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Steam formation &
Turbines
By:
Prof. Siddesh Kumar N M
Assistant Professor
Department of Mechanical Engineering
PES College of Engineering Mandya
Boiler
2
Prof. Siddesh Kumar N M PESCE Mandya
Classification of boilers
• According to content in the tube
• Fire tube boiler
• Water tube boiler
• According to the orientation of boiler
• Horizontal boiler
• Vertical boiler
• According to location of boiler
• Internal boiler
• External boiler
3
Prof. Siddesh Kumar N M PESCE Mandya
Classification of boilers
• According to method of circulation
• Natural circulation
• Forced circulation
• According to number of tubes
• Single tube boiler
• Multi tube boiler
• According to boiler mobility
• Stationary boiler
• Mobile or portable boiler
4
Prof. Siddesh Kumar N M PESCE Mandya
Classification of boilers
• According to boiler pressure
• Low pressure boiler
• Medium pressure boiler
• High pressure boiler
• Based on draft used
• Natural draft
• Artificial draft
• Based on fuel used
5
Prof. Siddesh Kumar N M PESCE Mandya
Water tube
boiler
• Furnace is situated outside
the boiler shell
• Water circulates between the
drum and the tube
• Complete combustion takes
place
• Thermal efficiency is high
• Steam generation is fast
• Easy for cleaning
• High cost
• Used in Power plants
6
Prof. Siddesh Kumar N M PESCE Mandya
Fire tube
boiler
• Furnace is situated inside the
boiler shell
• Water circulates within the drum
only
• Incomplete combustion takes
place
• Thermal efficiency is low
• Steam generation is slow
• Not Easy for cleaning
• Low cost
• Used in Process industries or
industrial plants
7
Prof. Siddesh Kumar N M PESCE Mandya
Difference between water tube boiler and fire
tube boiler
Water tube boiler Fire tube boiler
• Furnace is situated outside the boiler shell • Furnace is situated inside the boiler shell
• Water circulates between the drum and the
tube
• Water circulates within the drum only
• Complete combustion takes place • Incomplete combustion takes place
• Thermal efficiency is high • Thermal efficiency is low
• Steam generation is fast • Steam generation is slow
• Easy for cleaning • Not Easy for cleaning
• High cost • Low cost
• Used in Power plants • Used in Process industries or industrial plants
8
Prof. Siddesh Kumar N M PESCE Mandya
Applications of boilers
• These are used to generate power in steam turbines or
engines.
• These are used for various processes in process industries
• These are used in houses or buildings in cool weather for
generating a hot water supply
• In textile industry for sizing and humidification etc.
• In sugar and chemical industries
9
Prof. Siddesh Kumar N M PESCE Mandya
Steam
• Steam is the most common working
substance used in steam engines,
steam turbines and atomic power
plants for generation of power
• Steam is the vapor of water and
produced by the application of
thermal energy to the fluid
• Vapor is the intermediate phase
between liquid and gas
• If vapor is superheated then it obeys
gas laws
• The superheated steam is used for
power generation
10
Prof. Siddesh Kumar N M PESCE Mandya
Steam formation
11
Prof. Siddesh Kumar N M PESCE Mandya
Steam
formation
Steam is generated by the application of heat
or thermal energy to the water
The heat energy can be obtained from many
sources like coal, oil, gas, solar & nuclear fuels
The heating is done at different pressure and
temperature
Pressure plays an important role in the
generation of the steam
12
Prof. Siddesh Kumar N M PESCE Mandya
Steam generation can be divided into three
stages
Heating of water up to boiling point Evaporation of boiling water & its
conversion into dry saturated steam
Transformation of dry steam into
super saturated steam
13
Prof. Siddesh Kumar N M PESCE Mandya
Steam formation
14
Prof. Siddesh Kumar N M PESCE Mandya
Steam
formation
Generally steam formation is taken place
at constant pressure
Piston weight is applying constant
pressure on water
Vapors are formed by the addition of
heat input
The formation of steam is clearly
understood by T-H, T-V & T-S diagrams
Let us consider 1Kg of water at –10
degree Celsius as the initial point
15
Prof. Siddesh Kumar N M PESCE Mandya
T-H diagram
16
Prof. Siddesh Kumar N M PESCE Mandya
T-H diagram
• When heat is added its temperature
raises 0°C (273 K) there fore melting
starts (2 – 3) during this process solid
phase changes to liquid phase
• Entire ice is melted at (3) only liquid
water is present at that point
• Once the temperature becomes
100°C, vapor will start to form (3-4 & 4-
5) both liquid and vapor form will be
present
• Temperature remains constant while
converting (Isothermal process)
• Addtion of heat will cause the super
heating of steam
17
Prof. Siddesh Kumar N M PESCE Mandya
T-V diagram
18
Prof. Siddesh Kumar N M PESCE Mandya
T-V diagram
• Latent heat of fusion: Amount of
heat required to convert ice into
water (transformation of phases
from solid to liquid).
