Introduction to Thermochemistry Thats Me! Okaynot really Or is
it?
Slide 3
Why study thermochemistry? We depend on energy for nearly every
aspect of our lives Think about how you use energy every day
Electricity Cooking Automobiles Heating/Cooling Batteries Cars,
cell phones, iPods, watches Human Body Temperature regulation
Conversion of food into usable cellular energy
Slide 4
Seriously, why are we studying this? Energy crisis in the
world! Over-use/dependence on fossil fuels (petroleum, gasoline,
diesel, methane, propane) Research/Development of alternative
energy resources Nuclear Fuel Cells (H 2, Methanol, Solid oxide)
Hydro Wind Solar NEWS FLASH: This is going to be OUR problem!
Slide 5
Major Sources of Energy over the last 150 years
Slide 6
An interesting quote So called global warming is just a secret
ploy by wacko tree-huggers to make America energy independent,
clean our air and water, improve the fuel efficiency of our
vehicles, kick-start 21 st century industries, and make our cities
safer and more livable. Dont let them get away with it! - Chip
Giller Founder of Grist.com, where environmentally minded people
gather online.
Slide 7
Organizing the Universe Any process can be defined by the
following Universe = everything, the big enchilada, the whole kit
and caboodle, all that and a bag of chips, the whole shabang, all
that jazz, tout, todos, sarra, alles, everything-ay, Chuck Norris,
etc. System = the part of the universe we are studying i.e. a
particular chemical reaction, etc. System Surroundings Universe
Surroundings = everything else in the universe that is NOT being
studied i.e. the environment, the lab, the students, your mom,
etc.
Slide 8
Internal Energy Total Energy = Kinetic Energy + Potential
Energy Endothermic process: energy enters the system (from the
surroundings) Exothermic process: energy leaves the system (to the
surroundings) System Surroundings Energy System Surroundings Energy
due to motionstored energy
Slide 9
Kinetic Energy in Atoms & Molecules Temperature average KE
of particles in a sample Components of Kinetic Energy: KE tot = all
components added together is proportional to TranslationRotation
Vibration
Slide 10
Think of potential energy in terms of Coulombs Law Q = charge r
= distance Components of Potential Energy: Nucleus nucleus
interactions: + (repulsive, less stable) Electron electron
interactions: + (repulsive, less stable) Nucleus electron
interactions: (attractive, more stable) Intermolecular
forces:between molecules (attractive, more stable) PE total = all
interactions added together Potential Energy in Atoms &
Molecules - + + + + - + +
Slide 11
Potential Energy (PE) Chemical Change: intramolecular potential
energy Breaking and forming chemical bonds (PE nucleus-electron )
Example: 2H 2 + O 2 2H 2 O Physical Change: intermolecular
potential energy Disrupting or forming intermolecular attractions
(PE IMF ) Example: H 2 O ( ) H 2 O (g)
Slide 12
The Law of Conservation of Energy is also known as The First
Law of Thermodynamics Energy cannot be created or destroyed E
universe = 0 (reminder: = change in) E universe = E system + E
surroundings = 0 E system = - E surroundings Energy can be
transferred as:heat (q) work (w) E sys = q + w
Slide 13
The First Law of Thermodynamics Endothermic process: Exothermic
process: System Surroundings Energy System Surroundings Energy In
either case, the energy of the universe remains constant
Universe
Slide 14
Conservation of Energy in a Chemical Reaction Surroundings
System Surroundings System Energy Before reaction After reaction In
this example, the energy of the reactants and products increases,
while the energy of the surroundings decreases. In every case,
