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Optimal design of savonius wind turbines using ensemble of surrogates and CFD analysis

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Abstract

Current study presents fluid flow analysis using CFD and a surrogate based framework for design optimization of Savonius wind turbines. The CFD model used for the study is validated with results from a physical model in water tunnel experiment. Four variables that best define blade geometry are considered and a feasible design space consisting of different combinations of these variables that provide positive overlap ratio is identified. The feasible space is then sampled with Latin hyper cube design of experiment. Numerical simulations utilizing K-epsilon turbulence model are performed at each point in the Design of Experiments to obtain coefficient of performance and weighted average surrogate (WAS) is fitted to them. Novelty of the current work is the use of WAS for design of savonius turbine. The WAS is an ensemble of surrogates that consists of polynomial response surface, kriging and radial basis functions. Error metrics reveal that WAS performs better compared to any surrogate individually thus avoiding misleading optima and eliminates surrogate dependent optima. WAS is used to explore the design space and perform optimization with limited number of CFD analyses. It is observed that at the optimal profile, there is more power on the rotors and primary recirculation in the immediate downstream of rotor is high, enforcing maximum momentum on turbine.

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Notes

  1. Video of the water tunnel experiment: http://ed.iitm.ac.in/~palramu/wt.wmv, © 2013 Piyush Jadhav, Ranjana Meena, Sai Gole, Vishaal Dhamotharan, K Arul Prakash, Palaniappan Ramu

  2. Mentioned in ANSYS Software forum discussion: https://www.sharcnet.ca/Software/Ansys/16.0/en-us/help/cfx_mod/i1345899.html

Abbreviations

AR :

Aspect ratio

BAA:

Blade arc angle

CFD:

Computational fluid dynamics

DoE:

Design of experiments

HAWT:

Horizontal axis wind turbine

LHS:

Latin hypercube sampling

MS:

Numerical model specification

NB:

Number of blades

OR :

Overlap ratio

PRESS:

Predicted error sum of squares

PRS:

Polynomial response surface

RBF:

Radial basis function

RMS:

Root mean square

TSR:

Tip speed ratio

VAWT:

Vertical axis wind turbine

WAS:

Weighted average surrogate

D :

Diameter of the rotor

H:

Height

K :

Kinetic energy

L :

Characteristic length

Re :

Reynolds number

St :

Strouhal number

V :

Air velocity

X :

DoE sampling plan

d :

Perpendicular distance between blades

e:

Distance between the blades

fr :

Frequency of vortex shed by blades

p :

Number of design points

r :

Blade arc radius

u, v:

Inlet velocities in x and y directions respectively

y :

Response

α, β :

Angles made by curtains 1, 2

ε:

Kinetic energy dissipation rate

θ :

Blade rotation angle

λ :

Tip speed ratio

ϑ :

Coefficients attributed to individual distances in RBF

ϕ :

Blade arc angle

ψ :

Vector of basis function

ω:

Specific rate of dissipation of kinetic energy

C l :

Coefficient of lift

C M :

Coefficient of moment

C p :

Coefficient of power

C t :

Coefficient of torque

C TS :

Coefficient of static torque

D t :

Diameter of the turbine

U fluid :

Velocity of the fluid

α 0, α i, α ij :

Coefficients of the PRS

ci :

Center of the ith basis function

er i :

Error in ith iteration of the PRESS estimate

P c :

Basis function centers in RBF

q i :

Weight associated with the ith surrogate

ω i :

Weight of the ith basis function

θR :

Angular displacement.

\( \widehat{f} \) :

Approximation of f

\( {\widehat{y}}_{WAS} \) :

Predicted response by the WAS model

Δ:

Bias and random errors

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Correspondence to Palaniappan Ramu.

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Responsible Editor: Felipe A. C. Viana

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Appendices

Appendix 1

The mesh convergence information for the computer model used in the validation study is provided below in Table 7. Two meshes were generated for the same profile with ±10% difference in number of quad elements and the Cp values were compared. It is observed that there is ~ 4% change in Cp value when the mesh size is decreased and ~1% increase when the mesh cells are increased by 10%. Hence further study is performed by increasing the number of mesh cells by 75% and still the observed Cp value increases by ~1%. Therefore, the mesh size corresponding to iteration number 3 is used in the work.

Table 7 Mesh convergence information

Appendix 2

The weighted average surrogate (WAS) is formulated as a weighted sum of the three individual approximation methods. The weights are calculated in such a way that they (a) reflect the confidence in each individual surrogate and (b) filter out adverse effects associated with individual surrogates which represent the sample data well, but predict poorly at designs not included in the sample data. WAS can be expressed as follows:

$$ {\widehat{y}}_{WAS}(x)=\sum \limits_{i=1}^N{q}_i(x){\widehat{y}}_i(x)={Q}^T(x)\widehat{y}(x) $$
(12)
$$ \sum \limits_{i=1}^N{q}_i(x)=1 $$
(13)

where \( {\widehat{y}}_{WAS}(x) \) is the predicted response by the WAS model, qi(x) is the weight associated with the ith surrogate at x and and \( {\widehat{y}}_i(x) \) is the predicted response by the ith surrogate. The various functions that could be used for assigning weights for WAS are shown in Table 8. We use the Best PRESS in this work.

Table 8 Different forms of weights for WAS

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Dhamotharan, V., Jadhav, P.D., Ramu, P. et al. Optimal design of savonius wind turbines using ensemble of surrogates and CFD analysis. Struct Multidisc Optim 58, 2711–2726 (2018). https://doi.org/10.1007/s00158-018-2052-x

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  • DOI: https://doi.org/10.1007/s00158-018-2052-x

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