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Handbook of Turbomachinery Second Edition Revised - Ventech!

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streamwise diffusion terms are considered negligible. This assumption is<br />

valid for thin viscous layers, but is not appropriate for flows that contain<br />

substantial recirculation zones, or other significant viscous structures that<br />

would produce measurable streamwise diffusion.<br />

Other levels <strong>of</strong> approximation <strong>of</strong>fer even simpler representations <strong>of</strong> the<br />

governing equations; however, such flow models are not general enough to<br />

encompass many <strong>of</strong> the flows encountered in high-performance turbomachinery<br />

components. Although the use <strong>of</strong> approximations to the governing<br />

equations <strong>of</strong>fers benefits in terms <strong>of</strong> equation simplicity and, therefore,<br />

solution speed, the design tool that employs such a simplified model<br />

sacrifices generality. Often, the benefits <strong>of</strong> having a more general CFD<br />

analysis tool will far outweigh the benefits <strong>of</strong> a faster tool that is only<br />

appropriate over a subset <strong>of</strong> the expected flow conditions.<br />

The solution <strong>of</strong> the governing equations is performed over a finite<br />

space, on which a computational grid has been imposed. In order to<br />

properly model the flow physics within this space, a set <strong>of</strong> appropriate<br />

boundary conditions must be specified for the governing equations. Three<br />

different types <strong>of</strong> spatial boundaries may be identified for typical<br />

turbomachinery components: (1) wall boundaries, (2) inlet and exit<br />

boundaries, and (3) periodic boundaries.<br />

Wall boundaries consist <strong>of</strong> blade surfaces, passage end walls, or the<br />

solid surfaces <strong>of</strong> other objects in the flow path. These boundaries may be<br />

rotating, nonrotating, or a combination <strong>of</strong> both. For solid walls, a zerorelative-velocity<br />

or no-slip condition is appropriate. Thermal boundary<br />

conditions must also be considered, through the specification <strong>of</strong> a wall<br />

temperature or a normal temperature gradient.<br />

The most natural form <strong>of</strong> the inlet and exit boundary conditions is used<br />

to set the mass flow rate, by specifying both total pressure and temperature,<br />

along with flow angle or tangential velocity, upstream, and static pressure at<br />

the downstream boundary. Depending on the type <strong>of</strong> turbulence model<br />

selected, distributions <strong>of</strong> turbulent kinetic energy or some similar property at<br />

the inlet would also be required. The inlet and exit boundaries should be<br />

placed far enough away from the blade row that they are not influenced by<br />

its presence. Typically, this is achieved by positioning the boundaries<br />

anywhere from 50% to 100% <strong>of</strong> the blade chord upstream and downstream<br />

<strong>of</strong> the blade row. The distribution <strong>of</strong> inlet conditions may include spanwise<br />

variations, or possibly both spanwise and tangential variations, if the<br />

tangential distribution has the same period as the pitch <strong>of</strong> the solution space.<br />

Modeling <strong>of</strong> nonperiodic inlet conditions, as for inlet distortion, would<br />

essentially require that the solution space extend over the entire annulus.<br />

Periodic boundaries upstream and downstream <strong>of</strong> the blade row are<br />

used to model the repetitive nature <strong>of</strong> the flow conditions from one blade<br />

Copyright © 2003 Marcel Dekker, Inc.

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