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Physical Chemistry EPM/01 1
Order of lectures is, perhaps, not the most logical one, but it is partially
dictated by my desire to synchronize the lectures and tutorials.
A quote of the day (good for all the semester):
The camel’s hump is an ugly lump
Which you well may see in the Zoo.
But uglier yet is the lump you get
From having too little to do.
Rudyard Kipling
Hereby, I swear to do my best to get you out of this predicament.
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Physical Chemistry EPM/01 2
�Subject:
Physical and chemical transformations of the matter (of
any kind) and the accompanying flows of energy.
�Method:Mathematical, i.e., based on assuming or creating some
theoretical models based or tested on empirical
observations. This method leads to formulation of
hypotheses, theories and laws of nature related to their
specific subjects.
What is physical chemistry?
We are not interested here in any specific type of matter or substance (like in
inorganic chemsitry, organic chemistry, biochemistry, peptide chemistry, etc.
Physical chemsitry is the theory of chemsitry. Apparently, such subjects may exist
as inorganic physical chemistry, organic physical chemistry, etc., though major
statements in, say chemical kinetics apply to both organic and inorganic substances.
The very name „physical chemistry is ascribed sometimes to Lomonosov,
sometimes to Berzelius, who suggested that rigors and methods as strict as in
physics (the best developed natural science of their times) should be applied to
chemistry as well.
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Physical Chemistry EPM/01 3
Major sub-topics:• Photochemistry,
• Sonochemistry,
• Electrochemistry,
• Thermochemistry,
• Chemical kinetics,
• Chemical thermodynamics (equilibria),
• Surface chemistry,
• Spectroscopy,
• Solid state chemistry,
• Quantum chemistry,
• Chemical Physics.
What is physical chemistry?
(2)
The first four are related to interactions of energy in its different forms with the
matter.
The red marked ones are those, which will be covered, at least partially) in our
course.
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Physical Chemistry EPM/01 4
�Matter is everything possessing a feature known as inertia, due to its
mass (Newton).Chemical substance is a pure, isolated form of matter.The amount of matter is measured in moles.
�Energy is ability of a system (see later) to perform work (simplified).
(forms of energy, preservation of energy, energy conversion, energy carriers)
Basic concepts (1)
Mass-energy equivalence
E=mc2
In practice, relativistic (and quantum) effects are observed only in macro- or microscale and in the average observable scale are negligible.
Units, SI system
Forms of energy (work): mechanical, thermal, chemical, electric, nuclear, radiant
(electromagnetic), surface.
Energy carriers: mass (mechanical, heat), chemical bonds,electromagnetic field.
Rules of preservation of mass, energy (and related, for example, of momentum).
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Physical Chemistry EPM/01 5
Basic concepts (2)
Potential energy – depending on position of an object
in gravitation field in electric field
(of the Earth)
Ep=mgh Ep=q1q2/(4πε0r)
Kinetic energy – energy of movement:
Ek=½mv2
(translation, rotation, oscillation)
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Physical Chemistry EPM/01 6
�Law of nature is a clearly defined piece of theory, usually
addressing a single phenomenon, i.e., a relation between different
observables involved in this phenomenon.
�Verbal formulation:Boyle’s Law:
At constant temperature, volume of a gas changes inversely
proportionally to its pressure.
�Mathematical Formula:
Basic concepts (3)
const.const.at VPPVPV ;P
P
V
V T 2211
1
2
2
1 =====
Understanding physical chemistry is a process very similar to translation: symbolic
mathematics to human language and vice versa.
(Third way of expressing laws of nature is graphical – plots, one should practice this
way, known from math and physics classes).
Different types of physical laws:
Exact (always true), like Faraday law.
Limiting, when certain quantity determining the correctness of the law must
approach certain limit (usually zero or infinity). This type is very popular in
physical chemistry, e.g. gas laws, limited Debye-Huckel equation.
Empirical - approximate.
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Physical Chemistry EPM/01 7
System (definition)
System is a part of universe subject to
observation or being an object of theoretical
considerations, separated from the rest of
universe (surroundings) physically or just in our
imagination.
system + surroundings = universe
Introduction to
thermodynamics
We will cover here principally phenomenological (descriptive) thermodynamics,
and much less the statistical thermodynamics (deriving macroscale conclusions on
the basis of stastistical distributions describing behaviour of molecules in systems.
