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[613]1/*!
[944]2\page userguide_sim BDM Use - System, Data, Simulation
[613]3
[948]4This section serves as introduction to the scenario of data simulation. Since it is the simplest of all scenarios defined in \ref userguide0 it also serves as introduction to configuration of an experiment (see \ref ui) and basic decision making objects (bdm::RV and bdm::DS).
[613]5
[948]6All experiments are demonstrated on mex file \c simulator, which is also available as a standalone application.
[613]7
[948]8Table of contents:
9\section ug_sim_config
10\section ug_sim
11\section ug_memds
12\section ug_rvs
13\subsection ug_rv_connect
14\section ug_pdfds
15\section ug_arx_sim
16\subsection ug_ini
17\section ug_store
[613]18
[948]19
[944]20\section ug_sim_config Configuration of an experiment
[613]21
[617]22Configuration file (or config structure) is organized as a tree of information. High levels represent complex structures, leafs of the tree are basic data elements such as strings, numbers or vectors.
[613]23
[944]24Specific treatment was developed for objects. Since BDM is designed as object oriented library, the configuration was designed to honor the rule of inheritance. That is, offspring of a class can be used in place of its predecessor. Hence, objects (instances of classes) are configured by a structure  with compulsory field \c class. This is a string variable corresponding to the name of the class to be used. This information is stored in Matlab structures (or objects, see section on Matlab extensions).
[613]25
[948]26Advanced users can find more information in (\ref ui).
[613]27
[630]28\subsection ug_first First experiment
[613]29
[617]30The first experiment that can be performed is:
[613]31\code
32DS.class='MemDS';
33DS.Data =[1 2 3 4 5 6];
34\endcode
[617]35which can be found in file bdmtoolbox/tutorials/userguide/memds_example.m.
[613]36
[948]37The code above is the minimum necessary information to run scenario \c simulator in Matlab.
38To actually do so, make sure that Matlab paths are correctly set, as described in \ref install.
[617]39
40The expected result for Matlab is:
[613]41\code
[617]42>> M=simulator(DS)
[613]43
44M =
45
46    ch0: [6x1 double]
47\endcode
48
[617]49All that the simulator did was actually copying \c DS.Data to \c M.ch0. Explanation of the experiment and the logic used there follows.
[613]50
[630]51\section ug_sim Systems and DataSources
[613]52
[617]53In standard system theory, the system is typically illustrated graphically as:
54\dot
55digraph sys{
56        node [shape=box];
57        {"System"}
58        node [shape=plaintext]
59        {rank="same"; "u"; "System"; "y"}
60        "u" -> "System" -> "y" [nodesep=2];
61}
62\enddot
63Where \c u typically denotes input and \c y denotes output of the system. A causal dependence between input and output is typically presumed.
[613]64
[897]65We are predominantly concerned with discrete-time systems, hence, we will add indices \f$ _t \f$ to both input and output, \f$ u_t \f$ and \f$ y_t \f$. We presume that the causal dependence is \f$ u_t \f$ comes before \f$ y_t \f$.
[613]66
[617]67One of the definition of a system is that system is a "set of variables observed on a part of the world". Under this definition system is understood as generator of data. This definition may be a considered too simplistic, but it serves well as a description of what software object \c DataSource is.
68
[944]69DataSource is an object that is essentially able to:
70 -# return data observed at time \f$ t \f$,
71 -# perform one a time step.
[983]72 -# describe what these data are, via class RV, introduced in ref \ref ug_pdf_marg,
[944]73 -# store log of its activity into dedicated logger.
[617]74
[948]75No further specification, e.g. if the data are pre-recorded or computed on-the-fly, are given.
[944]76For a list of available DataSources, see ...
[617]77
78
[630]79\section ug_memds DataSource of pre-recorded data -- MemDS
[617]80
[661]81The first experiment run in \ref ug_first was actually an instance of DataSource of pre-recorded data that were stored in memory, i.e. the bdm::MemDS class.
[617]82
83Operation of such object is trivial, the data are stored as a matrix and the general operations defined above are specialized as follows:
[948]84 -# data observed at time \f$ t \f$  are columns of the matrix, getdata() returns current column,
[617]85 -# time step itself is performed by increasing the column index,
86 -# each row is named as "ch0","ch1",...
87
[948]88This is the default behavior. It can be customized using the UI mechanism. Full list of options is:
[613]89\code
[617]90DS.class = 'MemDS';
91DS.Data = (...);            // Data matrix or data vector
[613]92        --- optional ---
[617]93DS.drv = RV({"ch0",...} ); // Identification how rows of the matrix Data will be known to others
94DS.time = 0;               // Index of the first column to user_info,
[613]95\endcode
[617]96The compulsory fields are listed at the beginning; the optional fields are separated by string "--- optional ---".
