Thermochemistry:
Energy Flow
             and
       Chemical
       Reactions
        The Big Question
How are the energies involved in a
chemical reaction determined
experimentally and theoretically?
                       Outline
• thermodynamics
• internal energy – definition, first law
• enthalpy – definition, energy diagrams, calorimetry,
       theoretical calculation (heats of formation and
       Hess’ law), stoichiometry
•applications
              Thermodynamics
Thermodynamics is
the study of heat and
its transformations.
Thermochemistry is a branch of thermodynamics
that deals with the heat involved with chemical
and physical changes.
               Internal Energy
What is the difference of the two pictures above?
Energy state
If we go from cold water to boiling water as our reaction:
       H2O (solid)               H2O (gas)
       energy state 1              energy state 2
                     Internal Energy
we define E = a variable to denote the energy of our
            reacting substances
     = specifically, the internal energy of the substance
                    undergoing reaction
∆ E = change in energy
  = E (boiling water) – E (cold water)
since Energy (gas) > Energy (solid)
         ∆ E = positive , +
For the reaction to proceed, energy has to be supplied.
But where will it come from?
                  Internal Energy
A chemical system and its surroundings.
                                 the surroundings
                   the system
     System = the reaction itself, the object of our study
     Surroundings = the rest of the universe
Internal Energy
                  Internal Energy
Energy diagrams for the transfer of internal energy (E) between a
                system and its surroundings.
          DE = Efinal - Einitial = Eproducts - Ereactants
 Energy changes occurs because of the exchange of
 energy between the system and the surroundings!
                 Internal Energy
Notice that all the equations/energies refer to the system!
But we can also define it from the point of view of the
surroundings.
Case 1: surroundings supplied energy to the system
      ∆ E = E2surr - E1 surr = negative
We have to specify which we are referring to: system or
surroundings
                    E 1, sys                        E 2, sys
State 1:                            State 2:
                  E 1, surr                         E 2, surr
  E 2 sys - E1 sys = ∆ E system = positive, +
  E 2 surr - E1 surr = ∆ E surroundings = negative, -
                   Internal Energy
So we have a discrepancy of notations and definitions.
As per convention, whenever we have E1, E2, etc., we are
always referring to the system. Henceforth, we are always
referring to the system in all our studies of energies.
Notice, however that
       ∆ E system + ∆ E surr = 0
since: system + surroundings = universe
       ∆E   universe   = 0 = E2 universe - E1 universe = 0
               E2 universe = E1 universe
The energy of the universe is constant!
             Internal Energy
First Law of Thermodynamics:
The energy of the universe is
constant.
Thus, energy can neither be
created nor destroyed. It can
be only be converted from
one form to another.
                    Internal Energy
Let’s define formally E = internal energy
               = total energy of the system
               = summation of all the kinetic and potential
                      energies of the system
Experimentally:    ∆E =q+w
q = heat = energy transferred from a hotter object to a colder one
w = work = energy used to cause an object to move against a force
That means, we can change the energy of the system by
applying heat and doing work. Or,
When energy is transferred from one object to another,
it appears as work and/or as heat.
Internal Energy
A system transferring energy as heat only.
            Internal Energy
             A system losing energy as work only.
                              Zn(s) + 2H+(aq) + 2Cl-(aq)
Energy, E
                                    work done on
                           DE<0     surroundings
                               H2(g) + Zn2+(aq) + 2Cl-(aq)
                   Internal Energy
           The Sign Conventions* for q, w and DE
       q       +      w       =        DE
       +              +                 +
       +              -               depends on sizes of q and w
       -              +               depends on sizes of q and w
       -              -                 -
* For q: + means system gains heat; - means system loses heat.
* For w: + means work done on system; - means work done by system.
