<!DOCTYPE article PUBLIC "-//NLM//DTD JATS (Z39.96) Journal Archiving and Interchange DTD v1.0 20120330//EN" "JATS-archivearticle1.dtd">
<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>Method of statistical spline functions for solving problems of data approximation and prediction of objects state</article-title>
      </title-group>
      <contrib-group>
        <aff id="aff0">
          <label>0</label>
          <institution>Institute of Engineering Thermophysics of NAS of Ukraine</institution>
          ,
          <addr-line>Kyiv</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>University of Emerging Technologies</institution>
          ,
          <addr-line>Kyiv</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
      </contrib-group>
      <fpage>0000</fpage>
      <lpage>0001</lpage>
      <abstract>
        <p>The method of statistical spline functions is considered for problems of predicting the state of complex technical objects using the example of power transmission lines. The choice of parameters of spline fragments for building an adequate mathematical model is analyzed. Based on the experimental data, a short-term spline forecast of heating of overhead power lines has been created.</p>
      </abstract>
      <kwd-group>
        <kwd>spline functions</kwd>
        <kwd>mathematical model</kwd>
        <kwd>overhead power lines</kwd>
        <kwd>prediction</kwd>
        <kwd>technical state</kwd>
        <kwd>diagnostics</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>Introduction</title>
      <p>The basic idea of using the mathematical apparatus of statistical spline functions for
processing the spatial characteristics of a field is that some numerical characteristics
of physical processes change during the observation process (meteorological fields,
airspace in the vicinity of energy facilities, navigation space, etc.) for any
circumstances [1, 2, 3].</p>
      <p>Regular observations of the history of gradual changes in these parameters over
time provide an opportunity to obtain information on the trends of further changes in
the studied parameters and to predict the behavior of the field at certain points [4]. For
example, using the spline function algorithm, it can monitor and predict the
temperature at a particular point in the airspace [5]. Such a problem arises during temperature
control equipment of overhead power lines (OPL) using thermal imaging equipment
installed on the unmanned aerial vehicles (UAV) [6, 7].</p>
      <p>Using the spline functions, the problem of predict ting electrical equipment failures
is also solved. In this case, the main idea of predicting failures is that some numerical
characteristics of physical processes occurring in certain nodes of electrical
equipment change during the occurrence or development of faults and defects, which
allows to identify them [8, 9]. Observations of their gradual change in time provide
information on the development trends of the defect and provide a prediction of the
possible moment of failure [10, 11].</p>
      <p>In work the forecasting of values of temperature in certain points of an
arrangement of the equipment of the OPL will be considered. Due to a significant
temperature increase, failures of individual blocks of OPL are possible. So, the sharp heating
of metal wires of OPL can lead to sagging and short circuit on the earth. The
temperature factor may contribute to the occurrence of a breakdown or overlap of insulators
of OPL. It is also possible breakdown of insulators due to contamination of their
surface, or aging of the materials from which they are made. In addition, due to various
reasons, accumulation of microdefects can occur in the insulator material, which
contributes to their breakdown [12, 13, 14].</p>
      <p>The listed defects of equipment of OPL in the course of their operation can lead to
the emergence of so-called gradual failures. Accidental failures caused by
unpredictable factors (for example, the overlap of insulation of OPL by birds or animals) will
not be considered.
2
2.1</p>
    </sec>
    <sec id="sec-2">
      <title>Features of spline functions</title>
      <p>Mathematical model
To predict the possible failure of a selected node, you additionally need to have
statistics on the values of the monitored parameter for a certain period of time, which is
called the observation interval.</p>
      <p>Let some functional dependence be given on the segment</p>
      <p>
        y  f  x , A , x a, b , (
        <xref ref-type="bibr" rid="ref1">1</xref>
        )
where A is the deterministic vector of unknown real numeric parameters entering
linearly in y and do not depend on x.
