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<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>Qualitative evaluation of the process of functionally stable recovery control of the aircraft in emergencies with an algorithm based on solving inverse dynamic problems</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>State Ecology Academy of Postgraduate Education</string-name>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Management</string-name>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Ukraine mashkov_oleg_</string-name>
        </contrib>
        <contrib contrib-type="author">
          <string-name>@ukr.net</string-name>
          <email>chumakevich@ukr.net</email>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Lviv National Agrarian University</institution>
          ,
          <addr-line>Lviv</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>Lviv Polytechnic National University</institution>
          ,
          <addr-line>Lviv</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
        <aff id="aff2">
          <label>2</label>
          <institution>Zhytomyr Polytechnic State University</institution>
          ,
          <addr-line>Zhytomyr</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
      </contrib-group>
      <abstract>
        <p>The influence of the input data and a Hurwitz matrix on the stability of the system in general is investigated. The factors that influence the behavior and timing of the transient process are analyzed. An expression is obtained for finding the time of the transient process as well as its dependence on the parameters of the Hurwitz matrix.</p>
      </abstract>
      <kwd-group>
        <kwd>functional stability</kwd>
        <kwd>recovery control</kwd>
        <kwd>emergency</kwd>
        <kwd>inverse dynamic problem</kwd>
        <kwd>operationally programmed trajectory</kwd>
        <kwd>transient process</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>-</title>
      <p>
        Functional stability theory originated in the 1980s [
        <xref ref-type="bibr" rid="ref1 ref2 ref3 ref4 ref5">1–5</xref>
        ] and was used to control
complex dynamic objects and computing systems. This theory makes it possible to
respond promptly to system and block failures, to redistribute the functions of the failed
blocks between those capable of performing the final task [
        <xref ref-type="bibr" rid="ref10 ref11 ref12 ref4 ref5 ref6 ref7 ref8 ref9">4–12</xref>
        ]. The use of this
theory was limited by the capacities of computing systems and by the need to reserve
the main blocks of the control system. For this reason, this theory was used for the
control systems of large aircraft. With progress, the dimensions of control systems
elements have decreased and the characteristics of computing systems have improved
significantly, so this theory has evolved significantly and has become applicable to
complex dynamic control objects of a broader purpose [
        <xref ref-type="bibr" rid="ref13 ref14 ref15 ref16 ref17 ref18 ref19 ref20 ref6 ref7 ref8 ref9">6–9, 13–20,</xref>
        ].
      </p>
      <p>The dynamic object (Fig. 1) is written in the form of linear difference equations:</p>
      <p>Q( q )y( n )  qk Pu ( q )U( n )  P ( q ) ( n ) ,
where y(n) – initial value;</p>
    </sec>
    <sec id="sec-2">
      <title>U(n) – control influence; ξ(n) – external influence (disturbance);</title>
      <p>Q(q), Pu(q), Pξ(q) – polynomials of q; an, bn, cn;
q; an, bn, cn – coefficients of polynomials;
q – delay operator: qmχ(n) = χ(n–m) (sometimes the delay operator q–1 is used in the
literature, so q–mχ(n) = χ(n–m)).</p>
      <p>The control device (Fig. 2) is described as:</p>
      <p>R( q )U( n )  Pr ( q )r( n )  Py ( q )y( n ) ,
where r(n) – input influence.</p>
      <p>G(q) y(n)  qk 1Pu (q)Pr (q)r(n)  P (q)R(q)(n)</p>
      <p>In functionally stable systems, vector of reducing filter parameters (Fig. 4) must
change so as to ensure the optimality of the whole system over time.</p>
      <p>To solve this problem we will use the method of inverse dynamics problems
(Fig. 5).</p>
      <p>
        Description of the mathematical model
The mathematical description is based on the matrix equations of the form [
        <xref ref-type="bibr" rid="ref18 ref19 ref4 ref6 ref8">4, 6, 8, 18,
19</xref>
        ]:
      </p>
      <p>X (t)  F[ X (t),U (t), Z (t)]  P(t);</p>
      <p>X (t0 )  X 0,
t [t0, tT ],
(1)
where U(t) is a vector of control;
Z(t) is a vector of the object parameters;
P(t) is a vector of disturbances acting on the object;
X0 is the initial conditions.</p>
      <p>The presented theory is intended to provide a given programmatic movement
(state) of the object of control and may provide for solving the problems of
stabilization, terminal control, and adaptive tracking (Fig. 6). An object that can be described
by the system (1) must be on a given trajectory (correspond to a certain state) and
provide a minimum of the functionality of quality:</p>
      <p>
        J[Un0 (), X n0 ()]  min J[Un (), X n ()] ,
(2)
where X n0 (t) , U n0 (t) are optimal vectors of state and control.
