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Ch2.phase equlibrium
1. Bule Hora University
College of Health and Medical Sciences
Department Of Pharmacy
INTEGRATED PHYSICAL PHARMACY AND PHARMACEUTICS I
CHAPTER 2
PHASE EQUILIBRIUM
By: Aliyi Gerina [BSc, B.pharm]
4/5/2022
1
Phase Equilibrium By Aliyi Gerina
Bule Hora University
2. Out Line
Introduction to intermolecular force
The phase rule
Phase equilibrium of
single,
two and
three component systems (principles and
applications)
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
3. Introduction to intermolecular
force
There are three states of matters such as gas, liquid,
and solid.
The pharmacist will encounter three of these
» through dispensing them
» consulting on these pharmaceutical preparations.
Examples of the three states of matter would include
– gas in metered dose inhalers,
– liquids in syrups and
– solid dosage forms of tablets and capsules.
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
4. Introduction to intermolecular forces…
What makes some substances be gas, some liquid, some
solid?
The reason is differences in attractive forces between
particles;
» particles of water have greater affinity for one another
than particles of O2 have for each other.
There are two types of forces in matters:
• Intramolecular forces
• Intermolecular forces
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
5. Introduction to intermolecular forces…
The Intermolecular Forces (forces between molecules)
are weaker than Intramolecular Forces.
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
7. Introduction to intermolecular forces…
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
7
Intramolecular forces
Definition
An intramolecular force (or primary forces)
is any force that binds atoms together making up a
molecule or compound,
Not to be confused with intermolecular forces, which are
the forces present between molecules.
8. Introduction to intermolecular forces…
Ionic bonds
Ionic compounds contain oppositely charged particles
held together by extremely strong electrostatic
interactions.
These are the strongest intramolecular forces.
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
9. Introduction to intermolecular forces…
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
9
Covalent bond
Formed between the non metallic elements of the
periodic table.
It is formed by electron sharing.
H·+·H → H:H or H━H
10. Introduction to intermolecular forces…
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
10
Intermolecular Forces
Definition
Intermolecular forces are forces of attraction and
repulsion that exist between molecules or ions.
These forces help hold the ions and molecules of a
substance together.
11. Introduction to intermolecular forces…
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
11
Overview of Intermolecular Forces
We know that atoms in a molecule are held together by
chemical bonds. But what holds these molecules together?
The forces that hold one molecule to another in a substance
are called intermolecular forces.
Intermolecular forces are
highest among the molecules of solids and
least among the molecules of gases.
Attractive intermolecular forces were first classified by
Johannes Diderik van der Waals and are known as Van der
Waals forces. Does the same force exist between every
particle?
12. Introduction to intermolecular forces…
The forces that exist between two molecules or ions
depend upon the type of molecules or ions that interact:
Ion-Dipole Forces(IDF)
Dipole-Dipole Forces(DDF)
Ion-Induce Dipoles Forces(IIDF)
Dipole-Induced Dipole Forces(DIDF)
London Dispersion Forces (Induced Dipole -
Induced Dipole )(LDF)
Hydrogen Bonding(HB)
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
13. Introduction to intermolecular forces…
Ion-dipole forces
Exists between an ion and a dipole molecule.
A positive ion will be attracted to the negative pole of the
polar molecule, while
a negative ion will be attracted to the positive pole of the
polar molecule.
Example: NaCl dissolves in water
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
14. Introduction to intermolecular forces…
Dipole-dipole Forces
Results from all polar molecules (an unequal
distribution of electrons around these polar
molecules results in a “dipole’, positive and
negative sides that attract similar molecules).
HCl is a polar molecule with the partial
positive charge on the H and the partial
negative charge on the Cl.
A network of partial + and - charges attract
molecules to each other.
• Example: CH3CL, SO2 and H2S
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
15. Introduction to intermolecular forces…
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
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Ion-induced dipole Force
Interactiton between an ion and a non-polar molecule.
The charge of the ion causes distortion of the electron cloud on
the non-polar molecule.
So we have an non-polar molecule in iteracttion with an ion &
this ion produces a induced dipole from a non-polar molecule.
Fe2+ ion in the interaction with a non-polar molecule O2.