      </p>
      <p>At given points x i a,b  , i  1, n , random uncorrelated values of the function y
are observed, which we denote as  y i , i  1, n . For definiteness, we assume that
these observations are distributed according to the normal law, and
M y i  x i 0 a 0  x i1 a1    x i r a r

D y i   2 , i  1, n
where</p>
      <p>A   a1 , a 2 ,  , a r 
and
σ
are
unknown
parameters,
X  x i j , i  1, n ; j  0, r is a rectangular matrix of deterministic coefficients,
functionally dependent from xi and, as a rule, is called the planning matrix. It should
also be noted that the dependence of these coefficients from xi is not necessarily
linear.</p>
      <p>
        If we assume that Y and A are column vectors, which will be provided below, then
(
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) can be written in vector form: M Y  X A , DY   2 I . Here, M and D are the
expectation and variance operators, and I is the n-th unit matrix order.
      </p>
      <p>
        The paper considers the problem of constructing a statistical estimate of the
unknown parameters a j , j  1, r from the results of observations  y i , i  1, n . In
this case, an arbitrary choice of elements of the planning matrix X is allowed. If
nothing is assumed about the distribution of observation errors or observations
(
        <xref ref-type="bibr" rid="ref2">2</xref>
        )
 y i , i  1, n , then as a result of solving this problem the largest, what can we
expect, is the construction of point estimates for elements A. Under the assumption that
the distribution law of observations is normal, we can obtain a confidence interval for
the estimated parameters.
      </p>
      <p>Considering that in the task set the question of introducing the planning matrix is
solved in an arbitrary way, we specify this task by refining the choice of the planning
matrix X. At the same time, we construct statistical estimates of the A parameters
using the least squares method, which in the case of normally distributed yi leads to
the same result as maximum likelihood estimation.</p>
      <p>Concretization in the choice of the planning matrix, first of all, is connected with
the choice of the upcoming functions. The task was traditionally solved in the class of
polynomials. But polynomial approximations have several disadvantages, the most
significant of which is that the sequence of interpolation polynomials does not always
converge to the interpolated function. Therefore, in many problems, the more natural
and convenient approximation apparatus turned out to be splines, with the help of
which we will solve the problem posed.</p>
      <p>Splines are functions that are “glued together” from pieces of various functions in a
specific pattern. Polynomial splines “stick together” from pieces of various
polynomials in such a way as to ensure the necessary smoothness of the resulting spline. The
simplest example of a polynomial spline is a broken line.</p>
      <p>Let the grid be set on the segment a,b , a, b  R  , a  b (partition):
 n : a  x 0  x1    x n  x n  1  b ,
where n  N .</p>
      <p>Let also P m is the set of polynomials of degree not higher than m, m  0 , and
C k  C k a, b is the set of functions continuous on a , b that have a continuous
k-th derivative, k  Z  ; R  is the set of positive numbers; N is the set of natural
numbers; Z  is the set of positive integers.</p>
      <p>
        The function S m  x  S m,k  x ,  n  is called a polynomial spline of degree m of
defect k (1  k  m ) with nodes (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ), if
 Sm  x  Pm , x  xi , xi1  , i  0, r 1 ,
 Sm  x  Cmk a, b .
      </p>
      <p>The points x i  are called spline nodes, the m  k  1 -th derivative of S m  x
can be discontinuous on the segment a, b . Basically, it takes k = 1. There is a
representation (with a fixed grid  n ):</p>
      <p>
        m n  1 m
S m  x  S m, k  x,  n    a s x s   
s  0 s  1 r  m k  1
a r ,s  x  x s  r ,
where  x  x s  r  max 0, x  x s  r is a Peano’s core.
