1422-Chapt-15-Thermodynamics.good_notes (1).docx

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    Chapter 15

    (not much on E)

    Thermodynamics:

    Enthalpy, Entropy

    & Gibbs Free

    Energy

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    mo Thermodynamics: thermo = heat (energy)

    dynamics = movement, motion

    Some thermodynamic terms chemists use:

    System: the portion of the universe that we areconsidering

    open system: energy & matter can transfer

    closed system: energy transfers only

    isolated system: no transfers

    Surroundings: everything else besides the system

    Isothermal: a system that is kept at a constant

    temperatureby adding or subtracting heat from the

    surroundings.Heat Capacity: the amount of heat energy required to

    raise the temperature of a certain amount of material by

    1C (or 1 K).

    Specif ic Heat Capacity: 1 g by 1C

    Molar H eat Capacity: 1 mole by 1C

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    mo Calorie: the amount of heat required to raise the

    temperature of 1g of water by 1C.

    specific heat of water = 1 cal/g C

    1 calorie = 4.18 joules

    Specific Heats and Molar Heat Capacities

    Substance

    Al

    Specific Heat

    (J/C

    g Molar Heat (J/C

    mol)

    .0.380.450.84

    .24.425.183.8

    CuFe

    CaCO3

    Ethanol

    WaterAir

    2.43

    4.181.00

    112.0

    75.3~ 29

    important to: engineers chemists

    EXAMPLE: How many joules of energy are needed raise

    the temperature of an iron nail (7.0 g) from 25C to125C?The specific heat of iron is 0.45 J/CHeat energy = (specific heat)(mass)(T)

    Heat energy = (0.45 J/C g)(7.0 g)(100C) = 315

    J

    g.

    Note that T can be C or K, but NOT F. When jusbeing used

    in a scientific formula it will usually be kelvin

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    Problem: How much energy does it take to raise

    the body temperature 2.5C (a fever of just over

    103F) for someone who weighs 110 pounds (50 kg).

    Assume an average body specific heat capacity of3 J/C.g.

    Problem: What would be more effective at melting

    a frozen pipehot water or a hair dryer (hot air

    gun). Why?

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    mo State Functions

    System properties, such as pressure (P), volume (V),

    and temperature (T) are called state functions.

    The value of a state function depends only on the state

    of the system and not on the way in which the system

    came to be in that state.

    A change in a state function describes a difference

    between the two states. It is independent of the

    process or pathway by which the change occurs.

    For example, if we heat a block of iron from room

    temperature to 100C, it is not important exactly how

    we did it. Just on the initial state and the final state

    conditions. For example, we could heat it to 150C,

    then cool it to 100C. The path we take is unimportant,so long as the final temperature is 100C.

    Miles per gallon for a car, is NOT a state function. It

    depends highly on the path: acceleration, speed, wind,

    tire inflation, hills, etc.

    Most of the thermodynamic values we will discuss in

    this chapter are state functions.

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    mo Energy: " The capacity to do work

    and/or transfer heat"

    Forms of Energy:

    Kinetic (Ekinetic = mv2)

    Heat

    Light (& Electromagnetic)

    Electricity

    Sound

    Potential

    Gravitational

    Chemical

    Nuclear - Matter (E = mc2)

    WORK

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    mo

    First Law of Thermodynamics:

    The total amount of energy (and

    mass) in the universe is constant.

    In any process energy can be

    changed from one form to

    another; but it can never be

    created nor destroyed.

    You can' t get something for

    nothing

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    mo

    Enthalpy (Heats) of Reaction

    The amount of heat released or absorbed by a

    chemical reaction at constant pressure (as one woulddo in a laboratory) is called the enthalpy or heat or

    reaction. We use the symbol H to indicate

    enthalpy.

    Sign notation (EXTREMELY IMPORTANT!!):

    +H indicates that heat is being absorbed in the

    reaction (it gets cold)

    H indicates that heat is being given off in the

    reaction (it gets hot) exothermic

    endothermic

    Standard Enthalpy = H ( is called a not)

    Occurring under StandardConditions:

    Pressure 1 atm (760 torr)

    1.0 MConcentration

    Temperature is notdefined or part of Standard

    Conditions, but is often measured at 298 K (25C).

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    mo Standard Enthalpy of Formation -- Hf

    The amount of heat absorbed (endothermic) or

    released (exothermic) in a reaction in which one

    mole of a substance is formed from its elements in

    their standard states, usually at 298 K (25C).

