chapter 17: thermodynamics thermochemistry chapter 17: thermodynamics energy is the capacity to do...
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Chapter 17: Thermodynamics
Thermochemistry
Chapter 17: Thermodynamics
Energy is the capacity to do work.• Radiant energy comes from the sun and is
earth’s primary energy source
• 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
• Potential energy is the energy available by virtue of an object’s position
• Kinetic energy is the energy of motion
Chapter 17: Thermodynamics
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
Chapter 17: Thermodynamics
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
Surrounding: the rest of the universe.
Chapter 17: Thermodynamics
Collision Theory
• To explain factors affecting rxn rate
1. For two molecules to react, they must come in contact or collide.
2. When molecules collide,1. Ineffective collision occurs: molecules may
not orient in right position. No Rxn.
2. Effective collision occurs: molecules possess enough kinetic energy to position.
Chapter 17: Thermodynamics
What Happen Just Before Rxn
• Molecules approaches each other.• Repulsive force increases as they
approach each other.• There is a minimum energy to push the
molecules to collide Activation Energy (Ea)
• Supplying enough kinetic energy will “kick-start” the reaction.
Chapter 17: Thermodynamics
Graphing Rxn: Spontaneous
Chapter 17: Thermodynamics
Gibbs Free Energy (ΔG)
• If ΔG is positive, or ΔG > 0Indication: Rxn Nonspontaneous
• If ΔG is negative, or ΔG < 0Indication: System Spontaneous
• The previous example is spontaneous.
Chapter 17: Thermodynamics
Rate Influencing Factor
1. Surface Area
2. Temperature
3. Concentration
4. Presence of Catalysts
Chapter 17: Thermodynamics
Factor 1: Surface Area
• Similar to solubility• More surface area enhances collision
frequency• Homogeneous Rxn
– The reactants are in the same physical state.For example, gas reacting with gas
• Heterogeneous Rxn– The reactants are in DIFFERENT physical state
For example: Solid reacting with liquid/aq. soln
Chapter 17: Thermodynamics
Factor 2: Temperature
• Increase in temperature provide more kinetic energy for reaction to proceed
• Fast-moving molecules have better chance of “effective collision.”
• It also enhances frequency of collision.• Refrigerator is designed to SLOW reaction
rate.
Chapter 17: Thermodynamics
Factor 3: Concentration
• Higher chemical concentration generally promotes reaction rate
• Concentration is directly proportional to the frequency of collision, in general.
• Just like medicine, we need higher dosage for severely-ill patient.
Chapter 17: Thermodynamics
Factor 4: Catalyst
• In human body, we have enzymes acting as catalyst.
• It does not undergo permanent change.• It provides an alternative reaction pathway
of Lower Activation Energy.
• Inhibitor: reduces a reaction rate by preventing the reaction occurring in the usual way.– Example: Food preservatives
Chapter 17: Thermodynamics
Effect of Catalyst on Rxn
Chapter 17: Thermodynamics
Relating DE to Heat(q) and Work(w)• Energy cannot be created or destroyed.• Energy of (system + surroundings) is constant.• Any energy transferred from a system must be
transferred to the surroundings (and vice versa).
• From the first law of thermodynamics:
The First Law of Thermodynamics
wqE
Chapter 17: Thermodynamics
First Law of Thermodynamics
Energy can be converted from one form to another but energy cannot be created or destroyed.
Second Law of Thermodynamics
The entropy of the universe increases in a spontaneous process and remains unchanged in an equilibrium process.
DSuniv = DSsys + DSsurr > 0Spontaneous process:
DSuniv = DSsys + DSsurr = 0Equilibrium process:
Chapter 17: Thermodynamics
Enthalpy Changes
• The difference between the potential energy of the reactants and the products during a physical or chemical change is the Enthalpy change or ∆H.
• AKA: Heat of Reaction at constant pressure
Chapter 17: Thermodynamics
Thermochemical Equations
H2O (s) H2O (l) DH = 6.01 kJ
Is DH negative or positive?
System absorbs heat
Endothermic
DH > 0
6.01 kJ are absorbed for every 1 mole of ice that melts at 00C and 1 atm.
Chapter 17: Thermodynamics
Thermochemical Equations
CH4 (g) + 2O2 (g) CO2 (g) + 2H2O (l) DH = -890.4 kJ
Is DH negative or positive?
System gives off heat
Exothermic
DH < 0
890.4 kJ are released for every 1 mole of methane that is combusted at 250C and 1 atm.
Chapter 17: Thermodynamics
Graphing Rxn: EndothermicThe temperature goes down
Chapter 17: Thermodynamics
Graphing Rxn: ExothermicThe temperature goes up
Chapter 17: Thermodynamics
How does ΔH and ΔS affect spontaneity?
