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IJSRD - International Journal for Scientific Research & Development| Vol. 3, Issue 03, 2015 | ISSN (online): 2321-0613
All rights reserved by www.ijsrd.com 839
Non-Dimensional Aerodynamic Design of Centrifugal Compressor for
Small Scale Samkit V Shah
1 Prof. Nilesh R.Sheth
2 Prof. Samip P.Shah
3
1ME Student
2,3Professor
1Department of Energy Engineering 1,2
GEC Valsad 3
C.K.P.C.E.T SuratAbstract— This paper investigates the development of a
preliminary design method for centrifugal compressors. The
analysis and design of Turbo-machines, at any level of
sophistication, must ultimately be based on an
understanding of the thermodynamics and fluid mechanics
processes which take place in the machine. On the simplest
level a preliminary design may consist of no more than the
application of the basic equations to estimate the magnitude
of overall design parameters, while on more complex level
the design methods will attempt to simulate more closely the
actual flow. The present work describes the simplified
approach to optimum design of centrifugal compressor stage
with the help of fundamental equations, which describe
thermodynamics, and aero-fluid dynamic flow process in
Turbo-machines.
Key words: Conceptual Design for Centrifugal Compressor
Impeller, aero-fluid dynamic flow
NOMENCLATURE:
1) SYMBOLS
A- Flow area section of impeller, diffuser & volute channels
a -Speed of sound
C- Absolute velocity of gas (Air)
W- Relative velocity of gas with respect to rotating element
D2 -Impeller exit (tip) diameter
i -Blade incidence angle
Mu -Blade Mach number
M, M’- Absolute & Relative Mach number
m -Mass flow rate
N - Rotational speed of Impeller
P - Fluid static pressure
PR - Stage total pressure ratio
Po - Fluid Stagnation pressure
R - Universal gas constant, Radius
tb - Impeller blade thickness
U2 -Blade tip speed
x- Meridional (axial) distance from axis of rotation
Zb - Number of Impeller blades
z -Axial meridional distance along axis of rotation
SPECIAL CHARACTERS
α - Absolute flow angle w.r.t meridional (flow) direction
β -Relative flow angle w.r.t flow direction
βB -Blade angle
λ -Work input coefficient
γ -Isentropic index for air
ν -Impeller eye hub to shroud diameter ratio
μ -Slip factor
η -Efficiency
φ -Flow co-efficient
2) SUBSCRIPT
I -Impeller Total to Total
S -Stage Total to Total
01-Stagnation state at inlet to eye
02 -Stagnation state at impeller exit
1 -Static state at impeller eye
2 -Static state at impeller exit
1s - State at shroud of impeller eye inlet
1h -State at hub of impeller eye inlet
1m -State at mean section of impeller eye inlet
a -Axial meridional component
m -Radial meridional component
θ -Tangential component
I. INTRODUCTION
Centrifugal compressor, also called radial compressor, are
critical equipment in a wide variety of application in the
chemical process industries, power plant etc. As their name
suggest, their primary process is to compress a fluid in to
smaller volume while simultaneous increasing pressure and
temperature of fluid. In other words, compressor accepts a
mass of gas at some initial pressure and temperature and rise
pressure and temperature of a gas. A Solid foundation for
turbo machinery design must comprise basic fundamentals
and useful experience. Both the basic principles of fluid
mechanics and thermodynamics on the one hand and
appropriate design data on the other hand are essential. If
these two resources are utilized effectively, very fine design
can be prepared for new application. There are, however
probably as many different design techniques as there are
designers in the world. Each designer undoubtedly uses
similar basic principles with a different combination of
experimental data to achieve the desire result.
II. CONCEPTUAL DESIGN FOR CENTRIFUGAL COMPRESSOR
IMPELLER
The main requirement from an impeller design procedure is
the computation of the overall principal dimensions and the
inlet and discharge blade angles. Impeller design procedure
is carried out applying non dimensional parameters
thermodynamic correlation which disregard actual size of
machine and more general compared to dimensional
quantities.