                         Internal Energy
DE = (sign), (number), (unit)
Sign = gives direction as to the transfer of energy
+ = E final > E initial = system gained energy from the surroundings
- =E   final   < E initial = system lost energy to the surroundings
             Internal Energy
Units of Energy
      Joule (J)    1 J = 1 kg*m2/s2
      calorie (cal)    1 cal = 4.184 J
      British Thermal Unit   1 Btu = 1055 J
      Calorie (Cal)    1 Calorie = 1 000 calorie
               Sample Problem
Hydrogen and oxygen reacts in a cylinder. As the reaction
occurs, the system loses 1150 J of heat to the
surroundings and the expanding gas product does 480 J of
work on the surroundings as it pushes against the
atmosphere. What is the change in the internal energy of
the system?
      q = heat = - 1150 J
      w = work = - 480 J
      ∆E = q + w
         = (-1150 J) + (- 480 J)
          = - 1630 J
               Sample Problem
A system receives 425 J of heat and delivers 400 J of
work to its surroundings. What is the change in internal
energy of the system (in joules)?
    Answer:       ∆E =q+w
                   = (+ 425) + (- 400 J)
                   = + 25 J
Worksheet #1-1
 Some interesting
quantities of energy.
                Enthalpy
Two different paths for the energy change of a system.
Enthalpy
           Pressure-volume
                work.
                      Enthalpy
There is another energy variable we call enthalpy:
      H = E + PV
      PV = work
      ∆H = ∆E + P ∆V
Formal definition: Enthalpy is the thermodynamic quantity
that is the sum of internal energy and the product of the
pressure-volume work.
The change in Enthalpy equals the heat gained or lost at
constant pressure.
Most chemical reactions occur at constant pressure, so ∆H
is more relevant than ∆E.
                       Enthalpy
                                  DH ≈ DE in
     w = - PDV
                            1. Reactions that do not
    H = E + PV              involve gases.
      where H is enthalpy
                            2. Reactions in which the
  DH = DE + PDV             number of moles of gas does
                            not change.
qp = DE + PDV = DH          3. Reactions in which the
                            number of moles of gas does
                            change but q is >>> PDV.
                        Enthalpy
Let’s examine enthalpy and internal energy more closely:
We defined ∆E = E2 – E1
We can calculate ∆E from the first law of thermodynamics.
What about E2, E1 or the exact energy value of a system?
E, internal energy = summation of all the energies of the
        system, including KE and PE
For a number of particles (1, 2, 3 particles) energy can be
calculated, but if we are dealing with macroscopic amounts
(ex: a mole of water, 6.02 x 1023 particles), the exact value is
incalculable and impossible!
But is it important?
                      Enthalpy
We do not need to calculate the energy values exactly. But
we assume that the energy of a system at a defined
condition is exact, fixed and unchanging.
Example:
 1.0 mol of 2.5 L water at 90 C, 1.5 atm pressure has an
internal energy E and an enthalpy H whenever this condition
is specified
Mathematically,
we call ∆E and ∆H = state functions
state function = property of a system that is determined by
specifying its conditions or its state (ex. T, P, etc.)
 = the value of a state function does not depend on the
particular history of the sample, only on its present condition
                      Enthalpy
State function analogy: scaling a mountain
The height of the mountain is a state function. However, the
way you can climb the mountain is not.
H, E = state functions
q, w = not state functions, path dependent (value depends
       on how the process took place)
                      Enthalpy
Exothermic Reactions: ∆H = H final – H initial = negative, -
     energy is released by the system
Endothermic reactions: ∆H = H final – H initial = positive, +
     energy is absorbed by the system
The sign of enthalpy (like internal energy) indicates the
direction of heat transfer during a process that occurs at
constant pressure.
                                        Enthalpy
      Enthalpy diagrams for exothermic and endothermic processes.
CH4(g) + 2O2(g)                 CO2(g) + 2H2O(g)                       H2O(l)        H2O(g)
                  CH4 + 2O2                                            H2O(g)
                                          Hinitial                                            Hfinal
Enthalpy, H
                                                     Enthalpy, H
                       DH < 0         heat out                              DH > 0            heat in
                  CO2 + 2H2O                                           H2O(l)
                                          Hfinal                                               Hinitial
              A    Exothermic process                              B      Endothermic process
                      Enthalpy
It turns out experimentally that:
∆E = energy transferred at constant volume conditions
 ∆H = energy transferred at constant pressure conditions
In most chemical reactions, we are mostly concerned with
enthalpy. As most chemical reactions occur at constant
pressure.
Thermochemical equations
2H2 (gas)+ O2 (gas)→ 2H2O (gas)           ∆H = - 483.6 kJ
The enthalpy value is given at the end of the chemical
equation.
