------------------ WORK IN PROGRESS ------------------
flow5 v7.07 introduces a new module for the optimization of planes using the Multi-Objective Particle Swarm Optimization (MOPSO) algorithm. This algorithm and its many variants are well documented elsewhere, so that only the main features important to the correct use of the algorithm are mentioned here.
In its original and simplest form, the algorithm performs the optimization of a function towards a single objective and is designated by the acronym PSO. The general principle is to perform the optimization process in a manner similar to the one by which a swarm of birds or insects converges towards its target.
An alternative to the PSO is the Genetic Algorithm (GA). Preliminary tests performed in flow5 have shown so far that the GA does not converge as fast as the PSO, and tends to get stuck on local optimums. This is not a general conclusion however and is likely due to the specificities of the algorithm's implementation in flow5.
Given its apparent robustness, its simplicity and its versatility, the PSO has been selected as the algorithm to use in flow5.
Each of the swarm's particle is fully determined by its position in the space of variables, and by its velocity in this same space.
The space of variables in which the optimization is to be performed is determined by the user. It can be for instance the plane's CoG position, the main wing's aspect ratio and the elevator's tilt angle, in which case the design space has dimension 3.
The particle's position is used to evaluate its fitness vs. each objective, i.e. the value of the objective function at the particle's location, and the error or distance to the objectives.
All particles are moved simultaneously at each iteration.
The change of velocity of each particle follows loosely the laws of mechanic, with randomizing factors added in to increase the swarm's diversity.
The particle's position P and velocity V in the design space are deduced from their values at the previous iteration according to the formula on the right.
The rate of change is the sum of three quantities based on:
The idea is that each particle tries to modify its current velocity to improve its personal best.
The respective importance of these three quantities is determined by three coefficients called the inertia weight w, the cognitive weight c1 and the social weight c2.
The inertia weight w is analog to the mass in mechanic: the greater the mass, the more force it takes to change the velocity.
r1 and r2 are random numbers in the range [0,1] intended to add diversity to the swarm movement.
The algorithm ends when one of the particle's fitness satisfies the objective, or when the maximum number of iterations has been reached.
The MOPSO algorithm is an extension of the PSO and uses the same principle. The main difference is that there is no unique or simple definition of "the best" particle in the swarm since the distances to each of the objectives may be measured differently and cannot be compared.
To illustrate this, consider the optimization of a plane for the two simultaneous objectives |Cm| <ε and Cl/Cd ≥ 30 at a specified angle of attack. A pitching moment coefficient cannot be compared to a glide ratio, and the algorithm cannot determine by itself which of the two objectives is more important. Also there is usually no unique best configuration which satisfies all objectives, but instead several different solutions may satisfy both objectives.
The standard method to select the best particles is to build the Pareto front (or frontier) of the swarm, and to retain those particles which are non-dominated.
Similarly to the single objective PSO, the algorithm ends when one particle satisfies all objectives, or when the maximum number of iterations is reached.
A 2d visual demonstrator of the PSO and GA algorithms can be accessed in flow5 using the keyboard shortcut Ctrl+N and F11.
This demonstrator can be used to test the influence of the algorithms' key parameters.
As a proof of concept case, a PSO module has been implemented in flow5 to optimize a foil's shape to achieve a given inviscid pressure distribution.
As it turns out, the PSO converges robustly towards the target distribution.
The module can be accessed by switching to the Foil design module, selecting a foil, and using the keyboard shortcut F11.
The module is provided for information only and is of no practical use. It offers no advantage compared to XFoil's MDES and QDES modules. The goal was to determine the potential applicability of the PSO to the analog 3d case.
The MOPSO implemented in flow5 is the basic version of the algorithm, with the additional tweak of random particle regeneration each time the swarm moves.
Many improvements and variants of the algorithm have been published over time, and some of these variants may be evaluated in the future and included in flow5 if a benefit is seen.
As it is, the module is stable, operational and can be used to perform optimizations.
As of flow5 v7.07 however it is provided for user testing and feedback, since the interface lacks maturity and since the module may not address all user needs.
Depending on its potential utility a scripted optimization module may be added in a future version.
The objectives which can be selected are:
The module can be used to optimize an internal xfl-type plane. An illustration of the design variables is given in the image on the right.
Any number of design variables may be activated for a given optimization run.
Up to v7.13, a wing's geometry could be optimized using the scaling variables which are the span, the root chord, the average sweep, the twist, the area, and the aspect and taper ratios. Starting with v7.14, the section variables can be activated individually.
Note that activating simultaneously variables of each kind will create a conflict with unpredictable results. This could occur for instance when activating the span range variable and y-positions of one or more sections.