16. Introduction to intermolecular forces…
Dipole-Induced Dipole Forces
A non-polar molecule turns into a
induced dipole when it interacts with a
polar molecule.
E.g Interaction between the non-
polar molecule O2 and the
polar H2O molecule.
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
17. Introduction to intermolecular forces…
London Dispersion forces (Induced Dipole
-Induced Dipole )
Weakest of the intermolecular forces
The only intermolecular force of attraction between
non polar molecules.
The attractive force between positive and negative
charges that results from temporary dipoles.
In the Ne atom the induced dipole in one atom influences
the electron distribution in other atom and atoms attract.
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
18. Introduction to intermolecular forces…
Even though CH4 has no net dipole,
at any one instant its electron
density may not be completely
symmetrical,
resulting in a temporary dipole.
This can induce a temporary dipole in
another molecule.
The weak interaction of these
temporary dipoles constitutes
van der Waals forces.
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
19. Introduction to intermolecular forces…
Hydrogen Bond
Hydrogen bonding typically occurs
when a H atom bonded to F, O, or N
atom,
is electrostatically attracted to a lone
pair of electrons on an O, N, or F
atom in another molecule.
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
Interactions b/n H2O molecules.
The hydrogen bond if formed
between O2 [red] and H [white].
22. Physical Properties
affected by intermolecular forces
Boiling point(BP)
The BP of a compound is the temperature at which liquid
molecules are converted into gas.
In boiling, energy is needed to overcome the attractive forces
in the more ordered liquid state.
The stronger the intermolecular forces, the higher the BP.
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
23. Physical Properties,…
Melting point (MP)
The MP is the temperature at which a solid is converted to its liquid
phase
In melting, energy is needed to overcome the attractive forces in
the more ordered crystalline solid
The stronger the intermolecular forces, the higher the MP
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
24. The stronger the intermolecular forces between the
molecules of a substance , the higher the melting point
and boiling point of a substance.
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
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25. Physical Properties,…
Solubility
Like dissolves like
– Polar solutes dissolve in polar solvents
– Nonpolar solutes dissolve in nonpolar solvents
Molecules with similar intermolecular forces will mix freely.
In dissolving a compound, the energy needed to break up the
interactions between the molecules or ions of the solute .
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
26. Phase rule and Phase diagram
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
27. Out line
Phase Rule
Phase equilibrium of
Single component systems
Two component systems and
Three component systems
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
28. Phase Rule
It was first presented by Gibbs in 1875.
It is very useful to understand the effect of intensive
variables,
such as temperature, pressure, or concentration,
on the equilibrium between phases as well as between chemical
constituents.
It is used to deduce the number of degrees of freedom
(f) for a system. Sometimes called: “the variance of the
system”.
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
29. Phase Rule,…
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Bule Hora University
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It states that :
When the equilibrium between any number of phases is
influenced only by temperature, pressure and concentration
but
not influenced by gravity, or electrical or magnetic forces or
by surface action then
the number of Degrees of Freedom (F) of the system is
related to the number of Components (C) and Phases (P)
by the phase rule equation:
F = C - P + 2
30. Phase Rule,…
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Bule Hora University
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phase
defined as: any homogeneous part of a system
having all physical and chemical properties the
same throughout.
In another word , a uniform part of a system in
equilibrium is termed a ‘ phase’.
Represented by P in the phase Rule equation.
31. Phase Rule,…
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Bule Hora University
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A system may consist of one phase or more than one
phases.
A system containing only liquid water is one-phase or (P = 1)
A system containing liquid water and water vapor (a gas) is a
two-phase or (P = 2)
A system containing liquid water, water vapor and solid ice is
a three-phase or(P = 3)
32. Phase Rule,…
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Bule Hora University
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A system consisting of one phase only is called a
homogeneous system.
Water, ice, water vapor, sugar dissolved in water, gases in
general, etc.
A system consisting of two or more phases is called a
heterogeneous system
A cube of ice in water. (same chemical compositions but
different physical states)
Ice ↔ water ↔ vapour: Phases in equilibrium
34. Phase Rule,…
Substances comments
Phases
(P)
Oxygen gas (O2) Homogeneous gas 1
Liquid benzene (C6H6) Homogeneous liquid 1
Mixture of water and
alcohol
Miscible liquids 1
Mixture of water and oil
Immiscible,
heterogeneous
2
Solution of Nacl in water Solution, homogeneous 1
Mixture of ice-water- Equilibrium,
3
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
35. Phase Rule,…
Components(C)
The term component is defined as the least number of
independent chemical constituents
in terms of which the composition of every phase can be
expressed by means of a chemical equation. .