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Physical Chemistry EPM/01 8
The three types of systems:
� Open
�Closed
�Isolated
Introduction to
thermodynamics (2)
Classifications using other criteria are also possible (for example: homogenous and
nonhomogenous/heterogenous systems; single component and multicomponent
systems). Homogenous = single phase; heterogenous = multiphase.
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Physical Chemistry EPM/01 9
Ways of the energy transfer:
�work
�heat.
Types of work
Mechanical (change of volume, change of shape), change of the interface area,electrical.
Introduction to
thermodynamics (3)
When a system gains energy, its sign is „+”, while it loses energy, it is a „-”. Work
of expansion (the system works) is negative, work of compression is positive. This
is an arbitrary and conventional way adopted by the physical chemists. Point of
view of „the selfish system”.
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Physical Chemistry EPM/01 10
HEAT
Introduction to
thermodynamics (4)
If the flow of energy between the system and its surroundings depends on the
difference of temperatures, then one can say that energy is transferred as heat.
A system separated from its surrounding by the green barrier (diathermic) can
exchange heat with it.
A system separated from its surrounding by the red barrier (adiabatic) cannot
exchange heat with it, despite the difference in temperature.
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Physical Chemistry EPM/01 11
Endothermic process (systemlimited by a diathermic barrier)
Introduction to
thermodynamics (5)
before after
Exoenergetic and endoenergetic processes. Exothermic and endothermic processes.
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Physical Chemistry EPM/01 12
Endothermic process in an adiabatic system
Introduction to
thermodynamics (6)
before after
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Physical Chemistry EPM/01 13
Physical properties of systems:� Extensive (additive), depending on the size of thesystem (number of components, their type and amount of each)
(e.g. mass or volume of a system)
� Intensive are not additive.
(e.g. temperature, pressure, density, molar quantities, refraction index)
Introduction to
thermodynamics (7)
∑= ii Xnx
Intensive properties remain constant within a single „phase”, they chage stepwise at
the interface (phase border).
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Physical Chemistry EPM/01 14
State of a system:The following quantities permit complete
characterization of the state of a given system
P, V, T
Equation of state:
f(P,V,T)=0
For a system containing perfect gas only: pV=nRT
Introduction to
thermodynamics (8)
A given system, hence, its size is known, that’s why there is no „n” in the general
form of the equation of state.
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Physical Chemistry EPM/01 15
Thermochemistry (1)
• Enthalpy is heat exchanged at constant
pressure.
state property
• ∆∆∆∆H < 0 - exothermic process
• ∆∆∆∆H > 0 - endothermic process
initfinHHH −=∆
initfinHHH ∆−∆=∆
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Physical Chemistry EPM/01 16
Thermochemistry (2)
A standard reaction enthalpy is the reaction
enthalpy when reactants in their standard
states are converted to products in their
standard states. Denoted as:
The standard state of a substance is its pure
form at pressure of 105 Pa.
0H∆
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Physical Chemistry EPM/01 17
Thermochemistry (3)
• The standard molar enthalpy of formation
of a compound is the standard reaction
enthalpy per mole of compound for the
synthesis of the compound from its
elements in their most stable forms at 105 Pa
and specified temperature. Denoted as:
00 H ;H formf ∆∆
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Physical Chemistry EPM/01 18
Thermochemistry (4)
• Standard enthalpies of formation of
elements are equal to ZERO (at 298K).
When several allotropic forms of an
element exist, the statement applies to the
most stable form of the element.
• Standard molar enthalpy of formation of a
compound is standard molar enthalpy of
this compound.
Standard molar enthalpies of formation at 298K may be found in tables.
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Physical Chemistry EPM/01 19
Thermochemistry (5)
ProductsReactants→
initfinrreactionHHHH ∆−∆=∆=∆
fin
0
Pri,f,i H =Hn ∆∆∑ init
0
Rei,f,i H =Hn ∆∆∑
0
Rei,f,i
0
Pri,f,i
0
r Hn-Hn=H ∑∑ ∆∆∆
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Physical Chemistry EPM/01 20
Thermochemistry (6)
• The standard molar enthalpy of combustion is
the change in enthalpy per mole of the substance
(fuel) when it is burned (reacts with oxygen)
completely under standard conditions. Denoted as
• conditions superimposed on products in complete
combustion:
H →→→→ H2O(l); C →→→→ CO2(g); N →→→→ N2(g)
00 H ;H combc ∆∆
Indication of state (gas, liquid, solid, solution) and form (allotropic, polymorphic) is
required.
