Abstract
A two- and three-dimensional code solving the Reynolds-averaged compressible Navier-Stokes equations has been developed and successfully used for computation of the steady flow field in an aerodynamic diffuser of a high loaded centrifugal compressor. For the purpose of comparison the turbulence model of Baldwin and Lomax with and without an extension of Goldberg and Chakravarthy [1] for the determination of separated flow regions and the two equation k — ε model according to Kunz and Lakshminarayana [2, 3] are applied to compute the flow field of the diffuser on several operating points with the two-dimensional code. The three-dimensional solver in addition with the extended and unextended Baldwin-Lomax model has been applied to ascertain the three-dimensional flow field on the working point with the largest separation zone in the two-dimensional case. For comparison measured pressure distributions [4] of the examined operating points are presented likewise.
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Abbreviations
- D,ε :
-
functions of the k — ε model
- E :
-
total specific internal energy
- \(\vec{E}\) :
-
flux vector in ξ-direction
- f 2 ,f µ :
-
functions of the k — ε model
- F Kleb :
-
Klebanoff intermittency function
- F Wake :
-
wake function
- \(\vec{F}\) :
-
flux vector in ŋ-direction
- G :
-
Gaussian-distribution
- J :
-
Jacobian
- k :
-
turbulent kinetic energy(=k*/(p/ρ) * tot,∞ )
- n :
-
wall distance
- p :
-
static pressure (= p*/p * tot,∞ )
- P :
-
production rate of k
- Pr :
-
Prandtl-number
- q :
-
Cartesian component of heat transfer
- \(\vec{Q}\) :
-
vector of variables of state
- r :
-
radius (= r*/r *DE )
- r o :
-
impeller exit radius
- Re :
-
Reynolds-number\(\left( ={{r}^{*}}DE\sqrt{\left( p\rho \right)_{tot,\infty }^{*}}/\mu _{l,\infty }^{*} \right)\)
- R T :
-
local Reynolds-number
- \(\vec{S}\) :
-
source term vector
- t :
-
time \(\left( ={{t}^{*}}\sqrt{\left( p/\rho \right)_{tot,\infty }^{*}/r_{DE}^{*}} \right)\)
- Tu :
-
turbulence rate
- u :
-
velocity in x-direction \(\left( ={{u}^{*}}/\sqrt{\left( p/\rho \right)_{tot,\infty }^{*}} \right)\)
- u i :
-
velocity related to i-direction
- u s :
-
velocity-scale
- U ∞ :
-
mean velocity at diffuser inlet
- v :
-
velocity in y-direction (see u)
- w :
-
velocity in z-direction (see u)
- \(\vec{w}\) :
-
velocity vector
- x,y,z :
-
Cartesian coordinates (related to r * DE )
- x i :
-
Cartesian coordinate related to i-direction
- δ ij :
-
Kronecker-symbol
- ϵ :
-
dissipation rate of k
$$\left( ={{\varepsilon }^{*}}r_{DE}^{*}/{{\left[ \left( p/\rho \right)_{tot,\infty }^{*} \right]}^{1.5}} \right)$$ - k :
-
isentropic coefficient
- µ l :
-
dynamic viscosity (= (p/ρ)2/3)
- µ t :
-
turbulent viscosity
- w :
-
vorticity-scale
- ρ :
-
density (= ρ*/ρ * tot,∞ )
- τ ij :
-
Cartesian stress tensor component
- τ w :
-
wall shear stress
- ξ,ŋ,ς :
-
generalized curvilinear coordinates
- ξ x , ŋ x ..:
-
partial derivatives ξ, ŋ,.. to x,y,..
- ∼ :
-
density weighted value
- − :
-
time averaged value
- + :
-
modified value
- *:
-
dimensionalized value
- c :
-
inviscid
- DE :
-
diffuser exit
- i,j,k :
-
pointer related to x,y or z axis
- v :
-
viscous
- K :
-
suction duct upstream the compressor
- tot :
-
total value
- w :
-
wall
- ∞:
-
diffuser inlet
References
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Heinrich, M., Teipel, I. (1998). Flow Simulation in an Aerodynamic Diffusor of a High Loaded Radial Compressor using Different Turbulence Models. In: Rath, H.J., Egbers, C. (eds) Advances in Fluid Mechanics and Turbomachinery. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-72157-1_4
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DOI: https://doi.org/10.1007/978-3-642-72157-1_4
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