-ΔH +ΔH
+ΔS
-ΔS
Alwaysspontaneous
Spontaneity dependson temp
Spontaneity depends on
temp
neverspontaneous
Chapter 17: Thermodynamics
Cold and hot packs
• How do instant hot and cold packs work?
Chapter 17: Thermodynamics
Hot pack• Pressing the bottom , the diaphragm breaks.• Calcium chloride dissolves in water and warms it.• The beverage gets warm.
Chapter 17: Thermodynamics
EnergySurroundings
Exothermic process
• Heat flows into the surroundings from the system in an exothermic process.
Temperature rises
Hot pack
Chapter 17: Thermodynamics
Cold pack• Water and ammonium nitrate are kept in separate
compartments.• Pressing the wrapper, the ammonium nitrate dissolves in
water and absorbs heat.• The pack becomes cold.
It is used to treat sports injuries.
Chapter 17: Thermodynamics
Cold pack
Energy
Surroundings
Endothermic process
• Heat flows into the system from the surroundings in an endothermic process.
Temperature falls
Chapter 17: Thermodynamics
ExplosionsThis reaction is exothermic!
Chapter 17: Thermodynamics
PhotosyntesisThis reaction is endothermic!
Chapter 17: Thermodynamics
Combustions
These reactions are exothermic!
Chapter 17: ThermodynamicsEnthalpy Changes in Reactions
• All chemical reactions require bond breaking in reactants followed by bond making to form products
• Bond breaking requires energy (endothermic) while bond formation releases energy (exothermic)
Chapter 17: Thermodynamics
Chapter 17: ThermodynamicsEnthalpy Changes in Reactions
endothermic reaction - the energy required to break bonds is greater than the energy released when bonds form.
exothermic reaction - the energy required to break bonds is less than the energy released when bonds form.
Chapter 17: Thermodynamics
Enthalpy Changes in Reactions
∆H can represent the enthalpy change for a number of processes
1. Chemical reactions
∆Hrxn – enthalpy of reaction
∆Hcomb – enthalpy of combustion
Chapter 17: Thermodynamics
2. Formation of compounds from elements
∆Hof – standard enthalpy of formation
The standard molar enthalpy of formation is the energy released or absorbed when one mole of a compound is formed directly from the elements in their standard states.
Chapter 17: Thermodynamics
3. Phase Changes
∆Hvap – enthalpy of vaporization
∆Hfus – enthalpy of melting
∆Hcond – enthalpy of condensation
∆Hfre – enthalpy of freezing
4. Solution Formation
∆Hsoln – enthalpy of solution
Chapter 17: Thermodynamics
Time
Temp. (°C )
-40
0
100
140
q = mc∆T
q = n∆H
q = mc∆T
q = mc∆T
q = n∆H
Chapter 17: Thermodynamics
Data:
cice = 2.01 J/g.°C
cwater = 4.184 J/g.°C
csteam = 2.01 J/g.°C
ΔHfus = +6.02 kJ/mol
ΔHvap = +40.7 kJ/mol
Chapter 17: Thermodynamics
warming ice:
q = mc∆T
= (40.0)(2.01)(0 - -40)
= 3216 J
warming water:
q = mc∆T
= (40.0)(4.184)(100 – 0)
= 16736 J
warming steam:
q = mc∆T
= (40.0)(2.01)(140 -100)
= 3216 J
Chapter 17: Thermodynamics
melting ice:q = n∆H
= (2.22 mol)(6.02 kJ/mol)
= 13.364 kJ
boiling water:q = n∆H
= (2.22 mol)(40.7 kJ/mol)
= 90.354 kJ
n = 40.0 g 18.02 g/mol
= 2.22 mol
moles of water:
Chapter 17: Thermodynamics
Total Energy
90.354 kJ
13.364 kJ
3216 J
3216 J
16736 J
127 kJ
Chapter 17: Thermodynamics
Sample Problem• How much heat is required to change 36 g of
H2O from -8 deg C to 120 deg C?
Step 1: Heat the ice Q=mcΔT
Q = 36 g x 2.06 J/g deg C x 8 deg C = 593.28 J = 0.59 kJ
Step 2: Convert the solid to liquid ΔH fusion
Q = 2.0 mol x 6.01 kJ/mol = 12 kJ
Step 3: Heat the liquid Q=mcΔT
Q = 36g x 4.184 J/g deg C x 100 deg C = 15063 J = 15 kJ
Chapter 17: Thermodynamics
Sample Problem• How much heat is required to change 36 g of
H2O from -8 deg C to 120 deg C?