however, the total energy does not change. Myers, Oldham, Tocci,
Chemistry, 2004, page 41 Endothermic Reaction Reactant + Energy
Product
Slide 15
Conservation of Energy in a Chemical Reaction Surroundings
System Surroundings System Energy Before reaction After reaction In
this example, the energy of the reactants and products decreases,
while the energy of the surroundings increases. In every case,
however, the total energy does not change. Myers, Oldham, Tocci,
Chemistry, 2004, page 41 Exothermic Reaction Reactant Product +
Energy
Slide 16
Heat (q) Heat: the transfer of energy between objects due to a
temperature difference Flows from higher-temperature object to
lower-temperature object System (T 1 ) Surroundings (T 2 ) Heat If
T 1 > T 2 q system = - q surroundings = + exothermic System (T 1
) Surroundings (T 2 ) Heat If T 1 < T 2 q system = + q
surroundings = - endothermic
Slide 17
work = force distance force = pressure area = P m 2 distance =
m work = P m 2 m = P V Assuming external pressure (P ext ) is
constant, the volume can change (V) w system = -P ext V (in L atm)
Where V = V f V i (in L) Pressure/Volume Work (PV work)
Slide 18
Sign Conventions In chemistry, always take the systems
perspective (physics takes the surrs view) Heat (q) q > 0heat is
added to the sys by surr (q is +) q < 0heat is leaving sys to
surr (q is -) Work (w) w > 0work done on sys by surr (work added
to sys by surr, so w is +) w < 0work done by sys on surr (work
is leaving surr, so w is -)
Slide 19
Sign Conventions: Heat and Work System + q (endo) Heat - q
(exo) Work - w + w Surroundings
Slide 20
Practice with Work and Heat P ext = 2.0 atm V 1 = 5.0 L V 2 =
12.0 L An ideal gas expands from 5.0 L to 12.0 L against a constant
external pressure of 2.0 atm. How much work is done? w = -P ext V w
= -(P ext )(V final V initial ) w = -(2.0 atm)(12.0 L 5.0 L) w =
-14 L atm 1 L atm = 101.325 J w = -14 L atm (101.325 J/1 L atm) w =
-1400 J If E = 0 for this process, what is q? E = q + w = q +
(-1.42 10 3 J) = 0 q = 1400 J
Slide 21
Practice with Work and Heat Calculate the change in energy for
a system that loses 15 kJ of heat and expands from a volume of 10.
L to 200. L under a constant external pressure of 2.0 atm. E = q +
w w = -P ext V w = -(2.0 atm)(200L -10L) = w = -380 L atm (101.325
J/1 L atm) (1 kJ/1000 J) = -38.5035 kJ E = 15 kJ + -38.5035 kJ =
-53.5035 kJ -380 L atm - Remember: 101.325 J = 1 L atm 1000 J = 1
kJ -54 kJ
Slide 22
Calorimetry (Calorie Measuring) Calorimetry: the science of
measuring heat C = heat capacity the heat required to raise temp by
1C (or 1 K) Units Joules/ o C (J/ o C or J/K) Because the
temperature increase depends on the amount of stuff Specific heat
capacity (C p ) heat capacity per gram = J/g o C or J/gK Molar heat
capacity (C m ) heat capacity per mole = J/mol o C or J/mol K
Slide 23
Various Heat Capacities Substance Specific heat capacity (J/K
g) Molar heat capacity (J/K mol) Molar mass (g/mol) Gold Silver
Copper Iron Aluminum H 2 O (l) H 2 O (s) H 2 O (g) 0.129 0.235
0.385 0.449 0.897 4.184 2.03 1.998 197.0 107.9 63.55 55.85 26.98
18.02 25.4 24.5 25.1 24.2 75.3 36.6 36.0
Slide 24
q = m C T q (J) = mass (g) C (J/g o C) T ( o C) q = joules (J)
q (J) = moles (mol) C (J/K mol) T (K) q = joules (J) Mnemonic
device: q = m CAT Using heat capacities
Slide 25
Triple Point Diagrams Show the phases of a substance at
different temperatures and pressures. Courtesy Christy Johannesson
www.nisd.net/communicationsarts/pages/chem
Slide 26
Heating Curve of water Temperature ( o C) 40 20 0 -20 -40 -60
-80 -100 120 100 80 60 140 Energy Added Melting Point Boiling Point
Solid Liquid Gas s l l g
Slide 27
Heating Curve of Water Temperature ( o C) 40 20 0 -20 -40 -60
-80 -100 120 100 80 60 140 Energy Added
