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<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>Development of the Controlling Speed Algorithm of the Conveyor Belt Based on TOU Tarifs</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Oleh Pihnastyi</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Valery Khodusov</string-name>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>National Technical University "Kharkiv Polytechnic Institute"</institution>
          ,
          <addr-line>2, Kyrpychova str, Kharkiv, 61002</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>V.N. Karazin Kharkiv National University</institution>
          ,
          <addr-line>4, Svobody sq., Kharkiv, 61022</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
      </contrib-group>
      <abstract>
        <p>The article considers the synthesis of an optimal discrete control algorithm for the conveyor belt speed, based on the use of Time-Of-Use tarifs. Methods have been investigated that reduce the consumption of electricity required to transport material from the extracted place to the place of processing. It is shown that the uneven distribution of material along the transportation route for long multi-section conveyors leads to a significant increase in the share of transportation costs among the total costs of material extraction. The systems for controlling the flow parameters of the transport system are analyzed to ensure uniform distribution of material along the transport route and reduce the cost of transporting material. It has been demonstrated that energy management methodology is an efective tool to reduce the cost of material transportation. Analyzed the common classes of tarifs using electricity by industrial enterprises, which can be successfully used in the design of control systems for flow parameters of the conveyor line. When synthesizing algorithms for regulating the speed of the belt, the model of primary friction and the assumption of the absence of a stress wave in the belt during instantaneous switching of the speed modes were used. An analytical model of the conveyor is presented in a dimensionless form, taking into account the transport delay. The problem of optimal control of the speed of the conveyor belt at fixed energy consumption for the considered control interval is formulated. The ranges of variation of the model parameters are estimated. An algorithm for optimal regulation of the belt speed using the coeficients Ukraine - TOU periods is synthesized. The influence of the initial conditions on the belt speed control modes is analyzed.</p>
      </abstract>
      <kwd-group>
        <kwd>eol&gt;Transport conveyor</kwd>
        <kwd>distributed transport system</kwd>
        <kwd>energy management</kwd>
        <kwd>conveyor belt speed control</kwd>
        <kwd>transport delay</kwd>
        <kwd>uneven material distribution</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>1. Introduction</title>
      <p>For mining enterprises, an important issue associated with reducing the cost of extracting
material is the issue of reducing the cost of electricity for transporting material. The cost of
transporting material from the place of extraction to the place of distribution and processing
at the standard loading of the conveyor system is 20% of the cost of extracting material [1].
A typical mode of operation of a transport conveyor is a mode with an uneven supply of
material at the entrance of the transport system. This leads to a decrease in the load on the
conveyor line. The coeficient of loading the conveyor section with the material can be 0.5–0.7
of the full loading of the conveyor section [2]. This mode leads to a nonlinear increase in
energy consumption for the transportation of material of a unit weight due to a decrease in
the material load factor of the conveyor section [3]. For low loaded conveyor sections, the
energy consumption for transporting material of a unit weight can increase several times.
The uneven distribution of material along the conveyor section is especially important for
extended transport systems [4, 5, 6]. A common solution to reduce energy costs for material
transportation is the division of an extended conveyor into separate sections [7, 8, 9]. The
development of the mining industry is associated with a further increase in the length of the
transport route. The length of a separate section has exceeded ten km [10] and continues to
increase. The presence of the fact of uneven distribution of material along the transport route
for long multi-section conveyors leads to the fact that the cost of transporting material can reach
a significant share in the total cost of extracting material. To increase the loading factor of the
conveyor sections, systems for controlling the flow of material from between sectional bunker
[11, 12], the speed control systems of conveyor belts [13, 14] or combined control systems are
used. The division into sections increases the control eficiency of the transport route section
within a separate section and the reliability of the transport system functioning as a whole.
Reducing energy costs for material transportation is due to the fact that the conveyor belt
speed for these sections is selected depending on the optimizing transport costs conditions
for a separate section, is diferent for each section of the conveyor. In the absence of dividing
the transport route into sections, the speed of the conveyor belt is the same for each section,
which leads to additional electricity costs compared to multi-section conveyor systems. The
main control element in conveyor-type transport systems is an asynchronous motor, which
uses an electronic motor controller. Most control systems for transport system parameters
are based on the use of embedded systems that require the development of high-performance
algorithms for optimal control of transport system parameters with minimal use of computing
resources. An additional efective method for reducing unit energy costs is the use of energy
management methodologies [15]. An overview and analysis of the use of various types of
electricity consumption tarifs are given in [ 16, 17]. Among them, three common tarif classes
should be distinguished: tarif with a fixed price for electricity consumption (FPT); tarif with
the price for electricity consumption, depending on the time of use (TOU); real-time pricing
