Definition
of path function:-
The thermodynamic property of a system which
not depends upon initial and final state and depends upon the path followed by
the system is known as path function.
The
thermodynamic property which is not state function then this is called path
function
Thermodynamics equilibrium:-
The system is said to be in
thermodynamics equilibrium when state function of the system do not change with
time.
Process and types of processes
Process: - Transition from
one equilibrium state to another is called process.
Isothermal Process :- ( Iso = Same, Thermal = Temperature.)
The process in which the temperature of the
system remains constant throughout the transformation is known as isothermal
process.
In isothermal process T1 = T2
ΔT =T1 –T2
ΔT = 0(Zero) , ∆U =0
Isobaric process :- ( Iso = Same, Baric =
Pressure)
The process in which the pressures of the
system remain constant throughout the change is known as isobaric process.
In
isobaric process P1 = P2
ΔP =P1 –P2
ΔP = 0(Zero)
Isochoric process :- (
Iso = Same, Choric = Volume)
The process in which the
volumes of the system remain constant throughout the change is known as
isochoric process.
In
isochoric process V1 = V2
ΔV =V1 –V2
ΔV = 0(Zero)
Adiabatic process:-
The process in which there is no exchange of
heat between system and its surrounding known as adiabatic process.
In adiabatic
process q=0
Reversible
process:-
It is very slow process in which driving
force and opposing force is nearly equal and difference between this two are very –very small.
OR
Any
process conducted in such a manner that at every stage the driving force is
only infinitesimally greater than opposing force and which can be reversed by
slight increase in opposing force is called Reversible Process.
Driving force >~ Opposing
force
Example:
- Slow expansion of ideal gas in
cylinder fitted with weight less friction less piston.
Feature of reversible process –
1 * Driving and opposing forces are only infinitesimally different
from each other
2 * The process can be reversed at any point during the process by
making infinitesimal change in condition.
* The process takes place in an infinite number of step
* Maximum work is obtained during a reversible process
Difference between isothermal and
adiabatic processes-
Isothermal process
|
Adiabatic process
|
In this process temperature
remain constant.
|
In this process temperature
may be increases or decreases
|
Internal energy remain
constant.
ΔU = O
|
Internal energy is varies
ΔU # O
|
The maximum work is obtain
|
The maximum work done is not
obtain
|
For isothermal process q = -W
|
For adiabatic process q +W =∆U
|
The system is not thermally
isolated from its surrounding hence either open or closed System is required
|
The system is thermally
isolated from its surrounding hence isolated System is required
|
System can exchange heat with
surrounding
|
System cannot exchange heat
with surrounding
|
Example:- isothermal expansion of an ideal gas
|
Example:- Adiabatic expansion
of an ideal gas
|
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