In Refs. [
        <xref ref-type="bibr" rid="ref18 ref19 ref20">18–20</xref>
        ], examples of synthesis of functionally stable automatic systems for
stabilization of motion of dynamic objects based on the solving inverse problems of
dynamics are presented. To evaluate the quality of such systems, it is necessary to
evaluate their resilience and the characteristics of the transients.
      </p>
      <p>The system of matrix differential Eq. 1 can be represented as a structural diagram
(Fig. 7).</p>
      <p>To solve the problem, we assume that the programmatic movement is
asymptotically stable.</p>
      <p>The following conditions are imposed on this class of controlled dynamic systems.
1. There is a subspace R  Rm × Rn and a unique function U : R × Ξ → Rm such
that for any pair of points {X, Z}  R and the point {ξ}  Ξ, the identity is satisfied
Z  F[ X , U (x, z, ),  ] ,
(3)
i.e., Eq. 1 can be solved with respect to control on the subspace R.</p>
      <p>The condition (3) guarantees the existence and uniqueness of an ideal
programmatic control law of the form Un = Un(Xn, Ẋn, Ξ), which ensures the accurate
implementation of programmatic movement provided Xn(t0) = X0; P(t) = 0; (Xn(t), Ẋn(t))  R
t [t0 ,tT ] .</p>
      <p>
        2. The following restrictions are imposed on the initial and constant external
disturbances [
        <xref ref-type="bibr" rid="ref1 ref18 ref19 ref2 ref3 ref4">1–4, 18, 19</xref>
        ]:
      </p>
      <p>X (t0 )  X n (t0)   0;</p>
      <p>P(t)  C p ,
(4)
where δ0, Cp are positive parameters.</p>
      <p>3. There is a Hurwitz matrix Г with prime eigenvalues γi
where X(t0) = X0 is the determined initial vector of state;</p>
      <p>X  X ,
(5)
(6)
(7)
(8)
(9)
γi are the roots of the characteristic equation of the system, i  1, n , for any X  Rn,
the condition holds:</p>
    </sec>
    <sec id="sec-3">
      <title>4. For t  [t, ∞], the control law</title>
      <p>( X , X n (t)  ( X  X n (t)))  R , t  t0 .</p>
      <p>U (t, X )  U[ X , X n  ( X  X n ), ] .</p>
      <p>For any disturbances that satisfy the condition (4), the movement X(t) (X(t0)  R)
asymptotically approaches a determined programmatic movement Xn(t), i.e., it
provides the asymptotic stability of the programmatic movement in general.</p>
      <p>From the expressions (1), (3), (6), we find</p>
    </sec>
    <sec id="sec-4">
      <title>Thus, we can write it down</title>
      <p>F[ X (t),U (t), ]  X  X n (t)  ( X  X n (t)) .</p>
      <p>X  X n (t)  ( X  X 0 ) .</p>
      <p>
        Due to the selection of the Hurwitz matrix Г, the required transient process is
provided [
        <xref ref-type="bibr" rid="ref1 ref14 ref2 ref3 ref4">1–4, 14</xref>
        ]. For the system (9), the roots of the characteristic equation determine
the stability of the system in general. If Re γi &lt; 0, i  1, n , the roots have negative real
parts, the trivial solution of the system is unstable. When the roots do not have a
positive real part, but at least one with a zero real part, the system is on the limit of
stability.
      </p>
      <p>According to the condition (6), the matrix is chosen with prime eigenvalues, then
there are positive numbers C and γ such that</p>
      <p>Re i   , X (t)  X n (t)  C X (t0 )  X n (t0 ) e (t t0 ) , t  t0.
(10)</p>
      <p>Thus, the programmatic movement in general will be asymptotically stable.
