Difference between revisions of "Control of Heat Equation with Actuator Placement"
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− | + | We define the source term for all locations <math> | |
+ | l\in \{1,\dots,L\} <\math> and a | ||
+ | fix parameter <math>\varepsilon\in \R_+</math>: | ||
+ | <math> | ||
+ | f_l(x,y) = \frac{1}{\sqrt{2\pi\varepsilon}}e^{\frac{-((x_l-x)^2+(y_l-y)^2)}{2\varepsilon}} | ||
+ | <\math> | ||
+ | where <math>(x_l,y_l)</math> is the coordinate of the mesh point of the $l$th possible actuator location. | ||
+ | |||
+ | The parameters used are: | ||
<math> | <math> | ||
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− | The parameter <math> \kappa </math> describes the thermal dissipativity of the material in the domain <math> \Omega </math>, it may vary in space. | + | The parameter <math> \kappa </math> describes the thermal dissipativity of the material in the domain <math> \Omega </math>, it may vary in space: <math> \kappa(x,y) </math>. |
The parameter <math> L </math> indicates the number of possible actuator locations. They are distributed as indicated in the picture. | The parameter <math> L </math> indicates the number of possible actuator locations. They are distributed as indicated in the picture. | ||
− | + | The source budget is limited by <math>W<\math>. | |
− | + | ||
− | + | ||
− | + | ||
− | + | ||
− | + | ||
− | <\math> | + | |
− | + | ||
==Reference solution== | ==Reference solution== |
Revision as of 17:08, 23 February 2016
Control of Heat Equation with Actuator Placement | |
---|---|
State dimension: | 1 |
Differential states: | 1 |
Continuous control functions: | |
Discrete control functions: | |
Path constraints: | 3 |
Interior point equalities: | 2 |
This problem is governed by the heat equation and is adapted from Iftime and Demetriou ([Iftime2009]Author: Orest V. Iftime; Michael A. Demetriou
Journal: {A}utomatica
Number: 2
Pages: 312--323
Title: {O}ptimal control of switched distributed parameter systems with spatially scheduled actuators
Volume: 45
Year: 2009
).
Its goal is to choose a place to apply an actuator in a given area depending on time.
The objective function is quadratic, its first term captures the desired final state , the second term regularize the state over time and the third term regularize the continuous controls.
The constraints are a source budget, which limits the quantity of placed actuators, and the two-dimensional heat equation with some source function.
Additionally, we assume Dirichlet boundary conditions and initial conditions.
Mathematical formulation
Parameters
We define the source term for all locations Failed to parse (unknown function "\math"): l\in \{1,\dots,L\} <\math> and a fix parameter <math>\varepsilon\in \R_+
Failed to parse (unknown function "\math"): f_l(x,y) = \frac{1}{\sqrt{2\pi\varepsilon}}e^{\frac{-((x_l-x)^2+(y_l-y)^2)}{2\varepsilon}} <\math> where <math>(x_l,y_l)
is the coordinate of the mesh point of the $l$th possible actuator location.
The parameters used are:
The parameter describes the thermal dissipativity of the material in the domain , it may vary in space: .
The parameter indicates the number of possible actuator locations. They are distributed as indicated in the picture.
The source budget is limited by Failed to parse (unknown function "\math"): W<\math>. ==Reference solution== ==Source Code== ==References== <biblist/> <!--List of all categories this page is part of. List characterization of solution behavior, model properties, ore presence of implementation details (e.g., AMPL for AMPL model) here --> [[Category:MIOCP]]