• Sensible heat: Amount of heat
required to convert liquid state of
water into vapourization (0 – 100 C
boiling point).
• Saturation temperature:
Temperature at which vaporization
takes places at constant pressure.
• Latent heat of vapourization:
Amount of heat required to
complete transformaton of water
into vapor at constant temperature
19
Prof. Siddesh Kumar N M PESCE Mandya
P- V diagram
20
Prof. Siddesh Kumar N M PESCE Mandya
P- V diagram
• Convertion taking places at lower
pressure result in the phase
transformation of soild,
solid+liquid,mixture of liquid
+vapor,and vapor
• Increase in pressure will reduces the
straight horizontal line which results
in the reduction of phase
transformation
• At certain pressure the distance
becomes zero that point is critical
point
• The point at which the liquid phase
will not exit that point we call it as
critical point
21
Prof. Siddesh Kumar N M PESCE Mandya
P-T diagram
• This is also called as phase
diagram
• All three lines meet at a point
called as triple point
• All three phases co exits at a
point in equilibrium called as
triple point
22
Prof. Siddesh Kumar N M PESCE Mandya
Specific Volume
• Specific volume of steam can be
defined as the volume occupied by
unit mass of steam at given
temperature & pressure
23
Prof. Siddesh Kumar N M PESCE Mandya
Enthalpy
Enthalpy of wet steam
• Amount of heat supplied at
constant pressure to convert 1Kg
of water at 0 C to 1Kg of wet
steam at the specified dryness
fraction
Enthalpy of super heated steam
• Amount of heat supplied at
constant pressure to convert 1Kg
of water at 0 C to 1Kg of supper
heated steam at the saturated
temperature
24
Prof. Siddesh Kumar N M PESCE Mandya
Internal Energy
• It is the actual energy stored in the steam
• The total heat of the steam is sum of all sensible heat, internal latent heat and external work of
evaporation
• Work of evaporation is not stored in the steam as it is utilized in doing the external work
• Internal energy of steam is defined as the difference between entropy of steam and the external
work of evaporation
25
Prof. Siddesh Kumar N M PESCE Mandya
Dryness fraction
• It is defined as the ratio of mass of
actual dry steam to the total mass
of wet steam containing in it
26
Prof. Siddesh Kumar N M PESCE Mandya
27
Prof. Siddesh Kumar N M PESCE Mandya
Steam Turbines
28
Prof. Siddesh Kumar N M PESCE Mandya
29
Prof. Siddesh Kumar N M PESCE Mandya
Steam Turbine
30
Prof. Siddesh Kumar N M PESCE Mandya
Classification of Steam
turbines
Steam turbine can be classified into two types
• Impulse turbine:
• It works on the principle of impulse where kinetic
energy of the force impenges on the blades and
produces force which results in the change in
momentum
• Ex: De laval turbine,curtis turbine
• Reaction turbine:
• It works on the principle of reaction, a reaction force is
developed along with the development of centrifugal
force
• Ex: Parsons turbine
31
Prof. Siddesh Kumar N M PESCE Mandya
Impulse Turbine
32
Prof. Siddesh Kumar N M PESCE Mandya
Principle & Operation of Impulse steam turbine
De- Laval Turbine
• The centrifugal force is exerted all
along the curved surfaces
• Centrifugal forces causes the blade to
move
• Rotor is a device in which the blades
are arranged on the circumference of
the wheel
• They will be moved by dynamic action
of the wheel
33
Prof. Siddesh Kumar N M PESCE Mandya
Impulse Turbine or De
Laval Turbine
• In this turbine steam is initially expanded in nozzle from
high pressure to low pressure
• The high velocity jet of steam coming out of the nozzle is
made to glide over the curved vanes called blade
• The high velocity of steam deflects the blade in
circumferential direction
• This cause the change in motion and momentum
• The change is momentum is caused by centrifugal force
34
Prof. Siddesh Kumar N M PESCE Mandya
Principle & Operation of reaction
steam turbine
Parsons Turbine
35
Prof. Siddesh Kumar N M PESCE Mandya
Pressure velocity changes
in Reaction turbine
• High pressure steam passing in the first row causes
small pressure drop and increase in velocity
• When it enters moving blade again suffers from
pressure drop and velocity of steam gets converted
into mechanical energy of rotation
• After conversion the velocity of steam reduces and
this continues