Slide 28
Heating Curves Temperature Change within phase change in KE
(molecular motion) depends on heat capacity of phase C H 2 O (l) =
4.184 J/g o C C H 2 O (s) = 2.03 J/g o C C H 2 O (g) = 1.998 J/g o
C Phase Changes (s l g) change in PE (molecular arrangement)
temperature remains constant overcoming intermolecular forces
(requires the most heat) (requires the least heat)
Slide 29
Heating Curves Temperature ( o C) 40 20 0 -20 -40 -60 -80 -100
120 100 80 60 140 Energy Added Melting - PE Solid - KE Liquid - KE
Boiling - PE Gas - KE
Slide 30
Calculating Energy Changes Temperature ( o C) 40 20 0 -20 -40
-60 -80 -100 120 100 80 60 140 Energy Added q = ? q = mass x C
liquid x T q = mass x C gas x T q = mass x C solid x T Same
Formulas Different C Values
Slide 31
Phase Transitions During phase transitions, added heat is used
to overcome intermolecular forces rather than to increase
temperature H fusion = energy needed to convert solid to liquid For
water, H fusion = 6.02 kJ/mol For liquid to solid, H = - 6.02
kJ/mol H vaporization = energy needed to convert liquid to gas For
water, H vap = 40.7 kJ/mol For gas to liquid, H = - 40.7
kJ/mol
Slide 32
Depending on the process occurring, all qs are calculated
individually and then added together Note: steps 2 and 4 kJ steps
1, 3, 5 J Temperature ( o C) 40 20 0 -20 -40 -60 -80 -100 120 100
80 60 140 Energy Added 2. q = mol x H fus 4. q = mol x H vap 3. q =
mass x C liquid x T 5. q = mass x C gas x T 1. q = mass x C solid x
T Unit Conversions!
Slide 33
Heat q 1 : Heat the ice to 0C q 2 : Melt the ice into a liquid
at 0C q 3 : Heat the water from 0C to 100C q 4 : Boil the liquid
into a gas at 100C q 5 : Heat the gas above 100C Heating Curve of
Water From Ice to Steam in Five Easy Steps q = m C ice T ice q =
mol H fus q = m C water T water q = mol H vap q = m C steam T steam
1 2 3 4 5
Slide 34
5 4 3 2 1 Heating Curve Practice How much energy (J) is
required to heat 12.5 g of ice at 10 o C to water at 0.0 o C? 4,430
J q 1 : Heat the ice from -10 to 0C q 2 : Melt the ice at 0C to
liquid at 0 o C q = 12.5 g (2.03 J/g o C)(0.0 - -10.0 o C) = q =
12.5 g ice 6.02 kJ 18.016 g 1 mol = q tot = q 1 + q 2 253.75 J
4.177 kJ = 253.75 J + 4,177 J =
Slide 35
5 4 3 2 1 Heating Curve Practice How much energy (J) is
required to heat 25.0 g of ice at 25.0 o C to water at 95.0 o C?
19,560 J q 1 : Heat the ice from -25 to 0C q 2 : Melt the ice at 0C
to liquid at 0 o C q 3 : Heat the water from 0C to 95 C q = 25.0 g
(2.03 J/g o C)(0.0 - -25.0 o C) = q = 25.0 g ice 6.02 kJ 18.016 g 1
mol = q tot = q 1 + q 2 + q 3 1268.75 J 8.352 kJ = 1268.75 J +
8,352 J + 9937 J = q = 25.0 g (4.184 J/g o C)(95.0 0.0 o C) = 9937
J Notice that your q values are positive because heat is added
Slide 36
5 4 3 2 1 Heating Curve Practice How much energy (J) is removed
to cool 50.0 g of steam at 115.0 o C to ice at -5.0 o C? -153,000 J
q 5 : Cool the steam from 115.0 to 100C q 4 : Condense the steam
into liquid at 100C q 3 : Cool the water from 100C to 0 C q 2 :
Freeze the water into ice at 0 C q = 50.0 g H 2 O q 1 : Cool the
ice from 0C to 5.0 C q = 50.0 g (1.998 J/g o C)(100.0 - 115.0 o C)
= q = 50.0 g H 2 O - 40.7 kJ 18.016 g 1 mol = q tot = q 1 + q 2 + q
3 + q 4 + q 5 -1498.5 J -112.96 kJ = -1498.5 J + -112,960 J +
-20920 J + -16,710 J + -507.5 J = q = 50.0 g (4.184 J/g o C)(0.0
100.0 o C) = -20920 J - 6.02 kJ 18.016 g 1 mol = -16.71 kJ q = 50.0
g (2.03 J/g o C)(- 5.0 0.0 o C) = -507.5 J Notice that your q
values are negative because heat is removed
Slide 37
Heating Curve Challenge Problems 1. A sample of ice at -25 o C
is placed into 75 g of water initally at 85 o C. If the final
temperature of the mixture is 15 o C, what was the mass of the ice?
