upsc ese thermodynamics
TRANSCRIPT
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Himanshu Vasistha
Thermodynamics-1
for UPSC IES and GATE 2014 Mechanical Engineering
By
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Thermodynamics
The branch of science that deals with the relations
between heat and other forms of energy, and ofthe relationships between all forms of energy.
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System and Surroundings
!A system is a finite quantity of matter or a
prescribed region of space.
! The actual or hypothetical envelope
enclosing the system is called Boundary.
! Boundary may be fixed or moveable.
! Everything external to the system is
called Surroundings.
!A System and its Surroundings together
comprise a Universe.
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Types of System
! Open System- In this matter and
energy flow in or out of the
system. Most of the Engineering
Systems are Open Systems.
! Closed System- In this theboundary is impervious to the
flow of matter. A mass of gas and
vapour in an engine cylinder, with
a continuous boundary may be
regarded as a Closed System.
! Isolated System- In this the
system neither exchanges energy
nor matter with another system
or surroundings.
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Properties, Processes and Cycles
When properties like, volume, pressure, temperature etc. of
a system have definite values, then the system is said to
exist at a definite State.
Properties are the coordinates which describe the state of a
system.
An operation in which one or more properties of a system
changes is called change of state.
The succession of States passed during a change of state is
called aprocess.
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Process and Cycle
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Thermodynamic Equilibrium
Thermodynamic equilibrium exists in a system when no change of
macroscopic properties is registered, if the system is isolated from
its surroundings.
An isolated system always reaches in course of time a state ofthermodynamic equilibrium and can never depart from it
spontaneously.
If a system is in equilibrium, no spontaneous change in
macroscopic property can occur.
Thermodynamic equilibrium exists when, Mechanical, Thermal and
Chemical equilibrium exist simultaneously.
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Zeroth Law of Thermodynamics
When a body A is in thermal equilibrium with a body B, and
also separately with a body C, then B and C will be in thermal
equilibrium with each other.
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! Zeroth law is the basis of
temperature measurement.
! There are five kinds of
thermometer, each with its own
thermometric property.
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Thermometer Thermometric property
Constant vol. gas
thermometerPressure
Constant pressure gas
thermometerVolume
Electrical Resistance
ThermometerResistance
Thermocouple Thermal e.m.f
Mercury in glass
thermometerLength
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Work transfer
Work is done by a force as it acts upon a body moving in
the direction of the force.
When work is done by a system, it is taken to be positive,and if work is done on a system, it is taken to be negative.
Work is one of the forms in which a system and its
surroundings interact.
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Displacement work
! When the piston moves, the
volume changes, and the workdone can be calculated as
described in the figure.
! The magnitude of the work doneis the area under the P-V diagram.
! The path shown on the P-V
diagram must pass through
equilibrium states; i.e. must be
Quasi Static.
! The integration to calculate the
work done can be performed onlyif the process is quasi static.
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Path Function and Point Function
Area under the PV curve gives the amount of work done,
so it is not a function of the end states of a process, but
depends upon the path the process takes. Therefore,
work is called apath function.
Thermodynamic properties arepoint functions, since for a
given state, there is a definite value for each property.
Path Functions are called inexact or imperfect differential.
Point Functions are called exact or perfect differential.
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Work in various Quasi
Static Processes
PVk= constant
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Open and closed
system work
! The open system work is
calculated by plotting it on
volume axis.
! The closed system work is
calculated by plotting it on
pressure axis.
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Zero work transfer
Work transfer is ONLY identified at the boundaries of a
system. Therefore, it can be termed as a boundary
phenomenon.
The expansion of a gas against vacuum is called free
expansion. In this case the work done by the system is
zero, as no work crosses the boundary.
This free expansion process is not a quasi static process,
although the initial and end states are in equilibrium.
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Heat Transfer
It is defined as a form of energy that is transferred across
a boundary due to a temperature difference.
The direction of heat transfer is from a body at hightemperature to a body at lower temperature.
Heat flow into a system is taken to be positive, and heat
flow out of a system is taken to be negative.
Heat transfer is a transit, and occurs only at the boundary.
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Important points for a Heat and Work Transfer
Heat and work transfer are energy interactions.
The same e#ect in a closed system can be brought
about either by heat transfer or work transfer.
Both transfers are boundary phenomena, and both
represent energy crossing the boundaries of the system.
It is wrong to say 'total heat' of a closed system as heat and workare not a property of a system. They cannot be stored in the
system. Both are energies in transit
Heat transfer is the energy interaction due to temperature di#erence
only. All other energy interactions can be termed as work transfer
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