4</p>
      <p>Results and Discussions
Let us give an estimate of the maximum time of the transient process</p>
      <p>Case 1. external influences are absent π(t) = 0.</p>
      <p>
        Let the law of control that guarantees for any ξ  Ξ, π(t)  Qπ (ε is the closeness of
real and programmatic movements [
        <xref ref-type="bibr" rid="ref18 ref19 ref4 ref6">4, 6, 18, 19</xref>
        ], starting from the end time moment
tn &gt; t0) be synthesized, i.e.,
      </p>
      <p>The expression (11), given the expression (10), can be represented in the form:
hence</p>
      <p>X (t)  X n (t)   , t  tn .</p>
      <p>C X (t0 )  X n (t) e (tn t0)   ,</p>
      <p>C

 (tn  t0 )  ln</p>
      <p>X (t0 )  X n (t0 ) .</p>
      <p>Tn   1 ln</p>
      <p>C X (t0 )  X n (t0 )

.</p>
      <p>(11)
(12)
(13)
(14)
Denote as Tn = tn – t0 the time of the transient process in the system.</p>
      <p>The time Tn of the transient process can be estimated using the expression (13)
Case 2. External disturbances occur π(t)≠ 0.</p>
      <p>Let the controlled object be
X (t)  F[ X (t),U (t), ]  (t), X(t0) =X0,
X n (t)  ( X  X n ) QX .</p>
      <p>described
t  [t0,
tn].</p>
      <p>by</p>
      <p>the</p>
    </sec>
    <sec id="sec-5">
      <title>Moreover, equation</title>
      <p>X  QX,</p>
      <p>The control U is of the chosen form: U (t, X )  U[ X , X n  ( X  X n ), ] ,
t  [t0, ∞).</p>
      <p>The equations of the
X (t)  X n (t)  [ X (t)  X n (t)]  (t) .</p>
      <p>Suppose that Xn(t) and Ẋn(t) both lie on sets QX and QẊ with stocks δ1 and δ2,
respectively (Fig. 8), when
closed-loop
system
have
the
form:
1  C X0  X n (t0 ) ,  2  C X0  X n (t0 )   ,
or given   0.</p>
      <p>1  C X 0  X n (t0 )  0 ,
 2  1  C X 0  X n (t0 )  0 .
(15)
(16)
(17)</p>
      <p>X  min[1  C X 0  X n (t0 ) , 2  1  C X 0  X n (t0 ) ] ,</p>
      <p>Hence, given (20), it follows: C X 0  X n (t0 ) e (tt0 )  C 1C   .
Solving
the
obtained
inequality
with
respect
to
t = tn,
we
find
  C 1C  C X 0  X n (t0 ) e (tn t0) .
(20)
(21)
(22)
(23)
(24)</p>
    </sec>
    <sec id="sec-6">
      <title>The time of the transient process:</title>
      <p>tn  t0  1 ln</p>
      <p>C X 0  X n (t0 )
  C 1C</p>
      <p>.</p>
      <p>Tn   1 ln C X0  X n (t0) .</p>
      <p>  C 1C</p>
      <p>Comparing the expression (23) with the expression (14), we can conclude that in
the presence of external disturbances, the time of transient process increases
Tn (C  0)  Tn (C  0)   1 ln</p>
      <p>
  C 1C
.</p>
      <p>With great disturbances (increase in Cπ), the time of transient process increases
significantly.</p>
      <p>To reduce the time of the transient process in the system, it is necessary to increase
γ by means of an appropriate choice of control.
5</p>
      <p>Conclusions
For a multidimensional controlled object, satisfying det C ≠ 0, the structure of the
control algorithm does not explicitly contain the equation of motion of the object. The
proposed approach to the construction of control algorithms allows obtaining
algorithms without using detailed equations of the controlled process. Moreover, it is
sufficient to use as a mathematical model the generalized equations that reflect the
fundamental laws of motion.</p>
      <p>To synthesize the aircraft control algorithms, complete nonlinear equations of
motion can be used without linearizing them. The resulting algorithms are also nonlinear.
Their structure is adequate to the structure of mathematical models of controlled
processes, and the parameters of these algorithms are determined by the parameters of
mathematical models of assigned motion trajectories.</p>
      <p>In essence, the construction of aircraft motion control algorithms along the
assigned trajectory has two aspects. The first one is related to the direct formation of the
vector of the required control force f*[x], and the other is related to the calculation of
the values of the elements of the vector of the control function Un(t) that creates the
necessary force f*. The calculation relations according to which f* and Un(t) are
calculated form the contents of the motion control algorithm.</p>
      <p>The coefficients of the control system are determined by the basic parameters of
the motion of the object, as well as by the parameters of the assigned program
trajectory. This allows changing the parameters of the programmatic trajectory in the object
movement.</p>
    </sec>
  </body>
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