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Blade Design for Kaplan Turbine

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Presentation on theme: "Blade Design for Kaplan Turbine"— Presentation transcript:

1 Blade Design for Kaplan Turbine
P M V Subbarao Professor Mechanical Engineering Department Realization of Pure Reaction using Aerofoils.

2 Hydrodynamics of Kaplan Blade

3 DESIGN OF THE BLADE Two different views of a blade

4 Design of Blade Many factors play significant roles in design of blade. The leading edge is thicker than the trailing edge for a streamlined flow. Furthermore, the blade should to be as thin as possible to improve the cavitation characteristics; It is thicker near the flange becoming thinner and thinner towards the tip. In addition, the blade has to be distorted on the basis of the tangential velocity. The “Tragflügel theorie” is also an important factor in defining the shape of the profile and the distortion of the blade.

5 Design of Kaplan Runner
Drunner Dhub

6 Distortion of the blade under ideal circumstances
The velocity triangles, which occur on the blade, play a significant role in determining its distortion. Uwheel Vri Vai Vfi

7 Design of Kaplan Runner
Drunner Dhub

8 Details of Blade Arrangement
Uwheel Vri Vai Vfi Uwheel Vre Vae Vfe

9 Meridional plane : Conservation of Rothalpy
An ideal incompressible turbomachine:

10 Method for Real Kaplan Define Half Travel Point of a fluid particle as Vfi=Vfe Vri Vre V∞

11 The “Tragflügeltheorie”
V∞ Fideal lift Factual lift

12 The “Tragflügeltheorie” at Half Travel Point
The “Tragflügeltheorie” was developed by Ludwig Prandtl. According to the “Tragflügeltheorie” : A lifting force is generated at the blades of the runner due to the configuration of the flow stream and the whirling stream, which occur at the Center of Pressure of blade. Values such as the lift coefficient and the attack angle δ also play a significant role in the design of the blade. These coefficients can be determined via model tests. Using these results the profile, the chord and the exact distortion of the blade can be determined.

13 Vri

14 Radial Variation Velocity Vectors

15 Force at any radius on the blade:
Uwheel Vri Vai Vfi Uwheel Vre Vae Vfe

16 Radial Variation of Reaction
rvw

17 Characteristics of Blades
Ideal Blade lift coefficient at each radius: hdraft: Efficiency of draft tube: 0.88 to 0.91 K : Profile characteristic number: 2.6 to 3.0 hmin=2.0 – 2.5

18 When the lifting coefficient is known, the sufficiency of ratio l/t can be established as follows:
Allowable values of angle of slip l 2.5°-- 3°

19 The actual Lifting Coefficient

20 Drag Coefficient

21 Calculation of Actual Angle of Slip

22 Actual Angle of Attack

23 Radial Equilibrium Equation for Incompressible Fluid Machine

24 General Rules for Selection of Whirl Component
Free Vortex Whirl: Forced Vortex Whirl :

25 To define the distortion of the blade, the velocity triangles of at least six different radiuses of the blade are to be determined. The angle β of each radius gives conclusions on the distortion of the blade. The angles should be corrected for real hydraulics.

26 Power Developed by the Runner
Power developed by a differential blade surface

27 Calculation of Control Forces

28 Ganga Hydro Elecrtic Scheme
Ten Kaplan Turbine Power units along Ganga Canal. Ranipur, Pathri, Bahadrabad, Salawa, Chitaura, Nirganj, Mohammedpur, Sumera, Palra and Bhola. Capacity Range: 400 hp to 10,000hp. Head Range: 5.3 m to 9.6 m


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