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Steam turbines use the steam as a working fluid. In steam turbines, high
pressure steam from the boiler is expanded in nozzle, in which the enthalpy
of steam being converted into kinetic energy.
Thus, the steam at high velocity at the exit of nozzle impinges over the
moving blades (rotor) which cause to change the flow direction of steam and
thus cause a tangential force on the rotor blades.
Due to this dynamic action between the rotor and the steam, thus the
work is developed.
Compounding is the method of obtaining reasonable tangential speed
of rotor for a given overall pressure drop by using more than one
stages.
Compounding is necessary for steam turbines because
if the tangential blade tip velocity greater than 400 m/s, then the
blade tips are subjected to centrifugal stress. Due this, utilization is
low hence the efficiency of the stage is also low.
Compounding can be done by the following methods, namely,
(i)Velocity compounding,
(ii) Pressure compounding or Rateau stage
(iii) Pressure-Velocity compounding and
(iv) Impulse- Reaction staging.
Compounding Of Steam Turbines
Velocity Compounding (Curtis Stage) of Impulse Turbine :
 This consists of set of nozzles, rows of moving blades (rotor) & a rows of
stationary blades (stator).
The function of stationary blades is to direct the steam coming from the
first moving row to the next moving row without change in velocity.
All the kinetic energy available at the nozzle exit is successively absorbed by
all the moving rows &the steam is sent from the last moving row with low
velocity to achieve high utilization.
 The turbine works under this type of compounding stage is called velocity
compounded turbine.
e.g. Curtis stage steam turbine
Pressure Compounded (Rateau Stage ) Impulse Turbine :
A number of simple impulse stages arranged in series is called as pressure compounding.
 In this case, the turbine is provided with rows of fixed blades which acts
as a nozzles at the entry of each rows of moving blades.
 The total pressure drop of steam does not take place in a single nozzle
but divided among all the rows of fixed blade which act as nozzle for the
next moving rows.
Pressure compounding leads to higher efficiencies because very high flow
velocities are avoided through the use of purely convergent nozzles.
 For maximum utilization, the absolute velocity of steam at the outlet of
the last rotor must be axially directed.
It is usual in large turbines to have pressure compounded or reaction
stages after the velocity compounded stage.
Pressure -Velocity Compounding
Pressure drop from the chest pressure to the condenser pressure occurs at two
stages.
 First and second stage taken separately are identical to a velocity
compounding
 consists of a set of nozzles and rows of moving blades fixed to the shaft and
rows of fixed blades to casing.
The entire expansion takes place in the nozzles.
The high velocity steam parts with only portion of the kinetic energy in
the first set of the moving blades and then passed on to fixed blades
where only change in direction of jet takes place without appreciable
loss in velocity. This jet then passes on to another set of moving vanes
where further drop in kinetic energy occurs.
blade velocity coefficient or nozzle velocity coefficient.
For Impulse turbine, in ideal conditions. If the losses are considered, then,
Forces on the Blade and Work Done
Tangential force
due to change in whirl velocity or tangential component of
absolute velocities
Axial thrust
due to change in axial velocity components
Blade Efficiency or Diagram Efficiency :
It is defined as the ratio of work done per kg of steam by the
rotor to the energy available at the inlet per kg of steam.
The Stage Efficiency :
It is defined as “the ratio of work done per kg of steam by
the rotor to the isentropic enthalpy change per kg of steam in the
nozzle”
Condition for Maximum Utilization Factor or Blade efficiency
with Equiangular Blades for Impulse Turbine :
Example 1 :
A single stage Impulse turbine has a diameter of 1.5 m. and running at 3000 RPM.
The nozzle angle is 20 . Speed ratio is 0.45. Ratio of relative velocity at the outlet
to that at inlet is 0.9. The outlet angle of the blade is 3 less than inlet angle.
Steam flow rate is 6 kg/s. Draw the velocity diagrams and find the following.
(i) Change of Velocity of whirl
(ii) Axial thrust
(iii) Blade angles
(iv) Power developed.
Example 2:
Steam flows through the nozzle with a velocity of 450 m/s at a direction which is
inclined at an angle of 16 to the wheel tangent. Steam comes out of the moving
blades with a velocity of 100 m/s in the direction of 110 with the direction of
blade motion. The blades are equiangular and the steam flow rate is10 kg/s. Find:
(i)Power developed,
(ii)The power loss due to friction
(iii)Axial thrust
(iv) Blade efficiency and
(v) Blade coefficient.