(RTT) tarifs.</p>
      <p>The FPT tarif defines a constant energy price for all 24 hour periods throughout the year.
The TOU tarif has diferent prices depending on the time of use but is the same for the year or
season of the year (for example, winter or summer period). A dynamic RTT tarif has a variable
price throughout the day depending on expected demand and generator availability. The price
changes every hour. This period of time is consigned for making a decision on changing the
electricity consumption regime at the enterprise. The paper [18] analyzes the factors that
determine the choice of a specific tarif for the use of electricity by the company, presents the
structure of the distribution of tarif types by industry. The structure of TOU periods for South
Africa, Ukraine and Great Britain is shown in Fig.1-Fig.3. The coeficient   characterizes the
ratio of the price of electricity at a given tarif to the price of electricity at a fixed tarif. The
value   in the figures defines the line with the coeficient value for the price of the fixed tarif.
Long-distance transportation systems using the TOU tarif can greatly benefit from scheduling
the electrical equipment of the transportation system during periods of time with low electricity
costs. The mining enterprises may have additional costs if transport systems are not properly
scheduled. This is especially true of conveyor lines in South Africa, where the price of electricity
is very diferent during the peak and of-peak periods (Figure 1), [19, 20].</p>
      <p>The price for electricity consumption depending on the tarif and recommendations for the
use of tarifs are given in [ 21, 22, 23]. The electricity price for peak periods in the high demand
season is almost six times higher than the price for of-peak periods and more than four times
higher than the price at a fixed tarif. Due to such a strong diference in prices for peak and
of-peak periods, transport systems using Eskom TOU-tarif (Figure 1) require speed control
systems taking into account the TOU-tarif price schedule.</p>
      <p>The structure of TOU tarifs for diferent countries is qualitatively similar. Figure 2 shows the
structure of the TOU tarif in force in Ukraine [ 24]. The TOU tarif structure for Great Britain is
shown in Figure 3, which demonstrates a comparison of the price coeficients for the TOU-tarif
and for the RTT–tarif. The use of the RTT–tarif in speed control systems is of practical interest
for conveyor-type transport systems, which to move material during the day consume almost 2
times less electricity than the maximum allowable consumption.</p>
      <p>It should be noted that when using the RTT–tarif, the time that can be allocated for calculating
the optimal speed control algorithm and changeover of production operations is limited to 30
minutes (Figure 3). This imposes a strong constraint on the choice of conveyor system models
used to design conveyor belt speed control systems.</p>
    </sec>
    <sec id="sec-2">
      <title>2. Formal problem statement</title>
      <p>Reducing the cost of mining by using the TOU–tarif structure in the control speed algorithms of
the conveyor belt is an actual problem for mining enterprises. Using the TOU–tarif structure to
reduce the total cost of electricity consumption is not always successful in practice. A statistical
analysis of the data set on the successful and unsuccessful use of the TOU-tarif structure for
12000 enterprises in 44 industrial sectors is presented in [18]. This clearly demonstrates the fact
that the successful use of the TOU–tarif structure requires the development of an optimal speed
control algorithm, taking into account the TOU–tarif structure. The continuous operation of
the transport system and a significant share of the cost of material transportation in the cost
of the extracted material determines the relevance of designing conveyor control algorithms,
taking into account the use of the TOU strategy. When constructing an algorithm for optimal
speed control taking into account the structure of TOU–tarifs, the following assumptions were
used in this work: a) the conveyor system consumes a constant amount of electricity during
the day, which allows using the control quality criterion formulated for a period of 24 hours;
b) in accordance with DIN 22101, the primary friction model is used [25, 26]; c) the efects of
disturbances associated with instantaneous switching of speed modes are not taken into account.
The duration of the modes of acceleration (deceleration) of the belt is negligible compared to
the total transportation time.</p>
    </sec>
    <sec id="sec-3">
      <title>3. Model of the conveyor line</title>
      <p>To construct an optimal control algorithm of the conveyor belt speed, taking into account
the structure of TOU–tarifs, the analytical PiKh–model of the conveyor [ 27] was used. The
analytical PiKh–model for calculating the parameters of a separate one has the form:
where [ ]0 (,  ) ≤ [ ]0
lfow at the moment in time
 ∈ [0,   ]
moment of time</p>
      <p>; Ψ( ) ≤ [ ]0
time of the transportation
 = 0; [ ]0
, [ ]1 (,  ) are the linear density of the material and the material
 ∈ [0,   ] at the point of the transport route with the coordinate
is the distribution of material along the transport route at the initial
is maximum permissible material density;  
is the characteristic
process;  ( ) is speed of the conveyor belt;  1( ) is the material flow
at the input of the conveyor section;  ( ) is Dirac function;  ( ) is Heaviside function:
{</p>
      <p>0,  &lt; 0,
 ( ) =</p>
      <p>∞
1,  ≥ 0, ∫−∞  ( )
= 1</p>
      <p>The force required to move the conveyor belt with material distributed along the transport
the rotating parts [ ]0
route with density [ ]0 (,  ) at the specific mass of the belt [ ]0
[25] is determined by the expression [26]:</p>
      <p>and the linear loading from
 =     ∫
(2([ ]0 + [ ]0 ) + [ ]0 (, 
)),
resistance coeficient [ 25];  
takes into account the upper and lower conveyor belt.</p>
      <p>is eficiency. The doubled value of the parameters
which takes into account the model of primary resistances.   is coeficient of resistance to
belt indentation and rolling resistance of driving rollers [25];  
= 9.81(
/
2) ;  is secondary
[ ]0
, [ ]0
To model the transport conveyor let’s use dimensionless parameters [27]:</p>
      <p>[ ]0 (,  )  [ ]1 (,  )
+</p>
      <p>
        =  ( ) 1( ),