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Physical Chemistry EPM/01 21
Thermochemistry (7)
Using standard molar enthalpies of combustion
one can calculate the reaction enthalpy as follows:
This is an exceptional formula, where a property
of the products is subtracted from that of the
reactants.
0
Pri,c,i
0
Rei,c,i
0
r Hn-Hn=H ∑∑ ∆∆∆
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Physical Chemistry EPM/01 22
Hess law
A reaction enthalpy is the sum of the enthalpies of
any sequence of reactions (all at the same
temperature and pressure) into which the overall
reaction may be divided.
Hess's law results from a rigorous application of the statement
that enthalpy is a state property. It does not matter what was the
way to obtain the substance or into how many steps the overall
reaction was split.
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Physical Chemistry EPM/01 23
Hess law (2)
Hess law may be applied to each and every state
quantity (not only to enthalpy).
Another wording:
If any reaction (target reaction) may be represented
as a linear combination of some other reactions
(partial reactions) then any state property of this
reaction is the same linear combination of the
respective state properties of the partial reactions.
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Physical Chemistry EPM/01 24
Hess law (3)
Thermochemical equations:
1.State of matter (phase: solid, liquid, gaseous) and
any specific form of all reactants and products must
be indicated.
2.The heat released or absorbed, i.e., the ∆H must be
shown.
Form (allotropic, polymorphic).
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Physical Chemistry EPM/01 25
Hess law (4)
Rules of manipulation:
1.When the reaction is rewritten in reversed direction,
the sign of its ∆H is changed.
2.When stoichiometric coefficients in the reaction are
multiplied, the ∆H must be multiplied by the same
factor.
3.When two reactions are added, their enthalpy
changes must be added, too.
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Physical Chemistry EPM/01 26
Hess law. Example
Target reaction:
Component reactions:
Step 1. Begin with the thermochemical equation having at
least one of the reactants or products on the correct side of
the arrow in the target reaction:
?H O(l);H+(g)2CO(g)O2+(g)HC :T 0
T22221
22 =∆→
mol]226.75[kJ/=H (g);HC(g)H+2C(s) :A 0
A222 ∆→
mol]-393.5[kJ/=H (g);CO(g)O+C(s) :B 0
B22 ∆→
mol]-285.9[kJ/=H O(l);H(g)O+(g)H :C 0
C2221
2 ∆→
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Physical Chemistry EPM/01 27
Hess law. Example (2)
Hence, we start with reaction B and multiply both sides (as
well as its standard enthalpy) by a factor of 2:
Step 2. To add a reactant or product, add another reaction,
having the desired substance at the same side of the arrow
as in the overall reaction. To cancel a reactant or product
(which is not present in the target reaction), add another
reaction, having the desired substance at the opposite side of
the arrow than in the reaction obtained so far.
2B=D (g);2CO(g)2O+2C(s) 22 →
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Physical Chemistry EPM/01 28
Hess law. Example (3)
In our case, to complete the right side of reaction (T), we
add reaction (C) to reaction (D):
Step 3. If the reaction obtained in step 2 is identical with
reaction T, then the procedure is completed, else - repeat
step 2 (do not use reactions already used in it).
In our case, reaction (E) is not yet equal to reaction (T).
We repeat step 2 to eliminate carbon and hydrogen at the
left side of reaction (E), by adding reversed reaction (A) to
reaction (E) or subtracting (A) from (E).
C+2B=E O(l);H+2CO(g)O2+(g)H+2C(s) 22221
2 →
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Physical Chemistry EPM/01 29
Hess law. Example (4)
Our goal is achieved. Reaction (F) is equal to reaction (T).
The linear combination we found is T=2B+C–A. We
calculate the change in enthalpy in reaction (T) in the same
manner:
T=A-C+2B=F O(l);H+2CO(g)O2+(g)HC 22221
22 →
J/mol]-1299.65[k= ...
...=(-226.75)+(-285.5)+-393.52=H-H+H2=H 0
A
0
C
0
B
0
T ×∆∆∆∆