    Also called heat of formation.

    Hf = 0 for any element in its standard state (the

    natural elemental form at 1 atm or 1 M) at 298 K.

    EXAMPLES:

    grap e, s +O2(g) (g)H = 0 kJ/mol 0kJ/mol

    .kJ/mol

    rxn

    product(one mole)elements in

    theirstandard states

    nega ve s gnheat released --exotherm ic rxn

    H (CO2) = 393.5kJ/mol

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    mo10g +(g) (g)

    H = 0 kJ/mol 0kJ/mol

    .mol

    rxn

    elements intheirstandardstates

    product(twomoles

    v e yto puton per molebasis!!

    nega ve s gnheat released --

    exotherm ic rxn H (H O) = 241.8kJ/mol

    ote that I usually will nothave you calculate Hf onhomeworks or testsso you generally dont have to worry about normalizinanswer to a

    per mole basis.Hess's Law -- Adding Reactions

    The overall heat of reaction (Hrxn) is equal to the

    sum of the Hf (products) minus the sum of the Hf

    (reactants):

    (# eqiv)H(reactants)

    f

    = eq v(products)rxn

    Therefore, by knowing Hf of the reactants and

    products, we can determine the Hrxn for any

    reaction that involves these reactants and products.

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    mo11EXAMPLE: CO2 is used in certain kinds of fireextinguishers

    to put out simple fires. It works by smothering the fi" heavier" CO2 that replaces oxygen needed to maintfire.CO2 is not good, however, for more exotic electrical

    chemical fires.g s

    COg s

    C s =kJ/mol

    -kJ/mol

    - mokJ/mol

    TS TS

    (# eqiv)H(reactants)

    f

    = eq v (products)rxn

    (2 eqiv)(-602 kJ/mol) + (1

    eqiv)(0 kJ/mol)

    = rxn

    (2 eqiv)(0 kJ/mol) + (1 eqiv)

    393 kJ/mol)= -

    kJ/mol)-

    kJ/mol)rxn

    = - mo +

    393 kJ/mol

    rxn

    } highly exothermic

    rxn !!

    =kJ/mol

    x

    Therefore, Mg will " burn"CO2 !

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    mo12You can also add two reactions together to get the Hfor

    another new reaction:Calculate for the

    following reaction:

    HrxnH O l OH l =??4 5 nven ese wo reac ons an

    thermod namic data:a+ 3O2(g)b) C H (g) +

    3O (g)

    g3H2O(l)2CO2(g) +

    2H2O(l)

    = -kJ/moln = -kJ/mol4 n

    ow osolve:

    s on e pro uc s e o e rsreaction -- so we want to5sw c equa on a aroun o ge a son the roduct side:5

    g3H2O l

    g +1367 kJ/mol

    rxn

    *

    no e awhen we

    chan es si n! ! !

    reverse ereaction, H n

    ow we can a e wo reac ons oge erto ive us the desirednereaction:

    C2H5OH(l) + 3O2(g) H= +1367 kJ/mol

    rxn

    g3H2O l

    +H = -1411kJ/molrxn

    g3O

    g2H2O l4

    H = -44

    kJ/molrxn

    gH O l OH l4 5

    If we have to multiply one (or more) of the reactions someconstant to get them to add correctly, then we also wohaveto multiply Hrxn for that reaction by the same amo

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    mo14Problem: Calculate H for the followingrxnreactions given the following Hf values:

    Hf (SO2, g) = 297kJ/mol

    Hf (H2SO4, l) = 814

    kJ/mol

    Hf (H2O, l) = 286

    kJ/mol

    Hf (SO3, g) = 396kJ/mol

    Hf (H2SO4, aq) = 90

    kJ/mol

    Hf (H2S, g) = 20

    kJ/mol

    a) S(s) + O2(g) SO2(g)

    b) 2SO2(g) + O2(g)

    c) SO3(g) + H2O(l)

    d) 2H2S(g) + 3O2(g)

    2SO3(g)

    H2SO4(l)

    2SO2(g) + 2H2O(l)

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    mo15Internal Energy -- E

    The internal energy, E, represents all the energy

    contained within a material. It includes kinetic

    energy (heat), intra- and intermolecular forces

    (bond energies, electrostatic forces, van der Waals),

    and any other forms of energy present. As with

    enthalpy, H, the absolute value cant (or is extremely

    difficult) to define.What we can track is the change in E:

    E = EfinalEinital = Eproducts

    Ereactants

    A key relationship is:E = q + w

    Where q = heat and w = work performed on or by

    the system. Sign notations:

    q= positive = heat added to system (adds energy)

    q= negative = heat removed (removes energy)

    w= positive = work done on system (adds energy

    w= negative = work done by system (removes ener

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    mo16The most common type of work involvespressure/volume changes: e.g., explosion of gasoline

    vapors in an internal combustion engine. The

    explosion creates a dramatic pressure and volumeincrease that pushes the piston and creates work.