Temperature ( o C) 40 20 0 -20 -40 -60 -80 -100 120 100 80 60 140
Time H = mol x H fus H = mol x H vap Heat = mass x t x C p, liquid
Heat = mass x t x C p, gas Heat = mass x t x C p, solid 2.A 38 g
sample of ice at -5 o C is placed into 250 g of water at 65 o C.
Find the final temperature of the mixture assuming that the ice
sample completely melts. 3.A 35 g sample of steam at 116 o C are
bubbled into 300 g water at 10 o C. Find the final temperature of
the system, assuming that the steam condenses into liquid water.
52.8 g ice 45.6 o C 76.6 o C
Slide 38
C H 2 O (l) = 4.184 J/g o C C H 2 O (s) = 2.03 J/g o C C H 2 O
(g) = 1.998 J/g o C Temperature ( o C) 40 20 0 -20 -40 -60 -80 -100
120 100 80 60 140 Energy Added H fusion = 6.02 kJ/mol H vap = 40.7
kJ/mol Heating Curve of H 2 O Constants and Graph
Slide 39
What will happen over time? Zumdahl, Zumdahl, DeCoste, World of
Chemistry 2002, page 291
Slide 40
Lets take a closer look Zumdahl, Zumdahl, DeCoste, World of
Chemistry 2002, page 291
Slide 41
Eventually, the temperatures will equalize Zumdahl, Zumdahl,
DeCoste, World of Chemistry 2002, page 291
Slide 42
Calorimetry Allows us to measure the flow of heat Think back to
the H fus expt.. q system = - q surroundings In other words,
whatever energy is lost by one is gained by the other (direct E
transfer) Major Assumption: No E is lost to other parts of the
surroundings
Slide 43
Thermometer Styrofoam cover Styrofoam cups Stirrer Typical
Apparatus A Coffee Cup Calorimeter Zumdahl, Zumdahl, DeCoste, World
of Chemistry 2002, page 302 Used for calorimetry under constant
pressure i.e. normal lab conditions
Slide 44
Example: 5.8 g of NaCl dissolves in 50.0 mL H 2 O NaCl (s) Na +
(aq) + Cl - (aq) T i = 22.2 C T f = 20.5 C What is q rxn ? q rxn =
q system q surr = m C T q surr = (55.8 g)(4.184 J/C g)(20.5 C
22.2C) q surr = -397 J q system = -q surr = 397 J Constant-Pressure
Calorimetry Coffee cup calorimeter q rxn ? We cant directly measure
q sys = -q surroundings In this case, of the surroundings
Slide 45
Bomb Calorimeter Constant V calorimetry (as opposed to P) Bomb
has own heat capacity (kJ/ 0 C) Multiply heat capacity by the T to
find the total heat transferred Factor heat into # of g or mol
burned (kJ/g or kJ/mol)
Slide 46
Bomb Calorimeter Example A 1.800 g sample of sugar, C 12 H 22 O
11, was burned in a bomb calorimeter whose total heat capacity is
15.34 kJ/ o C. Once burned, the temperature of the calorimeter plus
contents increased from 21.36 o C to 28.78 o C. What is the heat of
combustion per gram of sugar? per mole of sugar? q = C bomb x T q =
15.34 kJ/ o C (28.78 o C 21.36 o C) q = 113.8 kJ 113.8 kJ released
per 1.800 g sugar More sugar = more energy! 113.8 kJ / 1.800 g =
63.23 kJ/g 63.23 kJ g 342.3 g mol = 21640 kJ/mol
Slide 47
Food and Energy Caloric Values Food joules/grams calories/gram
