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\begin_body

\begin_layout Standard
\begin_inset FormulaMacro
\newcommand{\isa}[1]{i_{\alpha#1}}
{i_{\alpha#1}}
\end_inset


\begin_inset FormulaMacro
\newcommand{\isb}[1]{i_{\beta#1}}
{i_{\beta#1}}
\end_inset


\begin_inset FormulaMacro
\newcommand{\Dt}{\Delta t}
{\Delta t}
\end_inset


\begin_inset FormulaMacro
\newcommand{\om}{\omega}
{\omega}
\end_inset


\begin_inset FormulaMacro
\newcommand{\th}{\vartheta}
{\vartheta}
\end_inset


\begin_inset FormulaMacro
\newcommand{\usa}[1]{u_{\alpha#1}}
{u_{\alpha#1}}
\end_inset


\begin_inset FormulaMacro
\newcommand{\usb}[1]{u_{\beta#1}}
{u_{\beta#1}}
\end_inset


\end_layout

\begin_layout Title
PMSM system description
\end_layout

\begin_layout Section
Model of PMSM Drive 
\end_layout

\begin_layout Standard
Permanent magnet synchronous machine (PMSM) drive with surface magnets on
 the rotor is described by conventional equations of PMSM in the stationary
 reference frame:
\begin_inset Formula \begin{align}
\frac{d\isa{}}{dt} & =-\frac{R_{s}}{L_{s}}\isa{}+\frac{\Psi_{PM}}{L_{s}}\omega_{me}\sin\th+\frac{\usa{}}{L_{s}},\nonumber \\
\frac{d\isb{}}{dt} & =-\frac{R_{s}}{L_{s}}\isb{}-\frac{\Psi_{PM}}{L_{s}}\omega_{me}\cos\th+\frac{\usb{}}{L_{s}},\label{eq:simulator}\\
\frac{d\om}{dt} & =\frac{k_{p}p_{p}^{2}\Psi_{pm}}{J}\left(\isb{}\cos(\th)-\isa{}\sin(\th)\right)-\frac{B}{J}\om-\frac{p_{p}}{J}T_{L},\nonumber \\
\frac{d\th}{dt} & =\omega_{me}.\nonumber \end{align}

\end_inset

Here, 
\begin_inset Formula $\isa{}$
\end_inset

, 
\begin_inset Formula $\isb{}$
\end_inset

, 
\begin_inset Formula $\usa{}$
\end_inset

 and 
\begin_inset Formula $\usb{}$
\end_inset

 represent stator current and voltage in the stationary reference frame,
 respectively; 
\begin_inset Formula $\om$
\end_inset

 is electrical rotor speed and 
\begin_inset Formula $\th$
\end_inset

 is electrical rotor position.
 
\begin_inset Formula $R_{s}$
\end_inset

 and 
\begin_inset Formula $L_{s}$
\end_inset

 is stator resistance and inductance respectively, 
\begin_inset Formula $\Psi_{pm}$
\end_inset

 is the flux of permanent magnets on the rotor, 
\begin_inset Formula $B$
\end_inset

 is friction and 
\begin_inset Formula $T_{L}$
\end_inset

 is load torque, 
\begin_inset Formula $J$
\end_inset

 is moment of inertia, 
\begin_inset Formula $p_{p}$
\end_inset

 is the number of pole pairs, 
\begin_inset Formula $k_{p}$
\end_inset

 is the Park constant.
\end_layout

\begin_layout Standard
The sensor-less control scenario arise when sensors of the speed and position
 (
\begin_inset Formula $\om$
\end_inset

 and 
\begin_inset Formula $\th$
\end_inset

) are missing (from various reasons).
 Then, the only observed variables are:
\begin_inset Formula \begin{equation}
y_{t}=\left[\begin{array}{c}
\isa{}(t),\isb{}(t),\usa{}(t),\usb{}(t)\end{array}\right].\label{eq:obs}\end{equation}

\end_inset

Which are, however, observed only up to some precision.
\end_layout

\begin_layout Standard
Discretization of the model (
\begin_inset CommandInset ref
LatexCommand ref
reference "eq:simulator"