(
        <xref ref-type="bibr" rid="ref3">3</xref>
        )
(
        <xref ref-type="bibr" rid="ref4">4</xref>
        )
      </p>
      <p>The coefficients a s and a r, s can take arbitrary values from R; the set
S m,k  x ,  n  with a fixed  n is linear with dimension m  1  n k . Therefore, for an
unambiguous definition of a spline, it is necessary to specify m  1  n k independent
conditions. For a linear spline this is n  2 , that is, for the statistics obtained, the
number of parameters that need to be estimated is found from condition r  n  2 .</p>
      <p>
        Thus, under the conditions of the formulated problem, it is necessary on the
segment a , b for given r to find a grid x j  r such that the spline
Sk  1  x  C ka, b , k  0,1, , constructed on the grid  r provides the minimum
(in terms of standard quadratic deviations) statistical estimate of the vector A, that is,
we assume that
r
 x i1 a 1    x i r  S k  1  x i  , i  1, n . (
        <xref ref-type="bibr" rid="ref5">5</xref>
        )
j  1
The equations written in the matrix form
      </p>
      <p>
        X * X A  X * Y (
        <xref ref-type="bibr" rid="ref6">6</xref>
        )
are called normal. They are obtained by minimizing the sum of squared differences
between observations and their mathematical expectations:
      </p>
      <p>n
Y  X A * Y  X A    y i  x i1 a 1    x i r a r  2 </p>
      <p>i  1
n
   y i  S k  1  x i  2</p>
      <p>i  1</p>
      <p>
        As the estimated parameters of the spline, the a j ordinates of the nodes of the grid
 r are chosen, whose estimates are now determined by solving the normal equations
(
        <xref ref-type="bibr" rid="ref6">6</xref>
        ) in the matrix form
0
0

0
0 
0 
 
0 
0 
 
0 
 
 c r  2 r  2
 c r  1 r  2
 0
s j 1
 x i j x i j  1 
i  1  s j
c j  m j  c j j  m  0 at m  2 , j  0 , r  2 ,
s j 1  x j  1  x i   x i  x j  , j  0 , r  1 ,

i  1  s j  x j  1  x j  2
,
j
and x i are the elements of the source data (experimental points), S j   k m ,
m  1
j  1 , r , s 0  0 , s r  n . The matrix C is rectangular r  1  r  1 .
      </p>
      <p>
        The above relations are obtained by directly multiplying the matrices X  and X
with (
        <xref ref-type="bibr" rid="ref9">9</xref>
        ) taken into account.
      </p>
      <p>Let us briefly discuss some properties of the matrix C.
1. The sum of the diagonal elements of the matrix C is equal to the sum of the squares
of all the elements of the planning matrix X, that is,
r c j j  n r x i2j  n   x 1  x i1  2 I x i1  x1  
j  0 i  1 j  1 i  1   x 1  x 0 
  x r  1  x i r  2 I x iir   x r  
 x r  x r  1 </p>
      <p></p>
      <p>
        The recurrence formula (
        <xref ref-type="bibr" rid="ref13">13</xref>
        ) can be obtained by direct calculation, by decomposing
the C row (or column) in r  1 minors.
      </p>
      <p>
        Thus, if for generalization we denote C 1  c 00 , then to calculate the determinant
of the matrix C, we obtain the following recurrence relations
 C 0  1; C 1  c 00 ;
 j  1, r . (
        <xref ref-type="bibr" rid="ref14">14</xref>
        )
 C j  1  c j j C j  c 2j j  1 C j  1 ;
      </p>
      <p>
        It can construct recurrent formulas for finding the elements of the inverse matrix C.
Let us briefly discuss the construction of these formulas. The determinant C r  1 is
calculated by the recurrent formula (
        <xref ref-type="bibr" rid="ref14">14</xref>
        ).
