Article | REF: BM4302 V1

Rotodynamic pumps - Operating mode

Authors: Robert REY, Farid BAKIR, Jean POULAIN

Publication date: January 10, 2012 | Lire en français

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    Overview

    ABSTRACT

    The flow inside a turbomachine is extremely complex as it is governed by time and three space variables. It cannot be analyzed through simple means of calculation and it is also difficult to describe and explain. It is therefore essential to simplify the presentation of this flow prior to studying it. Thus, at a given point or surface, the pressure and the different components of the velocity vector are considered as time-averaged values. In addition, the reasoning is based on a uniform flow depending on a single space variable.Although these simplified approaches are incomplete, as they do not integrate all the aspects of the way turbomachines function, they have nonetheless facilitated the rapid development of these pumps.

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    AUTHORS

    • Robert REY: Arts et Métiers engineer - Professor, DynFluid Laboratory – Arts et Métiers ParisTech

    • Farid BAKIR: Engineer École polytechnique d'Alger - Professor, DynFluid Laboratory – Arts et Métiers ParisTech

    • Jean POULAIN: Engineer from the École supérieure d'électricité - Former scientific advisor to the PROFLUID Association - Alumnus of the Von Karman Institute

     INTRODUCTION

    The article "Rotodynamic pumps" is the subject of several articles:

    • [BM 4 300] Presentation. Description ;

    • –[BM 4 302] How it works ;

    • [BM 4 303] Similarity and design of centrifugal pumps ;

    • [BM 4 304] Propeller pump project ;

    • [BM 4 306] Special mechanical problems ;

    • [BM 4 308] Operations ;

    • [BM 4 314] Cavitation resistance of rotodynamic pumps.

    The subjects are not independent of each other. Readers may need to refer to other articles.

    The flow inside a turbomachine is always highly complex. It is unsteady and three-dimensional, i.e. it depends on time and three space variables. Without prior simplification, it can neither be analyzed by simple means of calculation, nor even described or explained by ordinary means of communication.

    The flow is therefore represented by fictitious quantities. At a given point, the pressure and velocity components considered are time-averaged values. On a given surface, for example at the outlet of a centrifugal impeller, the pressures and velocities considered are values averaged over the entire surface.

    We reason as if the flow were uniform and depended on a single space variable. In the case...

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