The recommended way is to optimize first using the scaling variables and to switch to section variables only for a more refined optimization.
Experience so far has shown that the MOPSO algorithm works best by optimizing incrementally an existing plane. The subject plane should be analyzed and the reference performance points, e.g. lift coefficient or glide ratio, should be determined and used as the starting point.
In the case illustrated in the image below, the current glide ratio is 18 at the aoa 3° for which Cm=0. A reasonable optimization problem could be to achieve Cl/Cd = 21 in the range [2°-4°] with the constraint Cm=0.
The design variables should be selected for their influence on the ojectives. In this case they are chosen to be:
Since the MOPSO performs a very large number of calculations, it is important that each calculation runs in a fraction of a second. This implies that the mesh size in particular should be small, and how small depends on the platform's computing power.
Typically the analysis configuration should be:
Fine optimization of the model with more complex meshes and analysis types should be performed manually after the automatic optimization has determined the best qualitative solutions.
The optimization module is accessed by selecting the plane to optimize, then using the context menu action "Active plane/Optimize" or the keyboard shortcut F11.
The settings of the analysis and of the MOPSO algorithm are presented on the left side of the interface and the results on the right side.
The objectives are defined in the first tab of the left column.
The key points to check are that
In the case illustrated in the image on the right, the objective is to achieve Cl/Cd = 21 with maximum error 0.1 together with the constraint Cm=0 with maximum error 0.01.
A variable is activated by selecting different minimum and maximum values.
There is no limit to the number of variables which can be activated. The important thing is that the variables to activate and their range should be chosen so that they are consistent with the objectives to reach.
Increasing the number of variables may improve the chances of finding an optimal solution, but may also cause the algorithm to wander a little more. Experimentation is still on-going to establish guidelines.
The variables are inherently plane-dependent, so that a set of variables is kept in memory for each plane for the time of the session. The variables are not saved to the project file.
In the case illustrated in the image on the right, the design variables which have been activated are:
The convergence and robustness of the MOPSO algorithm are very sensitive to the value of the parameters, which should only be modified with care. Also, experimentation is still on-going so that the recommendations and default values may change in the future.
In the case illustrated in the image above,
the parameters have been set at their default values.
By default, the analysis set for the MOPSO is the last one defined in the plane module. The analysis settings can be modified by clicking the "Define" push button.
It is strongly recommended to use a simple type of analysis to limit the computation times, e.g.
Once the input data has been defined, click on the "Make random swarm" button, and wait for a confirmation message in the output pane that the Pareto frontier was successfully built.
Press the "Swarm" button to start the iterations. The algorithm can be interrupted by pressing this same button again, and can be resumed by pressing it another time.
Note that if the algorithm ends or is interrupted without convergence, the Pareto frontier will still be displayed in the bottom right table, however none of the particles will meet all objectives.
If the MOPSO failed to converge, it is possible to either:
Lastly, the swarm should be regenerated manually each time the selection of objectives has changed. If only their values have changed, regeneration is not necessary.
The results are presented on the right side of the interface.
Since there is no single best particle but instead several which constitute the Pareto frontier, flow5 selects for display the best particle with minimum normalized distance to the origin. The normalization is made by dviding the particle's error by the objective's maximum admissible error. This particle is highlighted in red in the Pareto graph.
The top right graph plots its position in a normalized space at each iteration. It may illustrate which variables have influence and which variables tend to remain constant or inversely tend to hit their boundary.
The middle graph plots the error of the same best particle with regard to each objective. It may illustrate which objectives remain out of reach in the design space.
The bottom table lists the particles in the Pareto frontier at each swarm iteration. Only one of these particles may meet all objectives, and only if the algorithm has converged. The index of the winning particle is given in the text output in the bottom left pane. In the present case the winner is particle p6 which meets all the objectives.
The particles may be sorted by clicking on the column headers.
Click on the three dots in the Action column on particle p6's row to save the plane to the project file.
In the case of an optimization run with two and only two objectives, it is possible to view the Pareto graph in the bottom right tab. The graph is updated after each iteration, which may help to visualize the swarm's convergence towards the target rectangle.
Each circle represents a particle, with the filled purple circles constituting the frontier.
The target rectangle is overlayed in blue.
The optimization target is reached when one particle enters the rectangle.
Note that the number of particles in the frontier is limited to the maximum size defined in the "PSO" tab, so that some particles which should be in the frontier are sometimes excluded.
It is is possible to change the values of the design variables and the target values of the objectives and to start a new optimization without regenerating the swarm. Note however that the swarm may lack diversity and that convergence may not be better than by starting with a fresh swarm.
If the selection of objectives has changed, e.g. targeting a lift coefficient instead of a glide ratio, the swarm must be regenerated.