Three Tank OED: Difference between revisions
RobertLampel (talk | contribs) Created page with "{{Dimensions |nd = 1 |nx = 21 |nw = 6 }} The '''Three Tank OED problem''' is a variation of the Three Tank multimode problem. It looks for optimal time intervals to measure the two states in order to minimize the uncertainty of a follow-up parameter estimation problem for the two unknown parameters. The mathematical equations form a small-scale ODE model. It also includes state sensitivities, the Fisher information matr..." |
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<math> | <math> | ||
\begin{array}{rcl} | \begin{array}{rcl} | ||
\dot{x}_1(t) & = -\sqrt{x_1(t)}+c_1 | \dot{x}_1(t) & =& -\sqrt{x_1(t)}+c_1 u_1(t) + c_2 u_2(t) - u_3(t) \sqrt{c_3 x_1(t)}, && t \in [0,t_f], \quad x_1(0) = 2, \\ | ||
\dot{x}_2(t) & = \sqrt{x_1(t)}-\sqrt{x_2(t)}, && t \in [0,t_f], \quad x_2(0) = 2, \\ | \dot{x}_2(t) & =& \sqrt{x_1(t)}-\sqrt{x_2(t)}, && t \in [0,t_f], \quad x_2(0) = 2, \\ | ||
\dot{x}_3(t) & = \sqrt{x_2(t)}-\sqrt{x_3(t)} + | \dot{x}_3(t) & =& \sqrt{x_2(t)}-\sqrt{x_3(t)} + u_3(t) \sqrt{c_3 x_1(t)}, && t \in [0,t_f], \quad x_3(0) = 2. | ||
\end{array} | \end{array} | ||
</math> | </math> | ||
</p> | </p> | ||
Additionally, the controls <math> | Additionally, the controls <math>u_1,u_2,</math> and <math>u_3</math> are constrained by: | ||
<math> | <math> | ||
\sum_{i=1}^3 | \sum_{i=1}^3 wui(t) = 1 \quad \forall t\in [0,t_f] | ||
</math> | </math> | ||
The initial values and <math>t_f = | The initial values and <math>t_f = 12</math> are fixed. We are interested in how to choose the controls <math>u_i, \ i=1,2,3,</math> and when to measure, with an upper bound <math>M</math> on the measuring time. We can measure the states directly, i.e., <math>h^i(x(t)) = x_i(t), \ i=1,2,3</math>. We use three different sampling functions, <math>w^i(\cdot), \ i=1,2,3,</math> in the same experimental setting. This can be seen either as a three-dimensional measurement function <math>h(x(t))</math>, or as a special case of a multiple experiment, in which <math>u(\cdot), x(\cdot)</math>, and <math>G(\cdot)</math> are identical. | ||
Now we formulate the OED problem with <math>\theta := (p_1, p_2)</math>: | Now we formulate the OED problem with <math>\theta := (p_1, p_2)</math>: | ||
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\quad \dot{F}(t) & = & \sum_{i=1}^{n_o} w_i(t)(h^i_x(x(t))G(t))^T(h^i_x(x(t))G(t)) \\ | \quad \dot{F}(t) & = & \sum_{i=1}^{n_o} w_i(t)(h^i_x(x(t))G(t))^T(h^i_x(x(t))G(t)) \\ | ||
\quad \dot{z}(t) & = & w(t), \\ | \quad \dot{z}(t) & = & w(t), \\ | ||
\quad x(0) & = & | \quad x(0) & = & (2,2,2) \\ | ||
\quad G(0) & = & \frac{\partial x(0)}{\partial \theta} \\ | \quad G(0) & = & \frac{\partial x(0)}{\partial \theta} \\ | ||
\quad F(0) & = & I \cdot \varepsilon_{\mathrm{reg}}, \\ | \quad F(0) & = & I \cdot \varepsilon_{\mathrm{reg}}, \\ | ||
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</p> | </p> | ||
The evolution of the symmetric matrix <math>F: \left[0,t_f \right] \rightarrow \mathbb{R}^{ | The evolution of the symmetric matrix <math>F: \left[0,t_f \right] \rightarrow \mathbb{R}^{3 \times 3}</math> is given by the weighted sum of observability Gramians | ||
<math>h^i_x (x(t)) G(t), \ i = 1,2</math> for each observed function of states. | <math>h^i_x (x(t)) G(t), \ i = 1,2,3,</math> for each observed function of states. | ||
== Parameters == | == Parameters == | ||
Revision as of 09:46, 26 March 2026
| Three Tank OED | |
|---|---|
| State dimension: | 1 |
| Differential states: | 21 |
| Discrete control functions: | 6 |
The Three Tank OED problem is a variation of the Three Tank multimode problem. It looks for optimal time intervals to measure the two states in order to minimize the uncertainty of a follow-up parameter estimation problem for the two unknown parameters.
The mathematical equations form a small-scale ODE model. It also includes state sensitivities, the Fisher information matrix entries and integrated sampling states.
Mathematical formulation
We are interested in estimating the parameters and of the initial value problem
Additionally, the controls and are constrained by:
The initial values and are fixed. We are interested in how to choose the controls and when to measure, with an upper bound on the measuring time. We can measure the states directly, i.e., . We use three different sampling functions, in the same experimental setting. This can be seen either as a three-dimensional measurement function , or as a special case of a multiple experiment, in which , and are identical.
Now we formulate the OED problem with :
The evolution of the symmetric matrix is given by the weighted sum of observability Gramians for each observed function of states.
Parameters
These fixed values are used within the model:
| Symbol | Value | Description |
|---|---|---|
| 1 | Unknown parameter | |
| 1 | Unknown parameter | |
| 10 | Horizon of the control problem | |
| 0.1 | Regularization of Fisher matrix | |
| [-0.5,] | Bounds of | |
| [-1,1] | Bounds of control function | |
| [0,1] | Bounds of measurement function | |
| 2 | Maximum measurement time |
Reference Solutions
Here is one local solution to the above control problem.
- Reference solution plots
-
States, control, and sampling functions for a local optimum.
References
There were no citations found in the article.