A. Impeller Design Steps:
Impeller design has been accomplished systematically for
complete control of aerodynamic parameters within
optimum recommended range. Input parameter are as
follows
Power (P)
Stagnation Pressure ratio (PR) from 1.5 to 5 bar[9]
Gas constant (R=287 kJ/kg. K)
Specific heat ratio (ϒ=1.4)
At inducer eye hub to shroud diameter ratio
(D1h/D1s) from 0.3 to 0.6[9]
shroud inlet diameter to Outlet diameter (D1s/D2)
from 0.4 to 0.9[9]
Impeller Total to Total Efficiency (ηI)
Non-Dimensional Aerodynamic Design of Centrifugal Compressor for Small Scale
(IJSRD/Vol. 3/Issue 03/2015/203)
All rights reserved by www.ijsrd.com 840
Stage Total to Total Efficiency (ηS) Inlet blade angle at shroud (β1s) from 560 to 640
[9]
Inlet absolute Flow angle (α1)
outlet Blade angle (β2 ) from 00 to -600 [9]
outlet absolute flow angle (α2) from 600 to 700 [9]
1) Step: 1 Determination of Blade Mach number (Mu)
It is governing parameter to decide the size and rotational
speed of impeller. Correlation between Mu and stagnation
pressure ratio is given as
For radial impeller βB2 = 0o, So λ=μ= 0.8 to 0.9
[3]
For high speed compressor developing high
pressure ratio, maximum allowable value of Mu would be
under 2.[4]
2) Step 2: Determination of stagnation temperature
ratio and pressure ratio (To2/T01 & P02/P01)
Generally, inlet stagnation condition is known to
designer. So knowledge of Mu gives the value of
developed stage total stagnation temperature.
Fig. 2.1: Main Component Of Centrigugal Compressor With
Velocity Triangle At Inlet And Exit[9]
3) Step 3: Determination of Absolute Impeller Exit
Mach number (M2) It depends on Mu and absolute
exit flow angle α2.
Fig. 2.2: Velocity Triangle At Outlet
[5]
Johnston and Dean (1966) showed that an optimum
swirl angle α2, for design purposes, lies between 63 to 68
degrees. Similarly Rodger and Sapiro (1972) considered the
optimum flow angles to lie between 60 to 70 degrees w.r.t
radial direction. [9]
4) Step 4: Determination of Relative outlet Mach
number ( ) at shroud
'
2M
Non-Dimensional Aerodynamic Design of Centrifugal Compressor for Small Scale
(IJSRD/Vol. 3/Issue 03/2015/203)
All rights reserved by www.ijsrd.com 841
5) Step 5: Determination of absolute and Relative
inlet Mach number ( M1s & ) at shroud
Fig. 2.3: Inlet Velocity Triangle At Hub Shroud And
Mean[5]
6) Step 6: Determination of Non-dimensional mass
flow rate, flow co-efficient Impeller Blade height
to outlet radius ratio.
Flow co-efficient:
Non-dimensional Mass flow rate ratio:
In actual case blade height at impeller exit (b2) is
higher than above calculated value due to consideration of
hub thickness of each vane, therefore let actual blade height
be found assuming b2 = 1.1 b2.
7) Step 7: Now specify the mass flow rate and inlet
stagnation condition to convert the Non-
dimensional geometry of impeller in to absolute
dimension
Density at inlet of impeller
Sound velocity at inlet
Outlet flow area from impeller
Outlet radius of impeller
s1
'M
Non-Dimensional Aerodynamic Design of Centrifugal Compressor for Small Scale
(IJSRD/Vol. 3/Issue 03/2015/203)
All rights reserved by www.ijsrd.com 842
Width of impeller blade flow passage at outlet
Inlet shroud radius
Inlet hub radius
8) Step 8: Determination of Impeller blade numbers
and maximum hub thickness (Zb, tbh)
Various correlations for estimation of slip factor
(μ) have been developed by many researchers
applied for wider range of impeller vane no.(Zb),
vane exit angle (βB2) and radius ratio.
Stodala equation:[13,14]
Where βB2 = 0 for radial vane
Weisner equation[10]
Stanitz equation:[10,14]
Impeller blade hub thickness (tbh) can be
determined from exit flow area correlation based
on blade thickness consideration as,
Where, b2t = 1.1b2
9) Step 9: Impeller geometry for Centrifugal
Compressor Vanes [11]
Wallace (1975) represented impeller geometry by
means of Lame Ovals equation of general form:
Where, x is radius (r) for hub or shroud lines for
radial blade impeller. The coefficients a, b, c and d are
obtained from the end conditions (x1, z1) and (x2, z2) for
shroud and hub curve with assumption and axial inlet and
radial exit blade. p and q are indices and can be varied to get
series of analytic curves.
From an aerodynamic standpoint, Birdi [5] has
suggested correlation for optimal axial length- tip
diameter ratio.
Where, K1 = 0.28 and K2 = 0.8
For hub, a = -Z1h, b = Z2h (L)-Z1h, c = -X2h, d =
X1h- X2h
For shroud, a = -Z1s, b = Z2s-Z1s, c = -X2s, d = X1s-
X2s;
p 2 3 2 3
q 1 1 2 2
p = 3 and q = 2 value is applied as it gives slight
long axial path inducer without prewhirl.
Fig. 2.4: Impeller meridional geometry
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(IJSRD/Vol. 3/Issue 03/2015/203)
All rights reserved by www.ijsrd.com 843
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