                       Enthalpy
Some Important Types of Enthalpy Change
      heat of combustion (DHcomb)
          C4H10(l) + 13/2O2(g)              4CO2(g) + 5H2O(g)
      heat of formation (DHf)
           K(s) + 1/2Br2(l)             KBr(s)
      heat of fusion (DHfus)
           NaCl(s)              NaCl(l)
      heat of vaporization (DHvap)
             C6H6(l)          C6H6(g)
                      Sample Problem
Write a balanced equation and draw an approximate
   enthalpy diagram for each of the following:
a) Combustion of one mol of methane in oxygen
b) The evaporation of liquid water
 Answer:
 a) CH4 + 2O2 → CO2 + 2H2O, exothermic
 b) H2O(l) → H2O(g), endothermic
                  CH4 + 2O2                       H2O(g)
    Enthalpy, H
                      heat out      Enthalpy, H            heat in
                       CO2 + 2H2O                      H2O(l)
Worksheet #1-2
                      Enthalpy
Properties of enthalpy:
1. Enthalpy is an extensive property. Thus its magnitude is
   directly proportional to the amount of substance reacted
   or produced.
Implication: in a thermochemical equation, if the equation is
  multiplied by 2, the ∆H is also multiplied by 2. If the
  equation is divided by 2, the ∆H is also divided by two.
Example:
CH4 (g) + 2O2 (g) → CO2 (g) + 2H2O (l)      ∆H = - 890 kJ
2CH4(g) + 4O2 (g) → 2CO2 (g) + 4H2O(l)      ∆H = 2(- 890) kJ
                       Enthalpy
2. ∆H reaction = - ∆H reverse reaction
 CO2 (g) + 2H2O (l) → CH2 (g) + 2O2 (g)     ∆H = 890 kJ
3. ∆H is dependent on the state of the chemical species used
   in the equation. The state of the substance has to be
   shown.
Example:
CO2 (g) + 2H2O (l) → CH4 (g) + 2O2 (g)         ∆H = 890 kJ
CO2 (g) + 2H2O (g) → CH4 (g) + 2O2 (g)         ∆H = 978 kJ
                     Enthalpy
Review of chemical stoichometry
CH4 (g) + 2O2 (g) → CO2 (g) + 2H2O (l)   ∆H = - 890 kJ
• How many moles of CH4 will react with 5.0 moles of O2?
      (answer = 2.5 moles CH4)
• How many moles of CO2 will be produced from the
  reaction of 2.8 moles CH4 with excess O2?
      (2.8 moles)
• How many grams of CO2 will be produced from the
  reaction of 15.7 grams of CH4 with excess O2?
      (43.2 grams)
• How much energy will be produced from the reaction of
  15.7 grams of CH4 with excess O2?
                       Enthalpy
Enthalpy and chemical stoichometry
-The calculation of the enthalpy for a particular reaction and
its relation to the chemical equation is governed the
extensive property of enthalpy.
Example:
CH4 (g) + 2O2 (g) → CO2 (g) + 2H2O (l)       ∆H = - 890 kJ
relationships: 1 mol CH4 is to ∆H = - 890 kJ
               2 mol O2 is to ∆H = - 890 kJ
               1 mol CO2 is to ∆H = - 890 kJ
                2 mol H2O is to ∆H = - 890 k
              Sample Problem
Consider the equation:
CH4 (g) + 2O2 (g) → CO2 (g) + 2H2O (l)    ∆H = - 890 kJ
1. How many moles of methane, CH4 (g) has to be burned
   to generate 1500 kJ of energy?
2. How many grams of carbon dioxide is produced if the
   enthalpy generated in the combustion is 1830 kJ?
                 Sample Problem
Consider the following balanced thermochemical equation
for a reaction sometimes used for H2S production:
     1/8 S8 + H2 → H2S       ΔH = - 20.2 kJ
a)   Is this an exothermic or endothermic reaction?
b)   What is the ΔHrxn for the reverse reaction?
c)   What is ΔH when 3.2 mol of S8 reacts?
d)   What is ΔH when 20.0 g of S8 reacts?
