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(1)

THE SPONTANEITY AND EQUILIBRIUM

MK. Kesetimbangan Kimia FMIPA UNS

Fitria Rahmawat

(2)

Fundamental concepts

• Kind of matters:

– Substances

– Mixture of substances Kind of Substances:

– elements: can not be broken into smaller substance by ordinary chemical method

– Compounds: can be broken into smaller substance by ordinary chemical method

– *ordinary chemical method: involving energy  1000

kJ/mol.

(3)

• Concept of atomic and molar mass

• The formulas

• The mole

• Chemical equations

– A shorthand method for describing chemical transformation

– Mn0 2 + 4HCl ---4 MnCl2 + 2H20 + Cl2

– The balance of chemical equation is an expression of law of conservation of the mass

– stoichiometri

(4)
(5)

Kinds of energy

(6)

The fundamental equation of thermodynamics

• The mechanical properties: p and V

• The three fundamental properties: U, S and T

• The three composite properties: H, G and A

• For present discussion: the expansion work,

The composite functions:

(7)

The Helmholtz free energy is a thermodynamic potential that measures the useful" work obtainable from a closed

thermodynamic system at a constant temperature and volume.

The negative of the difference in the Helmholtz energy is equal to maximum amount of work that the system can perform in a thermodynamic

process in which volume is held constant. 

Hermann Ludwig Ferdinand von Helmholtz August 31, 1821

(8)

Differentaton:

(9)

The propertes of A

(10)

The propertes of G

(11)
(12)

• The objects of Thermodynamics is to seek out logically the

relation between kinds of energy and their diverse manifestation.

• The laws of thermodynamics govern the transformation of

one kind of energy into another.

(13)

• THE FIRST LAW OF THERMODYNAMICS IS THE LAW OF ENERGY CONSERVATION

the total energy of an isolated system is constant; energy can be transformed from one form to another, but cannot be created or destroyed

(14)

• THE SECOND LAW OF THERMODYNAMICS: IS

CONCERN WITH THE DIRECTION OF NATURAL

PROCESS.

(15)

• THE ZEROTH LAW OF THERMPDYNAMICS: SYSTEMS IN

THERMAL EQUILIBRIUM WITH EACH OTHER HAVE THE

SAME TEMPERATURE

(16)

For ideal gas

(17)

Entropy and the third law of thermodynamics

The entropy of a perfect crystal, at absolute zero (zero kelvins ), is exactly equal to zero

(18)
(19)

THE SPONTANEITY AND EQUILIBRIUM

• Aim is to find out what characteristics distinguished the irreversible (real)

transformation to reversible (ideal) transformations.

• What relation between entropy changes with

the heat flow that accompany it

(20)

It’s the Clasius Inequality

(21)
(22)
(23)

Transformaton at constant temperature (isothermal)

It is known that:

TdS = dU + dW

For isothermal change : TdS = d(TS)

(24)

the work produced in an is othermal transf ormation is less than or equal to the decrease in the Helmholtz energy

(25)

Transformation at constant temperature and under constant pressure

And , TdS = d(TS)

or

(26)

Therefore under constant temperature and constant pressure:

(27)

G is called the free energy of the System.

At equilibrium:

the decrease in Gibbs energy associated with a change in state at constant T and p is equal to the maximum work

Wa, rev which is obtainable in the transf ormation

(28)

Spontaneous changes can continue to occur in such a system as long as the Gibbs energy of the system can decrease, that is, until the Gibbs energy o f the system reaches a minimum value, which is dG = 0

the algebraic sign tells us whether

a transf ormation can occur in the direction in which we imagine it.

There are three possibilities :

(29)
(30)

The word "spontaneous" applied to changes in state in a thermo dynamic sense must not be given too bro ad a meaning

.

It means only that the change in state is possible

What can be done about those transf ormations that have G po sitive and are thermo dynamically impossible, or

nonspontaneous ?

Human nature being what it is, it does not submit lightly to the jud gment that a certain change is "impossible ." The

"impossible “ flow of water uphill can be made "p ossible,"

(31)

Driving forces for natural changes

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