    If one has a constant volume situation, then no

    pressure/volume work will be done and w = 0.

    So under constant volume conditions:

    E = qThe change in internal energy is, therefore, equal to

    the amount of heat added or removed from the

    material (system).

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    mo17Relationship Between E & H

    E = q (at constant volume and temperature)

    H = q (at constant pressure and temperature)

    The difference is that volume changes occur for H athat typically involves work of some type. Remembethat significant volume changes only occur when gassare involved. So we only need to be concerned about

    volume work when there is a change in the amount oproduced in a chemical reaction.

    The relationship between H and E is defined,

    therefore, as:

    H = E + (n)RT

    Where R = gas constant; T = temperature in kelvin,and:

    n = equivalents (moles) of product gas

    equivalents (moles) of reactant gas

    If n = 0, then H = E.

    But even when n 0, the PV work component is ussmall. See example in textbook (pages 574-575).

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    mo18Entropy

    The final state of a system is more energetically

    favorable if:

    1. Energy can be dispersed over a greater number

    and variety of molecules.

    2. The particles of the system can be more

    dispersed (more disordered).

    The dispersal of energy and matter is described by

    the thermodynamic state function entropy, S.

    The greater the dispersal of energy or matter in a

    system, the higher is its entropy. The greater the

    disorder (dispersal of energy and matter, both in

    space and in variety) the higher the entropy.Adding heat to a material increases the disorder.

    -structure

    -disordered

    -disordered

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    mo19Unlike H, entropy can be defined exactly becauseof the Third Law of Thermodynamics:

    Third Law of Thermodynamics: Any

    pure crystalline substance at a

    temperature of absolute zero (0.0 K) has

    an entropy of zero (S = 0.0 J/Kmol).

    Sign notation (EXTREMELY IMPORTANT!!):

    +S indicates that entropy is increasing in the

    reaction or transformation (it's getting more

    disordered -- mother nature likes)

    S indicates that entropy is decreasing in thereaction or transformation (it's getting less

    disordered {more ordered} -- mother nature doesn't

    like, but it does happen)

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    mo20Qualitative " Rules" About Entropy:

    1) Entropy increases as one goes from a solid to a

    liquid, or more dramatically, a liquid to a gas.

    0d s

    0

    15

    0

    10

    0

    50

    uid

    p asetransi t ions

    re K2) Entropy increases if a solid or liquid is dissolved

    in a solvent.

    3) Entropy increases as the number of particles

    (molecules) in a system increases:

    N2O4(g) 2NO2(g)

    S= 304 J/K(1

    mole)

    S= 480 J/K (2

    moles)These first 3 above are most important forevaluating Srxn.

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    mo21The rules below are mainly for comparing theentropy of individual molecules or materials.

    4) The Entropy of any material increases with

    increasing temperature

    5) Entropy increases as the mass of a molecule

    increases

    S(Cl2(g)) > S(F2(g))

    S= 165 J/K mol S= 158 J/Kmol

    6) Entropy is higher for weakly bonded compounds

    than for compounds with very strong covalent

    bonds

    S(graphite) > S(diamond)

    S= 5.7 J/K mol S= 2.4 J/Kmol

    Note that for individual molecules(materials) the

    higher the entropy, the more likely the molecule will

    want to fall apart to produce a number of smallermolecules.

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    7) Entropy increases as the complexity (# of atoms,

    # of heavier atoms, etc.) of a molecule increases

    ntropy o a er es o Gaseous

    H drocarbons

    S = 186 J/KmolHe a

    ne

    S = 201 J/Kmol

    S = 220 J/Kmol

    ce y en e

    Hy e

    ne

    S = 230 J/Kmol

    S = 270 J/KmolH

    H H ane

    C

    H

    C

    HH ropane

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    mo23What are the biggest factors for evaluating Srxn for

    a chemical rxn?

