• Aucun résultat trouvé

Basie Instrumentation of a Low Speed Axial Compressor

N/A
N/A
Protected

Academic year: 2021

Partager "Basie Instrumentation of a Low Speed Axial Compressor"

Copied!
7
0
0

Texte intégral

(1)

HAL Id: jpa-00249362

https://hal.archives-ouvertes.fr/jpa-00249362

Submitted on 1 Jan 1995

HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers.

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.

Basie Instrumentation of a Low Speed Axial Compressor

Sami Blidi, Hubert Miton

To cite this version:

Sami Blidi, Hubert Miton. Basie Instrumentation of a Low Speed Axial Compressor. Journal de Physique III, EDP Sciences, 1995, 5 (7), pp.919-924. �10.1051/jp3:1995168�. �jpa-00249362�

(2)

Classification Physics Abstracts

47.80v 47.32Ff 47.40Hg

Short Communication

Basic Instrumentation of a Low Speed Axial Compressor

Sarni Blidi and Hubert Miton

L-E-M-F-I- URA CNRS 1504, Universit4 P. & M. Curie (Paris VI) Bit. sll, Campus Univer- sitaire, 91405 Orsay Cedex, France

(Received 4 February 1994, revised 31 May 1995, accepted I June 1995)

Abstract, The flow modelling depending on test results allows

a best aerodynamic com- prehension. For this reason, a test bed of L.E.M.F.I.'s axial compressor has been set and

instrumented for

a detailed exploration of the flow in a four-st.age tiJrbomachine cba,racterised by a little spacing between blade rows. In this paper, first are given brief descriptions of the

geometrical characteristics of this compressor, the test bed's control system operation and the instrumentation set. Next, measures for the exploration of flow are discussed. Finally, typical

results concerning the global and local performance measurements and their analysis are pre-

sented. This work permitted to instrument the L-E-M-F-I-'s four-stage axial compressor test bed and obtain the flow steady and unsteady characteristics using the five-hole and hot film probes.

R6sum6. Les 4tudes de mod41isation de l'4coulement dans les compresseurs axiaux doivent

s'appuyer sur des r4sultats exp4rimentaux permettant une meilleure compr4hension des ph4nombnes a4rodynamiques et convenant h la validation des codes num4riques. I cette fin,

un banc d'essais de compresseur axial basse vitesse a 4t4 mis au point et instrument4 au L-E-M-F-I- Iii pour des

explorations d4tail14es de l'4coulement darts une machine comportant 4 4tages, caract4ris4e par le faible espacement entre les rang4es d'aubages. Dans cet article, nous d4crivons bribvement les caract4ristiques g40m4triques du compresseur axial, les systbmes de contr61e du fonction-

nement du banc d'essais et l'instrumentation mise au point. Nous parlons ensuite des moyens

d'explorations de l'4coulement utilis4s. Nous fournissons enfin des exemples de r4sultats de

mesure des performances globales et locales du compresseur et analysons bribvement ces rd-

sultats. Le travail eIfectu4 a perrnis de mettre au point et d'instrumenter un banc d'essais de compresseur axial basse vitesse au L-E-M-F-I- et rendu possible la d4terrnination des grandeurs

stationnaires et instationnaires de l'4coulement entre les rang4es d'aubages en utilisant des son- des clinom4triques de pression et des sondes £ films chauds.

1. The Axial Compressor CMEI

CMEI is a four stage axial flow compressor. The main characteristic of this machine is the

narrow spacing of the adjacent blades rows (10 mm). Such a distance is just sufficient to allow

the introduction of probes between these rows, The axial lenght of the four stages is equal to

© Les Editions de Physique 1995

(3)

920 JOURNAL DE PHYSIQUE III N°7

Fig. I. Axial compressor CMEI.

624 mm. the diameter of the casing is equal to 550 mm. On the hub, the diameter varies from 371 mm in the inlet plane to 410 mm in the outlet one (Fig, I). The following tables give the

main characteristics of the blades in the fir>t stage.

Radius Chord Thickness Stagger angle Camber angle

mm mm ° °

Hub 82 7.4 44.77 51.65

Middle 82 6.4 55.17 37.12

Ti 82 4.8 64.02 25.61

Rotorl

Radius Chord Thickness Stagger angle Camber angle

mm mm ° °

Hub 88 5.2 19.67 75.30

Middle 88 5.2 16.72 71.55

Ti 88 5.2 15.07 67.75

Stator

For the stages 2 to 4 the geometry of the blades is similar excepted the stagger angle. The values of the stagger at the hub is given below for these stages.