Example 3:
An axial flow impulse sis team turbine has a mean rotor diameter of 0.55 m and
runs at 3300 rpm. The speed ratio is 0.45 the nozzle at rotor a inlet 22 such that
Vu1 is posotive The blade velocity coefficient is 0.91
Find (i) The rotor blade angles at inlet and outlet assuming
(a) The condition for maximum utilization
(b) The blades to be equiangular
(ii) The power output in each of the cases for a mass flow rate of 10 kg/s
(iii) The axial thrust in each cases
Example 3 :
Dry saturated steam at 10 atmospheric pressure is supplied to single rotor
impulse wheel, the condenser pressure being 0.5 atmosphere with the nozzle
efficiency of 0.94 and the nozzle angle at the rotor inlet is 18 to the wheel
plane. The rotor blades which moves with the speed of 450 m/s are
equiangular. If the coefficient of velocity for the rotor blades is 0.92, find
(i) The specific power output
(ii) (ii) The rotor efficiency
(iii) (iii) The Stage efficiency
(iv) (iv) Axial thrust
(v) (v) The direction of exit steam.
Analysis on Two Stages :
Condition of Maximum Efficiency for Velocity Compounded
Impulse Turbine (Curtis Turbine)
The speed and the angles should be so selected that the final
absolute velocity of steam leaving the second row is axial, so as to
obtain maximum efficiency. The tangential speed of blade for
both the rows is same since all the moving blades are mounted on
the same shaft.
Example :
The following data refers to a velocity compounded Impulse steam
turbine having two rows of moving blades and a fixed row between
them : Velocity of steam leaving the nozzle is 1200 m/s, nozzle
angle is 20 , blade speed is 250 m/s, blade angles of first moving
row are equiangular, blade outlet angle of the fixed blade is 25 .
Blade outlet angle of the second moving row is 30 . Friction factor
for all the rows is 0.9. Draw the velocity diagrams for a suitable
scale and calculate the power developed, axial thrust, diagram
efficiency for steam flow rate of 5000 kg/hr.
Example:
The velocity of steam at the exit of a nozzle is 440 m/s which is
compounded in an Impulse turbine by passing successively
through moving, fixed, and finally through a second ring of
moving blades. The tip angles of moving blades throughout the
turbine are 30 . Assume loss of 10% in velocity due to friction
when the steam passes over a blade ring. Find the velocity of
moving blades in order to have a final discharge of steam as axial.
Also determine the diagram efficiency.
Example:
In a curtis stage with two rows of moving blades, the rotor are
equiangular. The first rotor has an angle of 29 each while second
rotor has an angle of 32. The velocity of steam at the exit of
nozzle iss 530 m/s and the blade coefficients are 0.9 in the first,
0.95 in the stator and in the second rotor. If the absolute velocity
at the stage exit should be axial, find:
(i) Mean blade speed
(ii) The rotor efficiency
(iii) The power output for a flow rate of 32 kg/s
Reaction steam Turbines
Reaction Turbines :
The reaction turbine using now-a-days are of Impulse-
Reaction turbines. Pure reaction turbines are not in general
use.
 The expansion of steam and heat drop occur both in fixed
and moving blades. All reaction turbines are of axial flow type.
 In reaction turbine, steam continuously expands as it flows
over the blades. The effect of the continuous expansion during
the flow over the moving blades is to increase the relative
velocity of steam i.e. Vr2 >Vr1 ,
Degree of Reaction (R) :
The degree of reaction for reaction turbine stage is defined as
the ratio of enthalpy drop in the moving blades to the total
enthalpy drop in fixed and moving blades
Analysis on 50% Reaction (Parson's) Turbine :
When R = 0.5 , then V1 =Vr2 and V2 =Vr1 , also 1 = 2 & 2 = 1
Then the velocity become symmetric
Condition for Maximum Efficiency :
For maximum efficiency the following are assumed,
Reaction is 50%
 The moving and fixed blades are symmetrical
 The velocity of steam leaving the first stage is same as the
velocity of steam entering the next stage
i.e., there is no loss, V2 =V3
Example :1
The following data refers to a particular stage of a Parson's
reaction turbine. Speed of the turbine = 1500 RPM, Mean
diameter of the rotor = 1m, stage efficiency = 0.8, Blade outlet
angle = 20 , Speed ratio = 0.7, Determine the available isentropic
enthalpy drop in the stage.