    1) phase change 2) change in # of molecules

    Problem: For the following reactions, is the entropy

    of the reaction increasing or decreasing?

    a) Ag+(aq) + Cl-(aq)

    b) H2CO3(aq)

    AgCl(s)

    H2O + CO

    2(g)

    c) Ni(s) + 4CO(g)

    d) H2O(s)

    Ni(CO)4(l)

    H2O(l)

    e) graphite diamond

    f) 2Na(s) + 2H2O

    g) H2S(g) + O2(g)

    h) 2H2O(l)

    2Na+(aq) + 2OH (aq) +H2(g)

    -

    H2O(l) + SO(g)

    2H2(g) + O2(g)

    i) CO2(g) + CaO(s)

    ) CaCl2(s) + 6H2O(l)

    CaCO3(s)

    CaCl26H2O(s)

    k) 2NO2(g) N2O4(g)

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    Just as with enthalpies, one can calculate entropies

    of reaction.

    (# eqiv)S(reactants)

    S = (# eqiv)S

    (products)rxn

    EXAMPLE:

    g s +CO

    g s +C s

    S = 32 J/Kmol 215

    J/Kmol J/Kmol J/Kmol

    TS TS

    (# eqiv)S(reactants)

    S = (# eqiv)S

    (products)rxn

    = eq v mo + eq v

    (2 eqiv)(32 J/Kmol) + (1 eqiv

    J/Kmol)

    rxn

    =

    J/K.mol) J/K.mol)rxn

    }S = 218J/K.mol

    entropy s ecreas ng(reaction is becomingmore ordered

    rxn

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    mo25Spontaneous Processes

    A process that takes place without the net input of

    energy from an external source is said to be

    spontaneous (notinstantaneous).

    1) Rxn of sodium metal with water:

    -2Na(s) + 2H2O 2Na+(aq) + 2OH (aq) +

    H2(g)

    2) Combustion rxns:

    C3H8(g) + 5O2(g) 3CO2(g) + 4H2O(g)

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

    3) Expansion of a gas into a vacuum

    xCO2(g) yCO2(s) + zCO2(g) (x = y + z)

    4) A salt dissolving into solution:

    NH4NO3(s) + H2O(l) NH4+(aq) + NO3-(aq)

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    mo26Second Law of Thermodynamics: In

    any spontaneous process the entropy

    of the universeincreases

    Suniverse = Ssystem + Ssurroundings

    Second Law (variant): in trying to do

    work, you alwayslose energy to the

    surroundings.

    You can' t even break even!

    Neither entropy (S) or enthalpy (H)

    alone can tell us whether a chemical

    reaction will be spontaneous or not.

    An obvious (?) conclusion is that one

    needs to use some combination of the two.

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    mo27Gibbs Free Energy

    The combination of entropy, temperature

    and enthalpy explains whether a reaction is

    going to be spontaneous or not. The symbol

    Gis used to define the Free Energyof a

    system. Since this was discovered by J.

    Willard Gibbs it is also called the Gibbs

    Free Energy. "Free" energy refers to the

    amount of energy available to do work once

    you have paid your price to entropy. Note

    that this is not given simply by H, the heat

    energy released in a reaction.

    G = H TS

    When G is negative, it indicates that a

    reaction or process is spontaneous. A

    positive G indicates a non-spontaneous

    reaction.

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    mo28

    G = H TS

    S

    +

    G = negative G = ??

    spontaneous

    spontaneousat all

    temperaturesat hightemperatures

    - +0 H

    G = ?? G = positive

    spontaneousat lowtemperatures

    non-spontaneousat alltemperatures

    -

    Spontaneous = exoergic (energy releasing)

    Non-spontaneous = endoergic (energy releasing)

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    mo29Remember that entropies are

    given in units of J/Kmol while

    enthalpies and free energies are in

    kJ/mol.

    DON'T forget to convert all units to

    kJ or J when using both S and H

    in the same equation! !

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    mo30G vs. G: Standard vs. Non-Standard Condition

    Remember that the (not) on G indicates that th

    numerical value of G is based on the reaction atstandard conditions (1 M solution concentration, 1 atgas pressure). Temperature is NOT part of standardconditions!

    As soon as one has a concentration different than 1 M1 atm pressure, the not goes away and one has G

    Consider the reaction:

    Initial: 1 atm 1 atm 1 atm

    2SO2(g) + O2(g) 2SO3(g)

    Grxn = 142 kJ/mol

    The Grxnof 142 kJ/mol is for when each gas is pr

    with a concentration of 1 atm. This indicates that thereaction under these conditions will proceed to makeproducts (spontaneous).

