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thermodynamics
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Thermodynamics
deals with the interaction of
heat
and work associated with various
physical
and
chemical
transformations
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Forms of energy dealt in chemical thermodynamics are
electrical
energy and
heat
energy
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Work involved in chemical reactions is either
expansion
or
compression
of
gases
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All
chemical reactions
take place with either
absorption
or
liberation
of
heat
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Understanding
thermodynamics
helps chemists study the
conditions
under which
reactions
can take place
spontaneously
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System is a specified
portion of the universe under thermodynamic
study,
separated from the rest of
the
universe with
a
definite boundary surface
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Example:
Water
in a
beaker
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Types of
systems
:
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Open system:
Can exchange both
matter
and
energy
with the
surroundings
Example:
Hot water
in an
open beaker
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Closed
system:
Cannot exchange
matter
but can exchange
energy
in the form of
heat
,
work
, etc.
Example:
Hot water
in equilibrium with its
vapor
in a
closed beaker
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Isolated system:
Cannot
exchange either
matter
or
energy
with the surroundings
Example:
Water
in contact with its
vapor
in a closed
insulated
vessel
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State
of a system indicates the
position
of the system and is defined by
properties
like temperature, volume, pressure, etc.
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Standard state of a system is at
298
K and under
1
bar pressure
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State functions
or
thermodynamic functions
are
variables
like
temperature
,
pressure
,
volume
, etc. that define the
state
of a
system
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Process
is an operation by which a system
changes
from one
equilibrium
state to another
equilibrium
state
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Types of
processes
:
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Isothermal process:
Temperature
of the system remains
constant
Example: Experiment with a
reacting mixture
in a
thermostat
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Adiabatic
process:
No
heat
is
exchanged
between the
system
and the
surroundings
Example:
Liquefaction
of a
gas
by
Joule-Thomson effect
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Differences between
isothermal
and
adiabatic
process:
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Isothermal process:
Heat is
exchanged
with the
surroundings
Temperature
remains
constant
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Adiabatic process:
No
heat exchange
with the surroundings
Temperature
does not remain
constant
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Reversible
process is carried out
infinitesimally slowly
and can be
reversed
at any
stage
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Irreversible
process takes place in one step and cannot be
reversed
at any stage
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Differences between
reversible
and
irreversible
process:
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Reversible
process involves
infinite
steps and requires
infinite
time
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Irreversible
process involves
single
or a
few
steps and is a
sudden
process
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Cyclic process
is where the system returns to its
initial
state after a series of
changes
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Isobaric
process takes place at
constant
pressure
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Isochoric
process takes place at
constant
volume
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Intensive property
does not depend on the quantity of the
substance
present in the system
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Extensive property depends on the quantity of the substance present in the
system
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Internal energy
is the sum of different energies possessed by a system and is a
state function
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First
law of thermodynamics states that
energy
can
neither
be
created
nor
destroyed
, but can be
converted
from one
form
into
another
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Mathematically represented as ΔU =
q + w
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Where ΔU is the change in
internal energy
, q is the amount of
energy absorbed
or
liberated
, and w is the
work done
by the
system
or on the
system
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Derivation of the
first
law of thermodynamics involves the
internal energy
of the system at
initial
and
final
states,
energy
absorbed, and
work done
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Derivation of the First Law of Thermodynamics:
Internal energy of the system at
initial
state: U1
Internal energy of the system at
final
state: U2
System absorbs q kJ of energy
Work done on the system to attain the
final
state: w
Total energy of the system in the initial state = U1
Total energy of the system in the
final
state = U1 + q + w = U2
ΔU = q + w
dU = dq + dw
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Sign conventions used in Thermodynamics:
w =
+ve
if work is done on the system
w =
-ve
if work is done by the system
q =
+ve
if heat is absorbed by the system
q =
-ve
if heat is liberated from the system
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Applications of the
First
Law of Thermodynamics:
Case-1:
Isothermal
process, dT = 0, ΔU = 0, w = -q
Case-2:
Adiabatic
process, q = 0, w = ΔU
Case-3:
No work done by the system
, w = 0, ΔU = q
Case-4: Work done by the system for
gas expansion
, w = -PΔV, q = ΔU + PΔV
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Work (w):
Transferring energy is called
work
Unit:
Joule
(
J
)
Mechanical work =
force
x
displacement
Electrical work =
Charge
x
potential difference
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See all 127 cards
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