\end_inset

) was performed using Euler method with the following result:
\begin_inset Formula \begin{align*}
\isa{,t+1} & =(1-\frac{R_{s}}{L_{s}}\Dt)\isa{,t}+\frac{\Psi_{pm}}{L_{s}}\Dt\omega_{t}\sin\vartheta_{e,t}+\usa{,t}\frac{\Dt}{L_{s}},\\
\isb{,t+1} & =(1-\frac{R_{s}}{L_{s}}\Dt)\isb{,t}-\frac{\Psi_{pm}}{L_{s}}\Dt\omega_{t}\cos\vartheta_{t}+\usb{,t}\frac{\Dt}{L_{s}},\\
\om_{t+1} & =(1-\frac{B}{J}\Dt)\om_{t}+\Dt\frac{k_{p}p_{p}^{2}\Psi_{pm}}{J}\left(\isb{,t}\cos(\th_{t})-\isa{,t}\sin(\th_{t})\right)-\frac{p_{p}}{J}T_{L}\Dt,\\
\vartheta_{t+1} & =\vartheta_{t}+\omega_{t}\Dt.\end{align*}

\end_inset

In this work, we consider parameters of the model known, we can make the
 following substitutions to simplify notation, 
\begin_inset Formula $a=1-\frac{R_{s}}{L_{s}}\Dt$
\end_inset

, 
\begin_inset Formula $b=\frac{\Psi_{pm}}{L_{s}}\Dt$
\end_inset

, 
\begin_inset Formula $c=\frac{\Dt}{L_{s}}$
\end_inset

, 
\begin_inset Formula $d=1-\frac{B}{J}\Dt$
\end_inset

, 
\family roman
\series medium
\shape up
\size normal
\emph off
\bar no
\noun off
\color none

\begin_inset Formula $e=\Dt\frac{k_{p}p_{p}^{2}\Psi_{pm}}{J}$
\end_inset

, which results in a simplified model:
\family default
\series default
\shape default
\size default
\emph default
\bar default
\noun default
\color inherit
 
\begin_inset Formula \begin{align}
\isa{,t+1} & =a\,\isa{,t}+b\omega_{t}\sin\vartheta_{t}+c\usa{,t},\nonumber \\
\isb{,t+1} & =a\,\isb{,t}-b\omega_{t}\cos\vartheta_{t}+c\usb{,t},\label{eq:model-simple}\\
\om_{t+1} & =d\om_{t}+e\left(\isb{,t}\cos(\th_{t})-\isa{,t}\sin(\th_{t})\right),\nonumber \\
\vartheta_{t+1} & =\vartheta_{t}+\omega_{t}\Dt.\nonumber \end{align}

\end_inset


\end_layout

\begin_layout Standard
The above equations can be aggregated into state 
\begin_inset Formula $x_{t}=[\isa{,t},\isb{,t},\om_{t},\th_{t}]$
\end_inset

 will be denoted as 
\begin_inset Formula $x_{t+1}=g(x_{t},u_{t})$
\end_inset

.
\end_layout

\begin_layout Subsection
Transformation to d-q coordinates
\end_layout

\begin_layout Standard
For many applications, it is advantageous to consider altervative coordinate
 system denoted d-q as follows
\begin_inset Formula \begin{eqnarray*}
\left[\begin{array}{c}
d\\
q\end{array}\right] & = & \left[\begin{array}{cc}
\cos\vartheta & \sin\vartheta\\
-\sin\vartheta & \cos\vartheta\end{array}\right]\left[\begin{array}{c}
\alpha\\
\beta\end{array}\right]\\
\left[\begin{array}{c}
\alpha\\
\beta\end{array}\right] & = & \left[\begin{array}{cc}
\cos\vartheta & -\sin\vartheta\\
\sin\vartheta & \cos\vartheta\end{array}\right]\left[\begin{array}{c}
d\\
q\end{array}\right]\end{eqnarray*}

\end_inset

Under this transformation, the whole model (
\begin_inset CommandInset ref
LatexCommand ref
reference "eq:model"