• This continues up to the complete reduction of
pressure of the steam
36
Prof. Siddesh Kumar N M PESCE Mandya
Reaction turbine (Parsons
Turbine)
• The reaction turbine is also called as Impulse reaction turbine
• Consists of both fixed and moving blades fitted on the
circumference
• Here the high pressure steam does not expand initially in the nozzle
instead passes through moving blades and fixed blades
• The steam experience a nozzle effect in between
• The pressure drop increase simultaneously with increase in velocity
• Along with the force backward reaction takes place thus the sum of
forces acting on the blades are reaction force and centrifugal force
37
Prof. Siddesh Kumar N M PESCE Mandya
Difference between the Impulse turbine & Reaction turbine
Impulse turbine Reaction turbine
Complete expanssion takes place in
nozzle
Steam expands continuously and
sucessively in bith fixred and moving
blades
Blades are symmetrical in shape Blades are not symmetrical and aerofoil
in shape
Rotor runs at high speed Rotor runs at relativly low speed
Occupies less place per unit power Occupies more space per unit power
Suitabke for small scale power
generation
Suitable for medium and large scale
power generation
Pressure of the steam remains constant
throught the blade
Pressure reduction takes places from
inlet to outlet of the blade
Size of the impuse turbine is less Size of the reaction turbine is more
38
Prof. Siddesh Kumar N M PESCE Mandya
Gas Turbines
39
Prof. Siddesh Kumar N M PESCE Mandya
Gas turbines
• Gas turbine is a devices which uses
combust gases to produce mechanical
energy
• Based on the cycle of operation gas turbine
is divied into two types
• Open type gas turbine
• Closed type gas turbine
• Instead of steam here combust gases will
be used
40
Prof. Siddesh Kumar N M PESCE Mandya
Working Principle of open cycle gas turbine
• IT consists of compressor, combustion
chamber and gas turbine
• Both compress and gas turbine are coupled
and mounted on the same shaft
• The atmospheric air is drawn and
compressed into high pressure
• The high pressure air is drawn into the
combustion chamber and heat is addded
• The high temperature gas is passed into
turbine and expanssion takes place
• The gas after expansion sent into
atmosphere
41
Prof. Siddesh Kumar N M PESCE Mandya
Working Principle of closed cycle gas turbine
• IT consists of compressor, combustion
chamber, gas turbine and coller
• Both compress and gas turbine are coupled
and mounted on the same shaft
• The atmospheric air is drawn and
compressed into high pressure
• The high pressure air is drawn into the
combustion chamber and heat is addded
• The high temperature gas is passed into
turbine and expanssion takes place
• The gas after expansion sent into cooler,
again it is compressed and sent to
compressor
42
Prof. Siddesh Kumar N M PESCE Mandya
Difference between the Open cycle gas turbine & closed cycle
turbine
Open cycle gas turbine Closed cycle gas turbine
Working fluid is replacced after every
cycle
Working fluid is replaced after certain
number of cycles
Exhxaut gas is sent to atmosphere Exhaust gas is sent to cooler
Mixture of air and product of
combustion gas is used as a fuel
Any fuel can be used as working
substance
High grade fuels are used to supply of
heat
Any grade fuel is used to supply of heat
There will be heat and mass transfer
takes places
There will be only heat transfer between
system and surroundings
Loss of working substance takes places No loss of working substance
Cooling wate is not required Cooling water is required
43
Prof. Siddesh Kumar N M PESCE Mandya
Thank You
By:
Prof Siddesh Kumar N M
Assistant Professor
Department of Mechanical
Engineering
PES College of Engineering
Mandya
Mail Id:
siddeshkumarnm@pesce.ac.in
44
Prof. Siddesh Kumar N M PESCE Mandya

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Steam formation and turbines

  • 1. Steam formation & Turbines By: Prof. Siddesh Kumar N M Assistant Professor Department of Mechanical Engineering PES College of Engineering Mandya
  • 2. Boiler 2 Prof. Siddesh Kumar N M PESCE Mandya
  • 3. Classification of boilers • According to content in the tube • Fire tube boiler • Water tube boiler • According to the orientation of boiler • Horizontal boiler • Vertical boiler • According to location of boiler • Internal boiler • External boiler 3 Prof. Siddesh Kumar N M PESCE Mandya