A system ‘C’ in the Phase Rule equation stands for the number of
components of a system in equilibrium.
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
36. Phase Rule,…
System component
Number of
component
s
Phase
Ice-water Water (H2O) 1 2
Ice-vapour Water (H2O) 1 2
Mixture of oxygen
and nitrogen
O2 and N2 2 1
Sodium chloride
solution
Nacl and
water
2 1
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
37. Phase Rule,…
Degrees of freedom (F):
defined as the least number of variable factors (concentration,
pressure and temperature) which must be specified
so that the remaining variables are fixed automatically and the
system is completely defined.
Represented by F in the phase Rule equation (F = C – P + 2)
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
38. Phase Rule,…
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Bule Hora University
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A system with F = 0 is known as non variant or having
=>no degree of freedom.
A system with F = 1 is known as univariant or having
=> one degree of freedom.
A system with F = 2 is known as bivariant or having
=> two degrees of freedom.
i.e F = 0 => Neither temperature nor pressure can be varied
independently.
F = 1 => Only one out of temperature and pressure can be
varied independently
F = 2 => Both temperature and pressure can be varied
39. Phase Rule,…
Substance/system Degree of freedom Intensive properties
Pure gas
F=1-1+2=2
(bivariant)
Pressure &
temperature
Mixture of two gases
F=2-1+2=3
(Trivariant)
Press, temp &
concentration
Water & water vapor in
equilibrium
F=1-2+2=1
(univariant)
Vapor press or
temperature
Saturated NaCl solution
with undissolved solid &
vapor
F=2-3+2=1
(univariant)
Temperature
Ice-water-water vapour
F=1-3+2=0
(Invariant)
No need of mention
any properties. Which
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
40. Phase Rule,…
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Bule Hora University
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phase diagram
is a plot showing the conditions of pressure and
temperature under which two or more physical states can
exist together in a state of dynamic equilibrium
They are one of the most important sources of information
concerning the behavior of elements, compounds and
solutions as a function of T, P & C.
They also show the preferred physical states of matter at
different T and P .
41. Phase Rule,…
Depending on number of components
One component system
Two component system
Three component system
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
43. One Component System
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Bule Hora University
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For a one-component system the phase rule equation as:
F = C – P + 2 =
=1 – P + 2
=3 – P
Three cases may arise:
Case 1.
When only one phase is present
F = 3 – 1
= 2
Thus the system is bivariant.
It can be completely defined by specifying
the two variables T and P. Or both the T and P can be varied independently.
44. One Component System,…
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Bule Hora University
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Case 2.
When two phases are in equilibrium,
F = 3 – 2
= 1
The system then has one degree of freedom and
is termed uni-variant or mono variant.
This means that the pressure cannot be changed independently
if we change the temperature.
The pressure is fixed automatically
for a given temperature.
45. One Component System,…
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Bule Hora University
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Case 3.
When three phases are in equilibrium,
F = 3 – P = 3 – 3 = 0 ,
F = 0
The system has zero degree of freedom and
is termed non variant or invariant.
This special condition can be attained at a definite T and P.
At this point the three phases (solid, liquid, vapor)
are in equilibrium and,
therefore, it is called Triple point.
46. One Component System,…
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Triple Point
The triple point of a substance is the T and P at which the three
phases (gas, liquid and solid) of that substance coexist in
thermodynamic equilibrium.
For example,
Triple point of water is 273.16 K at 611.2Pa (0.00980C at 4.58
mm of Hg).
47. One Component System,…
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Bule Hora University
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A triple point shows the conditions under which all three
phases
can coexist in equilibrium.
Thus, the system at the triple point may be represented as:
Solid ⇌ Liquid ⇌Vapor
Applying the phase rule equation we have
F = C – P + 2
= 1 – 3 + 2
= 0
This predicts that the system has no degree of freedom at its
triple point.