\end_inset

) can be transformed into d-q coordinates.
\end_layout

\begin_layout Standard
In this text, we will transform only one single quantity, 
\begin_inset Formula $L_{d}$
\end_inset

 and 
\begin_inset Formula $L_{q}$
\end_inset

 for which it holds 
\begin_inset Formula $L_{d}=kL_{q}$
\end_inset

.
 Then,
\begin_inset Formula \begin{eqnarray*}
\left[\begin{array}{c}
L_{\alpha}\\
L_{\beta}\end{array}\right] & = & \left[\begin{array}{cc}
\cos\vartheta & -\sin\vartheta\\
\sin\vartheta & \cos\vartheta\end{array}\right]\left[\begin{array}{c}
L_{d}\\
L_{q}\end{array}\right].\\
 & = & L_{d}\left[\begin{array}{cc}
\cos\vartheta & -\sin\vartheta\\
\sin\vartheta & \cos\vartheta\end{array}\right]\left[\begin{array}{c}
k\\
1\end{array}\right]\\
 & = & L\left[\begin{array}{cc}
k\cos\vartheta & -\sin\vartheta\\
k\sin\vartheta & \cos\vartheta\end{array}\right]=L\left[\begin{array}{c}
k_{c\vartheta}\\
k_{s\vartheta}\end{array}\right].\end{eqnarray*}

\end_inset

Then, model of the drive is changed to
\begin_inset Formula \begin{align*}
\isa{,t+1} & =(1-\frac{R_{s}}{L_{s}k_{c\vartheta}}\Dt)\isa{,t}+\frac{\Psi_{pm}}{L_{s}k_{c\vartheta}}\Dt\omega_{t}\sin\vartheta_{e,t}+\usa{,t}\frac{\Dt}{L_{s}k_{c\vartheta}},\\
\isb{,t+1} & =(1-\frac{R_{s}}{L_{s}k_{s\vartheta}}\Dt)\isb{,t}-\frac{\Psi_{pm}}{L_{s}k_{s\vartheta}}\Dt\omega_{t}\cos\vartheta_{t}+\usb{,t}\frac{\Dt}{L_{s}k_{s\vartheta}},\\
\om_{t+1} & =(1-\frac{B}{J}\Dt)\om_{t}+\Dt\frac{k_{p}p_{p}^{2}\Psi_{pm}}{J}\left(\isb{,t}\cos(\th_{t})-\isa{,t}\sin(\th_{t})\right)-\frac{p_{p}}{J}T_{L}\Dt,\\
\vartheta_{t+1} & =\vartheta_{t}+\omega_{t}\Dt.\end{align*}

\end_inset

Transformation to full d-q
\begin_inset Formula \begin{eqnarray*}
i_{d,t+1} & = & (1-\frac{R_{s}}{L_{d}}\Dt)i_{d,t}+\frac{L_{q}}{L_{d}}i_{q,t}\Dt\omega_{t}+u_{d,t}\frac{\Dt}{L_{d}},\\
i_{q,t+1} & = & -\frac{L_{d}}{L_{q}}\Dt\omega_{t}i_{d,t}+(1-\frac{R_{s}}{L_{q}}\Dt)i_{q,t}-\frac{\Psi_{pm}}{L_{q}}\Dt\omega_{t}+u_{q,t}\frac{\Dt}{L_{q}},\\
\omega_{t+1} & = & \underbrace{(1-\frac{B}{J}\Dt)}_{\approx1}\om_{t}+\Dt\frac{k_{p}p_{p}^{2}}{J}((L_{d}-L_{q})i_{d}+\Psi_{pm})i_{q}\\
\vartheta_{t+1} & = & \vartheta_{t}+\Delta t\omega_{t}\end{eqnarray*}

\end_inset


\end_layout

\begin_layout Standard
Observation:
\begin_inset Formula \[
\left[\begin{array}{c}
i_{\alpha}\\
i_{\beta}\end{array}\right]=\left[\begin{array}{cc}
\cos\vartheta & -\sin\vartheta\\
\sin\vartheta & \cos\vartheta\end{array}\right]\left[\begin{array}{c}
i_{d}\\
i_{q}\end{array}\right]+e_{t}\]

\end_inset


\end_layout

\begin_layout Subsection
Gaussian model of disturbances
\end_layout

\begin_layout Standard
This model is motivated by the well known Kalman filter, which is optimal
 for linear system with Gaussian noise.
 Hence, we model all disturbances to have covariance matrices 
\begin_inset Formula $Q_{t}$
\end_inset

 and 
\begin_inset Formula $R_{t}$
\end_inset

 for the state 
\begin_inset Formula $x_{t}$
\end_inset

 and observations 
\begin_inset Formula $y_{t}$
\end_inset

 respectively.
\begin_inset Formula \begin{align}
x_{t+1} & \sim\mathcal{N}(g(x_{t}),Q_{t})\label{eq:model}\\
y_{t} & \sim\mathcal{N}([\isa{,t},\isb{,t}]',R_{t})\nonumber \end{align}