Rotor 17 1.027

Stator 24 0.682

Rotor 2 19 0.936

Stator 2 27 0,618

Rotor 3 19 0,950

Stator 3 27 0.626

4 Rotor 4 19 0.962

Stator 4 27 0.634

2. Test Bed AX200

The main components of the experimental set-up are represented in Figure 2, It is a test bed aspirating and discharging in the athmosphere. The power available is, at the present time, limited to 200 Kw and the maximum speed of rotation is 4500 rpm.

In view to reduce the duration of the tests programs, the systems of measurements have been fully automatized. The rotational speed of the compressor is regulated by the frequency of the current of the AC motor, This speed is controled using a optical detector fitted in the

casing in the plane of the first rotor, It gives a TTL type pulse for each passage of a moving blade. This apparatus also serves to the synchronisation of unstationnary measurements. The

(4)

Diaphragm Outlet

Flow Convergent

adjuster

Inlet

Filter *-

Fig. 2. Test bed AX200. Settling Chamber

n~~r~~ ~ ~~~~ ~

fi

RS 232 ~ ASCII ~ 'FA 100 anemometer

fi

interface (6channels) probe

~ fi

~ ~

measurement probe

(8cha~~ls)

~ ZOC is

~

multi-pressure ~ Pressure

~ ~

~ff

~ ~

~~~~f~s

~"'~ ~

~ ~~

Flow rate Static and total

regulation

~

pressure plugs /

~

,/ Rotating speed

÷÷L card < rec°trier

~~~ ~~~~~~

> Probe azimuth

displacement

~

Fig. 3. Global configuration of the system.

mass flow rate of the compressor is controled using a diaphgram fitted in the exhaust duct and regulated by the axial displacement of the conical hub wall just downstream the outlet plane of the compressor. This wall is automatically driven by a DC motor. Inlet and outlet temperatures are obtained from platiniurn resistances gauges introduced radially in the inlet and the outlet planes of the compressor. The pressures are measured with Kiel rakes, radially

and circonferentially located. They are used to know the global pressure ratio of the compressor

an equally to detect the presence of stationnary distorsions in the inlet plane. Alls the operating

proccess (control of mass flora rate, speed of rotation) probes displacements, data acquisitions

are driven by a PC type computer. The global configuration of this system is shown in Figure 3.

(5)

922 JOURNAL DE PHYSIQUE III N°7

3. Global Performance of the Compressor

The basic components of the performance of the compressor are:

the mass flow rate the rotational speed

the total pressure ratio

The results of the global performance of the CMEI axial compressor are represented in

Figure 4.

Measurements has been performed using the instrumentation mentionned above:

Keel probes rakes and temperature resistors probes for pressures and temperatures, di- aphragm for mass flow rate. With such instruments, the relative incertitude as calculated in

reference iii are closed to:

1.1% for mass flow rate o.1% for pressure ratio

np 30

25

Surge ~

20

line

~

/ 5

/

lo

~

rPm

.05 ~~~~ ~~°~

3000 rpm

00

4 5 6 7 7

Qm(k9/S)

Fig. 4. Compressor global performance.

4. Instrumentation for Velocity and Pressure Measurements in the Stages of the

Compressor

4.I. FIVE HOLE PRESSURE PROBES "COBRA" (FIG. 5). These five hoie-probes give the three components of the velocity, static an total pressures at the location of measurement.

Each hole is connected to a pressure transducer (pressure scanner SCANIVALVE ZOC 16:

range ~5 psi). However these datas are values averaged/time, through a characteristic mode

depending on the geometry and on the installation of the probe. Then, data collected by such probes, in a strongly unsteady flow, close to the rotating blades, are to be considered with a great care.

(6)

Yaw plane ())

Pitch planela)

20

14

6

Fig. 5. Five-hole pressure probe.

9QO

'~ ' /

' ,, 38, 501

~~j ~7§~ -~._,

~

10 i,0yP<cdl Spacinc

041

Fig. 6. Hot films probe.