      </p>
      <p>
        The algebraic complement of the element c min which located on the main diagonal
is equal to the multiplication of two determinants similar in structure to the
determinant of the matrix and calculated by recurrent formulas (
        <xref ref-type="bibr" rid="ref14">14</xref>
        ), which in this case take
the form
 C 0  1; C 1  c 00 ;
 C j  1  c j j C j  c 2j j  1 C j  1 ;
 C 0  1; C 1  c r r ;
 C j  1  c r  j r  j C j  c r2  j r  j  1 C j  1 ;

j  1, m  1 ;
      </p>
      <p>j  1 , r  m  1 ,</p>
      <p>C j j  C j C r  1 .</p>
      <p>The ratio for calculating the algebraic complements of the elements of the matrix C
that are not on the main diagonal is calculated by the ratio
where C j is the determinant of the matrix obtained with C by crossing out the first
r  j  1 g rows and first r  j  1 columns in it.</p>
      <p>The recurrence formulas (15) allow to find the corresponding determinants of the
matrices C r  m</p>
      <p>
        moving in the direction of the main diagonal from the periphery
inward towards the center of the matrix. These formulas can also be rewritten in
another form, using the movement from the middle to the periphery, namely, taking into
account (
        <xref ref-type="bibr" rid="ref14">14</xref>
        ) we have
(15)
(16)
(17)
 C 0  1; C 1  c m  1m  1 ;
 2
 C j  1  c m  1  j m  1  j C j  c m  1  j m  j C j  1 ;
j  1, m  1 ;
 C 0  1; C 1  c m  1m 1 ;
 2 j  1 , r  m  1 ,
 C j  1  c m  1  j m  1  j C j  c m  1  j m  j C j  1 ;

and now C j is the determinant of the matrix obtained by crossing out the first rows
j  1 and columns in the C matrix and r  m  1 last rows and columns, and C j is
the determinant of the matrix obtained from the matrix C by crossing out m  1 first
rows and columns and r  j  1 last rows and columns, C j and C j are the main
minors of the matrix.
      </p>
      <p>It should be noted that the final results of calculations by the recurrence relation
(15) and (16) for a fixed matrix are the same, and the intermediate ones may differ.</p>
      <p>Thus, the algebraic complement of the element of the matrix C, standing on the
main diagonal, is determined by the ratio
where X  is the matrix transposed with respect to the planning matrix, and Y
(matrix-column) is the output of the observations.</p>
      <p>The elements of the matrix H are defined as follows.</p>
      <p>k 1 k 1  x 1  x i  y i ;
h 0   x i 0 y i  </p>
      <p>i  1 i  1 x 1  x 0
h j 
s j 1

i  1  s j 1
x i j y i 
 x j  1  x i  y i 
x j  x j  1
s j 1  x j  1  x i  y i

i  1  s j 1 x j  1  x j
;
  i  2 
c j i  1 i  j 1  sign i  j   C p p  1  1 C j C r  1 , j  i  0 , r ;
   p  j 
 c j i  c i j , r  1.</p>
      <p>Denote by H the matrix, which is determined by the expression</p>
      <p>H  X  Y .</p>
      <p>The accuracy of approximation of the desired dependence using the selected spline
is estimated by the sum of the squares of the deviations of the ordinates of the
observation points from the found dependence</p>
      <p> a j x u  x j  1   a j  1  x j  x u 
r s j 
d  j 1 u  1 s j 1  x j  x j  1  y u  2 . (22)
The confidence interval for the found estimates of a j is calculated by the formula
 x r  1  x i  y i
n n
h j   x i r y i   ; j  1, r  1 .</p>
      <p>i  1  n  k r i  1  n  k r x r  x r  1</p>
      <p>Then the estimates of the ordinates of the points of connection of the linear parts of
the spline (the elements of the A matrix-column) are determined by the formula
a i  C 1 j i h j , i  0 , r .</p>
      <p>
I j  a j   

 C 1
d </p>
      <p> .
j j n  r 1 
where   is a value that satisfies the relation P tnr1      1  , if the random
variable tnr1 is distributed according to Student's law with n  r 1 degrees of
freedom; d is the sum of the squares of the deviations of the observations yi s from the
values of the resulting spline at the corresponding points.</p>
      <p>The prediction of the confidence interval for the values of the function xt  at the
point x r  1 is carried out by enumerating all the splines and choosing one that
minimizes this interval at the prediction point. In this case, the spline itself, in the
meansquare sense, is closer to the points, and is observed experimentally.</p>
      <p>The relation (23) allows to build confidence intervals in each node of the spline,
and on the whole interval - a confidence corridor.</p>
      <p>
        To obtain a forecast using a statistical spline, an additional node is introduced to
the set of nodes of the spline, the abscissa of which corresponds to the forecast
interval. Using a computer search method, a grid is selected that satisfies equation (
        <xref ref-type="bibr" rid="ref8">8</xref>
        ) and
at the same time minimizes it on the set of possible non-uniform grids and the width
of the confidence interval in the forecast node.