\end_inset


\end_layout

\begin_layout Standard
Under this assumptions, Bayesian estimation of the state, 
\begin_inset Formula $x_{t}$
\end_inset

, can be approximated by so called Extended Kalman filter which approximates
 posterior density of the state by a Gaussian 
\begin_inset Formula \[
f(x_{t}|y_{1}\ldots y_{t})=\mathcal{N}(\hat{x}_{t},S_{t}).\]

\end_inset

Its sufficient statistics 
\begin_inset Formula $S_{t}=\left[\hat{x}_{t},P_{t}\right]$
\end_inset

 is evaluated recursively as follows:
\begin_inset Formula \begin{eqnarray}
\hat{x}_{t} & = & g(\hat{x}_{t-1})-K\left(y_{t}-h(\hat{x}_{t-1})\right).\label{eq:ekf_mean}\\
R_{y} & = & CP_{t-1}C'+R_{t},\nonumber \\
K & = & P_{t-1}C'R_{y}^{-1},\nonumber \\
S_{t} & = & P_{t-1}-P_{t-1}C'R_{y}^{-1}CP_{t-1},\\
P_{t} & = & AS_{t}A'+Q_{t}.\label{eq:ekf_cov}\end{eqnarray}

\end_inset

where 
\begin_inset Formula $A=\frac{d}{dx_{t}}g(x_{t})$
\end_inset

, 
\begin_inset Formula $C=\frac{d}{dx_{t}}h(x_{t})$
\end_inset

, 
\begin_inset Formula $g(x_{t})$
\end_inset

 is model (
\begin_inset CommandInset ref
LatexCommand ref
reference "eq:model-simple"

\end_inset

) and 
\begin_inset Formula $h(x_{t})$
\end_inset

 direct observation of 
\begin_inset Formula $y_{t}=[\isa{,t},\isb{,t}]$
\end_inset

, i.e.
\begin_inset Formula \[
A=\left[\begin{array}{cccc}
a & 0 & b\sin\th & b\om\cos\th\\
0 & a & -b\cos\th & b\om\sin\th\\
-e\sin\th & e\cos\th & d & -e(\isb{}\sin\th+\isa{}\cos\th)\\
0 & 0 & \Dt & 1\end{array}\right],\quad C=\left[\begin{array}{cccc}
1 & 0 & 0 & 0\\
0 & 1 & 0 & 0\end{array}\right]\]

\end_inset


\end_layout

\begin_layout Standard
\begin_inset Formula \[
B=\left[\begin{array}{cc}
c & 0\\
0 & c\\
0 & 0\\
0 & 0\end{array}\right]\]

\end_inset


\end_layout

\begin_layout Standard
Covariance matrices of the system 
\begin_inset Formula $Q$
\end_inset

 and 
\begin_inset Formula $R$
\end_inset

 are supposed to be known.
\end_layout

\begin_layout Subsubsection
Reduced order version
\end_layout

\begin_layout Standard
Equations (
\begin_inset CommandInset ref
LatexCommand ref
reference "eq:model"

\end_inset

) ca be restructured by considering 
\begin_inset Formula $i_{s\alpha}$
\end_inset

 and 
\begin_inset Formula $i_{s\beta}$
\end_inset

 as external observations.
 Then the state variables are 
\begin_inset Formula $x_{t}=[\omega_{t},\vartheta_{t}]$
\end_inset

 and as follows:
\begin_inset Formula \begin{align}
\om_{t+1} & =d\om_{t}+e\left(\isb{,t}\cos(\th_{t})-\isa{,t}\sin(\th_{t})\right),\label{eq:rord-state}\\
\vartheta_{t+1} & =\vartheta_{t}+\omega_{t}\Dt.\nonumber \end{align}

\end_inset

and the onbservation equations are
\begin_inset Formula \begin{align}
\isa{,t+1} & =a\,\isa{,t}+b\omega_{t}\sin\vartheta_{t}+c\usa{,t},\nonumber \\
\isb{,t+1} & =a\,\isb{,t}-b\omega_{t}\cos\vartheta_{t}+c\usb{,t},\label{eq:rord-obs}\end{align}

