publicImage/gprMax
1
0
派生 0
镜像自地址 https://gitee.com/sunhf/gprMax.git 已同步 2025-08-07 15:10:13 +08:00
代码 工单 软件包 项目 版本发布 百科 动态

Removal of Taguchi optimisation. Move towards high-level config module, rather than settings in Grid class.

浏览代码
这个提交包含在：
Craig Warren
2019-05-24 09:54:32 +01:00
父节点 142b9b4064
当前提交 61e9d43e26
共有 35 个文件被更改，包括 349 次插入 和 1525 次删除
下载 Patch 文件 下载 Diff 文件 展开所有文件 折叠所有文件

1
docs/source/index.rst
查看文件

@@ -41,7 +41,6 @@ gprMax User Guide
user_libs_antenna_patterns
user_libs_austinman
user_libs_materials
user_libs_opt_taguchi
.. toctree::
:maxdepth: 2

149
docs/source/user_libs_opt_taguchi.rst
查看文件

@@ -1,149 +0,0 @@
User libraries is a sub-package where useful Python modules contributed by users are stored.
*******************************
Optimisation - Taguchi's method
*******************************
Information
===========
**Author/Contact**: Craig Warren (craig.warren@northumbria.ac.uk), Northumbria University, UK
**License**: `Creative Commons Attribution-ShareAlike 4.0 International License <http://creativecommons.org/licenses/by-sa/4.0/>`_
**Attribution/cite**: Warren, C., Giannopoulos, A. (2011). Creating finite-difference time-domain models of commercial ground-penetrating radar antennas using Taguchi's optimization method. *Geophysics*, 76(2), G37-G47. (http://dx.doi.org/10.1190/1.3548506)
The package features an optimisation technique based on Taguchi's method. It allows users to define parameters in an input file and optimise their values based on a fitness function, for example it can be used to optimise material properties or geometry in a simulation.
.. warning::
This package combines a number of advanced features and should not be used without knowledge and familiarity of the underlying techniques. It requires:
* Knowledge of Python to contruct an input file to use with the optimisation
* Familiarity of optimisation techniques, and in particular Taguchi's method
* Careful sanity checks to be made throughout the process
Taguchi's method
----------------
Taguchi's method is based on the concept of the Orthogonal Array (OA) and has the following advantages:
* Simple to implement
* Effective in reduction of experiments
* Fast convergence speed
* Global optimum results
* Independence from initial values of optimisation parameters
Details of Taguchi's method in the context of electromagnetics can be found in [WEN2007a]_ and [WEN2007b]_.
Package overview
================
.. code-block:: none
antenna_bowtie_opt.in
fitness_functions.py
OA_9_4_3_2.npy
OA_18_7_3_2.npy
plot_results.py
* ``antenna_bowtie_opt.in`` is a example model of a bowtie antenna where values of loading resistors are optimised.
* ``fitness_functions.py`` is a module containing fitness functions. There are some pre-built ones but users should add their own here.
* ``OA_9_4_3_2.npy`` and ``OA_18_7_3_2.npy`` are NumPy archives `containing pre-built OAs <http://neilsloane.com/oadir/>`_
* ``plot_results.py`` is a module for plotting the results, such as parameter values and convergence history, from an optimisation process when it has completed.
Implementation
--------------
The process by which Taguchi's method optimises parameters is illustrated in the following figure:
.. figure:: images/user_libs/taguchi_process.png
:width: 300 px
Process associated with Taguchi's method.
In stage 1a, one of the 2 pre-built OAs will automatically be chosen depending on the number of parameters to optimise. Currently, up to 7 independent parameters can be optimised, although a method to construct OAs of any size is under testing.
In stage 1b, a fitness function is required to set a goal against which to compare results from the optimisation process. A number of pre-built fitness functions can be found in the ``fitness_functions.py`` module, e.g. ``minvalue``, ``maxvalue`` and ``xcorr``. Users can also easily add their own fitness functions to this module. All fitness functions must take two arguments:
* ``filename`` a string containing the full path and filename of the output file
* ``args`` a dictionary which can contain any number of additional arguments for the function, e.g. names of outputs (rxs) in the model
Additionally, all fitness functions must return a single fitness value which the optimsation process will aim to maximise.
Stages 2-6 are iterated through by the optimisation process.
Parameters and settings for the optimisation process are specified within a special Python block defined by ``#taguchi`` and ``#end_taguchi`` in the input file. The parameters to optimise must be defined in a dictionary named ``optparams`` and their initial ranges specified as lists with lower and upper values. The fitness function, it's parameters, and a stopping value are defined in dictionary named ``fitness`` which has keys for:
* ``name`` a string that is the name of the fitness function to be used
* ``args`` a dictionary containing arguments to be passed to the fitness function. Within ``args`` there must be a key called ``outputs`` which contains a string or list of the names of one or more outputs (rxs) in the model