[613]97
[944]98Fields \c time denotes the first record to start counting from. Field \c drv is a the one that specifies identification of the data elements, (point 3. of the general requirements of a DataSource).
[617]99
100All optionals fields will be filled by default values, it this case:
[613]101\code
[617]102DS.drv  = RV({'ch0'},1,0);
103DS.time = 0;
[613]104\endcode
[617]105Where the first line specifies a universal identification structure: random variable (bdm::RV).
[613]106
[630]107\section ug_rvs What is RV and how to use it
[613]108
[944]109RV stands for \c random \c variable which is a description of random variable or its realization. However, this object serves as general descriptor of fields in vectors of data.
[613]110
[944]111It is used for:
[948]112 - description of RV in pdfs, ways how to define marginalization and conditioning,
[944]113 - connection between source of data and computational objects that use them,
114 - connection <b>time</b>, more exactly time shift from \f$ t \f$, defaults to 0.
[613]115
[948]116For example, the estimators will request the data from the above mentioned data source by asking for rv 'ch0'. If a more meaningful names are available, the fields drv can be added to read:
[947]117\code
118DS.class='MemDS';
119DS.Data =[1 2 3 4 5 6];
120DS.drv = RV('y');
121\endcode
[948]122Data from this data source will be available when estimators ask for rv 'y'.
[947]123
[944]124\subsection ug_rv_connect Storing results
[632]125
[948]126results of an experiment can be stored in many ways. This functionality was abstracted into a class called logger. Exact form of the stored results is chosen by choosing appropriate class.
127For example, \c stdlog writes all output in the console, \c dirfilelog writes all data in the dirfilelog format for high-speed data processing, \c mexlog writes data into Matlab structure.
[944]128The \c mexlog is the default option in bdmtoolbox.
[632]129
[948]130Connection between computational blocks and loggers is controlled by structure called \c log_level which governs the level of details to be logged.
[944]131A standard Data source has two levels, \c logdt and \c logut which means "log all outputs, dt" and "log all inputs, ut".
[617]132Readers familiar with Simulink environment may look at the RV as being unique identifiers of inputs and outputs of simulation blocks. The inputs are connected automatically with the outputs with matching RV. This view is however, very incomplete, RV have more roles than this.
[613]133
[944]134\section ug_pdfds How to create a simulator from pdfs
135For example, we would like to simulate a random Uniform distributed noise on interval <-1,1>.
136This is achieved by plugging an object representing uniform pdf into general simulator of independent random samples, pdfDS. Uniform density is implemented as class bdm::euni, which is created from the following structure:
[613]137\code
138U.class='euni';
[617]139U.rv   = RV({'a'});
[613]140U.high = 1.0;
141U.low  = -1.0;
142\endcode
[617]143which encodes information:\f[
144f(a) = \mathcal{U}(-1,1)
145\f]
[613]146 
[948]147The datasource itself, i.e. the instance of \c EpdfDS can be then configured via:
[613]148\code
[944]149DS.class = 'pdfDS';
150DS.pdf  = U;
[613]151\endcode
[617]152where \c U is the structure defined above.
[613]153
[617]154Contrary to the previous example, we need to tell to algorithm \c simulator how many samples from the data source we need. This is configured by variable \c experiment.ndat. The configuration has to be finalized by:
[613]155\code
156experiment.ndat = 10;
[617]157M=simulator(DS,experiment);
[613]158\endcode
159
[944]160The result is as expected in field \c M.DS_dt_a the name of which corresponds to results form "datasouce" / "output_dt" / "name given in U.rv".
[613]161
[947]162If the task was only to generate random realizations, this would indeed be a very clumsy way of doing it.
[948]163However, the power of the proposed approach will be revealed in more demanding examples, one of which follows next.
[613]164
[947]165By default, data from this datasouce will be named after the rvs in given by the pdfs. When pdf with no rv is used, drv of the data source is set again to 'ch0'.
166
[630]167\section ug_arx_sim Simulating autoregressive model
[613]168
169Consider the following autoregressive model:
170\f[
[617]171f(y_t|y_{t-3},u_{t-1}) = \mathcal{N}( a y_{t-3} + b u_{t-1}, r)
[613]172\f]
173where \f$ a,b \f$ are known constants, and \f$ r \f$ is known variance.