\end_inset

These equations are used by the EKF to update estimates of mean values.
 The new matrices 
\begin_inset Formula $A$
\end_inset

 and 
\begin_inset Formula $C$
\end_inset

 are
\begin_inset Formula \[
A=\left[\begin{array}{cc}
d & -e(\isb{}\sin\th+\isa{}\cos\th)\\
\Dt & 1\end{array}\right],\quad C=\left[\begin{array}{cc}
b\sin\th & b\om\cos\th\\
-b\cos\th & b\om\sin\th\end{array}\right].\]

\end_inset


\end_layout

\begin_layout Subsection
Test system
\end_layout

\begin_layout Standard
A real PMSM system on which the algorithms will be tested has parameters:
\end_layout

\begin_layout Standard
\begin_inset Formula \begin{eqnarray*}
R_{s} & = & 0.28;\\
L_{s} & = & 0.003465;\\
\Psi_{pm} & = & 0.1989;\\
k_{p} & = & 1.5\\
p & = & 4.0;\\
J & = & 0.04;\\
\Delta t & = & 0.000125\end{eqnarray*}

\end_inset

which yields
\begin_inset Formula \begin{eqnarray*}
a & = & 0.9898\\
b & = & 0.0072\\
c & = & 0.0361\\
d & = & 1\\
e & = & 0.0149\end{eqnarray*}

\end_inset

The covaraince matrices 
\begin_inset Formula $Q$
\end_inset

 and 
\begin_inset Formula $R$
\end_inset

 are assumed to be known.
 For the initial tests, we can use the following values:
\end_layout

\begin_layout Standard
\begin_inset Formula \begin{eqnarray*}
Q & = & \mathrm{diag}(0.0013,0.0013,5e-6,1e-10),\\
R & = & \mathrm{diag}(0.0006,0.0006).\end{eqnarray*}

\end_inset


\end_layout

\begin_layout Standard
Limits:
\begin_inset Formula \begin{align*}
u_{\alpha,max} & =50V, & u_{\alpha,min} & =-50V,\\
u_{\beta,max} & =50V. & u_{\beta,min} & =-50V,\end{align*}

\end_inset


\end_layout

\begin_layout Standard
Perhaps better:
\begin_inset Formula \[
u_{\alpha}^{2}+u_{\beta}^{2}<100^{2}.\]

\end_inset


\end_layout

\begin_layout Standard

\end_layout

\begin_layout Section
Control
\end_layout

\begin_layout Standard
The task is to reach predefined speed 
\begin_inset Formula $\overline{\omega}_{t}$
\end_inset

.
\end_layout

\begin_layout Standard
For simplicity, we will assume additive loss function:
\begin_inset Formula \begin{eqnarray*}
l(x_{t},u_{t}) & = & (\omega_{t}-\overline{\omega}_{t})^{2}+q(\usa{,t}^{2}+\usb{,t}^{2}).\\
 & = & (\omega_{t}-\overline{\omega}_{t})\Xi(\omega_{t}-\overline{\omega}_{t})+[\usa t,\usb t]\underbrace{\left[\begin{array}{cc}
\upsilon & 0\\
0 & \upsilon\end{array}\right]}_{\Upsilon}\left[\begin{array}{c}
\usa t\\
\usb t\end{array}\right]\end{eqnarray*}

\end_inset

Here, 
\begin_inset Formula $\Upsilon$
\end_inset

 is the chosen penalization of the inputs, which remains to be tuned.
\end_layout

\begin_layout Standard

\series bold
Note
\series default
: classical notation of penalization matrices is 
\begin_inset Formula $Q$
\end_inset

 and 
\begin_inset Formula $R$
\end_inset

, but it conflicts wit 
\begin_inset Formula $Q$
\end_inset

 and 
\begin_inset Formula $R$
\end_inset

 in (
\begin_inset CommandInset ref
LatexCommand ref
reference "eq:model"

\end_inset

).
\end_layout

\begin_layout Standard
Following the standard dynamic programming approach, optimization of the
 loss function can be done recursively, as follows:
\begin_inset Formula \[
V(x_{t-1},u_{t-1})=\arg\min_{u_{t}}\mathsf{E}_{f(x_{t},y_{t}|x_{t-1})}\left\{ l(x_{t},u_{t})+V(x_{t},u_{t})\right\} ,\]