      </p>
      <p>As a result, the expected value and the confidence interval for the selected
controlled parameter at the end of the forecast interval will be obtained. The boundaries
of the confidence corridor are formed by linear interpolation of the upper and lower
boundaries of the confidence intervals in all nodes of the resulting spline, including
the forecast node.
 the number of temperature measurements n  11 (in our case);
 the number of hours of the forecast n for  3 ;
 the number of intervals, interpolates spline r  5 ;
 the number of intervals of the time interval, on which the temperature is measured
(the breakdown is performed in order to find the optimal interpolation spline),
n break  10 ;
 confidence probability of estimating the prediction of the length of the time
interval to reach the critical temperature of the power lines, P  0.95 .</p>
      <p>As a result of the calculation of the program we obtain the data that are presented
in Table 1 and in Fig. 1.</p>
      <p>The graph presented in Fig. 1 is a spline approximation in the form of a channel
consisting of six sections. The spline docking points at the upper boundary of the
channel are designated 1u - 7u (these points are denoted by the symbol Δ), and at the
lower boundary 1d - 7d (the symbol is used to designate these points). In the main line
of approximation, the notation □ is selected for the designation of docking points.</p>
      <p>The width of the channel is determined by the adopted confidence probability
P=0.95. Sections 1 - 6 of the graph characterize the observation interval ΔTobserv, and
sections 6 - 7 characterize the forecast interval ΔTforecast. The forecast was carried out
at 3:00 ahead regarding to14:00 hours, the last point from the observation interval. As
can be seen from the graph, with an increase in the time interval of the forecast, its
upper and lower limits expand, that is, the probability of the forecast decreases with
increasing time.</p>
      <p>The statistical spline (Fig. 1) is based on the results of observation of the values of
the temperature of wires in OPL, which is in operation. Temperature measurement
was carried out on the time interval T observ  9 14 every 0.5 hours using a thermal
imager mounted on the UAV. The quantitative values of the measured temperature,
given in the bottom line of the table, are shown on the graph as black dots located on
the observation interval ΔTobserv.</p>
      <p>A spline was built (Fig. 1), divided into two sections, namely, the section where
interpolation of the data on the measured temperature of the power transmission lines
over the time interval T observ  9  14 and section T forecast 14 17 was carried
out with the given probability (P = 0.95). The predicted value of the time interval
T cr where the temperature of OPL can reach a critical level is determined by the
length of the time interval between the points of intersection of the temperature limit
line with the upper tup and lower td boundaries of the constructed spline. The threshold
temperature value line tlim=70oC is constructed parallel to the x-axis in accordance
with the existing regulatory documents on the operation of OPL. In fig. 1 the
predicted length T cr is indicated by a black line with arrows.</p>
      <p>In order to verify the performance of the proposed method for predicting the
possible values of the temperature of power lines, an experimental measurement of the
temperature of these wires in the time period was carried out using the UAV, which
corresponds to the forecast interval T forecast . The data of the results of these
measurements (6 points denoted by ○) is plotted on a specified interval T forecast of the
graph. Almost all (except for one point, the temperature value, which was measured at
T=1700), experimental data were obtained that did not exceed the upper and lower
limits of the constructed spline forecast. This confirms the efficiency of the proposed
method for predicting the values of the time interval in which the wires of OPL can
reach unacceptable temperature values.</p>
      <p>Based on the constructed spline forecast, the time interval when the power
transmission lines can reach the maximum permissible temperature value of 70 °C is
between 3:00 pm and 4:45 pm with a confidence level of P = 0.95. It should also be
emphasized once again that the achievement of such a temperature can occur only
under constant conditions of operation of OPL.</p>
      <p>During constructing a short-term spline forecast, it was assumed that the heating of
the wires was caused by the random nature of changes in the load of OPL and the
invariance of other (primarily meteorological) conditions during the entire
observation interval.