Calories/gram Protein 17,000 4,000 4 Fat 38,000 9,000 9
Carbohydrates 17,000 4,000 4 Smoot, Smith, Price, Chemistry A
Modern Course, 1990, page 51 1000 calories = 1 Calorie "science"
"food" 1 calorie = 4.184 joules or 1 Kcal = 1 Calorie
Slide 48
Does water have negative calories? How many Calories
(nutritional) will you burn by drinking 1.0 L of water, initially
at 36.5 o F (standard refrigeration temperature)? Assume that the
body must expend energy to heat the water to body temperature at
98.6 o F. 37 o C 2.5 o C 1 L = 1000 mL 1 mL = 1 g q = 1.0 x 10 3 g
(4.184 J/g o C)(37 o C - 2.5 o C) = 144,348 J 1000 calories = 1
Calorie 1 calorie = 4.184 joules 144348 J1 cal 4.184 J = 35 Cal 1
Cal 1000 cal
Slide 49
150. mL 20.0 C Heat Transfer Experiments - q Cu = q water q = m
x C x T for both cases, although specific values differ Plug in
known information for each side Density of water = 1 g/mL(150 mL H
2 O) = 150 g H 2 O -m Cu C Cu T = m water C water T -20 g (0.385
J/g o C)(T f 250 o C) = 150 g (4.184 J/g o C)(T f 20 o C) Solve for
T f... T f = 22.8 C Cu 20.0 g 250.0 C C = 0.385 J/C g What is the
final temperature, T f, of the mixture?
Slide 50
240. g of water (initially at 20.0 o C) are mixed with an
unknown mass of iron initially at 500.0 o C (C Fe = 0.4495 J/g o
C). When thermal equilibrium is reached, the mixture has a
temperature of 42.0 o C. Find the mass of the iron. T = 500 o C
mass = ? grams T = 20 o C mass = 240 g LOSE heat = GAIN heat - - [
(mass) (C Fe ) ( T)] = (mass) (C H2O ) ( T) - [ (X g) (0.4495 J/g o
C) (42 o C - 500 o C)] = (240 g) (4.184 J/g o C) (42 o C - 20 o C)]
- [ (X) (0.4495) (-458)] = (240 g) (4.184) (22) 205.9 X = 22091 X =
107 g Fe -q 1 = q 2 Fe
Slide 51
A 97.0 g sample of gold at 785 o C is dropped into 323 g of
water, which has an initial temperature of 15.0 o C. If gold has a
specific heat of 0.129 J/g o C, what is the final temperature of
the mixture? Assume that the gold experiences no change in state of
matter. T = 785 o C mass = 97.0 g T = 15.0 o C mass = 323 g LOSE
heat = GAIN heat - - [(C Au) (mass) ( T)] = (C H 2 O) (mass) ( T) -
[(0.129 J/g o C) (97 g) (T f - 785 o C)] = (4.184 J/g o C) (323 g)
(T f - 15 o C)] - [(12.5) (T f - 785 o C)] = (1.35) (T f - 15 o C)]
-12.5 T f + 9.82 x 10 3 = 1.35 x 10 3 T f - 2.02 x 10 4 3 x 10 4 =
1.36 x 10 3 T f T f = 22.1 o C Au
Slide 52
If 59.0 g of water at 13.0 o C are mixed with 87.0 g of water
at 72.0 o C, find the final temperature of the system. T = 13.0 o C
mass = 59.0 g LOSE heat = GAIN heat - - [ (mass) (C H 2 O) ( T)] =
(mass) (C H 2 O) ( T) - [ (59 g) (4.184 J/g o C) (T f - 13 o C)] =
(87 g) (4.184 J/g o C) (T f - 72 o C)] - [(246.8) (T f - 13 o C)] =
(364.0) (T f - 72 o C)] -246.8 T f + 3208 = 364 T f - 26208 29416 =
610.8 T f T f = 48.2 o C T = 72.0 o C mass = 87.0 g