Abstract
The improvement of existing turbines requires time-consuming computations that often limit the number of parameters that can be optimized. To address this challenge, this study uses through-flow code, which is about 200 times faster than 3D Computational Fluid Dynamics (CFD), to optimize a two-stage axial turbine with 112 geometrical parameters using a deep learning surrogate model. The surrogate model is a Convolutional Neural Network (CNN) that predicts the flow field and performance indicators of the turbine based on an input database generated by an airfoil generation method and an in-house through-flow code. The surrogate model has two components: a flow field prediction component and a performance prediction component. The network architecture is named conv2D-conv3D, as it employs 2D convolutional layers to map the geometry to the flow field and 3D convolutional layers to extract features from the flow field and output the performance indicators. The optimal hyperparameters of the network are determined by comparing different activation functions, batch sizes, and train-data sizes. The network achieves high accuracy (\({R}^{2}> 0.93\)) even with a small fraction of the dataset (30% of data) and it is more than \({10}^{5}\) times faster than the through-flow code. A vectorized genetic algorithm is applied to the surrogate model to maximize the efficiency and power of the turbine under a constant mass flow rate constraint. The optimization results are validated by through-flow and 3D CFD simulations of the baseline and optimized turbine. The efficiency and power are increased by 0.83% and 1.02%, respectively.
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Abbreviations
- \(\dot{\mathrm{m}}\) :
-
Mass flow rate \([\frac{\mathrm{kg}}{\mathrm{s}}]\)
- \(\mathrm{h}\) :
-
Specific enthalpy \([\frac{\mathrm{J}}{\mathrm{kg}.}]\)
- \(\mathrm{I}\) :
-
Rothalpy \([\frac{\mathrm{J}}{\mathrm{kg}}]\)
- \(\mathrm{m}\) :
-
Meridional direction \(\left[\mathrm{m}\right]\)
- \(\mathrm{M}\) :
-
Mach number [−]
- \({\mathrm{S}}_{\mathrm{i}}\) :
-
Defining point coordinates \(\left[\mathrm{m}\right]\)
- \(\mathrm{q}\) :
-
Quasi orthogonal direction [m]
- V:
-
Absolute velocity \(\left[\frac{\mathrm{m}}{\mathrm{s}}\right]\)
- \({\mathrm{R}}_{\mathrm{c}}\) :
-
Streamline local radius \(\left[\mathrm{m}\right]\)
- \(\mathrm{s}\) :
-
Specific entropy \([\frac{\mathrm{J}}{\mathrm{kg}..\mathrm{K}}]\)
- \(\mathrm{U}\) :
-
Blade velocity \(\left[\frac{\mathrm{m}}{\mathrm{s}}\right]\)
- \(\mathrm{N}\) :
-
Number of blades \([-]\)
- \({\mathrm{P}}_{\mathrm{i}}\) :
-
Optional point coordinates \(\left[\mathrm{m}\right]\)
- r:
-
Section radius of the airfoil \(\left[\mathrm{m}\right]\)
- \(\mathrm{P}\) :
-
Pressure [Pa]
- 0:
-
Stagnation condition
- 1:
-
Leading edge
- 2:
-
Trailing edge
- \(\mathrm{g}\) :
-
Gauging
- tt:
-
Total-to-total
- \(\beta\) :
-
Camber line angle [∘]
- \(\upphi\) :
-
Meridional slope angle [∘]
- \(\upgamma\) :
-
Quasi orthogonal angle, stagger angle [∘]
- \(\Delta \beta\) :
-
Wedge angle [∘]
- \(\upeta\) :
-
Efficiency \([-]\)
- \(\mathrm{\alpha }\) :
-
Flow angle [∘]
- \(\uprho\) :
-
Density \([\frac{\mathrm{kg}}{{\mathrm{m}}^{3}}]\)
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This paper has provided all the essential information to obtain the turbine optimization data and the deep learning surrogate model that can reproduce the results. The results can be replicated by following this information. The Python code to reproduce the results, including the conv2D-conv3D network, is also available from the corresponding author upon reasonable request.
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Esfahanian, V., Izadi, M.J., Bashi, H. et al. Aerodynamic shape optimization of gas turbines: a deep learning surrogate model approach. Struct Multidisc Optim 67, 2 (2024). https://doi.org/10.1007/s00158-023-03703-9
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DOI: https://doi.org/10.1007/s00158-023-03703-9