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Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of the universe (the system) Definitions: System: part of the universe in which we are interested Surroundings: where we make our observations (the universe) Boundary: separates above two

Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

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Page 1: Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

Thermodynamicsfrom Greek thermo dy’namis (heat and power)Studies energy changes and the direction of flow of energy usually in a well-defined

part of the universe (the system)

Definitions:

System: part of the universe in which we are interested

Surroundings: where we make our observations (the universe)

Boundary: separates above two

Page 2: Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

Heat and WorkHeat: transfer of energy that changes motions of atoms in the surroundings in a chaotic manner

Work: transfer of energy that changes motions of atoms in the surroundings in a uniform manner

= F x d

Page 3: Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

Energy• Definition: the capacity to do WORK• Units are Joules (J) = kg.m2/s2

(from KE=1/2mv2)

Work done on a system - system gains energy (w +ve)Work done by the system - system loses energy (w -ve)Heat absorbed by the system (endothermic) - system gains energy (q +ve)Heat released by the system (exothermic) - system loses energy (q +ve)

SYSTEM TOTAL ENERGY (kinetic plus potential) is the INTERNAL ENERGY (U sometimes E)

Usually measure CHANGE in internal energy ( U )U=Ufinal – Uinitial

U is a STATE FUNCTION (independent of path)

Page 4: Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

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Page 5: Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

1st LAW of ThermodynamicsInternal energy of an isolated system is constant

(energy can neither be created nor destroyed)

U = q+w

Pressure-Volume work

Against constant external pressure

w = -F.dz but Pex=F/A therefore w= -Pex.dV

Free expansion

w = 0

Page 6: Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

Calorimetry

Can measure internal energy changes in a “bomb” calorimeter

U=q-P V, but in a constant volume “bomb”, V=0

Thus U=q

Page 7: Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

Heat Capacity

Amount of energy required to raise the temperature of a substance by 1C (extensive property)

For 1 mol of substance: molar heat capacity (intensive property)

For 1g of substance: specific heat capacity (intensive property)

VV

VV

qTCU

T

UC

If heat capacity is independent of Temperature over the range of interest

Most reactions we investigate occur under conditions of constant PRESSURE (not Volume)

Page 8: Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

EnthalpyHeat of reaction at constant pressure!

PqH

VPbut

VPUH

PVUH

- w

Use a “coffee-cup” calorimeter

to measure it

PP

PP

qTCH

T

HC

Heat capacity

Excercise: When 50mL of 1M HCl is mixed with 50mL of 1M NaOH in a coffee-cup calorimeter, the temperature increases from 21oC to 27.5oC. What is the enthalpy change, if the density is 1g/mL and specific heat 4.18 J/g.K?

Page 9: Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

Problem: Heat Capacities & Temperature ChangesHow much heat is required to raise the temperature of 10 g of water and 10g of lead from 0 to 50oC?specific heat of H2O = 4.18 J/g-oCspecific heat of Pb = 0.128 J/g-oC

q = m×c×∆Tq(H2O) = 10g×4.18 J/g-oC×50oC= 2090 Jq(Pb) = 10g×0.128 J/g-oC×50oC= 64 J

Page 10: Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

Problem: Heats of Chemical Reaction100 ml solutions of 1.00 M NaCl and 1.00 M AgNO3 at 22.4 oC are mixed in coffee cup calorimeter and the resulting temperature rises to 30.2 oC.What is the heat per mole of product? Assume the solution density and specific heat

are the same as pure water.Write balanced chemical reaction:Net ionic: Ag+(aq) + Cl-(aq) → AgCl(s)Determine heat of reaction:qrxn= -qcal = -m×c×∆T

m = 200 ml × 1.0g/ml = 200gc = cH2O = 4.18 J/g-oC

= -200g × 4.18 J/g-oC × (30.2-22.4)= -6,520 JDetermine heat per mole of product:stoichiometric reactants, 0.1 mol in 100 mlqrxn/mol = -6.52 kJ/0.1 mol= -65.2 kJ/mol

See student activities

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Page 12: Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

U and H (see chapter 10)

RTnUH

P

RTn

P

nRTV

VPUH

g

g

Only differ significantly when gases are involved

Standard Enthalpy Changes, Ho

H for a process in which the initial and final species are in their standard states.

Can be reported for any T. Use 298K unless otherwise indicated

Hvapo:1 mole pure liquid vapourises to a gas at 1bar

(+40.66 kJmol-1 at 373K for water) endothermicHfus

o:1mole pure solid melts to a pure liquid at 1bar (+6.01 kJmol-1 at 273K for ice) endothermic

Page 13: Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

Standard Reaction Enthalpy Changes

Hess’s LawIf a reaction is the sum of two

separate reactions then the enthalpy change during that reaction is also the sum of the enthalpy changes in

the component reactions.