     Answers:
     a) Exothermic
     b) 20.2 kJ
     c) -517 kJ
     d) -12.6 kJ
                     Enthalpy
                      Summary of the relationship
AMOUNT (mol)          between amount (mol) of
of compound A
                      substance and the heat (kJ)
                      transferred during a reaction.
                      AMOUNT (mol)
                       of compound B
 molar ratio from
balanced equation
                                          HEAT (kJ)
                    DHrxn (kJ/mol)      gained or lost
Worksheet #1 - 3
                  Enthalpy
Calorimetry = measurement of heat flow
Calorimeter = apparatus that measures heat flow
∆H reaction can be determined experimentally
using a calorimeter.
      Enthalpy
How do you measure
enthalpy (ΔH)
experimentally?
                          Enthalpy
Coffee-cup calorimeter.
                          Enthalpy
In chemical equations, energy changes can be calculated by
monitoring the temperature changes in the reaction.
             q is proportional to ∆T
In equation form:   q α    ∆T
                    q = C ∆T
where C = constant of proportionality
       = heat capacity
       = amount of heat required to raise the temperature of
       a substance by 1.0 Kelvin
The larger the heat capacity the greater the heat required to
produce a given rise in temperature.
For 1.0 mol substance , C = C (mol)
                             Enthalpy
Lets look at another experiment:
1.0 L water and 10.0 ml water are heated separately such that each would
have its temperature increase by 10.0 C. What would be the result?
The 10.0 ml water sample will have a greater increase in energy as some of
its molecules can turn into gas.
Implication: mass is also a factor in measuring enthalpies.
                q = C ∆T
As there is no mass in the equation, it can be in the heat capacity factor.
               C=mc
        where m = mass of the substance
               c = specific heat of the substance
Thus,           q = m c ∆T
                Enthalpy
Heat Capacity   C = q / ΔT
           unit: J/K
Specific heat capacity (c) = q / (mass x ΔT)
           unit: J/gK
Molar heat capacity (C mol) = q / (moles x ΔT)
           unit: J/mol K
Table 6.2 Specific Heat Capacities of Some Elements, Compounds, and Materials
    Substance             Specific Heat            Substance            Specific Heat
                         Capacity (J/g*K)                              Capacity (J/g*K)
       Elements                                    Materials
        aluminum, Al        0.900                      wood               1.76
        graphite,C          0.711                      cement             0.88
        iron, Fe            0.450                      glass              0.84
        copper, Cu          0.387                      granite            0.79
        gold, Au            0.129                      steel              0.45
                     Compounds
                       water, H2O(l)                           4.184
                       ethyl alcohol, C2H5OH(l)                2.46
                       ethylene glycol, (CH2OH)2(l)            2.42
                       carbon tetrachloride, CCl4(l)           0.864
                        Enthalpy
Relation of enthalpy and q (from calorimetry experiments)
      q = m c ∆T = q solution
      q solution = - q reaction = ∆H reaction
      ∆H reaction = - m c ∆T
               Sample Problem
A 295 g aluminum engine part at an initial temperature of
3.0 C absorbs 85.0 kJ of heat. What is the final
temperature of the part (specific heat of aluminum = 0.900
J/g K)?
    q = m c ∆T
    85 000 J = 295 g Al (0.900 J/gK) (Tf – 3.0 C)
    Answer: Tf = 323 C
                Sample Problem
When 165 ml of water at 22 C is mixed with 85 mL of water
at 82 C, what is the final temperature? Assume that no
heat is lost to the surroundings (density of water is 1.0
g/mL).
      (m c ∆T) water 1 = - (m c ∆T) water 2
      165 ml ( Tf – 22 C ) = - 85 ml (Tf – 82 C)
       Answer: Tf = 42 C
Worksheet #1 - 4
A bomb calorimeter
           Internal Energy
In a bomb calorimeter, the conditions are
such the volume of the set-up is constant.
Thus, the internal energy, ∆E is the one
obtained.