3</p>
    </sec>
    <sec id="sec-3">
      <title>Conclusions</title>
      <p>It has been experimentally confirmed that using the method of statistical spline
functions in combination with new information technologies implemented using UAV and
maintaining unchanged meteorological conditions, allows a short-term forecasting of
the time interval during which the OPL can reach critical temperatures with a given
probability.</p>
    </sec>
  </body>
  <back>
    <ref-list>
      <ref id="ref1">
        <mixed-citation>
          1.
          <string-name>
            <surname>Velimirovic</surname>
            ,
            <given-names>L.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Peric</surname>
            ,
            <given-names>Z.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Stankovic</surname>
            ,
            <given-names>M.</given-names>
          </string-name>
          :
          <article-title>Approximation of the optimal compressor function combining different spline functions in segments</article-title>
          .
          <source>2013 11th International Conference on Telecommunications in Modern Satellite, Cable and Broadcasting Services (TELSIKS)</source>
          ,
          <fpage>16</fpage>
          -
          <lpage>19</lpage>
          October,
          <year>2013</year>
          , Nis, Serbia. doi:
          <volume>10</volume>
          .1109/TELSKS.
          <year>2013</year>
          .6704436
        </mixed-citation>
      </ref>
      <ref id="ref2">
        <mixed-citation>
          2.
          <string-name>
            <surname>Kabore</surname>
            ,
            <given-names>P.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Wang</surname>
          </string-name>
          , H.:
          <article-title>A B-spline neural network based actuator fault diagnosis in nonlinear systems</article-title>
          .
          <source>Proceedings of the 2001 American Control Conference</source>
          . (Cat No.
          <year>01CH37148</year>
          )
          <fpage>25</fpage>
          -
          <lpage>27</lpage>
          June,
          <year>2001</year>
          , Arlington,
          <string-name>
            <surname>VA</surname>
          </string-name>
          , USA. doi:
          <volume>10</volume>
          .1109/ACC.
          <year>2001</year>
          .945873
        </mixed-citation>
      </ref>
      <ref id="ref3">
        <mixed-citation>
          3.
          <string-name>
            <surname>Zaporozhets</surname>
            ,
            <given-names>A.A.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Eremenko</surname>
            ,
            <given-names>V.S.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Serhiienko</surname>
            ,
            <given-names>R.V.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Ivanov</surname>
            ,
            <given-names>S.A.</given-names>
          </string-name>
          :
          <article-title>Development of an Intelligent System for Diagnosing the Technical Condition of the Heat Power Equipment</article-title>
          .
          <source>2018 IEEE 13th International Scientific and Technical Conference on Computer Sciences and Information Technologies (CSIT)</source>
          ,
          <fpage>11</fpage>
          -
          <lpage>14</lpage>
          September,
          <year>2018</year>
          , Lviv, Ukraine. doi:
          <volume>10</volume>
          .1109/STC-CSIT.
          <year>2018</year>
          .8526742
        </mixed-citation>
      </ref>
      <ref id="ref4">
        <mixed-citation>
          4.
          <string-name>
            <surname>Zaporozhets</surname>
            ,
            <given-names>A.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Redko</surname>
            ,
            <given-names>O.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Babak</surname>
            ,
            <given-names>V.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Eremenko</surname>
            ,
            <given-names>V.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Mokiychuk</surname>
            ,
            <given-names>V.</given-names>
          </string-name>
          :
          <article-title>Method of indirect measurement of oxygen concentration in the air</article-title>
          .
          <source>Naukovyi Visnyk Natsionalnoho Hirnychoho Universytetu</source>
          ,
          <year>2018</year>
          , №
          <issue>5</issue>
          , pp.
          <fpage>105</fpage>
          -
          <lpage>114</lpage>
          . doi:
          <volume>10</volume>
          .29202/nvngu/2018-5/
          <fpage>14</fpage>
        </mixed-citation>
      </ref>
      <ref id="ref5">
        <mixed-citation>
          5.