48. The Water System
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‘Water’ is a three-phase, one-component system.
The total number of phases which can exist in
equilibrium any time
depends on the conditions of temperature and pressure.
49. Phase Diagram of water
system
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50. Phase Diagram of water,…
The phase diagram or P-T graph of
the system/ water/ice/vapour is
shown in the Figure.
The salient features of the phase
diagram are listed below.
(1) The Curves OA, OB, OC
(2) The Triple Point O
(3) The Areas AOC, AOB, BOC
Let us proceed to discuss the
significance of each of these
features.
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51. Phase Diagram of water,…
1. The Curves OA, OB, OC
These three curves meet at the point O and
divided the diagram in to three region or area.
Curve OA, the Vapor Pressure curve
It represents the vapour pressure of liquid
water at different temperatures.
The two phases water and water vapour
coexist in equilibrium along this curve.
Liquid ⇌Vapor
The curve OA terminates at A’,
the critical point (218 atm, temp. 374ºC) at
this point the liquid and vapour
are indistinguishable from each other. 4/5/2022
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
52. Phase Diagram of water,…
Curve OB, the Sublimation curve.
It shows the vapour pressure of
solid ice at different temperatures.
The two phases solid ice and
vapour coexist in equilibrium along
this curve.
Solid ⇌ Vapor
The curve terminates at the point B,
where no vapour exists.
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
53. Phase Diagram of water,…
Curve OC, the Fusion curve.
It depicts the effect of pressure on
the melting point of ice.
Here ice and water coexist in
equilibrium.
Solid ⇌ Liquid
The OC slopes to the left
indicates
the melting point of ice
decreases with increase of
Pressure.
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
54. Phase Diagram of water,…
Along the curves OA, OB, OC
there are two phases in equilibrium and
one component.
Therefore,
F = C – P + 2 = 1 – 2 + 2
= 1
Hence each two-phase system :
Liquid ⇌ Vapor represented by OA
Solid ⇌ Vapor represented by OB
Solid ⇌ Liquid represented by OC
has one degree of freedom
i.e., is mono variant.
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
F=1
55. Phase Diagram of water,…
2.The Triple point ‘O’
The curves OA, OB and OC meet at the
triple point ‘O’ where
all the three phases liquid water/
ice/vapour are in equilibrium.
Solid ⇌ Liquid ⇌Vapor
This occurs at 0.00980ºC and vapour
pressure 4.58 mmHg.
Since there are three phases and one
component, we have
F = C– P + 2 = 1 – 3 + 2 = 0
i.e., the system is non variant.
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
F=0
56. Phase Diagram of water,…
3. Area AOC, AOB, BOC
Within the areas a single is capable of
stable existence. Thus,
Area AOC represents conditions for the
one-phase system water.
Area AOB represents conditions for the
one-phase system water vapour.
Area BOC represents conditions for the
one-phase system ice.
In all the three areas there being one-
phase and one component, we have
F = C – P + 2 = 1 – 1 + 2 = 2
Thus the system is bi-variant. 4/5/2022
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
F=2
57. Why ice skating is possible??
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
58. Summary for one component system
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
60. Cont’d,…
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Bule Hora University
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When a single phase is present in a two component
system,the degree of freedom is three,
F = 2 – 1 + 2 = 3
This means that three variables must be specified in
order to describe the condition of the phase.
Thus in such a system, in addition to P and T.
the concentration of one of the components
has also to be given.
61. Cont’d,…
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For graphic representation of these variables,
three coordinate axes at right angles to each other
would be required.
Therefore the phase diagram obtained would be a
solid model.
For the sake of having simple plane diagrams we
generally consider only two variables,
the third one being a constant.
62. Cont’d,…
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For example, for a solid-liquid equilibrium, the gas phase
is usually absent and
the effect of pressure on the equilibrium is very small.
Thus, when a two-component system consists of solid and
liquid phases only,
the effect of pressure may be disregarded.
Then it is necessary to take into account the remaining
variables , temperature and concentration.
Such a solid/liquid system with the gas phase absent is
Called Condensed System.
63. Cont’d,…
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Since the degree of freedom in such a case is reduced by one,
we may write the Reduced Phase rule as
F' = C – P + 1
Where, F' gives the remaining degrees of freedom of the
system.