           Enthalpy of Formation
∆H formation = ∆H f = enthalpy associated with the
       formation of a compound from its constituent elements
Examples of formation equations:
C (graphite) + O2 (gas) → CO2 (gas)
2C (graphite) + H2 (gas) → C2H2 (gas)
C (graphite) + 2H2 (gas) + 1/2 O2 (gas) + N2 (gas) → CH4N2O(urea)
The reactants should be elements in their natural form
             Enthalpy of Formation
Write balanced formation equations at standard conditions
   for each of the following substances:
a) CaCl2
b) NaHCO3
c) CCl4
d) HNO3
  Answer:
  a) Ca(s) + Cl2(g) → CaCl2(s)
  b) Na(s) + ½ H2(g) + Cgraph + 3/2 O2(g) → NaHCO3(s)
  c) Cgraph + 2Cl2(g) → CCl4(l)
  d) ½ H2(g) + ½ N2(g) + 3/2 O2(g) → HNO3(l)
               Enthalpy of Formation
∆H = depends of various conditions such as T, P, state of matter, etc., of the
reactants and products
To compare enthalpies, it is convenient to define a set of conditions called a
standard state at which the enthalpies are tabulated.
Standard state = pure form of the substance at 1.0 atmospheric pressure
         and at 25 C (298 K)
∆Ho = standard enthalpy = enthalpy at standard conditions of all species
∆Hof = standard enthalpy of formation
      = change in enthalpy of reaction that forms 1.0 mol of compound
         from its elements with all the substances in their standard states
If the element exists in more than one form under standard conditions, the
most stable form of that element is used for ∆Hof
              Enthalpy of Formation
2C (graphite) + 3H2 (gas) + ½ O2 (gas) → C2H5OH ∆Hof = -277.7 kJ
C (graphite) + O2 (gas) → CO2 (gas)         ∆Hof = - 393.5 kJ
2C (graphite) + 3H2 (gas) →    C2H6 (gas)    ∆Hof = - 84.68 kJ
The standard enthalpy of formation, ∆Hof values are tabulated in books
and can be consulted every time it is needed.
Table 6.5 Selected Standard Heats of Formation at 250C(298K)
  Formula      DH0f(kJ/mol)   Formula DH0f(kJ/mol)   Formula DH0f(kJ/mol)
  calcium                                            silver
                                 Cl2(g)      0
    Ca(s)            0                                   Ag(s)        0
                                 HCl(g)    -92.3
    CaO(s)        -635.1                                 AgCl(s)   -127.0
    CaCO3(s)     -1206.9      hydrogen
                                H(g)       218       sodium
  carbon
                                H2(g)        0           Na(s)        0
     C(graphite)      0
     C(diamond)       1.9     nitrogen                   Na(g)      107.8
     CO(g)         -110.5        N2(g)       0           NaCl(s)   -411.1
     CO2(g)        -393.5        NH3(g)    -45.9     sulfur
     CH4(g)         -74.9        NO(g)      90.3         S8(rhombic) 0
     CH3OH(l)      -238.6                                S8(monoclinic) 2
                              oxygen
     HCN(g)         135                                  SO2(g)     -296.8
                                 O2(g)       0
     CSs(l)        87.9
                                 O3(g)     143           SO3(g)    -396.0
   chlorine                      H2O(g)   -241.8
      Cl(g)        121.0         H2O(l)   -285.8
        Enthalpy of Formation
Using the tabulated values, we can calculate the
enthalpy of reaction
DH0rxn = S mDH0f(products) - S nDH0f(reactants)
      where m = number of moles of each product
             n = number of moles of each reactant
                       Enthalpy of Formation
              The general process for determining DH0rxn from DH0f values.
                                              Elements
                              decomposition
Enthalpy, H
                                              -DH0f               DH0f
                                                      formation
                  Reactants
                                                                                Hinitial
                                                                              DH0rxn
                                                                   Products
                                                                                Hfinal
                        DH0rxn = S mDH0f(products) - S nDH0f(reactants)
                Sample Problem
Calculate the enthalpy of reaction of the equation below
using standard enthalpies of formation.
C3H8 (g) + 5 O2 → 3 CO2 (g) + 4 H2O (l)
Solution:
∆Ho reaction = 3∆Hof [CO2(g)] + 4Hof [H2O (l)] - ∆Hof [C3H8 (g)] -
                       5∆Hof [O2 (g)]
       = 3 (-393.5 kJ) + 4 (-285.8 kJ) – (-103.85 kJ) – 5( 0 kJ)
       = - 2220 kJ
               Sample Problem
Calculate the enthalpy of reaction of the equation below
using standard enthalpies of formation.
