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    Chemistry 5

    Chapter-7

    Thermochemistry

    Part-2

    21 October 2002

    Great Job on Exam!

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    Three ways to increase energy of system?

    Work = force x distance

    Consider expansion of gas how much work is done?

    Demonstration- Observations?

    Heat & Work

    adding material to it

    heating it

    doing work on it -- for example, winding up a spring or pushinga weight.-- it takes energy to do work

    If pressure inside can exceeds external pressure, then

    lid flys off! How much work is done???

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    Pressure-Volume Work:

    Work ( w ) = force (F) x distance (h)

    ==

    w = - P ext x V

    significance of negative sign?

    significance of P ext ?

    Units

    WORK

    (remember: P = F/A)

    P x A x hP x V

    When gas expands ( V > 0), work is done on surroundings; thenegative sign signifies energy leaves (as work) the system.

    External pressure against which system expands or thatcompressing the system.

    The pressure-volume work (L-atm) can be expressedin more familiar energy units of joule (J) using idealgas constants: 101.33 J/L-atm

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    Internal Energy, U

    Changing the internal energy The internal energy of a system can bechanged by heating or doing work.

    cold water hot water

    Energy, Heat & Work

    Is the total kinetic + potential energy of the system

    Includes energy associated with molecular motions:

    A system only containsinternal energy; it does not contain energy in the form of heat or work.

    Ucold Uhot

    U = U hot U cold , change in internal energy

    = U final - U initial

    heat

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    Change in internal energy is the sum of theenergy transferred as heat and thattransferred as work.

    Heat and work are equivalent ways of changing the energy of a system.

    Changing the Internal Energy

    I N T E R N A L E N E R G Y

    , U

    initial state, U

    final state, U f

    heat, q

    work, w U = U

    f U

    i= q + w

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    First Law

    isolated system

    system not isolated

    Some conventions:

    energy entering system

    energy leaving system

    First Law of Thermodynamics

    The internal energy of an isolated system isconstant: U isolated sys = 0

    For a system that is not isolated: U = q + w

    Energy entering the system has positive sign:

    heat absorbed by system, q > 0work done on system, w > 0

    Energy leaving the system hasnegative sign:

    heat released by system, q < 0work done by system, w < 0

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    Changing Internal Energy

    U = q + w

    C 8H 18(l) + (25/2) O 2(g)

    8 CO 2(g) + 9H 2O(g) E lost asHEAT

    and WORK

    U initial

    U finalE lost as

    HEAT

    E N E R G Y

    Extract all the energy change as heatExtract energy as work and heat (a car)

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    Changing Internal Energy

    U = q + w

    E N E R G Y Initial State

    Final State

    We can have different combinations of q and w, toreach same final state.

    U depends only on initial and final states!

    q < 0w = 0

    q < 0w < 0

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    What is a state function

    Internal energy is a state function

    Path Dependent Functions

    heat & work

    Example consider expansion of ideal gas onevs. two steps.

    State Functions

    A state function is a property with a value that depends only on the current state of system and not how it was prepared.

    Key to thermochemistry is that the change in a state function is independent about how changeoccurred; that is, independent of pathway.

    It is difficult to obtain an absolute value of U ;however, it is generally the change in internal energy, U , that is most important.

    values depend on the path followed when a system undergoes change!

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    Constant Volume

    U = q + w

    Constant Pressure

    importance?

    Enthalpy Change, H

    Heats of Reaction Enthalpy

    = q P ext V = q 0= q V

    Many (most) chemical and biochemical reactionsare carried out under constant pressure (not constant volume); q V q P

    At constant pressure: U = q P + w = q P - P V

    q P =

    U + P

    V Since U, P & V are all state functions, q P is also one.We give this a special name enthalpy, H!

    H = U + P V

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    U = H P V; how important is work term?

    Enthalpy vs. Internal Energy Changes

    2CO(g) + O 2(g) 2CO 2(g)

    q P = -566 kJ = H

    Evaluate P-V work: P V = P(V f V i )=RT(n f n i )

    U = H P V, constant pressure= -564 kJ

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    Changes of State

    vaporization

    melting

    sublimation

    Standard States

    Endothermic & Exothermic Processes

    Enthalpy: Other Key Points

    Compound (l) Compound (g), H vap > 0

    Compound (s) Compound (l), DH melt > 0

    Compound (s) Compound (g), DH sub > 0

    Enthalpy changes are precisely defined with respect to state. We can define standard state enthaply, H o ,which corresponds to change for reactants and products in standard state.Temperature usually specified as 298.15 K.

    Endothermic heat goesinto system during reaction.

    Exothermic hear released by system during reaction.