  • 4. Classification of boilers • According to method of circulation • Natural circulation • Forced circulation • According to number of tubes • Single tube boiler • Multi tube boiler • According to boiler mobility • Stationary boiler • Mobile or portable boiler 4 Prof. Siddesh Kumar N M PESCE Mandya
  • 5. Classification of boilers • According to boiler pressure • Low pressure boiler • Medium pressure boiler • High pressure boiler • Based on draft used • Natural draft • Artificial draft • Based on fuel used 5 Prof. Siddesh Kumar N M PESCE Mandya
  • 6. Water tube boiler • Furnace is situated outside the boiler shell • Water circulates between the drum and the tube • Complete combustion takes place • Thermal efficiency is high • Steam generation is fast • Easy for cleaning • High cost • Used in Power plants 6 Prof. Siddesh Kumar N M PESCE Mandya
  • 7. Fire tube boiler • Furnace is situated inside the boiler shell • Water circulates within the drum only • Incomplete combustion takes place • Thermal efficiency is low • Steam generation is slow • Not Easy for cleaning • Low cost • Used in Process industries or industrial plants 7 Prof. Siddesh Kumar N M PESCE Mandya
  • 8. Difference between water tube boiler and fire tube boiler Water tube boiler Fire tube boiler • Furnace is situated outside the boiler shell • Furnace is situated inside the boiler shell • Water circulates between the drum and the tube • Water circulates within the drum only • Complete combustion takes place • Incomplete combustion takes place • Thermal efficiency is high • Thermal efficiency is low • Steam generation is fast • Steam generation is slow • Easy for cleaning • Not Easy for cleaning • High cost • Low cost • Used in Power plants • Used in Process industries or industrial plants 8 Prof. Siddesh Kumar N M PESCE Mandya
  • 9. Applications of boilers • These are used to generate power in steam turbines or engines. • These are used for various processes in process industries • These are used in houses or buildings in cool weather for generating a hot water supply • In textile industry for sizing and humidification etc. • In sugar and chemical industries 9 Prof. Siddesh Kumar N M PESCE Mandya
  • 10. Steam • Steam is the most common working substance used in steam engines, steam turbines and atomic power plants for generation of power • Steam is the vapor of water and produced by the application of thermal energy to the fluid • Vapor is the intermediate phase between liquid and gas • If vapor is superheated then it obeys gas laws • The superheated steam is used for power generation 10 Prof. Siddesh Kumar N M PESCE Mandya
  • 11. Steam formation 11 Prof. Siddesh Kumar N M PESCE Mandya
  • 12. Steam formation Steam is generated by the application of heat or thermal energy to the water The heat energy can be obtained from many sources like coal, oil, gas, solar & nuclear fuels The heating is done at different pressure and temperature Pressure plays an important role in the generation of the steam 12 Prof. Siddesh Kumar N M PESCE Mandya
  • 13. Steam generation can be divided into three stages Heating of water up to boiling point Evaporation of boiling water & its conversion into dry saturated steam Transformation of dry steam into super saturated steam 13 Prof. Siddesh Kumar N M PESCE Mandya
  • 14. Steam formation 14 Prof. Siddesh Kumar N M PESCE Mandya
  • 15. Steam formation Generally steam formation is taken place at constant pressure Piston weight is applying constant pressure on water Vapors are formed by the addition of heat input The formation of steam is clearly understood by T-H, T-V & T-S diagrams Let us consider 1Kg of water at –10 degree Celsius as the initial point 15 Prof. Siddesh Kumar N M PESCE Mandya
  • 16. T-H diagram 16 Prof. Siddesh Kumar N M PESCE Mandya
  • 17. T-H diagram • When heat is added its temperature raises 0°C (273 K) there fore melting starts (2 – 3) during this process solid phase changes to liquid phase • Entire ice is melted at (3) only liquid water is present at that point • Once the temperature becomes 100°C, vapor will start to form (3-4 & 4- 5) both liquid and vapor form will be present • Temperature remains constant while converting (Isothermal process) • Addtion of heat will cause the super heating of steam 17 Prof. Siddesh Kumar N M PESCE Mandya