Example:2
In a reaction turbine, the blade tips are inclined at 35 and 20 in
the direction of rotor. The stator blades are the same shape as
the moving blades, but reversed in direction. At a certain place in
the turbine, the drum is 1m diameter and the blades are 10 cm
high. At this place, the steam has a pressure of 1.75 bar and
dryness is 0.935. If the speed of the turbine is 250 RPM and the
steam passes through the blades without shock find the mass of
steam flow and power developed in the ring of moving blades.
Dm = 1 + 0.1 = 1.1m
U = 14.4 m/s
Af =  Dm h = 0.3456 m2
Vw = 45.45 m/s
Vf = 10.8 m/s
From Mollier Chart
corresponds to 17.5 bar
line and 0.935 dryness line
V = 0.96 m3/kg
m’ = 3.89 kg/s
P = 2.545 kW
Example:3
A reaction turbine has a drum diameter of 2.15m, the speed is
750 rpm and steam consumption is 14.5 kg/s. The height of
blades at a certain location is 16cm, while the discharge angle is
25 and the specific volume of steam is 4.071 m3/kg. estimate
the power developed in this particular ring and assuming turbine
efficiency of 75%, find the heat drop while the steam is passing
through this turbine stage.
Dm = 2.31 m ; U = 90.7 m/s ; Vf = 50.84 m/s
Vw = 203 m/s
h = 18.41 kJ/kg
P = 267 kW
h’ = 24.55 kJ/kg
Example:4
A twenty stage parson’s turbine receives steam at 15 bar and
300C and the steam leaves the turbine at 0.1 bar. The turbine
has a stage efficiency of 80% and reheat factor is 1.06. The total
power developed is 10658 kW. Find the steam flow rate.
Reheat Factor:
The ratio of summation of isentropic enthalpy drop for individual
stage to the total isentropic enthalpy drop as a whole
Assignments-III
Jan-2017
July-2016
Jan-2016
July-2015
Jan-2015

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Steam turbines, Shankarappa K

  • 1.
  • 2. Steam turbines use the steam as a working fluid. In steam turbines, high pressure steam from the boiler is expanded in nozzle, in which the enthalpy of steam being converted into kinetic energy. Thus, the steam at high velocity at the exit of nozzle impinges over the moving blades (rotor) which cause to change the flow direction of steam and thus cause a tangential force on the rotor blades. Due to this dynamic action between the rotor and the steam, thus the work is developed.
  • 3.
  • 4.
  • 5.
  • 6. Compounding is the method of obtaining reasonable tangential speed of rotor for a given overall pressure drop by using more than one stages. Compounding is necessary for steam turbines because if the tangential blade tip velocity greater than 400 m/s, then the blade tips are subjected to centrifugal stress. Due this, utilization is low hence the efficiency of the stage is also low. Compounding can be done by the following methods, namely, (i)Velocity compounding, (ii) Pressure compounding or Rateau stage (iii) Pressure-Velocity compounding and (iv) Impulse- Reaction staging. Compounding Of Steam Turbines
  • 7. Velocity Compounding (Curtis Stage) of Impulse Turbine :
  • 8.  This consists of set of nozzles, rows of moving blades (rotor) & a rows of stationary blades (stator). The function of stationary blades is to direct the steam coming from the first moving row to the next moving row without change in velocity. All the kinetic energy available at the nozzle exit is successively absorbed by all the moving rows &the steam is sent from the last moving row with low velocity to achieve high utilization.  The turbine works under this type of compounding stage is called velocity compounded turbine. e.g. Curtis stage steam turbine
  • 9. Pressure Compounded (Rateau Stage ) Impulse Turbine :
  • 10. A number of simple impulse stages arranged in series is called as pressure compounding.  In this case, the turbine is provided with rows of fixed blades which acts as a nozzles at the entry of each rows of moving blades.  The total pressure drop of steam does not take place in a single nozzle but divided among all the rows of fixed blade which act as nozzle for the next moving rows. Pressure compounding leads to higher efficiencies because very high flow velocities are avoided through the use of purely convergent nozzles.  For maximum utilization, the absolute velocity of steam at the outlet of the last rotor must be axially directed. It is usual in large turbines to have pressure compounded or reaction stages after the velocity compounded stage.
