Simulation of unsteady viscous turbomachinery flowfields is presently impractical as a design tool due to the long run times required. Designers rely predominantly on steady-state simulations, but these simulations do not account for some of the important unsteady flow physics. Unsteady flow effects can be modeled as source terms in the steady flow equations. These source terms, referred to as Lumped Deterministic Stresses (LDS), can be used to drive steady flow solution procedures to reproduce the time-average of an unsteady flow solution. The goal of this work is to investigate the feasibility of using inviscid lumped deterministic stresses to model unsteady combustion hot streak migration effects on the turbine blade tip and outer air seal heat loads. The LDS model is obtained from an unsteady inviscid calculation. The inviscid LDS model is then used with a steady viscous computation to simulate the time-averaged viscous solution. The feasibility of the inviscid LDS model is demonstrated on a single-stage, three-dimensional, vane-blade turbine with a hot streak entering the vane passage at midpitch and midspan. The steady viscous solution with the LDS model is compared to the time-averaged viscous, steady viscous, and time-averaged inviscid computations. The LDS model reproduces the time-averaged viscous temperature distribution on the outer air seal to within 2.3 percent, while the steady viscous has an error of 8.4 percent, and the time-averaged inviscid calculation has an error of 17.2 percent. The solution using the LDS model is obtained at a cost in CPU time that is 26 percent of that required for a time-averaged viscous computation. [S0889-504X(00)00601-2]

1.
Saxer
,
A. P.
, and
Felici
,
H. M.
,
1996
, “
Numerical Analysis of Three-Dimensional Unsteady Hot Streak Migration and Shock Interaction in a Turbine Stage
,”
ASME J. Turbomach.
,
118
, pp.
268
277
.
2.
Dorney
,
D. J.
,
Davis
,
R. L.
, and
Edwards
,
D. E.
,
1992
, “
Unsteady Analysis of Hot Streak Migration in a Turbine Stage
,”
J. Propul. Power
,
8
, No.
2
, pp.
520
529
.
3.
Rai, M. M., and Dring, R. P., 1990, “Navier-Stokes Analyses of the Redistribution of Inlet Temperature Distortions in a Turbine,” J. Propul. Power, 6.
4.
Takahashi, R., and Ni, R. H., 1991, “Unsteady Hot Streak Simulation Through 1-12 Stage Turbine,” AIAA Paper No. 91-3382.
5.
Adamczyk, J. J., 1985, “Model Equation for Simulating Flows in Multistage Turbomachinery,” ASME Paper No. 85-GT-226.
6.
Davis, R. L., Shang, T., Buteau, J., and Ni, R. H., 1996, “Prediction of 3-D Unsteady Flow in Multi-stage Turbomachinery Using an Implicit Dual Time-Step Approach,” AIAA Paper No. 96-2565.
7.
Ni
,
R. H.
,
1981
, “
A Multiple Grid Scheme for Solving the Euler Equations
,”
AIAA J.
,
20
, No.
11
, pp.
1565
1571
.
8.
Ni, R. H., and Bogoian, J. C., 1989, “Predictions of 3-D Multi-Stage Turbine Flow Fields Using a Multiple-Grid Euler Solver,” AIAA Paper No. 89-0203.
9.
Ni, R. H., and Sharma, O. P., 1990, “Using a 3-D Euler Flow Simulation to Assess Effects of Periodic Unsteady Flow Through Turbines,” AIAA Paper No. 90-2357.
10.
Baldwin, B. S., and Lomax, H., 1978, “Thin Layer Approximation and Algebraic Model for Separated Turbulent Flows,” AIAA Paper No. 78-257.
11.
Giles
,
M.
,
1990
, “
Nonreflecting Boundary Conditions for Euler Equation Calculations
,”
AIAA J.
,
28
, No.
12
, pp.
2050
2058
.
12.
Sondak, D. L., Dorney, D. J., and Davis, R. L., 1996, “Modeling Turbomachinery Unsteadiness With Lumped Deterministic Stresses,” AIAA Paper No. 96-2570.
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