Already published in this series: FLIGHT TEST INSTRUMENTATION, Volume 1 Edited by M. A. Perry, 1961. RECENT DEVELOPMENTS IN NETWORK THEORY Edited by S. R. Deards, 1963. FLIGHT TEST INSTRUMENTATION, Volume 2 Edited by M. A. Perry, 1963. ADVANCES IN AUTOMOBILE ENGINEERING, Part I "Edited by G. H. Tidbury, 1963. ADVANCES IN AUTOMOBILE ENGINEERING, Part II Edited by N. A. Carter, 1963. FLIGHT TEST INSTRUMENTATION, Volume 3 Edited by M. A. Perry, 1965. ADVANCES IN AUTOMOBILE ENGINEERING, Part III Edited by G. H. Tidbury, 1965. ADVANCES IN AUTOMOBILE ENGINEERING, Part IV Edited by D. Hodgetts, 1966. AEROSPACE INSTRUMENTATION, Volume 4 Edited by M. A. Perry, 1967. COMBUSTION IN ADVANCED GAS TURBINE SYSTEMS Edited by I. E. Smith, 1968. COMBUSTION AND HEAT TRANSFER IN GAS TURBINE SYSTEMS Proceedings of an International Propulsion Symposium held at the College of Aeronautics, Cranfield, April 1969 Edited by E. R. NORSTER PERGAMON PRESS OXFORD NEW YORK TORONTO SYDNEY BRAUNSCHWEIG Pergamon Press Ltd., Headington Hill Hall, Oxford Pergamon Press Inc., Maxwell House, Fair view Park, Elmsford, New York 10523 Pergamon of Canada Ltd., 207 Queen's Quay West, Toronto 1 Pergamon Press (Aust.) Pty. Ltd., 19a Boundary Street, Rushcutters Bay, N.S.W. 2011, Australia Vieweg & Sohn GmbH, Burgplatz 1, Braunschweig Copyright © 1971 Pergamon Press Ltd. All Rights Reserved. No part of this publication may be reproduced, stored in a retrieval system, or trans mitted, in any form or by any means, electronic, mechanical, photocopying, recording or otherwise, without the prior permission of Pergamon Press Ltd. First edition 1971 Library of Congress Catalog Card No. 72-143801 Printed in Great Britain at The Pitman Press, Bath 08 016524 9 FOREWORD WITH the accelerating development of the gas turbine engine in size and complexity and the growth of its technology, there is an obvious need to supplement this type of Symposium with others covering related topics in the Gas Turbine field. However, the success of the 1967 Cranfield International Propulsion Symposium stimulated so much interest in gas turbine combustion systems that the Organizing Committee felt the format for the 1969 Symposium should be virtually the same. The papers selected for this Symposium gave a good balance between the work of academic and research establishments and that of industrial organi zations in the field of Combustion and Heat Transfer in Gas Turbine Systems. Additional topics of atomization, fuels and high-temperature materials have been introduced to highlight the increasing spectrum of the technology associated with the gas turbine engine. Four of the nineteen papers presented came from outside the United Kingdom and illustrate the increasing international flavour of Cranfield Symposia. The discussion of these papers, exchange of ideas and feedback of infor mation have not only proved to be useful stepping-stones for technical staff and designers but also stimulus for those engaged in applied combustion research. The editor, on behalf of the Organizing Committee, would like to express thanks to Authors, Chairmen, Delegates and members of the Propulsion Department of the College of Aeronautics who contributed to the success of the 1969 Propulsion Symposium and for making the compilation of this volume possible. E. R. NORSTER Vlll THE COMBUSTION SYSTEM FOR THE OLYMPUS 593 CONCORDE ENGINE D. W. HARVEY Rolls-Royce Limited (Bristol Engine Division) Introduction The original concept of an engine for Concorde was an uprated version of the previous Olympus Mark, the 320, two of which powered the TSR2. However, the thrust level of 30,0001b was insufficient when in 1964 com mercial demands on the aircraft necessitated a minimum of 35,000 lb to cope with increased payload and range—the latter design requirement being 3500, miles typical of a London or Paris to New York run. The familiar twin-spool straight turbojet design of the Olympus series was retained together with a cannular configuration of combustion system—on which considerable experience had been obtained from the 1000's of opera ting hours of the previous marks including the early Vulcan power units, marks 104, 201 and 301 and the 320 in the ill-fated TSR2. Hence the selection of 8 x 10 in. diam. flame tubes each supported up stream on a sprayer mounted spherical and downstream on the first stage turbine stators or nozzle guide vanes (Fig. 1). Principally due to powerplant installation considerations the same major scantling dimensions as the Olympus 320 were retained—and although the inlet and outlet duct heights have been altered to meet the demands of compressor and turbine, the maximum area annulus dimensions remained unchanged as they have done since the original 201 mark. Operating Conditions Figure 2 shows the increases in the major operating conditions of the combustion system throughout the Olympus series. Maximum inlet pressure has steadily risen from 10-17 atm.—a relatively low value by present-day standards but then a high-pressure ratio engine is not necessary for a S.S.T. The high outlet temperature requirement which was achievable for the first time with the introduction of cooled turbine blades is shown by the significant rise from the 1200°K level up to 1510°K—although this figure includes a built-in margin used for combustion development, full-thrust Concorde engines will operate some 50°C below this figure. 