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  • 标题:Geometrical outline of the aerodynamic profile of wind turbine blades.
  • 作者:Dubau, Calin ; Catas, Adriana
  • 期刊名称:Annals of DAAAM & Proceedings
  • 印刷版ISSN:1726-9679
  • 出版年度:2010
  • 期号:January
  • 语种:English
  • 出版社:DAAAM International Vienna
  • 摘要:The turbine variant which has been analyzed is addressed to a harness domain of 4-5 m/s, and the maximum revolution imposed by the electrical generator is n = 250 rpm, [omega] = 26,2 rad/s, uR = 40 m/s (maximum - to minimize noise).
  • 关键词:Aerodynamics;Air-turbines;Blades;Blades (Equipment components);Wind turbines

Geometrical outline of the aerodynamic profile of wind turbine blades.


Dubau, Calin ; Catas, Adriana


1. INTRODUCTION

The turbine variant which has been analyzed is addressed to a harness domain of 4-5 m/s, and the maximum revolution imposed by the electrical generator is n = 250 rpm, [omega] = 26,2 rad/s, uR = 40 m/s (maximum - to minimize noise).

2. MATERIAL AND METHODS

The geometrical outline of the aerodynamic profile of the blade is made analytically, by combining two mathematical functions (see Dubau, 2007 and Bej, 2003): the skeleton function and the thickness function. The aerodynamic profiles which have been chosen are those from the NACA series with four figures: NACA 4424 (at the hub) and 4415 (at the margin), (see Gyulai, 2000 and 2003). The axis Oy falls perpendicularly on the chord in the board of attack, while the thickness function is given by the following expression:

for [MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (5)

[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (6)

for [MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (7)

The functioning of the aerodynamic profile, which is placed in a draught, primarily depends on the position of the profile against the draught speed, through the angle of incidence value. Based on it, we have represented the following drawings, regarding the geometrical outline of the blade.

The algorithm of calculation for the determination of the geometrical outlines implies the following steps:

> defining the calculation variants for each radius (r), correlated with the profile chord (l) and the relative thickness of profile (d/l)

> the profile chord has been divided into ten equal intervals, noted with (0,1 0,2 ... 1) x l

[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (1)

The curvature radii of the boards of attack and run-off, which are both rounded, are determined using the relations: (A attack, F--run-off)

[r.sub.A] / 1 = 1,1019. [([d.sub.m] / 1).sup.2] (2)

[r.sub.F] / 1 = 1,105. [([d.sub.m] / 1).sup.2] (3)

The skeleton function is defined using the relations below, the skeleton is made of two parabola arcs, which are connected in [MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII].

[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (4)

> for each partition noted with x, we have determined the thickness function [y.sub.d] / l ([+ or -]), the curvature radius of the board of attack [r.sub.A] /l, and of the board of run-off respectively, as well as the skeleton function [y.sub.f]/l

> the front side and back side calculation of the profile has been determined according to the thickness and skeleton of the profile

> the calculation for each partition is illustrated in a grid where the relative values are presented (in relations to the profile chord - l) and another grid which has been turned into length units expressed in mm, in order to ease the performance of the profile drawings

These data will be utilized for the energy balances of the assembly H2500, which will be determined through a mathematical model used for the assessment of the system curves of energetic revaluation.

The configuration of the turbine blade is represented below in Figure 1. Section positions have been defined according to radius position, the blade chord profile of each section calculated in part (L) and blade thickness (D) respectively, with corresponding values of each string. Data are included in Tables 1 and 2.

[FIGURE 1 OMITTED]

[FIGURE 2 OMITTED]

3. CONCLUSIONS

1. The calculation of the blade profile has been made by determining the geometrical outline of the aerodynamic profile, as we can see in Figure 2, defined analytically through the combination of two mathematical functions, the skeleton and the thickness functions.

2. The model presented has been illustrated in seven calculation sections, which have configurated the final shape of the blade, taking into account the running of the aerodynamic profile which has been placed in air draught, based on a calculation algorithm.

3. The turbine variant which has been analyzed is addressed to a harness domain of 4-5 m/s, and the maximum revolution imposed by the e1ectric[a.sub.1] generator is n = 250 rpm, [omega] = 26,2 rad/s, [u.sub.R] = 40 m/s (maximum - to minimize noise).