4.2. HOT FILMS PROBEB (FIG. 6). These probes includes two quartz wires, each of them

supporting a platinium film (TSI 1240). They can be used in airflows with velocities up to 350 mIs and temperatures limited to 150 °C. The cut-off frequency is 250 kHz. They give the

unsteady components of the velocity in the plane parallel to the two wires. The problem of the third component of the velocity is quite complex. Indeed, it requires a third wire. It is very difficult to integrate such a third wire in a small sized probe, due to the interactions between the wakes generated by the pins supporting the wire and the other wires.

These hot films probes are linked to a constant temperature anemometer (TSI IFA 100), including 6 channels. It talks with the computer through RS232 protocol.

4.3. USE OF THE COBRA AND HOT FILMS PROBES FOR INVESTIGATIONS OF THE FLOW

BETWEEN THE BLADE Rows. Cobra probes and and hot films probes are calibrated in

a convenient wind tunnel specially setted up in LEMFI; calibration procedures are described in details in reference ill and reference [2]. These probes are used only in the planes defined

(7)

924 JOURNAL DE PHYSIQUE III N°7

~~

~

p

caner <

Hw

"..

Statorj

~

l'..,, ~'

-~

~

hub

/

Fig. 7. Five-hole probe replaced in a blade to blade Field.

by a constant axial position between the rows of blades. Indeed, due to the size of the probes

relatively to that of the blades channels, it would be out of sense to use these probes in view of velocity and pressure measurements in the stators blades channels for exemple.

The probes are introduced radially between the rows and moved both in tangentiel and radial directions (Fig. 7). The spatial grid of measurement is identical for the two types of probes, including 150 points (10 along radius and 15 in the direction of rotation).

The "Cobra" probes allow steady measurements only; average /time values are obtained from sets of 50 pressure datas collected at a frequency of10 Hz.

For the hot wires probes, sets of 4096 voltages from each wire, are collected at a frequency

of10 kHz. Then, the measurement duration represents about 30 revolutions of the rotor.

Conclusions

The present paper reports the set-up of a test bed of axial compressor and the development of its basic instrumentation including sytems of exploration of the flow like "Cobra" probes and hot films probes to be used between the rotating and static rows of blades. These systems of

instrumentation are suitable for measurements restricted to regions between the rows of blades.

At this time, other techniques are in development in view of detailed investigations of the flow

along the walls of the stator blades: unsteady static pressures with miniature transducers and heat flux with hot films, for a better knowledge of the unsteady boundary layer behaviour, from the leading to the trailing edge of the blades.

References

[Ii Blidi S., Mise au point et instrumentation d'un compresseur axial 4 4tages basse vitesse, Thbse U-P-M-C-, Paris 6 (Janvier 1993).

[2] Treaster A-L- and Yocum A-M-, The calibration and application of five-hole probes, ISA Trans.

18 (1979) 23-24.

[3] Miton H., Blidi S. and Ayaz Y., Mesure des 4coulements en environnement machine dans un

compresseur axial multi-4tages basse vitesse, Rapport de synthbse finale, D-R-E-T- N°89-217 (1990).

Références

Documents relatifs

.ب :قيقدتلا و ةبساحملا مظن يف ةيفافشلا في مدقت و ةفافش نوكت ةكرشلل ةيلام ريراقت ىلع لوصلحا لجأ نم ( دعاوقلا و يرياعلماب مازتللاا ةرداببم ةصالخا ريراقتلا نم

Bisher hat sich die Psychologiedidaktik aber noch kaum mit der Frage auseinandergesetzt, welche fachlichen Kernfragen sich in den einzelnen Teilgebieten oder

Il y a trois variables d’états qui sont (1) la biomasse de poissons, définie pour chaque site de pêche, (2) le prix du poisson défini en fonction de la capture totale,

Il existe donc une signature caractéristique, à l’échelle élastique, des Soft Porous Crystals : une large anisotropie de leurs propriétés mécaniques combinée à l’existence

In case of a LOOP event, a major safety issue is to remove the decay heat of the reactor until the reaching of a stable cold shutdown state (defined by a homogeneous sodium

theories present serious drawbacks: (i) the spin fluctu- ation effects are automatically ruled out since the RKKY interactions only occur at the following order in 1/N  [11], (ii)

[2008] provides useful new information on the distribution of aftershocks following the 2003 Boumerdes earthquake, but we show that their interpretation of the position and geometry

Last but not least, the model dis- played significant differences between N and P limited sys- tems and we used these results to explain how DOC accu- mulation in the surface layer