174
175We need to handle two issues:
176 -# extra unsimulated variable \f$ u \f$,
[948]177 -# time delays of the values.
[613]178
[617]179The first issue can be handled in two ways. First, \f$ u \f$ can be considered as input and as such it could be externally given to the datasource. This solution is used in scenario \c closedloop.
180However, for the \c simulator scenario we will apply the second option, that is we complement \f$ f(y_{t}|y_{t-3},u_{t-1})\f$ by extra pdf:\f[
181f(u_t) = \mathcal{N}(0, r_u)
[613]182\f]
[617]183where \f$ r_u \f$ is another known constant.
[613]184Thus, the joint density is now:\f[
185f(y_{t},u_{t}|y_{t-3},u_{t-1}) = f(y_{t}|y_{t-3},u_{t-1})f(u_{t})
186\f]
187and we have no need for input since the datasource have all necessary information inside. All that is required is to store them and copy their values to appropriate places.
188
[944]189That is done in automatic way (via bdm::datalink_buffered). The only issue a user may need to take care about is the missing initial conditions for simulation.
[613]190By default these are set to zeros. Using the default values, the full configuration of this system is:
191\code
192y = RV({'y'});
193u = RV({'u'});
194
[661]195fy.class = 'mlnorm\<ldmat\>';
[613]196fy.rv    = y;
197fy.rvc   = RV({'y','u'}, [1 1], [-3, -1]);
198fy.A     = [0.5, -0.9];
199fy.const = 0;
200fy.R     = 0.1;
201
202
[661]203fu.class = 'enorm\<ldmat\>';
[613]204fu.rv    = u;
205fu.mu    = 0;
206fu.R     = 0.2;
207
[693]208DS.class = 'pdfDS';
209DS.pdf.class  = 'mprod';
[711]210DS.pdf.pdfs  = {fy, fu};
[613]211\endcode
212
213Explanation of this example will require few remarks:
[661]214 - class of the \c fy object is 'mlnorm\<ldmat\>' which is Normal pdf with mean value given by linear function, and covariance matrix stored in LD decomposition, see bdm::mlnorm for details.
[948]215 - naming convention 'mlnorm\<ldmat\>' relates to the concept of templates in C++. For those unfamiliar with this concept, it is basically a way how to share code for different flavors of the same object. Note that mlnorm exist in three versions: mlnorm\<ldmat\>, mlnorm<chmat>, mlnorm<fsqmat>. Those classes act identically the only difference is that the internal data are stored either in LD decomposition, choleski decomposition or full matrices, respectively.
[613]216 - the same concept is used for enorm, where enorm<chmat> and enorm<fsqmat> are also possible. In this particular use, these objects are equivalent. In specific situation, e.g. Kalman filter implemented on Choleski decomposition (bdm::KalmanCh), only enorm<chmat> is approprate.
[944]217 - class 'mprod' represents the chain rule of probability, see \ref ug_pdf_cond.
[613]218 
[948]219The code above can be immediately run, using the same execution sequence of \c estimator as above.
[613]220
[630]221\subsection ug_ini Initializing simulation
[613]222
[944]223When zeros are not appropriate initial conditions, the correct conditions can be set using additional commands:
[613]224\code
225DS.init_rv = RV({'y','y','y'}, [1,1,1], [-1,-2,-3]);
226DS.init_values = [0.1, 0.2, 0.3];
227\endcode
228
229The values of \c init_values will be copied to places in history identified by corresponding values of \c init_rv.
[948]230Initial data is not checked for completeness, i.e. values of random variables missing from \c init_rv (in this case all occurrences of \f$ u \f$) are still initialized to 0.
[613]231
[630]232\section ug_store Storing results of simulation
233
[651]234If the simulated data are to be analyzed off-line it may be advantageous to store them and use later on.
[630]235This operation is straightforward if the class of logger used in the \c simulator is compatible with some datasource class.
236
237For example, the output of \c MemDS can be stored as an .it file (filename is specified in configuration structure) which can be later read by bdm::ITppFileDS.
238
[948]239In Matlab, the output of mexlog is a structure of vectors or matrices. The results can be saved in a Matlab file using:
[630]240\code
241Data=[M.y; M.u];
242drv = RVjoin({y,u});
[693]243save pdfds_results Data drv
[630]244\endcode
245Such data can be later provided e.g. by MemDS
246\code
247mxDS.class   = 'MemDS';
248mxDS.Data    = 'Data';
249mxDS.drv     = drv;
250\endcode
251
[944]252For list of all DataSources and loggers, see \ref app_base
[613]253*/
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