C6H6 (l) + 15/2 O2 → 6 CO2 (g) + 3 H2O (l)
Solution:
∆Ho reaction = 6∆Hof [CO2(g)] + 3Hof [H2O (l)] - ∆Hof [C6H6 (g)] -
                       15/2 ∆Hof [O2 (g)]
       = 6 (-393.5 kJ) + 3 (-285.8 kJ) – (49.0 kJ) – 15/2(0 kJ)
       = - 3267.4 kJ
                    Sample Problem
Acetylene burns in air according to the following equation:
     C2H2 + 5/2 O2 → 2CO2 + H2O              ΔH = -1255.8 kJ
Given that ΔHfo of CO2 = - 393.5 kJ/mol and ΔHfo of H2O =
-241.8 kJ/mol, what is the ΔHfo of acetylene?
Solution:
∆Ho reaction = 2∆Hof [CO2(g)] + Hof [H2O (l)] - ∆Hof [C2H2 (g)] -
                     5/2 ∆Hof [O2 (g)]
∆Hof [C2H2 (g)] = 227 kJ/mol
Worksheet #1 - 5
        Enthalpies of Reaction
Which is a more accurate calculation?
• the one using the enthalpies of formation
(state of substances indicated, position of
atoms indicated, values are not averaged, etc..)
• bond energies are used to only estimate the
enthalpy of reaction and if enthalpy of formation
of some substances are unknown
                           Hess Law
Hess’s Law of Heat Summation
 = the enthalpy change of an overall process is the sum
    of the enthalpy changes of its individual steps
Steps in calculating an unknown ΔH
1. Identify the target equation, the step whose ΔH is unknown and note
    the number of moles of reactants and products.
2. Manipulate the equations with known ΔH values so that the target
    numbers of moles of reactants and products are on the correct side.
        Remember:
        - change the sign of ΔH when you reverse an equation
        - multiply numbers of moles and ΔH by the same factor
3. Add the manipulated equations to obtain the target equation. Add their
    ΔH values to obtain the unknown ΔH .
              Sample Problem
Calculate ΔHrxn for:
      Ca + ½ O2 + CO2 → CaCO3
Given the following set of reactions:
      Ca + ½ O2 → CaO              ΔH = - 635.1 kJ
      CaCO3 → CaO + CO2 ΔH = 178.3 kJ
        Answer: - 813.4 kJ
            Sample Problem
Calculate ΔHrxn for:
      C2H4 + 6F2 → 2CF4 + 4HF
Given the following set of reactions:
      H2 + F2 → 2HF           ΔH = - 537 kJ
      C + 2F2 → CF4            ΔH = - 680 kJ
      2C + 2H2 → C2H4          ΔH = + 52.3 kJ
        Answer: - 2490 kJ
      Heats of Formation and Hess’s Law
The common lead-acid car battery produces a large burst of
currrent, even at low temperatures, and is rechargeable. The
reaction that occurs while recharging a dead battery is:
2PbSO4(s) + 2H2O(l) → Pb(s) + PbO2(s) + 2H2SO4(l)
a. Use ΔHfo values to calculate ΔHrxn.
b. Use the following equations to check your answer in part (a).
Pb(s) + PbO2(s) + 2SO3(g) → 2PbSO4(s)                 ΔH = -768 kJ
SO3(g) + H2O(l) → H2SO4(l)                            ΔH = -132 kJ
  Answer: = 2(-813.99) + (-276.6) + 0 - 2(- 918.39) – 2(-285.84)
          = 503.88 kJ
Worksheet #1 - 6
                  Energy from Foods
Heats of Combustion of Some Fats and Carbohydrates
    Substance                     DHcomb(kJ/g)
    Fats
     vegetable oil                   -37.0
     margarine                       -30.1
     butter                          -30.0
    Carbohydrates
     table sugar (sucrose)           -16.2
     brown rice                      -14.9
     maple syrup                     -10.4
            Points to ponder…….
Which is a better source of energy for our body?
Proteins
Carbohydrates
Fats
       Points to ponder…….
How do cold packs and hot packs work?