Principles of Turbomachinery
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1 Principles of Turbomachinery
2 To J. M. T.
3 Principles of Turbomachinery R. K. Turton Lecturer in Mechanical Engineering Loughborough University of Technology London New York E. & F. N. Spon
4 ISBN First published 1984 by E. & F. N. Spon Ltd 11 New Fetter Lane, London EC4P 4EE Published in the USA by E. & F. N. Spon 733 Third Avenue, New York NY R. K. Turton 1984 Softcover reprint ofthe hardcover 1st edition 1984 J. W. Arrowsmith Ltd, Bristol ISBN (ebook) DOI / This title is available in both hardbound and paperback editions. The paperback edition is sold subject to the condition that it shall not, by way of trade or otherwise, be lent, re-sold, hired out, or otherwise circulated without the publisher's prior consent in any form of binding or cover other than that in which it is published and without a similar condition including this condition being imposed on the subsequent purchaser. All rights reserved. No part of this book may be reprinted, or reproduced or utilized in any form or by any electronic, mechanical or other means, now known or hereafter invented, including photocopying and recording, or in any information storage and retrieval system, without permission in writing from the Publisher. British Library Cataloguing in Publication Data Turton, R. K. Principles of turbomachinery. 1. Turbomachines-Fluid dynamics 2. Thermodynamics I. Title 621.8'11 TJ267 ISBN Library of Congress Cataloging-in Publication Data Turton, R. K. (Robert Keith) Principles of turbomachinery. Bibliography: p. Includes index. 1. Turbomachines. I.Title. TJ267.T ISBN
5 Contents Preface Symbols used: their meaning and dimensions 1 Fundamental principles 1.1 Introduction 1.2 Euler equation 1.3 Reaction 1.4 Application to a centrifugal machine 1.5 Application to axial pumps and turbines Axial pump or fan Axial turbine stage 1.6 Alternative operating modes 1.7 Compressible flow theory General application to a machine Compression process Expansion process 1.8 Shock wave effects 1.9 Cavitation Phenomenon of cavitation Suction pressure and NPSH (or NPSE) 1.10 Illustrative examples Radial outflow machine (pump) Axial pump and turbine Compressible flow problem Example of an NPSE calculation 2 Principles and practice of scaling laws 2.1 Introduction 2.2 Performance laws Page IX xi
6 vi Contents 2.3 Concept of specific speed 2.4 Cavitation parameters 2.5 Scale effects in incompressible units Hydraulic machines Cavitation problems Fans and blowers 2.6 Scale effects in compressible machines 2.7 1llustrative examples Similarity laws applied to a water turbine Compressor performance prediction problem 3 Principles of axial flow machines 3.1 Introduction 3.2 Wing theory 3.3 Isolated aerofoil data 3.4 Cascade data 3.5 Radial equilibrium theories 3.6 Actuator disc approach 3.7 Stall and surge effects Introduction Stalling offans and compressor stages Surge and stall in compressors 4 Principles of radial and mixed flow machines 4.1 Introduction 4.2 One-dimensional approach 4.3 Two-dimensional approach Passage shapes Impeller or rotating cascade 4.4 Three-dimensional problem 4.5 Discussion of theoretical approaches to analysis and design 5 Centrifugal machines 5.1 Introduction 5.2 Inlet or intake systems 5.3 Impeller Eye or inducer section Impeller design
7 5.4 Outlet systems Vaneless diffuser Volute or spiral casing Vaned diffuser systems 5.5 Thrust loads due to hydrodynamic effects Radial thrust forces Axial thrust loads 6 Axial machines for incompressible ftow 6.1 Introduction 6.2 Axial flow pumps and fans 6.3 Axial water turbines 6.4 Forces on blades and their implications for design Static blades Rotating blades 6.5 Concluding remarks 7 Axial turbines and compressors for compressible ftow 7.1 Introduction 7.2 Approach to axial compressor principles 7.3 Axial turbine principles General principles Partial admission problem 7.4 Other problems 8 Radial flow turbines 8.1 Introduction 8.2 Water turbines 8.3 Radial inflow gas turbine Nozzle systems Rotor geometry Worked example 8.4 Ljungstrom or radial outflow turbine Contents vii Cavitation and other matters 9.1 Introduction 9.2 Effects of cavitation on machines Surface damage and erosion effects Hydrodynamic effects
8 viii Contents Thermodynamic effects on pump cavitation Inducer Problems involved in special pumping applications Gas suspension problems Solids pumping Pumping viscous fluids Pumped storage systems Some comments on output control of rotating machines 185 References 188 Additional bibliography 195 Index 196
9 Preface This text outlines the fluid and thermodynamic principles that apply to all classes of turbomachines, and the material has been presented in a unified way. The approach has been used with successive groups of final year mechanical engineering students, who have helped with the development of the ideas outlined. As with these students, the reader is assumed to have a basic understanding of fluid mechanics and thermodynamics. However, the early chapters combine the relevant material with some new concepts, and provide basic reading references. Two related objectives have defined the scope of the treatment. The first is to provide a general treatment of the common forms of turbo machine, covering basic fluid dynamics and thermodynamics of flow through passages and over surfaces, with a brief derivation of the fundamental governing equations. The second objective is to apply this material to the various machines in enough detail to allow the major design and performance factors to be appreciated. Both objectives have been met by grouping the machines by flow path rather than by application, thus allowing an appreciation of points of similarity or difference in approach. No attempt has been made to cover detailed points of design or stressing, though the cited references and the body of information from which they have been taken give this sort of information. The first four chapters introduce the fundamental relations, and the succeeding chapters deal with applications to the various flow paths. The last chapter covers the effects of cavitation, solids suspensions, gas content and pumped storage systems, and includes a short discussion of the control of output. These topics have been included to highlight the difficulties encountered when the machine is not dealing with a clean Newtonian fluid, or in systems where problems are posed that can only be solved by compromise. Chapter 5 discusses all the conventional centrifugal machines, covering in a uniform manner the problems faced with liquids and gases: since high pressure rise machines have a number of stages, the ways in which fluid is