  • 18. T-V diagram 18 Prof. Siddesh Kumar N M PESCE Mandya
  • 19. T-V diagram • Latent heat of fusion: Amount of heat required to convert ice into water (transformation of phases from solid to liquid). • Sensible heat: Amount of heat required to convert liquid state of water into vapourization (0 – 100 C boiling point). • Saturation temperature: Temperature at which vaporization takes places at constant pressure. • Latent heat of vapourization: Amount of heat required to complete transformaton of water into vapor at constant temperature 19 Prof. Siddesh Kumar N M PESCE Mandya
  • 20. P- V diagram 20 Prof. Siddesh Kumar N M PESCE Mandya
  • 21. P- V diagram • Convertion taking places at lower pressure result in the phase transformation of soild, solid+liquid,mixture of liquid +vapor,and vapor • Increase in pressure will reduces the straight horizontal line which results in the reduction of phase transformation • At certain pressure the distance becomes zero that point is critical point • The point at which the liquid phase will not exit that point we call it as critical point 21 Prof. Siddesh Kumar N M PESCE Mandya
  • 22. P-T diagram • This is also called as phase diagram • All three lines meet at a point called as triple point • All three phases co exits at a point in equilibrium called as triple point 22 Prof. Siddesh Kumar N M PESCE Mandya
  • 23. Specific Volume • Specific volume of steam can be defined as the volume occupied by unit mass of steam at given temperature & pressure 23 Prof. Siddesh Kumar N M PESCE Mandya
  • 24. Enthalpy Enthalpy of wet steam • Amount of heat supplied at constant pressure to convert 1Kg of water at 0 C to 1Kg of wet steam at the specified dryness fraction Enthalpy of super heated steam • Amount of heat supplied at constant pressure to convert 1Kg of water at 0 C to 1Kg of supper heated steam at the saturated temperature 24 Prof. Siddesh Kumar N M PESCE Mandya
  • 25. Internal Energy • It is the actual energy stored in the steam • The total heat of the steam is sum of all sensible heat, internal latent heat and external work of evaporation • Work of evaporation is not stored in the steam as it is utilized in doing the external work • Internal energy of steam is defined as the difference between entropy of steam and the external work of evaporation 25 Prof. Siddesh Kumar N M PESCE Mandya
  • 26. Dryness fraction • It is defined as the ratio of mass of actual dry steam to the total mass of wet steam containing in it 26 Prof. Siddesh Kumar N M PESCE Mandya
  • 27. 27 Prof. Siddesh Kumar N M PESCE Mandya
  • 28. Steam Turbines 28 Prof. Siddesh Kumar N M PESCE Mandya
  • 29. 29 Prof. Siddesh Kumar N M PESCE Mandya
  • 30. Steam Turbine 30 Prof. Siddesh Kumar N M PESCE Mandya
  • 31. Classification of Steam turbines Steam turbine can be classified into two types • Impulse turbine: • It works on the principle of impulse where kinetic energy of the force impenges on the blades and produces force which results in the change in momentum • Ex: De laval turbine,curtis turbine • Reaction turbine: • It works on the principle of reaction, a reaction force is developed along with the development of centrifugal force • Ex: Parsons turbine 31 Prof. Siddesh Kumar N M PESCE Mandya
  • 32. Impulse Turbine 32 Prof. Siddesh Kumar N M PESCE Mandya
  • 33. Principle & Operation of Impulse steam turbine De- Laval Turbine • The centrifugal force is exerted all along the curved surfaces • Centrifugal forces causes the blade to move • Rotor is a device in which the blades are arranged on the circumference of the wheel • They will be moved by dynamic action of the wheel 33 Prof. Siddesh Kumar N M PESCE Mandya
  • 34. Impulse Turbine or De Laval Turbine • In this turbine steam is initially expanded in nozzle from high pressure to low pressure • The high velocity jet of steam coming out of the nozzle is made to glide over the curved vanes called blade • The high velocity of steam deflects the blade in circumferential direction • This cause the change in motion and momentum • The change is momentum is caused by centrifugal force 34 Prof. Siddesh Kumar N M PESCE Mandya