    As the reactants start reacting, however, theirconcentrations decrease (SO2twice as fast as O2) an

    G turns into G and becomes less negative.

    When G = 0 the reaction has reached equilibrium.Although for this rxn, SO2is probably the limiting

    reagent (not enough present to complete the rxn).

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    mo32Just as with enthalpies and entropies, one cancalculate free energies of reaction.

    (# eqiv)

    G(reactants)f

    = eq v

    (products)

    rxn

    EXAMPLE:

    g s +CO (g)

    g s +C(s)

    G = 0kJ/mol

    -kJ/mol

    - mokJ/mol

    TS S

    (# mol) G(reactants)

    f

    = mo (products)rxn

    = mo - mo + mo m (2 mol)(0 kJ/mol) + (1 mol)(

    kJ/mol)

    rxn

    G = (-1140kJ)

    -rxn = - +

    394 kJrxn

    } rxn!highly exothermicrxn !!

    =kJrxn

    ompare o w c was - orthe same rxn.

    rxn

    e mssng o energy wen oENTROPY!

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    mo33Example: To make iron, a steel mill takes Fe2O3 (rust

    or iron ore) and reacts it with coke (a complex, impure

    form of carbon) to make iron and CO2. Based on the

    data below, this is a non-spontaneous reaction at roomtemperature, but it becomes spontaneous at higher

    temperatures. Assuming that H and S do not

    change much with temperature, calculate the temp-

    erature above which the reaction becomes spontaneous

    (i.e., Grxn = 0).

    Hrxn= +465 kJ/mol

    Srxn= +552 J/molK (or0.552 kJ/molK

    Grxn= +301 kJ/mol (at 298 K)

    Grxn = Hrxn TSrxn

    as we raise the temperature, G will eventuallyreach 0 andthen go negative & spontaneous, so let G = 0solve forT, the temperature at which this will happen:0 = Hrxn TSrxn

    rearrang ng o so ve orgives:

    /T = (Hrxn) (Srxn)

    T = (465 kJ/mol) / (0.552 kJ/molK)

    T = 842 K

    (above this temperature Grxn will be negat ivewill have

    a spontaneous reaction)

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    mo34Problem: Calculate Grxn for the following.

    Gf (SO2, g) = 300kJ/mol

    Gf (SO3, g) = 371kJ/mol

    Gf (H2SO4, l) = 690 kJ/mol Gf (H2SO4, aq) 742 kJ/molGf (H2O, l) = 237kJ/mol

    Gf (H2S, g) = 34kJ/mol

    a) S(s) + O2(g) SO2(g)

    b) 2SO2(g) + O2(g)

    c) SO3(g) + H2O(l)

    d) 2H2S(g) + 3O2(g)

    2SO3(g)

    H2SO4(l)

    2SO2(g) + 2H2O(l)

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    mo35Comparisons of Hrxn and Grxn

    S(s) + O2(g) SO2(g)

    Hrxn = 297 kJ/molSrxn = 11 J/mol K

    Grxn = 300 kJ/mol

    2SO2(g) + O2(g) 2SO3(g)

    Hrxn = 198 kJ/mol

    Grxn = 142 kJ/mol

    SO3(g) + H2O(l) H2SO4(l)

    Hrxn = 132 kJ/mol

    Grxn = 82 kJ/mol

    2H2S(g) + 3O2(g) 2SO2(g) + 2H2O(l)

    Hrxn = 1126 kJ/mol

    Grxn = 1006 kJ/mol

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    mo36Entropy of Fusion and Vaporization

    While the entropy of a substance increases steadily

    with increasing temperature, there is a considerable

    ump in the entropy at a phase transition:

    250

    o as

    150

    100

    50

    d

    phasetransi t ions

    Temperature(K)This jump at the melting point is called the entropy

    of fusion, Sfusion, and as you might expect, it is

    related to the enthalpy (or heat) of fusion, Hfusion:

    HfusionSfusion

    Tm

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    Problem: Calculate the boiling point for ethanol

    (CH3CH2OH) from the data in the thermodynamic

    tables.

    (literature value = 78.5C)

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    mo39

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    mo40

    , , ,Davis, Peck & Stanley. Thomson Brooks/ColePublisher.