3 4 D. W. HARVEY Inlet temperatures at the take-off conditions have also shown a steady rise over the years culminating with 450°C in the 593. But here we meet the significant feature unique to this S.S.T. engine where combustion inlet temperature at cruise is 100°C greater than the take-off value. FIG. 1. Early design of Olympus 593 flame tube. The final curve in Fig. 2 shows the stator choking flow function. Bearing in mind that casing sizes have remained constant and that at windmilling conditions combustion system temperatures are similar in all marks, then the W\/T increase from a value of —-— at outlet of 45 to nearly 75 is indicative of the increased severity of altitude ignition and relight. The mean air velocity through the system is nearly 70% greater than in the Olympus 201, COMBUSTION SYSTEM FOR THE OLYMPUS 593 5 It is important to appreciate that not only have there been general in creases in combustion operating levels, but also a very wide range of condi tions is experienced during the normal transatlantic flight profile of the Concorde. Apart from wide ranges of inlet pressure, temperature and fuel flow, the variations in system air loading and air-fuel ratio as shown in Fig. 3 are particularly demanding. FIG. 2. The increasing demand on the combustion system at take-off. The highest loading phases are those of approach and taxi, descent, and a typical diversion, and unfortunately these are also the régimes during which the weakest operation of the system is prevalent. Therefore we were faced in the initial design of either ensuring a reasonable primary zone air-fuel ratio at these weaker, highly loaded conditions and accept rich operation during the take-off phase with the inevitable high level of smoke generation—or to 6 D. W. HARVEY run weak during these phases with consequent loss of thermal efficiency and relight capability. Combustion Performance Criticality From the detailed breakdown of the conditions encountered during a typical flight profile, fairly simple calculations enable the effect of combustion inefficiency on take-off weight to be determined. An operating point repre senting each of seven phases was selected and by considering the total amount FIG. 3. Typical transatlantic flight profile maximum chamber operating loading, air fuel ratio and fuel temperature. of fuel used in that phase the efficiency equation shown in Fig. 4 was derived. The relative importance of maintaining high efficiency levels during each phase was therefore obtained and is shown graphically in the same figure. The cruise condition is critical, a 1 % reduction in efficiency necessitating an extra 1750 lb of fuel to be included to meet the predetermined flight plan. These figures are based on an overall aircraft weight at take-off of 350,000 lb, including a payload of 20,000 lb. Next in order of importance are the sub sonic climb, diversion or hold at alternate and the descent phase, all of which COMBUSTION SYSTEM FOR THE OLYMPUS 593 7 are conditions of high loading and weak air/fuel operation. If a 1 % loss in efficiency at all conditions is incurred, then the take-off weight penalty is over 2500 lb. The efficiency at take-off, however, is relatively unimportant in this context. Because of the considerable performance penalty arising from inefficiency at these weak operating conditions, it was concluded that a comparatively rich primary zone operation at the take-off condition was essential. A value of 14/1 was selected, but even this gives nearly 70/1 during the descent phase. FIG. 4. Effect on fuel penalty of combustion efficiency. Fuel penalty is computed by the equation: where a fuel penalty of 10 = 1520 lb. The criticality of the combustion performance is also experienced when pressure loss is considered. Engine cycle calculations show that a 1 % increase in combustion system loss necessitates an extra 1350 lb weight of fuel to be put aboard. The rate of exchange is similar for loss reduction giving a worth while design incentive. 8 D. W. HARVEY A large proportion of the system loss is incurred in diffusing from the compressor outlet guide vanes to the maximum area annulus. Gradual controlled diffusion to achieve minimum loss would necessitate increasing the length of the system. The actual weight increase/inch length local to the combustion system for the Olympus 593 engine is 8 lb, representing a take-off weight penalty for the aircraft of 64 lb/in. This comparatively small increase would therefore be adequately compensated by the return through reducing the overall system loss. However, at the design stage length priority was given to both intakes and compressors, and at the present time such a major redesign would be uneconomic. Altitude Relight Considerations Operating conditions are significantly extended when the possibility of a flight relight is considered. Inlet pressures of less than half an atmosphere and temperatures of —40° are liable if the guaranteed 30,000 ft clearance at all subsonic Mach numbers is to be achieved. The air loading of the chamber during windmilling is nearly doubled compared with the Oly. 201, making the problem twice as difficult. The simple loading parameter shown earlier is not only employed in correlating combustion efficiency but can also be applied to ignition and relight. Figure 5 shows the lines of constant loading derived from the windmilling characteristics of an Olympus 593 in Concorde. Included on this plot are ignition and relight results from an early series of engine tests in an altitude cell at N.G.T.E. The similarity of the loading and relight loops is clearly shown. Ignition of the igniter flame tubes must, of course, be followed by cross- ignition via interconnectors to the adjacent flame tubes together with sufficient heat release to provide the necessary energy for accelerating the engine. Within a range of normal fuel flows thermal efficiency at this condi tion is therefore important—noting that a loading value of approximately 23 is required at 30,000 ft M = 0-6 the demanding conditions can be seen in Fig. 6 where a typical loading/combustion efficiency plot is shown. Efficiency levels of less than 40 % may be expected at such air loadings. Metal Temperatures The fixing of casing sizes to be the same as the Oly. 320 therefore accen tuated the problems of relight and the achievement of acceptable efficiency levels. However, as this constraint led to smaller sized flame tubes than would have otherwise resulted from a "carte-blanche" design the problem of flame tube wall temperatures was at least minimized. Fundamental rig tests have shown that all the flame tube metal temperatures increase at the same rate as inlet temperatures, whilst the dilution and turbine entry duct zones