The reduced phase rule is more convenient to apply to
solid/liquid two-component condensed system.
64. Cont’d,…
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Since the only variables for two-component solid/liquid
systems are temperature and composition,
the phase diagrams for such systems consist of Temperature-
Concentration graphs(TC graphs).
65. Two-Component Systems Containing
Solid and Liquid Phases:
Eutectic Mixtures
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Component which completely miscible but do not
react.
The general form of the phase diagram of such a 2-
component condensed system is shown in Figure.
Here the two components A and B are completely
miscible in the liquid state, and
these solutions on cooling yield only pure A or pure B as
solid phases.
66. Phase diagram of Eutectic Mixtures
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67. phase diagram,…
Curve AC; the Freezing
point curve of A.
The point A represents the
freezing point of A.
The curve AC shows that the
freezing point of A falls by
the addition of B to A.
Thus along this curve, the
solid A is in equilibrium with
the liquid solution of B in A.
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Phase Equilibrium By Aliyi Gerina
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68. phase diagram,…
Curve BC; the Freezing
point curve of B.
The point B shows the freezing
point of B.
The curve BC exhibits the fall
of freezing point by the
addition of A to B.
Along this curve, the solid B is
in equilibrium with the liquid
solution of A in B.
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69. phase diagram,…
Applying the reduced phase
rule equation to the
equilibrium represented by the
curve AC & CB
i.e., solid A/solution and solid
B/solution respectively,
we have
F’ = C – P + 1 = 2 – 2 + 1 = 1
The degree of freedom is one
i.e., both equilibrium are mono
variant.
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70. phase diagram,…
The Eutectic point C.
The two curves AC and BC meet at the
point C.
Here both the solids A and B must be in
equilibrium with the solution phase
(solution of A and B).
The number of phases is 3.
By applying the reduced phase rule
equation , we have
F' = C – P + 1 = 2 – 3 + 1 = 0
Thus, the system represented by the point
C is non variant.
In other words, both temperature and
composition of the system solid A-solid B-
solution are fixed.
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71. phase diagram,…
The mixture of components A and B
as at point C,
melts at the lowest temperature TE
indicated on the graph.
The point C is therefore, called the Eutectic
point (Greek eutectos = easy melting).
The corresponding composition (CE) and
temperature (TE) are known as the eutectic
composition and the eutectic temperature
respectively of the system.
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72. phase diagram,…
The Area above the curves AC
and BC.
Here the two components A and B are
present as liquid solutions of varying
compositions.
As a homogeneous solution of A and B
constitutes one phase only, this system
is bivariant.
F’ = C – P + 1 = 2 – 1 + 1 = 2
Therefore, to define the system at any
point in this area, both temperature
and composition have to be specified.
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73. phase diagram,…
Effect of Cooling
When the A/B solution at any point in the
area above ACB is cooled,
the cooling dashed line meets the curve AC,
say at Y.
Here solid A separates and the equilibrium
shifts down along the curve AC.
The change of composition and T
continues till the eutectic point C is
reached when solid B also separates.
Thus in the area below AC and above TE line,
there exist two phases, solid A and solution A/B, and
the system is bivariant.
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74. phase diagram,…
Similarly, cooling of solution B/A on the other
side of eutectic, on reaching the curve BC would
yield solid B/solution system.
Thus, the area below BC up to TE line would
represent solid B and solution.
the system is bivariant.
If the solution just below the eutectic point is
cooled,
a solid mixture (eutectic mixture) of eutectic
composition CE.
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Phase Equilibrium By Aliyi Gerina
Bule Hora University
75. Two component system containing liquid
phases
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There are liquids:
Showing complete miscibility e.g. water & ethyl alcohol
Showing complete immiscibility e.g. water & mercury
Showing partial miscibility e.g. water & phenol
76. Two component system containing liquid
phases…
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The components of an ideal solution are miscible in all proportions.
e.g. ethanol and water, under normal conditions.
Attractions between the molecules of one component are greater
than those between its molecules and those of the other component,
i.e. if a positive deviation from Raoult's law occurs, the miscibility of the
components may be reduced.
The greater the strength of the self-association the greater the
immiscibility,the greater the degree of +ve deviation from Raoult's
law.
e.g. large +ve deviat.: water and Hg binary system.