\end_inset

where 
\begin_inset Formula $V(x_{t},u_{t})$
\end_inset

 is the Bellman function.
 Since the model evolution is stochastic, we can reformulate it in terms
 of sufficient statistics, 
\begin_inset Formula $S$
\end_inset

 as follows:
\begin_inset Formula \[
V(S_{t-1})=\min_{u_{t}}\mathsf{E}_{f(x_{t},y_{t}|x_{t-1})}\left\{ l(x_{t},u_{t})+V(S_{t})\right\} .\]

\end_inset


\end_layout

\begin_layout Standard
Representation of the Bellman function depends on chosen approximation.
\end_layout

\begin_layout Subsection
LQG control
\end_layout

\begin_layout Standard
Control of linear state-space model with Gaussian noise
\begin_inset Formula \begin{eqnarray*}
x_{t} & = & Ax_{t-1}+Bu_{t}+Q^{\frac{1}{2}}v_{t},\\
y_{t} & = & Cx_{t}+Du_{t}+R^{\frac{1}{2}}w_{t}.\end{eqnarray*}

\end_inset

to minimize loss function
\begin_inset Formula \[
L_{t}=(x_{t}-\overline{x}_{t})'\Xi(x_{t}-\overline{x}_{t})+u_{t}'\Upsilon u_{t}.\]

\end_inset


\end_layout

\begin_layout Standard
Optimal solution in the sense of dynamic programming on horizon 
\begin_inset Formula $t+h$
\end_inset

 is:
\begin_inset Newline newline
\end_inset


\begin_inset Formula \begin{eqnarray*}
u_{t} & = & L_{t}\left(\hat{x}_{t}-\overline{x}_{t}\right),\\
L_{t} & = & -(B'S_{t+1}B+\Upsilon)^{-1}B'S_{t+1}A,\\
S_{t} & = & A'(S_{t+1}-S_{t+1}B(B'S_{t+1}B+\Upsilon)^{-1}B'S_{t+1})A+\Xi,\end{eqnarray*}

\end_inset

This solution is certainty equivalent, i.e.
 only the first moment, 
\begin_inset Formula $\hat{x}$
\end_inset

, of the Kalman filter is used.
\end_layout

\begin_layout Subsection
PI control
\end_layout

\begin_layout Standard
The classical control is based on transformation to 
\begin_inset Formula $dq$
\end_inset

 reference frame:
\begin_inset Formula \begin{eqnarray*}
i_{d} & = & i_{\alpha}\cos(\vartheta)+i_{\beta}\sin(\vartheta),\\
i_{q} & = & i_{\beta}\cos(\vartheta)-i_{\alpha}\sin(\vartheta).\end{eqnarray*}

\end_inset

Desired 
\begin_inset Formula $i_{q}$
\end_inset

 current, 
\begin_inset Formula $\overline{i}_{q}$
\end_inset

, is derived using PI controller
\begin_inset Formula \[
\overline{i}_{q}=PI(\overline{\omega}-\omega,P_{i},I_{i}).\]

\end_inset

This current needs to be achieved through voltages 
\begin_inset Formula $u_{d},u_{q}$
\end_inset

 which are again obtained from a PI controller
\begin_inset Formula \begin{eqnarray*}
u_{d} & = & PI(-i_{d},P_{u},I_{u}),\\
u_{q} & = & PI(\overline{i}_{q}-i_{q},P_{u},I_{u}).\end{eqnarray*}

\end_inset

These are compensated (for some reason) as follows:
\begin_inset Formula \begin{eqnarray*}
u_{d} & = & u_{d}-L_{S}\omega\overline{i}_{q},\\
u_{q} & = & u_{q}+\Psi_{pm}\omega.\end{eqnarray*}

\end_inset

Conversion to 
\begin_inset Formula $u_{\alpha},u_{\beta}$
\end_inset

 is 
\begin_inset Formula \begin{align*}
u_{\alpha} & =|U|\cos(\phi), & u_{\beta} & =|U|\sin(\phi)\\
|U| & =\sqrt{u_{d}^{2}+u_{q}^{2}}, & \phi & =\begin{cases}
\arctan(\frac{u_{q}}{u_{d}})+\vartheta & u_{d}\ge0\\
\arctan(\frac{u_{q}}{u_{d}})+\pi+\vartheta & u_{d}<0\end{cases}\end{align*}