10 x Preface guided from stage to stage are introduced. Thrust load problems are described and the common solutions adopted are outlined. The discussion of axial machines has been divided between two chapters, as the technologies of pumps, fans and water turbines are similar but differ from those used in compressible machines. Radial flow turbines form the subject matter of Chapter 8, and the common designs in use in industry and in turbochargers are discussed. Worked examples have been included in all chapters but the last. They are intended to provide illustration of the main points of the text, and to give a feel for both the shape of the velocity triangles and the sizes of the velocity vectors that normally apply. They are of necessity simplified, and must not be regarded as representing current practice in all respects. No problems for student solution have been provided. Teachers normally prefer to devise their own material, and may obtain copies of examination qu~stions set by other institutions if they wish. As a matter of course the SI system of units has been used throughout, except in some diagrams. To assist the reader, a list of symbols used in the early chapters, together with a statement of the conventional dimensions used, follows the Preface. As far as possible the British Standard on symbols has been followed but, where current and hallowed practice dictates the use of certain symbols, these have been used; it is hoped that where the same symbol appears to have different meanings the context makes the usage clear. The material presented forms the core of a lecture course of about 46 hours, and the author hopes that in the inevitable distillation no ambiguities have occurred. He will be grateful for comments and suggestions, as he is still an earnest 'seeker after truth'. Finally, it is necessary to offer some words of thanks, especially to Mrs Redman, who ensured that the diagrams were clear, to Mrs Smith and Mrs McKnight, who helped with the typing, and finally to my dear wife, who was so patient and who ensured that the proof-reading was done properly.
11 Symbols used: their meaning and dimensions a acoustic velocity b passage height C L lift coefficient (Table 3.1) CD drag coefficient (Table 3.1) C p pressure rise coefficient (Equation 3.15) Cp specific heat at constant pressure Cy specific heat at constant volume D diameter D drag force on an aerofoil Fa for~ acting in the axial direction on a foil or blade FI force acting in the tangential direction on a foil or blade 9 acceleration due to gravity gh specific energy h specific enthalpy H head K lattice coefficient (Equation 3.11) k an alternative to '}' ( = CJCy ) k. dimensionless specific speed L lift force on an aerofoil M pitching moment acting on a foil Mn Mach number (= V fa) m mass flow rate N rotational speed ms- 1 m kjkg- 1 K- 1 kjkg- 1 K- 1 m N N N ms- 2 Jkg- 1 Jkg- 1 m of liquid N Nm kgs- 1 rev min- 1
12 xii Symbols used: their meaning and dimensions NPSE net positive suction energy kjkg- 1 NPSE a net positive suction energy available kjkg- 1 NPSE R net positive suction energy required kjkg- 1 NPSH net positive suction head m ofliquid Ns specific speed 0 opening or throat in a turbine cascade m P pressure Nm- 2 Po stagnation pressure Nm-2 Pv vapour pressure Nm- 2 p power Js- 1 = W Q volumetric flow rate m3 s- 1 R reaction (Section 1.3) R specific gas constant kjkg- 1 K- 1 Re Reynolds number Rem model Reynolds number S suction specific speed t blade thickness m t blade passage minimum width or throat m T temperature (absolute) K To stagnation temperature (absolute) K T torque Nm u Peripheral velocity ms- 1 V absolute velocity ms- 1 v.. axial component of absolute velocity ms- 1 v.. normal component of absolute velocity ms- 1 "is or ("isen) isentropic velocity (Equation 1.34) ms- 1 V R radial component of absolute velocity ms- 1 v.. peripheral component of absolute velocity ms- 1 W relative velocity ms- 1 w.. peripheral component of relative velocity ms- 1 YN,YR loss coefficients (Equation 3.27) (X angle made by absolute velocity degrees p angle made by relative velocity degrees y ratio of specific heats y stagger angle degrees,() deviation angle degrees B fluid deflection degrees loss coefficient (Equation 3.13)
13 Symbols used: their meaning and dimensions 11 efficiency I1ss static to static efficiency I1TS total to static efficiency I1rr total to total efficiency () camber angle degrees K elastic modulus kgm- 1 S-2 J.1 absolute viscosity kgm- 1 S-l v kinematic viscosity m2 S-l e Markov's loss coefficient (Equation 3.26) p density kgm- 3 (J Thoma's cavitation parameter (J velocity ratio (Equation 3.29) flow coefficient (V./u) specific energy coefficient '" I1rr/2cxf. (Equation 3.30) n '" Howell's work done factor w angular velocity rads- 1 Subscripts 1, 2 etc indicate the point of reference. For a complete definition of blade terminology please refer also to Fig. 3.2 and Table 3.1. xiii
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