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An Exclusive Conservation Equation for Ideal Turbo-machines P M V Subbarao Professor Mechanical Engineering Department Invention of New Property for CVs with Work ... – PowerPoint PPT presentation

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Title: An%20Exclusive%20Conservation%20Equation%20for%20Ideal%20Turbo-machines


1
An Exclusive Conservation Equation for Ideal
Turbo-machines
  • P M V Subbarao
  • Professor
  • Mechanical Engineering Department

Invention of New Property for CVs with Work
Transfer.
2
Conservation of Rothalpy
or
  • A cornerstone of the analysis of steady, relative
    flows in rotating systems has, for many years,
    been the immutable nature of the fluid mechanical
    property rothalpy.
  • "In a moving passage the rothalpy is therefore
    constant provided
  • the flow is steady in the rotating frame
  • no friction from the casing
  • there is no heat flow to or from the flow.

3
Novel Idea for Creation of Variety
Ideas for creation of a variety in turbo-machine.
4
Blade Velocity Vs Tangential Component of Fluid
Velocity
In maridional plane at mean radius of rotor
5
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6
Relative Angular Velocity
Constant in an ideal turbo-machine
7
For stator Ublade 0
For rotors
For a true axial flow machines Ublade constant
8
Complex Geometrical Features of A Turbo-Machinne
9
A turbomachine working with incompressible fluid
will be isothermal and hence U(T) is constant
throughout the machine.
For an Ideal Hydro Power Plant
10
A Two-Way Welfare for the Globe
11
Hydro Electric Plant with High Heads
12
Option for High Head Hydro Station
In an ideal Penstock
In an ideal Nozzle
In an ideal turbo-machine
13
Vri
Vri
U
Vre
14
More Ideas
For an Ideal Hydro Power Plant
15
Turbo-machines working with Vapors/Gas
For an ideal gas
16
For simple compressible fluid Like Inert Gas
17
The Fourth Generation Nuclear Power Plants
18
An Advanced Nuclear Power Plant
19
Geometrical Details along the Third Direction
  • True flow through a turbo-machinery is
    three-dimensional.
  • Flow and tangential flow velocities are very
    important for better operation of a
    turbo-machine.
  • The third component, which is normal to flow and
    tangential direction is in general of no use.
  • This direction can better represented as blade
    height direction.

20
Third Direction of an Axial Flow Turbo-Machines
  • The third direction in an axial flow machine is
    the radial direction.
  • The direction of Centrifugal forces!
  • Strong centrifugal forces are exerted on blades
    fluid in radial direction.
  • The centrifugal field distorts the flow velocity
    profiles considerably.
  • Fluid particles tend to move outwards rather
    than passing along cylindrical stream surfaces as
    classically assumed.
  • Particularly in tall blade (low hub tip) ratio
    designs.
  • An approach known as the radial equilibrium
    method, widely used for three-dimensional design
    calculations in a an axial flow machine.

21
Radial Equilibrium Theory of Turbo-machines
  • P M V Subbarao
  • Professor
  • Mechanical Engineering Department

A Model for Stable Operation of A Machine A
guiding equation for distribution of load along
blade length .
22
Radial Variation Blade Geometry
23
Radial Equilibrium Theory
  • Assumes that flow is in radial equilibrium before
    and after a blade row.
  • Radial adjustment takes place through the row.
  • More important for Axial Flow Machines.

24
Radial Equilibrium Analysis
The centrifugal force (rrdrdq)w2r Vq rw
The centrifugal force is
The pressure force on the element
25
If the two forces are the only ones acting
(viscous and other effects neglected), the
particle will move at constant radius if
26
Equilibrium Condition for A Rotating Fluid
An equivalent equation for compressible flow can
be developed by using the following
thermodynamic relation
The radial variation of whirl velocity should be
according to above equation. How to implement on
a machine?
27
Total Energy Equation for A Rotating Fluid
Stagnation enthalpy should conserve, as there are
not interactions with rotor at inlet or exit.
28
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29
Radial component of velocity should be constant
(zero) along radial direction for radial
equilibrium of flow.
30
Constant in a turbo-machine along meridonial
Plane
Stagnation enthalpy is Constant in a
turbo-machine along radial direction at intake
and discharge.
31
Twisted Blades for Large Turbines
32
Lessons from Nature
THE VORTEX
  • In the case of a vortex, the flow field is purely
    tangential.

The complex potential function
33
General Rules for Selection of Whirl Component
  • Free Vortex Whirl
  • Forced Vortex Whirl

34
More complex Models
  • Weighted mean of free and forced vortices

Inlet
Exit
  • General Whirl Distribution

35
Radial Variation of Flow Velocity in Real Machine
Discharge
Intake
36
Radial Variation of Whirl Velocity
Intake
Discharge
37
Radial Variation of Mass flow rate
Intake
Discharge
38
Design of Compact Machine
39
Kaplan Turbine
40
DESIGN OF THE BLADE
90 or better in efficiency
Two different views of a blade
41
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42
Basic Rules for Design of An Ideal Turbo-machine
43
Basic Rules for Design of An Ideal Turbo-machine
  • Enumerate the details of source or demand.
  • Calculate Specific speed and identify the
    fundamental concept of operation.
  • X1 (Impulse)X2(Reaction)(1-X1-X2)(centrifugal)
  • Y1 (Radial)(1-Y1 )(Axial)
  • Design of Flow Path using Conservation of
    rothalpy.
  • Design blade cascade using conservation of mass
    and momentum.
  • Design of Radial Geometry using Radial
    Equilibrium Theory.
  • A design of an Ideal Machine..
  • Real Performance will be lower

44
Basic Rules for Design of A Real Turbo-machine
  • More customized rules along with the general
    rules.
  • Customized rules are specific to application
  • Power consumption Vs Power Generation.
  • Radial Vs Axial.
  • Incompressible flow Vs Compressible.
  • In Reality
  • Design analysis of A Real Machine is an Exclusive
    Scientific Art.
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