  • 12. Pressure drop from the chest pressure to the condenser pressure occurs at two stages.  First and second stage taken separately are identical to a velocity compounding  consists of a set of nozzles and rows of moving blades fixed to the shaft and rows of fixed blades to casing. The entire expansion takes place in the nozzles. The high velocity steam parts with only portion of the kinetic energy in the first set of the moving blades and then passed on to fixed blades where only change in direction of jet takes place without appreciable loss in velocity. This jet then passes on to another set of moving vanes where further drop in kinetic energy occurs.
  • 13. blade velocity coefficient or nozzle velocity coefficient. For Impulse turbine, in ideal conditions. If the losses are considered, then,
  • 14. Forces on the Blade and Work Done Tangential force due to change in whirl velocity or tangential component of absolute velocities Axial thrust due to change in axial velocity components
  • 15. Blade Efficiency or Diagram Efficiency : It is defined as the ratio of work done per kg of steam by the rotor to the energy available at the inlet per kg of steam. The Stage Efficiency : It is defined as “the ratio of work done per kg of steam by the rotor to the isentropic enthalpy change per kg of steam in the nozzle”
  • 16. Condition for Maximum Utilization Factor or Blade efficiency with Equiangular Blades for Impulse Turbine :
  • 17. Example 1 : A single stage Impulse turbine has a diameter of 1.5 m. and running at 3000 RPM. The nozzle angle is 20 . Speed ratio is 0.45. Ratio of relative velocity at the outlet to that at inlet is 0.9. The outlet angle of the blade is 3 less than inlet angle. Steam flow rate is 6 kg/s. Draw the velocity diagrams and find the following. (i) Change of Velocity of whirl (ii) Axial thrust (iii) Blade angles (iv) Power developed.
  • 18.
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  • 20. Example 2: Steam flows through the nozzle with a velocity of 450 m/s at a direction which is inclined at an angle of 16 to the wheel tangent. Steam comes out of the moving blades with a velocity of 100 m/s in the direction of 110 with the direction of blade motion. The blades are equiangular and the steam flow rate is10 kg/s. Find: (i)Power developed, (ii)The power loss due to friction (iii)Axial thrust (iv) Blade efficiency and (v) Blade coefficient.
  • 21.
  • 22. Example 3: An axial flow impulse sis team turbine has a mean rotor diameter of 0.55 m and runs at 3300 rpm. The speed ratio is 0.45 the nozzle at rotor a inlet 22 such that Vu1 is posotive The blade velocity coefficient is 0.91 Find (i) The rotor blade angles at inlet and outlet assuming (a) The condition for maximum utilization (b) The blades to be equiangular (ii) The power output in each of the cases for a mass flow rate of 10 kg/s (iii) The axial thrust in each cases
  • 23. Example 3 : Dry saturated steam at 10 atmospheric pressure is supplied to single rotor impulse wheel, the condenser pressure being 0.5 atmosphere with the nozzle efficiency of 0.94 and the nozzle angle at the rotor inlet is 18 to the wheel plane. The rotor blades which moves with the speed of 450 m/s are equiangular. If the coefficient of velocity for the rotor blades is 0.92, find (i) The specific power output (ii) (ii) The rotor efficiency (iii) (iii) The Stage efficiency (iv) (iv) Axial thrust (v) (v) The direction of exit steam.
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  • 26. Analysis on Two Stages : Condition of Maximum Efficiency for Velocity Compounded Impulse Turbine (Curtis Turbine) The speed and the angles should be so selected that the final absolute velocity of steam leaving the second row is axial, so as to obtain maximum efficiency. The tangential speed of blade for both the rows is same since all the moving blades are mounted on the same shaft.
  • 27.
  • 28. Example : The following data refers to a velocity compounded Impulse steam turbine having two rows of moving blades and a fixed row between them : Velocity of steam leaving the nozzle is 1200 m/s, nozzle angle is 20 , blade speed is 250 m/s, blade angles of first moving row are equiangular, blade outlet angle of the fixed blade is 25 . Blade outlet angle of the second moving row is 30 . Friction factor for all the rows is 0.9. Draw the velocity diagrams for a suitable scale and calculate the power developed, axial thrust, diagram efficiency for steam flow rate of 5000 kg/hr.