Step 4: Convert the liquid to gas ΔH vaporization
Q = 2.0 mol x 44.01 kJ/mol = 88 kJ
Step 5: Heat the gas Q=mcΔT
Q = 36 g x 2.02 J/g deg C x 20 deg C = 1454.4 J = 1.5 kJ
Now, add all the steps together
0.59 kJ + 12 kJ + 15 kJ + 88 kJ + 1.5 kJ = 118 kJ
Chapter 17: Thermodynamics
specific heat capacity - the amount of energy , in Joules (J,SI unit), needed to change the temperature of one gram (g) of a substance by one degree Celsius (°C).
• c: does not depend on mass, so intensive property.
• The symbol for specific heat capacity is a lowercase c
• The unit is J/ g°C or kJ/ g°C
Heat/Enthalpy Calculations
Chapter 17: Thermodynamics
• A substance with a large value of c can absorb or release more energy than a substance with a small value of c.
• with the larger c will undergo a smaller temperature change with the same amount of heat applied.
Chapter 17: Thermodynamics
FORMULA
q = mc∆T
q = heat (J)
m = mass (g)
c = specific heat capacity
∆T = temperature change
= T2 – T1
= Tf – Ti
Chapter 17: Thermodynamics
eg. How much heat is needed to raise the temperature of 500.0 g of water from 20.0 °C to 45.0 °C?
Solve q = m c ∆T
for c, m, ∆T, T2 & T1
Chapter 17: Thermodynamics
heat capacity - the quantity of energy , in Joules (J, SI unit), needed to change the temperature of a substance by one degree Celsius (°C)
• The symbol for heat capacity is uppercase C
• C: depends on mass, so extensive property.
• The unit is J/ °C or kJ/ °C
Chapter 17: Thermodynamics
FORMULA
C = mc
q = C ∆T
C = heat capacity
c = specific heat capacity
m = mass
∆T = T2 – T1
Chapter 17: Thermodynamics
Heat Capacity and Specific Heat• Calorimetry = measurement of heat flow (follow Law of
conservation of energy).• Heat lost by one substance = Heat gained by other
substance• Calorimeter = apparatus that measures heat flow.• Heat capacity = the amount of energy required to raise the
temperature of an object (by one degree). • Molar heat capacity = heat capacity of 1 mol of a
substance.• Specific heat = specific heat capacity = heat capacity of 1
g of a substance.
Calorimetry
Tq substance of gramsheat specific
Chapter 17: ThermodynamicsCalorimetry
Constant Pressure Calorimetry
TSqrxn solution) of mass total(
interest of species of moles**mol
qH rxn
rxn
The heat capacity (C) of a substance
C = ms
Heat (q) absorbed or released:
q = msDt
q = CDt
Dt = tfinal - tinitial
Chapter 17: Thermodynamics
How much heat is given off when an 869 g iron bar cools from 940C to 50C?
s of Fe = 0.444 J/g • 0C
Dt = tfinal – tinitial = 50C – 940C = -890C
q = msDt = 869 g x 0.444 J/g • 0C x –890C = -34,000 J
6.5
Chapter 17: Thermodynamics
More practice1. 5 g of copper was heated from 20C to 80C.
How much energy was used to heat the Cu?
2. If a 3.1 g ring is heated using 10.0 J, it’s temp. rises by 17.9C. Calculate the specific heat capacity of the ring. Is the ring pure gold?
q=cmT = 0.38 J/(gC) x 5 g x 60 C = 114 J
3.1 g
q=cmT10.0 J
x 17.9C= 0.18 J/(g°C)c = q/mT=
The ring is not pure. Gold is 0.13 J/(gC)
Chapter 17: Thermodynamics
H2O (s) H2O (l) DH = 6.01 kJ/mol ΔH = 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 DH changes
H2O (l) H2O (s) DH = -6.01 kJ
• If you multiply both sides of the equation by a factor n, then DH must change by the same factor n.
2H2O (s) 2H2O (l) DH = 2 mol x 6.01 kJ/mol = 12.0 kJ
Chapter 17: Thermodynamics
Standard enthalpy (heat) of formation (DH0) is the heat change that results when one mole of a compound is formed from its elements at a pressure of 1 atm.
f
The standard enthalpy of formation of any element in its most stable form is zero.
DH0 (O2) = 0f
DH0 (O3) = 142 kJ/molf
DH0 (C, graphite) = 0f
DH0 (C, diamond) = 1.90 kJ/molf
Chapter 17: Thermodynamics
Chapter 17: Thermodynamics
The standard enthalpy of reaction (DH0 ) (heat of reaction) is the enthalpy of a reaction carried out at 1 atm.
rxn
aA + bB cC + dD
DH0rxn dDH0 (D)fcDH0 (C)f= [ + ] - bDH0 (B)faDH0 (A)f[ + ]
DH0rxn DH0 (products)f= S DH0 (reactants)fS-
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.