77. Two component system containing liquid
phases…
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77
In cases of partial miscibility
Degree of miscibility may be dependent on Temperature.
1. Solubility with in temperature (water-phenol)
2. Solubility with in temperature
(water-triethylamine)
3. Solubility with & in temperature (water-nicotine)
4. Solubility not affected by temperature
In case of three component system
the third liquid may influence the degree of solubility of the 2
liquid systems.
78. Two component system containing liquid
phases…
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Effect of temperature variation on the degree of miscibility
in these systems is described by means of phase diagrams.
Phase diagrams
= graphs of temperature versus composition at constant P.
79. 1. Systems showing an increase in
miscibility with rise in temperature
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A +ve deviation from Raoult's law due to difference in
the cohesive forces that exist between the molecules
of each component in a liquid mixture.
T => +ve deviation => miscibility
Each phase consists of a saturated solution of one
component in the other liquid.
Such saturated solutions are known as conjugate solutions
80. Phenol and water system phase diagram.
Two factors affecting
miscibility of phenol &
water.
1- Concentration of
phenol in water
2- Temperature
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81. Phenol and water system phase diagram…
Increasing quantities of phenol from b
to c ,
we form systems in w/c
the amount of the phenol-rich phase (B)
continually increases.
At the same time the amount of the
water-rich phase (A) decreases.
Once the total conc. of phenol exceeds
63 % at 50 0 C
a single phenol-rich liquid phase is
formed.
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82. Phenol and water system phase diagram…
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Point a 100% water (pure water)
Phenol
Point b (11 % phenol): 2 phases,
water rich phase& phenol rich phase
More Phenol
Point c ( >63% phenol): 1 phase,
Completely miscible
83. Phenol and water system phase diagram…
The critical solution temperature
(upper consolute temperature):
Is the maximum T at which
the two phase region exists.
In the case of the phenol-water
system this is 66.8° (point h).
All combinations of phenol and
water above this temperature
are completely miscible and
yield one-phase liquid systems.
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84. Phenol and water system phase diagram…
Line bc drawn across the region
containing two phases is termed as tie
line.
It is always parallel to the base line.
All system prepared on a tie line at
equilibrium will separate into phase of
constant composition.
» These phase are called conjugate phases
Phenol rich (63% phenol) (c)&
water rich (11% phenol)(b) layers
(phases) at 50 0C.
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85. PHASE COMPOSITION AND LEVER RULE
Lever rule: the fractional amounts of two phases are
inversely proportional to their distances along the tie
line from the bulk composition axis.
Tie line can be used to determine the weight and
composition of the phases.
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86. Cont’d,…
• The lengths of dc and bd can be measured with a ruler
in centimeters or inches from the phase diagram.
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87. Cont’d,…
Example 1
– point d = 24% b = 11%, c = 63%,
𝑑𝑐
𝑏𝑑
=
63−24
24−11
=
39
13
=
3
1
For every 10 g of a liquid
system in equilibrium at
point d
Phase A = 7.5 g &
Phase B = 2.5 g
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88. Cont’d,…
At point f =50%
𝑓𝑐
𝑏𝑓
=
63−50
50−11
=
13
39
=
1
3
– For every 10 g of system f
Phase A = 2.5 g &
phase B 7.5
At Point e = 37 %
𝑒𝑐
𝑏𝑒
=
63−37
37−11
=
26
26
=1
Equal weight of phase A & phase
B .
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89. 2. Systems showing a decrease in miscibility
with rise in T.
Systems showing a decrease in miscibility
with rise in T.
E.g : triethylamine-water
Below TCST the two liquids are miscible
because
they can form weak complexes
(internal forces).
Above T CST increases, these weak
complexes break up and
immiscible systems is being formed.
Cooling mixture during ppn allows more
solution.
Such systems should be store in cool place
is recommended
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90. 3. Systems showing upper and lower critical
solution T.
Other systems show both an upper
and lower consolute temperatures.
Such systems are known as closed
miscibility loops:
Example: nicotine-water system
After the weak complexes have been
disrupted, the two liquids are show
only partial miscibility at an
intermediate temperature region
The thermal motion at higher T
homogenizes the mixture again .