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  • 30. Example: The velocity of steam at the exit of a nozzle is 440 m/s which is compounded in an Impulse turbine by passing successively through moving, fixed, and finally through a second ring of moving blades. The tip angles of moving blades throughout the turbine are 30 . Assume loss of 10% in velocity due to friction when the steam passes over a blade ring. Find the velocity of moving blades in order to have a final discharge of steam as axial. Also determine the diagram efficiency.
  • 31.
  • 32. Example: In a curtis stage with two rows of moving blades, the rotor are equiangular. The first rotor has an angle of 29 each while second rotor has an angle of 32. The velocity of steam at the exit of nozzle iss 530 m/s and the blade coefficients are 0.9 in the first, 0.95 in the stator and in the second rotor. If the absolute velocity at the stage exit should be axial, find: (i) Mean blade speed (ii) The rotor efficiency (iii) The power output for a flow rate of 32 kg/s
  • 34. Reaction Turbines : The reaction turbine using now-a-days are of Impulse- Reaction turbines. Pure reaction turbines are not in general use.  The expansion of steam and heat drop occur both in fixed and moving blades. All reaction turbines are of axial flow type.  In reaction turbine, steam continuously expands as it flows over the blades. The effect of the continuous expansion during the flow over the moving blades is to increase the relative velocity of steam i.e. Vr2 >Vr1 ,
  • 35.
  • 36. Degree of Reaction (R) : The degree of reaction for reaction turbine stage is defined as the ratio of enthalpy drop in the moving blades to the total enthalpy drop in fixed and moving blades
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  • 38.
  • 39. Analysis on 50% Reaction (Parson's) Turbine : When R = 0.5 , then V1 =Vr2 and V2 =Vr1 , also 1 = 2 & 2 = 1 Then the velocity become symmetric
  • 40. Condition for Maximum Efficiency : For maximum efficiency the following are assumed, Reaction is 50%  The moving and fixed blades are symmetrical  The velocity of steam leaving the first stage is same as the velocity of steam entering the next stage i.e., there is no loss, V2 =V3
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  • 44.
  • 45.
  • 46. Example :1 The following data refers to a particular stage of a Parson's reaction turbine. Speed of the turbine = 1500 RPM, Mean diameter of the rotor = 1m, stage efficiency = 0.8, Blade outlet angle = 20 , Speed ratio = 0.7, Determine the available isentropic enthalpy drop in the stage.
  • 47.
  • 48. Example:2 In a reaction turbine, the blade tips are inclined at 35 and 20 in the direction of rotor. The stator blades are the same shape as the moving blades, but reversed in direction. At a certain place in the turbine, the drum is 1m diameter and the blades are 10 cm high. At this place, the steam has a pressure of 1.75 bar and dryness is 0.935. If the speed of the turbine is 250 RPM and the steam passes through the blades without shock find the mass of steam flow and power developed in the ring of moving blades.
  • 49. Dm = 1 + 0.1 = 1.1m U = 14.4 m/s Af =  Dm h = 0.3456 m2 Vw = 45.45 m/s Vf = 10.8 m/s From Mollier Chart corresponds to 17.5 bar line and 0.935 dryness line V = 0.96 m3/kg m’ = 3.89 kg/s P = 2.545 kW
  • 50. Example:3 A reaction turbine has a drum diameter of 2.15m, the speed is 750 rpm and steam consumption is 14.5 kg/s. The height of blades at a certain location is 16cm, while the discharge angle is 25 and the specific volume of steam is 4.071 m3/kg. estimate the power developed in this particular ring and assuming turbine efficiency of 75%, find the heat drop while the steam is passing through this turbine stage.
  • 51. Dm = 2.31 m ; U = 90.7 m/s ; Vf = 50.84 m/s Vw = 203 m/s h = 18.41 kJ/kg P = 267 kW h’ = 24.55 kJ/kg
  • 52. Example:4 A twenty stage parson’s turbine receives steam at 15 bar and 300C and the steam leaves the turbine at 0.1 bar. The turbine has a stage efficiency of 80% and reheat factor is 1.06. The total power developed is 10658 kW. Find the steam flow rate. Reheat Factor: The ratio of summation of isentropic enthalpy drop for individual stage to the total isentropic enthalpy drop as a whole