13. REFERENCES

Bej, A. (2003). Wind turbines, "Power" collection, Politehnica Publishing House, Timisoara, ISBN 973-625-098-9, pp. 43-44.

Dubau, C. (2007). Utilizarea microagregatelor eoliene in componenfa unor sisteme complexe, Politehnica Publishing House, Timisoara, ISSN: 1842-4937, ISBN: 978-973-625408-6, pp. 150-157.

Gyulai, Fr. (2000). Specialization course in sustainable energy technologies. Modules: Installations Wind and Wind Units, Timisoara.

Gyulai, Fr. (2000). Contributions on horizontal axis wind turbine theory, A V-a ConferintaInternaionala de Masini Hidrau1ice si Hidrodinamica, Timisoara, Romania.

Gyulai, Fr. (2003). Vocational Traning in Sustainable Energy-Course Wind Energy.

4. CORRESPONDING ADDRESSES

Calin Dubau, University of Oradea, Faculty of Environmental Protection, Gen. Magheru Street, No. 26, Oradea, Romania. E-mail: dubau.calin@rdslink.ro

Adriana Catas, University of Oradea, Faculty of Sciences, Department of Mathematics and Computer Science, 1 University Street, 410087, Oradea, Romania E-mail: acatas@gmail.com
Tab. 1. Calculation of the blade regarding relative
thickness of profile (d/l)

Variant 1.1. r = 0,3 ; l = 355 ; d/l = 0,282

x = 0,1x1 0,2x1 0,3x1

[Y.sub.d]/l (+) 0,1100 0,1348 0,1410
[Y.sub.d]/l (-) -0,1100 -0,1348 -0,1410
[r.sub.a]/l 0,0876
[r.sub.f]/l 0,0084
[Y.sub.f]/l 0,0175 0,03 0,0375
extrados 0,1275 0,1648 0,1785
intrados -0,0925 -0,1048 -0,1035

x = 0,4x1 0,5x1 0,6x1

[Y.sub.d]/l (+) 0,1364 0,1244 0,1072
[Y.sub.d]/l (-) -0,1364 -0,1244 -0,1072
[r.sub.a]/l 0,0876
[r.sub.f]/l 0,0084
[Y.sub.f]/l 0,04 0,0389 0,0356
extrados 0,1764 0,1633 0,1428
intrados -0,0964 -0,0855 -0,0717

x = 0,7x1 081x1

[Y.sub.d]/l (+) 0,0861 0,0616
[Y.sub.d]/l (-) -0,0861 -0,0616
[r.sub.a]/l 0,0876
[r.sub.f]/l 0,0084
[Y.sub.f]/l 0,0300 0,0222
extrados 0,1161 0,0839
intrados -0,0561 -0,0394

x = 0,9x1 1

[Y.sub.d]/l (+) 0,0340 0,0030
[Y.sub.d]/l (-) -0,0340 -0,0030
[r.sub.a]/l 0,0876
[r.sub.f]/l 0,0084
[Y.sub.f]/l 0,0122 0
extrados 0,0462 0,0030
intrados -0,0218 -0,0030

Tab. 2. Calculation of the blade regarding thickness of profile

Variant 1.1. r = 0,3 ; l = 355 ; d = 100

x = 0,1x1 0,2x1 0,3x1 0,4x1 0,5x1

x 35,5 71 106,5 142 177,5
[Y.sub.d]/(+) 39,07 47,87 50,07 48,41 44,17
[Y.sub.d]/(-) -39,07 -47,87 -50,07 -48,41 -44,17
[r.sub.a] 31,11
[r.sub.f] 2,96
[y.sub.f] 6,21 10,65 13,31 14,20 13,81
Extrados 45,28 58,52 63,38 62,61 57,97
Intrados -32,85 -37,22 -36,76 -34,21 -30,36

x = 0,6x1 0,7x1 081x1 0,9x1 1

x 213 248,5 284 319,5 355
[Y.sub.d]/(+) 38,07 30,57 21,88 12,08 1,05
[Y.sub.d]/(-) -38,07 -30,57 -21,88 -12,08 -1,05
[r.sub.a] 31,11
[r.sub.f] 2,96
[y.sub.f] 12,62 10,65 7,89 4,34 0,00
Extrados 50,69 41,22 29,77 16,42 1,05
Intrados -25,45 -19,92 -13,99 -7,74 -1,05
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