Pext is often just represented as P
  10. Note that this conversion factor is simply kPa/atm.
  11. Temperature must be specified because H varies with temperature.
  12. Absolute enthalpy cannot be determined. H is a state function so changes in enthalpy, H, have unique values. Reference forms of the elements in their standard states are the most stable form of the element at one bar and the given temperature. The superscript degree symbol denotes that the enthalpy change is a standard enthalpy change and The subscript “f” signifies that the reaction is one in which a substance is formed from its elements.