          <string-name>
            <surname>Yao</surname>
            ,
            <given-names>L.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Guan</surname>
            ,
            <given-names>Y.</given-names>
          </string-name>
          :
          <article-title>Minimum entropy fault diagnosis and fault tolerant control for the nonGaussian stochastic system</article-title>
          .
          <source>2016 American Control Conference (ACC)</source>
          .
          <volume>6</volume>
          -
          <issue>8</issue>
          <year>July</year>
          ,
          <year>2016</year>
          , Boston, MA, USA. doi:
          <volume>10</volume>
          .1109/ACC.
          <year>2016</year>
          .7526753
        </mixed-citation>
      </ref>
      <ref id="ref6">
        <mixed-citation>
          6.
          <string-name>
            <surname>Peng</surname>
            ,
            <given-names>X.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Qian</surname>
            ,
            <given-names>G.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Li</surname>
            ,
            <given-names>X.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Gao</surname>
            ,
            <given-names>F.</given-names>
          </string-name>
          :
          <article-title>Intelligent trip-out fault diagnosis of overhead transmission line</article-title>
          .
          <source>High Voltage Engineering</source>
          ,
          <year>2012</year>
          , Vol.
          <volume>38</volume>
          , Issue 8, pp.
          <fpage>1965</fpage>
          -
          <lpage>1972</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref7">
        <mixed-citation>
          7.
          <string-name>
            <surname>Li</surname>
            ,
            <given-names>P.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Li</surname>
            ,
            <given-names>Q.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Cao</surname>
            ,
            <given-names>M.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Gao</surname>
            ,
            <given-names>S.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Huang</surname>
            ,
            <given-names>H.</given-names>
          </string-name>
          :
          <article-title>Time series prediction for icing process of overhead power transmissions line based on BP neural networks</article-title>
          .
          <source>Proceedings of the 30th Chinese Control Conference</source>
          .
          <volume>22</volume>
          -
          <issue>24</issue>
          <year>July</year>
          ,
          <year>2011</year>
          , Yantai, China.
        </mixed-citation>
      </ref>
      <ref id="ref8">
        <mixed-citation>
          8.
          <string-name>
            <surname>Kuts</surname>
            ,
            <given-names>Y.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Eremenko</surname>
            ,
            <given-names>V.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Monchenko</surname>
            ,
            <given-names>E.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Protasov</surname>
            ,
            <given-names>A.</given-names>
          </string-name>
          :
          <article-title>Ultrasound method of multi-layer material thickness measurement</article-title>
          .
          <source>AIP Conference Proceedings 1096</source>
          ,
          <year>2009</year>
          , Vol.
          <volume>1115</volume>
          . doi:
          <volume>10</volume>
          .1063/1.3114079
        </mixed-citation>
      </ref>
      <ref id="ref9">
        <mixed-citation>
          9.
          <string-name>
            <surname>Zaporozhets</surname>
            ,
            <given-names>A.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Eremenko</surname>
            ,
            <given-names>V.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Serhiienko</surname>
            ,
            <given-names>R.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Ivanov</surname>
            ,
            <given-names>S.</given-names>
          </string-name>
          :
          <article-title>Methods and Hardware for Dianosing Thermal Power Equipment Based on Smart Grid Technology</article-title>
          ,
          <source>Advances in Intelligent Systems and Computing III</source>
          ,
          <year>2019</year>
          , Vol.
          <volume>871</volume>
          , pp.
          <fpage>476</fpage>
          -
          <lpage>492</lpage>
          . doi:
          <volume>10</volume>
          .1007/978-3-
          <fpage>030</fpage>
          -01069-0_
          <fpage>34</fpage>
        </mixed-citation>
      </ref>
      <ref id="ref10">
        <mixed-citation>
          10.
          <string-name>
            <surname>Babak</surname>
            .,
            <given-names>V.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Mokiychuk</surname>
            ,
            <given-names>V.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Zaporozhets</surname>
            ,
            <given-names>A.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Redko</surname>
            ,
            <given-names>O.</given-names>
          </string-name>
          :
          <article-title>Improving the efficiency of fuel combustion with regard to the uncertainty of measuring oxygen concentration</article-title>
          .