* ``stop`` a value from the fitness function which when exceeded the optimisation should stop
Optionally a variable called ``maxiterations`` maybe specified which will set a maximum number of iterations after which the optimisation process will terminate irrespective of any other criteria. If it is not specified it defaults to a maximum of 20 iterations.
There is also a builtin criterion to terminate the optimisation process is successive fitness values are within 0.1% of one another.
How to use the package
======================
The package requires ``#python`` and ``#end_python`` to be used in the input file, as well as ``#taguchi`` and ``#end_taguchi`` for specifying parameters and setting for the optimisation process. A Taguchi optimisation is run using the command line option ``--opt-taguchi``.
Example
-------
The following example demonstrates using the Taguchi optimisation process to optimise values of loading resistors used in a bowtie antenna. The example is slighty contrived as the goal is simply to find values for the resistors that produces a maximum absolute amplitude in the response from the antenna. We already know this should occur when the values of the resistors are at a minimum. Nevertheless, it is useful to illustrate the optimisation process and how to use it.
.. figure:: images/user_libs/antenna_bowtie_opt.png
:width: 600 px
FDTD geometry mesh showing bowtie antenna with slots and loading resistors.
The bowtie design features three vertical slots (y-direction) in each arm of the bowtie. Each slot has different loading resistors, but within each slot there are four resistors of the same value. A resistor is modelled as two parallel edges of a cell. The bowtie is placed on a lossless substrate of relative permittivity 4.8. The antenna is modelled in free space, and an output point of the electric field (named ``Ex60mm``) is specified at a distance of 60mm from the feed of the bowtie (red coloured cell).
.. literalinclude:: ../../user_libs/optimisation_taguchi/antenna_bowtie_opt.in
:language: none
:linenos:
The first part of the input file (lines 1-6) contains the parameters to optimise, their initial ranges, and fitness function information for the optimisation process. Three parameters representing the resistor values are defined with ranges between 0.1 :math:`\Omega` and 1 :math:`k\Omega`. A pre-built fitness function called ``min_max_value`` is specified with a stopping criterion of 10V/m. Arguments for the ``min_max_value`` function are ``type`` given as ``absmax``, i.e. the maximum absolute values, and the output point in the model that will be used in the optimisation is specified as having the name ``Ex60mm``.
The next part of the input file (lines 8-92) contains the model. For the most part there is nothing special about the way the model is defined - a mixture of Python, NumPy and functional forms of the input commands (available by importing the module ``input_cmd_funcs``) are used. However, it is worth pointing out how the values of the parameters to optimise are accessed. On line 29 a NumPy array of the values of the resistors is created. The values are accessed using their names as keys to the ``optparams`` dictionary. On line 30 the values of the resistors are converted to conductivities, which are used to create new materials (line 34-35). The resistors are then built by applying the materials to cell edges (e.g. lines 55-62). The output point in the model in specifed with the name ``Ex60mm`` and as having only an ``Ex`` field output (line 42).
The optimisation process is run on the model using the ``--opt-taguchi`` command line flag.
.. code-block:: none
python -m gprMax user_libs/optimisation_taguchi/antenna_bowtie_opt.in --opt-taguchi
Results
^^^^^^^
When the optimisation has completed a summary will be printed showing histories of the parameter values and the fitness metric. These values are also saved (pickled) to file and can be plotted using the ``plot_results.py`` module, for example:
.. code-block:: none
python -m user_libs.optimisation_taguchi.plot_results user_libs/optimisation_taguchi/antenna_bowtie_opt_hist.pickle
.. code-block:: none
Optimisations summary for: antenna_bowtie_opt_hist.pickle
Number of iterations: 4
History of fitness values: [4.2720928, 5.68856, 5.7023263, 5.7023263]
History of parameter values:
resinner [250.07498, 0.87031555, 0.1, 0.1]
resmiddle [250.07498, 0.87031555, 0.1, 0.1]
resouter [250.07498, 0.87031555, 0.1, 0.1]
.. figure:: images/user_libs/taguchi_fitness_hist.png
:width: 600 px
History of values of fitness metric (absolute maximum).
.. figure:: images/user_libs/taguchi_parameter_hist.png
:width: 600 px
History of values of parameters - ``resinner``, ``resmiddle``, and ``resouter`` (in this case they are all identical).
The optimisation process terminated after 4 iterations because succcessive fitness values were within 0.1% of one another. A maximum absolute amplitude value of 5.7 V/m was achieved when the three resistors had values of 0.1 :math:`\Omega`.