1.2 introduction to thermodynamics
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What is Thermodynamics?
Thermodynamics i s a branch of phys ica l
sc iences that t reats o f var ious phenomena
of energy and the re lated propert ies o f
matter , espec ia l ly of the laws of
t ransformation of heat into other formsof energy and v ice versa .
S imply put , thermodynamics i s a sc ience
of energy; the energy that has anabi l i ty to make changes.
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History of Thermodynamics
The name thermodynamics s tems f rom
the Greek words therme (heat ) and
dynamis (power) , which i s most
descr ipt ive of the ear ly e f for ts to convert
heat into pow er. Today the same name is broadly
interpreted to inc lude a l l aspects o f
energy and energy t ransformat ions ,
i n c l u d i n g p o w e r g e n e r a t i o n ,
re f r igerat ion, and re lat ionsh ips among
the prop ert ies o f matter.
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History of Thermodynamics
In 1712, Thomas Newcomen built an improved
steam engine, but it was expensive to build and notvery reliable.
James Watt invented the first inexpensive, reliable
steam engine in 1765. Wattssteam engine was more
than six times more efficient than Newcomens!
Watts steam engine catalyzed the industrial
revolution.
In 1798, Count Rumford noticed that canons becamehot as they were bored out. Rumsford showed that
more heat was released in the boring process than
could have been originally contained in the metal.
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History of Thermodynamics
He concluded that the mechanical boring process
was producing heat. This was a major departurefrom the caloric theory that was widely accepted at
the time.
In 1824, Carnot introduced ideal gas cycle analysis inhis work Reflectionon the Motive Power of Fire.
In the 1840sMayer, Joule and Helmholtz developed
the idea that energy could not be created or
destroyed. Energy is conserved. This principle is now
known as the 1st Law of Thermodynamics.
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History of Thermodynamics
Rudolf Clausius stated that nocycle can transfer heat
from a low temperature region to a high temperatureregion with no other interaction with its
surroundings.
This principle is known as the 2nd Law of
Thermodynamics.
The contribution of these scientists and many others
led to the development of the broad field of
thermodynamics that we know today.
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Topics in Modern Thermodynamics include:
Classical Thermodynamics
Characterize the behaviour of large groups ofmolecules based on properties of the entire group of
molecules, such as temperature and pressure.
Statistical ThermodynamicsCharacterize the behaviour of groups of molecules
based on the properties of each individual molecule
and the ways in which molecules interact.
Phase Equilibrium Thermodynamics
Characterize the behaviour of multiple phases that
exist in equilibrium with each other.
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Topics in Modern Thermodynamics include:
Chemical Reaction Equilibrium Thermodynamics
Characterize the behaviour of systems in which the
reactants and products of one or more reversible
chemical reactions are at equilibrium.
Solution Thermodynamics
Characterize the behaviour of systems that contain
more than one chemical species in a mixture.
Pure Component Thermodynamics
Characterize the behaviour of systems that contain a
pure component.
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Thermodynamics
Our s tudy wi l l be governed by two major
law: F i r s t & Second Law of Thermo-dynamics .
Thermodynamics appl ies s imple laws to a
wide range of energy systems that havemajor impact in our soc iety , for example ,
energy use in agr icu l ture , e lect r i c power
generat ion, and t ransportat ion systems.
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Thermodynamics
F i rs t Law of Thermodynamics
Th i s s tates that energy can be ne i ther
created nor destroyed. However , energy
can change forms, and energy can f low
f rom one p lace to another.
Second Law of Thermodynamics
The second law te l l s us how much
thermal energy can be converted intowork ; not a l l o f i t can be .
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Microscopic & Macroscopic
Microscopic thermodynamics we must
look at every molecu le and analyzecol lect ive molecular act ion by stat ist ica l
methods .
Macroscopic thermodynamics we look forthe overa l l e f fect o f the ind iv idual
molecu lar interact ions . Sample : The way
we l ive ; we measure the d istance in
meters and t ime in seconds . Thesemeasurements are very large compared
with the measurement of events on the
molecu lar leve l .
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Concepts & Definitions
In thermodynamics , the f i r s t
cons iderat ion i s that there must besometh ing that per forms the energy
transformat ion.
This someth ing i s ca l led substance. Say, in the fami ly automobi le engine, the
substance i s usual ly the mixture of
gasol in e and a i r.
In a steam turbine the substance i s
probably the steam. The substance may
be a so l id , l iqu id, vapor, or a mixture .
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Concepts & Definitions
SYSTEMS F ixed Mass and F ixed Space
A substance does not ex i st a lone, i t need
to be conta ined. Th is br ings us the to the
concept of a system.
A system i s def ine as any co l lect ion ofmatter or space of f i xed ident i ty and th is
concept i s one of the most important in
the s tudy of thermodynamics .
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Intensive & Extensive Properties
The state of substance complete ly
descr ibes how the substance ex ists temperature , pressure , dens i ty , and other
macroscopic propert ies and by knowing
these propert ies we can determine the
state of substance.
A property i s a character i st ic qual i ty o f
the ent i re system and depends not on how
the system changes state but only on thef ina l system states .
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Intensive & Extensive Properties
TWO TYPES OF PROPERTY
1.Extens ive depends on the s i ze on the
s ize or extent of the system (mass and
volume)
2. Intens ive independent on the s i ze of thesystem ( temperature and pressure)
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Phases of a Substance
So l id so l id i fy ing
Melt ing in t roduct ion of heat so that a
sol id substance wi l l turn into a l iquid
Vapor izat ion cont inuous addi t ion of
heat wi l l turn the l iquid substance into avapor or gas
Subl imat ion some substance in so l id
state turns into gas without pass ing
through l iqu id and vapor s tate .
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Processes and Cycles
A process i s a change i n the system state .
A thermodynamic cyc le i s a co l lect ion of
two or more processes for which the
in i t ia l and f ina l s tates are the same
Systems of Units
Newtons law states that the acce lerat ion
of a part icu lar body i s d i rect ly proport ionalto the resu l tant force act ing on i t and
inversely proport ional to i t s mass