          <source>EasternEuropean Journal of Enterprise Technologies</source>
          ,
          <year>2016</year>
          , Vol.
          <volume>6</volume>
          , №8, pp.
          <fpage>54</fpage>
          -
          <lpage>59</lpage>
          . doi:
          <volume>10</volume>
          .15587/
          <fpage>1729</fpage>
          -
          <lpage>4061</lpage>
          .
          <year>2016</year>
          .85408
        </mixed-citation>
      </ref>
      <ref id="ref11">
        <mixed-citation>
          11.
          <string-name>
            <surname>Klevtsov</surname>
            ,
            <given-names>S.</given-names>
          </string-name>
          :
          <article-title>Identification of the state of technical objects based on analyzing a limited set of parameters</article-title>
          .
          <source>2016 International Siberian Conference on Control and Communications (SIBCON)</source>
          ,
          <fpage>12</fpage>
          -14 May,
          <year>2016</year>
          , Moscow, Russia. doi:
          <volume>10</volume>
          .1109/SIBCON.
          <year>2016</year>
          .7491752
        </mixed-citation>
      </ref>
      <ref id="ref12">
        <mixed-citation>
          12.
          <string-name>
            <surname>Manusov</surname>
            ,
            <given-names>V.Z.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Orlov</surname>
            ,
            <given-names>D.V.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Frolova</surname>
            ,
            <given-names>V.V.</given-names>
          </string-name>
          :
          <article-title>Diagnostic of Technical State of Modern Transformer Equipment Using the Analytical Hierarchy Process</article-title>
          .
          <source>2018 IEEE International Conference on Environment and Electrical Engineering and 2018 IEEE Industrial and Commercial Power Systems Europe (EEEIC / I&amp;CPS Europe)</source>
          ,
          <fpage>12</fpage>
          -
          <lpage>15</lpage>
          June,
          <year>2018</year>
          , Palermo, Italy. doi:
          <volume>10</volume>
          .1109/EEEIC.
          <year>2018</year>
          .8493904
        </mixed-citation>
      </ref>
      <ref id="ref13">
        <mixed-citation>
          13.
          <string-name>
            <surname>Ming</surname>
            ,
            <given-names>J.</given-names>
          </string-name>
          , Zhang,
          <string-name>
            <given-names>L.</given-names>
            ,
            <surname>Sun</surname>
          </string-name>
          ,
          <string-name>
            <surname>J.</surname>
          </string-name>
          , Zhang,
          <string-name>
            <surname>Y.</surname>
          </string-name>
          :
          <article-title>Analysis models of technical and economic data of mining enterprises based on big data analysis</article-title>
          .
          <source>2018 IEEE 3rd International Conference on Cloud Computing and Big Data Analysis (ICCCBDA)</source>
          ,
          <fpage>20</fpage>
          -
          <lpage>22</lpage>
          April,
          <year>2018</year>
          , Chengdu, China. doi:
          <volume>10</volume>
          .1109/ICCCBDA.
          <year>2018</year>
          .8386516
        </mixed-citation>
      </ref>
      <ref id="ref14">
        <mixed-citation>
          14.
          <string-name>
            <surname>Dmitriev</surname>
            ,
            <given-names>S.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Manusov</surname>
            ,
            <given-names>V.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Ahyoev</surname>
          </string-name>
          , J.:
          <article-title>Diagnosing of the current technical condition of electric equipment on the basis of expert models with fuzzy logic</article-title>
          .
          <source>2016 57th International Scientific Conference on Power and Electrical Engineering</source>
          of Riga Technical University (RTUCON),
          <fpage>13</fpage>
          -
          <lpage>14</lpage>
          October,
          <year>2016</year>
          , Riga, Latvia. doi:
          <volume>10</volume>
          .1109/RTUCON.
          <year>2016</year>
          .7763126
        </mixed-citation>
      </ref>
    </ref-list>
  </back>
</article>