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Dielectrophoretic Particle OED

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Dielectrophoretic Particle OED
State dimension: 1
Differential states: 13
Discrete control functions: 3


The Dielectrophoretic Particle OED problem is a variation of the Dielectrophoretic Particle 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 α and c of the initial value problem

x1˙(t)=x2(t)u(t)+αu(t)2,t[0,tf],x1(0)=1,x2˙(t)=cx2(t)+u(t),x2(0)=0.

The initial values and tf=10 are fixed. We are interested in how to fish and when to measure, with an upper bound M on the measuring time. We can measure the states directly, h1(x(t))=x1(t) and h2(x(t))=x2(t). We use two different sampling functions, w1() and w2() in the same experimental setting. This can be seen either as a two-dimensional measurement function h(x(t)), or as a special case of a multiple experiment, in which u(),x(), and G() are identical.

Now we formulate the OED problem:

miny,G,F,z,wtrace(F1(tf))subject toy˙(t)=f(y(t),θ)G˙(t)=fy(y(t),θ)G(t)+fθ(y(t),θ)F˙(t)=i=1nowi(t)(hyi(y(t))G(t))T(hyi(y(t))G(t))z˙(t)=w(t),y(0)=y0G(0)=y(0)θF(0)=0,z(0)=0w(t)𝒲zi(tf)Mi

The evolution of the symmetric matrix F:[0,tf]2×2 is given by the weighted sum of observability Gramians hyi(y(t))G(t), i=1,2 for each observed function of states.

Parameters

We use tf=8, α=0.75, and c=1. The upper bound on the measurement time intervals is chosen as M1=M2=2.

Reference Solutions

Here is one local solution to the above control problem.

References

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