ΔH for the overall rxn will equal to the sum of the
enthalpy changes for the individual steps.
Chapter 17: Thermodynamics
1. Calculate H forNH3 (g) + HCl (g) NH4Cl (s).
Standard heats of formation:NH3(g) = - 45.9 kJ/mol, HCl(g) = - 92.3 kJ/mol, NH4Cl(s) = - 314.4 kJ/mol
a. 176.2 kJ.b 360.8 kJ.c 176.2 kJ.d 268 kJ .
17.4 Section Quiz.
Chapter 17: ThermodynamicsBenzene (C6H6) 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 49.04 kJ/mol.
2C6H6 (l) + 15O2 (g) 12CO2 (g) + 6H2O (l)
DH0rxn DH0 (products)f= S DH0 (reactants)fS-
DH0rxn 6DH0 (H2O)f12DH0 (CO2)f= [ + ] - 2DH0 (C6H6)f[ ]
DH0rxn = [ 12 × -393.5 + 6 × -285.8 ] – [ 2 × 49.04 ] = -6535 kJ
-6535 kJ2 mol
= - 3267 kJ/mol C6H6
Chapter 17: Thermodynamics
2. The heat of formation of Cl2(g) at 25°C is
a. the same as that of H2O at 25°C.
b. larger than that of Fe(s) at 25°C.
c. undefined.
d. zero.
17.4 Section Quiz.
Chapter 17: Thermodynamics
Example:
CH4(g) + 2O2(g) CO2(g) + 2H2O(g) H = -802 kJ
2H2O(g) 2H2O(l) H= - 88 kJ
CH4(g) + 2O2(g) CO2(g) + 2H2O(l) H = -890 kJ
Hess’s Law
Given:
C(s) + ½ O2(g) CO(g) DH = -110.5 kJ
CO2(g) CO(g) + ½ O2(g) DH = 283.0 kJ
Calculate DH for: C(s) + O2(g) CO2(g)
Chapter 17: Thermodynamics
Calculate the standard enthalpy of formation of CS2 (l) given that:C(graphite) + O2 (g) CO2 (g) DH0 = -393.5 kJrxn
S(rhombic) + O2 (g) SO2 (g) DH0 = -296.1 kJrxn
CS2(l) + 3O2 (g) CO2 (g) + 2SO2 (g) DH0 = -1072 kJrxn
1. Write the enthalpy of formation reaction for CS2
C(graphite) + 2S(rhombic) CS2 (l)
2. Add the given rxns so that the result is the desired rxn.
rxnC(graphite) + O2 (g) CO2 (g) DH0 = -393.5 kJ
2S(rhombic) + 2O2 (g) 2SO2 (g) DH0 = -296.1x2 kJrxn
CO2(g) + 2SO2 (g) CS2 (l) + 3O2 (g) DH0 = +1072 kJrxn+
C(graphite) + 2S(rhombic) CS2 (l)
DH0 = -393.5 + (2x-296.1) + 1072 = 86.3 kJrxn
Chapter 17: Thermodynamics
1. According to Hess’s law, it is possible to calculate an unknown heat of reaction by usinga. heats of fusion for each of the compounds in the
reaction.b. two other reactions with known heats of reaction.
c. specific heat capacities for each compound in the reaction.
d. density for each compound in the reaction.
17.4 Section Quiz.
Chapter 17: Thermodynamics
Chapter 17: Thermodynamics
The critical temperature (Tc) is the temperature above which the gas cannot be made to liquefy, no matter how great the applied pressure.
The critical pressure (Pc) is the minimum pressure that must be applied to bring about liquefaction at the critical temperature.
Chapter 17: Thermodynamics
Where’s Waldo? Can you find…
The Triple Point?
Critical pressure?
Critical temperature?
Where fusion occurs?
Where vaporization occurs?
Melting point (at 1 atm)?
Boiling point(at 6 atm)?Carbon Dioxide
Chapter 17: Thermodynamics
Mel
ting
Fre
ezin
g
H2O (s) H2O (l)
The melting point of a solid or the freezing point of a liquid is the temperature at which the solid and liquid phases coexist in equilibrium
Chapter 17: Thermodynamics
Sub
limat
ion
Dep
ositi
on
H2O (s) H2O (g)
Molar heat of sublimation (DHsub) is the energy required to sublime 1 mole of a solid.
DHsub = DHfus + DHvap
( Hess’s Law)
Chapter 17: Thermodynamics