\end_inset


\end_layout

\begin_layout Standard
PI controller is defined as follows:
\begin_inset Formula \begin{eqnarray*}
x & = & PI(\epsilon,P,I)\\
 & = & P\epsilon+I(S_{t-1}+\epsilon)\\
S_{t} & = & S_{t-1}+\epsilon\end{eqnarray*}

\end_inset

Constants for the system:
\begin_inset Formula \[
P_{i}=3,\,\, I_{i}=0.00375,\,\, P_{u}=20,\,\, I_{u}=0.5.\]

\end_inset

The requested values for 
\begin_inset Formula $\omega$
\end_inset

 should be kept in interval 
\begin_inset Formula $<-30,30>$
\end_inset

.
\end_layout

\begin_layout Subsection
Cautious LQG control
\end_layout

\begin_layout Standard
Uncertainty in 
\begin_inset Formula $A$
\end_inset

.
\end_layout

\begin_layout Standard
Sigma points: 
\begin_inset Formula $x^{(i)}=\hat{x}+hv_{i}$
\end_inset

, 
\begin_inset Formula $v_{i}$
\end_inset

 are eigenvectors of 
\begin_inset Formula $P$
\end_inset

.
\end_layout

\begin_layout Standard
\begin_inset Formula \begin{eqnarray*}
E\{x'A(x)QA(x)x\} & = & \frac{1}{n}\sum x'A(x^{(i)})QA^{(i)}(x)x\\
 & = & x'Zx'\end{eqnarray*}

\end_inset


\end_layout

\begin_layout Standard
Uncented transform...
\end_layout

\begin_layout Subsection
Poor-man's dual LQG control
\end_layout

\begin_layout Standard
Various heuristic solutions to dual extension of LQG has been proposed.
 Most of them is based on approximation of the loss function 
\begin_inset Formula \[
L_{t}=(x_{t}-\overline{x}_{t})'\Xi(x_{t}-\overline{x}_{t})+(u_{t}-\overline{u}_{t})'\Upsilon(u_{t}-\overline{u}_{t})+DUAL\_TERM.\]

\end_inset

where DUAL_TERM is typically a function of 
\begin_inset Formula $P_{t+2}$
\end_inset

.
 
\end_layout

\begin_layout Standard
To be continued...
\end_layout

\begin_layout Subsection
Test Scenarios
\end_layout

\begin_layout Standard
With almost full information, design of the control strategy should be almost
 trivial:
\begin_inset Formula \begin{eqnarray*}
\hat{\isa{}} & = & 0,\,\hat{\isb{}}=0,\hat{\omega}=1,\th=\frac{\pi}{2},\\
P_{t} & = & \mathrm{diag}([0.01,0.01,0.01,0.01]).\end{eqnarray*}

\end_inset


\end_layout

\begin_layout Standard
The difficulty arise with growing initial covariance matrix:
\begin_inset Formula \begin{eqnarray*}
\hat{\isa{}} & = & 0,\,\hat{\isb{}}=0,\hat{\omega}=1,\th=\frac{\pi}{2},\\
P_{t} & = & \mathrm{diag}([0.01,0.01,0.01,1]).\end{eqnarray*}

\end_inset


\end_layout

\begin_layout Standard
Or even worse:
\begin_inset Formula \begin{eqnarray*}
\hat{\isa{}} & = & 0,\,\hat{\isb{}}=0,\hat{\omega}=1,\th=\frac{\pi}{2},\\
P_{t} & = & \mathrm{diag}([0.01,0.01,0.01,10]).\end{eqnarray*}

\end_inset

==\SpecialChar \-
=
\end_layout

\begin_layout Standard
The requested value 
\begin_inset Formula $\overline{\omega}_{t}=1.0015.$
\end_inset


\end_layout

\begin_layout Conjecture
It is sufficient to consider hyper-state 
\begin_inset Formula $H=[\hat{i}_{\alpha},\hat{i}_{\beta},\hat{\omega},\hat{\vartheta},P(3,3),P(4,4)]$
\end_inset

.
\end_layout

\begin_layout Conjecture
\begin_inset CommandInset bibtex
LatexCommand bibtex
bibfiles "bibtex/vs,bibtex/vs-world,bibtex/world_classics,bibtex/world,new_bib_PS"
options "plain"

\end_inset


\end_layout

\end_body
\end_document