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91. 4. Systems with no critical solution T
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The pair, ethyl ether and water,
has neither an upper nor a lower consolute temperature
and
shows partial miscibility over the entire temperature
range at which the mixture exists.
93. Three-component system (Ternary system)
The addition of a third liquid to a binary liquid system
produce
a ternary or three-component system.
The mutual solubility of the original pair will be
decreased If the third liquid is
Soluble in only one of the two original liquids or
Its solubility in the two original liquids is markedly
different,
The addition of a liquid having roughly the same
solubility in both components of the original pair will
result in an increase in their mutual solubility
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94. Three-component system (one phase)
In non condensed system
In systems containing three component but only one phase
F = C – P + 2
F = 3 - 1+ 2 = 4
F = 4 (P,T, Conc. of two of the three components).
In condensed system and constant temp
If we regard the system as condensed system(p constant) and hold
the T constant
F = C – P + 0
F = 3 – 1 + 0
F = 2 (conc. of 2 component)
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95. Rules of triangular diagrams
Planar diagram to illustrate the phase equilibrium
An equilateral-triangle graph may be used to represent ternary
system.
Each side of the triangle represent 0% of one of the
components and
the apex opposite that side represent 100% of that component
A point on one of the sides of the triangle will give the composition of a
mixture in which only two components are present, While
a point within the triangle will represent the composition of a ternary
mixture.
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96. Rules of triangular diagrams,…
The area within the triangle
represents all the possible
combinations of A, B, and C
to give three component
systems.
The location of a particular
three component system
within the triangle,
e.g. point x may be undertaken
as follows:
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X
97. Rules of triangular diagrams,…
The line AC, opposite apex B ,
represents systems, containing
A and C. B is absent, i.e., B.= 0
.
The horizontal lines running
across the triangle parallel to
AC indicate increasing % of B
from B = 0 (on line AC) to B =
100 (at point B).
The line parallel to AC which
cuts point x is equivalent to 15
% B; consequently, the system
contains 15 percent of B and 85
percent of A and C together.
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98. Rules of triangular diagrams,…
Applying similar arguments to the other
two components in the system,
we can say that along the line AB, C=0.
As we proceed from the line AB towards
C across the diagram, the concentration of
C increases until at the apex, C = 100
percent.
The point x lies on the line parallel to AB,
that is equivalent to 30 percent of C.
Therefore the concentration of A is
100 - (B + C) = 100 - (15 + 30) = 55%
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99. Ternary Systems with One Pair of Partially
Miscible Liquids
A, B and C represent water,
alcohol, and benzene,
respectively.
The line AC represents binary
mixtures of A and C
The curve afdeic termed a
binodal curve
marks the extent of the two
phase region
The remainder of the triangle
contains 1 liquid phase
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100. Ternary Systems with One Pair of Partially Miscible
Liquids,…
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100
Ternary systems water, benzene and alcohol contains one pair
of partially miscible liquids.
Water and benzene are miscible only to a slight extent and
so a mixture of the 2 produces a 2 phase system,
water saturated with benzene and benzene saturated with water.
On the other hand, alcohol is completely miscible with both
benzene and water.
Thus, the addition of alcohol to a two phase system of benzene and
water would produce a single liquid phase
in which all 3 components are miscible.
101. Ternary Systems with One Pair of Partially Miscible
Liquids,…
Tie line fi
Systems g and h prepared along
the tie line fi both rise to two
phases having the compositions
denoted by the points f and i.
For example, system g, after
reaching equilibrium, will
separate into two phases, f and i.
The ratio of phases f to phase i,
on a weight basis, is given by the
ratio gi : fg.
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102. Ternary Systems with One Pair of Partially Miscible
Liquids,…
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102
Effect of Temperature
The area of binodal decrease as the temp. is
raised &
miscibility increase till it is completely miscible &
the binodal disappear.
103. Another Examples of tertiary component systems
Chloroform-water-acetic acid Oil-Alcohol-Water
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104. Applications of Three-component system
Application of three component system diagram
– Surfactant/oil/water system
– Flavor/water/alcohol system
– Drug/water/propylene glycol system
The pharmacist can pick any combination from
the region miscible depending on
safety, efficacy, stability or cost .
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