Thermochemical equations: standard heats of reaction,

rxnHo

Represent by an Enthalpy Diagram

CaO(s) + CO2(g) CaCO3(s) rxnHo = -178.3kJmol-1

Page 14: Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

Hess’s Law

rxnHo = Hoproducts - Ho

reactants

Page 15: Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

Standard Heats of FormationIf one mole of the compound is formed under standard conditions

from its elements in their standard state then the resulting enthalpy change is said to be the standard molar enthalpy (Heat)

of formation, fHo where the subscript indicates this.

By definition the enthalpies of formation of the elements in their standard states are zero.

H2 (g) + 1/2O2 (g) H2O (l) fHo = -285.8kJmol-1

2C (s) + 3H2(g) + 1/2O2(g) C2H5OH (l) fHo = -277.7kJmol-1

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Page 17: Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

Hess’s LawHess‘s Law is particularly useful for calculating fHo which would not be easy to measure experimentally. fHo for CO cannot be measured

as CO2 is also formed when graphite is burned

C(s) + 1/2O2 CO fHo = x

CO + 1/2O2 CO2 rxnHo = -283 kJmol-1

_______________________________________

C(s) + O2 CO2 fHo = -393.5 kJmol-1

From looking at these equations it is fairly obvious that the sum of the first two enthalpies is equal to the third by Hess‘s Law.

i.e. x - 283 = -393.5 or x = -110.5 kJmol-1.

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1/2H2(g)

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Page 24: Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

Enthalpy Changes and Bond Energies

Energy is absorbed when bonds break. The energy required to break the bonds is absorbed from the surroundings.

If there was some way to figure out how much energy a single bond absorbed when broken, the enthalpy of reaction could be estimated by subtracting the bond energies for bonds formed from the total bond energies for bonds broken.

O2(g) 2O(g) H°=490.4 kJ H2(g) 2H(g) H° =431.2 kJ

H2O(g)2H(g) + O(g) H°=915.6 kJ

We can estimate the bond enthalpies of O=O, H-H, and O-H as 490.4 kJ/mol, 431.2 kJ/mol, and 457.7 kJ/mol, respectively.

2H2(g) + O2(g) 2H2O(g) H°= ?

Page 25: Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

2H2(g) + O2(g) 2H2O(g)

moles of bonds broken

Energy absorbedmoles of bonds formed Energy released

2 H-H @ 431.2 kJ each 862.4kJ 4 O-H @ 457.7 kJ each 1830.9kJ

1 O=O @ 490.4 kJ each 490.4kJ_____________________________________________

1352.7kJ 1830.9kJ

H°= 1352.7 - 1830.9 kJ = -478.2 kJ.

(Remember that the minus sign means "energy released", so you add the bond energies for broken bonds and subtract energies for bonds formed to get the total energy.)

A calculation based on enthalpies of formation gave H° = -483.7 kJ

Bonds in a molecule influence each other, which means that bond energies aren't really additive. An O-H bond in a water molecule has a slightly different energy than an O-H bond in H2O2,

because it's in a slightly different environment.

Reaction enthalpies calculated from bond energies are very rough approximations!

Page 26: Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

Foods and FuelsEnthalpies (heats) of combustion: complete reaction of compounds

with oxygen. Measure using a bomb calorimeter.Most chemical reactions used for the production of heat are

combustion reactions. The energy released when 1g of material is combusted is its Fuel Value. Since all heats of combustion are exothermic, fuel values are reported as positive.

Most of the energy our body needs comes from fats and carbohydrates. Carbohydrates are broken down in the intestines to glucose. Glucose is transported in the blood to cells where it is oxidized to produce CO2, H2O and energy:

C6H12O6(s) + 6O2(g) 6CO2(g) + 6H2O(l) H°rxn=-2816 kJThe breakdown of fats also produces CO2 and H2O

Any excess energy in the body is stored as fats

CompoundFuel Value (kJ/gram)

Fats 38

Carbohydrates

17

Proteins 17

About 100 kJ per kilogram of body weight per day is required to keep the body functioning at a minimum level

Page 27: Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

Fuels

The greater the percentage of carbon and hydrogen in the fuel the higher the fuel value

FuelC

(%)H

(%)O

(%)

Fuel Value (kJ/g)

Wood 50 6 44 18

Coal 77 5 7 32

Petrol 85 15 0 48

Hydrogen 0 100 0 142

Energy comes primarily from the combustion of fossil fuels Coal represents 90% of the fossil fuels on earth. However, it typically contains sulfur, which when combusted can lead to environmental pollution (acid rain)Solar energy: on a clear day the sun's energy which strikes the earth equals 1kJ

per square meter per second. Hydrogen: clean burning (produces only water) and high fuel value. Hydrogen

can be made from coal as well as methane C(coal) + H2O(g) CO(g)+H2(g)

CH4(g) + H2O(g) CO(g) + 3H2(g)

Page 29: Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of

Global Energy Consumption