  • 35. Principle & Operation of reaction steam turbine Parsons Turbine 35 Prof. Siddesh Kumar N M PESCE Mandya
  • 36. Pressure velocity changes in Reaction turbine • High pressure steam passing in the first row causes small pressure drop and increase in velocity • When it enters moving blade again suffers from pressure drop and velocity of steam gets converted into mechanical energy of rotation • After conversion the velocity of steam reduces and this continues • This continues up to the complete reduction of pressure of the steam 36 Prof. Siddesh Kumar N M PESCE Mandya
  • 37. Reaction turbine (Parsons Turbine) • The reaction turbine is also called as Impulse reaction turbine • Consists of both fixed and moving blades fitted on the circumference • Here the high pressure steam does not expand initially in the nozzle instead passes through moving blades and fixed blades • The steam experience a nozzle effect in between • The pressure drop increase simultaneously with increase in velocity • Along with the force backward reaction takes place thus the sum of forces acting on the blades are reaction force and centrifugal force 37 Prof. Siddesh Kumar N M PESCE Mandya
  • 38. Difference between the Impulse turbine & Reaction turbine Impulse turbine Reaction turbine Complete expanssion takes place in nozzle Steam expands continuously and sucessively in bith fixred and moving blades Blades are symmetrical in shape Blades are not symmetrical and aerofoil in shape Rotor runs at high speed Rotor runs at relativly low speed Occupies less place per unit power Occupies more space per unit power Suitabke for small scale power generation Suitable for medium and large scale power generation Pressure of the steam remains constant throught the blade Pressure reduction takes places from inlet to outlet of the blade Size of the impuse turbine is less Size of the reaction turbine is more 38 Prof. Siddesh Kumar N M PESCE Mandya
  • 39. Gas Turbines 39 Prof. Siddesh Kumar N M PESCE Mandya
  • 40. Gas turbines • Gas turbine is a devices which uses combust gases to produce mechanical energy • Based on the cycle of operation gas turbine is divied into two types • Open type gas turbine • Closed type gas turbine • Instead of steam here combust gases will be used 40 Prof. Siddesh Kumar N M PESCE Mandya
  • 41. Working Principle of open cycle gas turbine • IT consists of compressor, combustion chamber and gas turbine • Both compress and gas turbine are coupled and mounted on the same shaft • The atmospheric air is drawn and compressed into high pressure • The high pressure air is drawn into the combustion chamber and heat is addded • The high temperature gas is passed into turbine and expanssion takes place • The gas after expansion sent into atmosphere 41 Prof. Siddesh Kumar N M PESCE Mandya
  • 42. Working Principle of closed cycle gas turbine • IT consists of compressor, combustion chamber, gas turbine and coller • Both compress and gas turbine are coupled and mounted on the same shaft • The atmospheric air is drawn and compressed into high pressure • The high pressure air is drawn into the combustion chamber and heat is addded • The high temperature gas is passed into turbine and expanssion takes place • The gas after expansion sent into cooler, again it is compressed and sent to compressor 42 Prof. Siddesh Kumar N M PESCE Mandya
  • 43. Difference between the Open cycle gas turbine & closed cycle turbine Open cycle gas turbine Closed cycle gas turbine Working fluid is replacced after every cycle Working fluid is replaced after certain number of cycles Exhxaut gas is sent to atmosphere Exhaust gas is sent to cooler Mixture of air and product of combustion gas is used as a fuel Any fuel can be used as working substance High grade fuels are used to supply of heat Any grade fuel is used to supply of heat There will be heat and mass transfer takes places There will be only heat transfer between system and surroundings Loss of working substance takes places No loss of working substance Cooling wate is not required Cooling water is required 43 Prof. Siddesh Kumar N M PESCE Mandya
  • 44. Thank You By: Prof Siddesh Kumar N M Assistant Professor Department of Mechanical Engineering PES College of Engineering Mandya Mail Id: siddeshkumarnm@pesce.ac.in 44 Prof. Siddesh Kumar N M PESCE Mandya