[ ]0 (0,  ) = Ψ( ),
[ ]1 (,  ) =  ( ) [ ]0 (,  ),
(
        <xref ref-type="bibr" rid="ref1">1</xref>
        )
(
        <xref ref-type="bibr" rid="ref2">2</xref>
        )
(
        <xref ref-type="bibr" rid="ref3">3</xref>
        )
(
        <xref ref-type="bibr" rid="ref4">4</xref>
        )
(
        <xref ref-type="bibr" rid="ref5">5</xref>
        )
(
        <xref ref-type="bibr" rid="ref6">6</xref>
        )
(
        <xref ref-type="bibr" rid="ref7">7</xref>
        )
(
        <xref ref-type="bibr" rid="ref8">8</xref>
        )
(
        <xref ref-type="bibr" rid="ref9">9</xref>
        )
(
        <xref ref-type="bibr" rid="ref10">10</xref>
        )
0
 

 

 
 
  [ ]0
[ ]0
 =
,  =
      </p>
      <p>,  ( ) =    ( ),
Ψ( )
[ ]0</p>
      <p>[ ]0
 ( ) =
,  1( ) =  1( )</p>
      <p>,  ( ) =  ( )
 0 =
[ ]0 ,  0 =
[ ]0 ,   ( ) =   ( )
 
  ,  0( ,  ) =</p>
      <p>[ ]0
[ ]0 (,  )</p>
      <p>
        .
[ ]0
 2

which will make it possible to represent the solution of equation (
        <xref ref-type="bibr" rid="ref1">1</xref>
        )–(
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) in the form
 0( ,  ) = ( ( ) −  ( −  ( )))
      </p>
      <p>
        +  ( −  ( )) ( −  ( ))
 1(  )
 (  )
  =  −1( ( ) −  ),  ( ) = ∫  ( ),
where △  ( ) =  −   is the transport delay. The transport delay determines the time interval
during which the material moves from the input of the conveyor section to the point of the
transport route with the coordinate  at the moment in time  . The value  0( , 1) and  1( , 1) at
the output from the conveyor section (
        <xref ref-type="bibr" rid="ref6">6</xref>
        ) is determined through the value of the transport delay
△ 1( ) =  −  −1( ( ) − 1):
 0( , 1) =
 1( −△ 1)
 ( −△ 1) ,  ( ) ≥ 1,  ≥  −1(
        <xref ref-type="bibr" rid="ref1">1</xref>
        ),
(  (1 −  ( )),  ( ) &lt; 1,  &lt;  −1(
        <xref ref-type="bibr" rid="ref1">1</xref>
        ),
 1( , 1) =  0( , 1) ( ).
      </p>
      <p>
        (
        <xref ref-type="bibr" rid="ref11">11</xref>
        )
      </p>
      <p>
        Dimensionless electrical power   ( ) (
        <xref ref-type="bibr" rid="ref8">8</xref>
        ), required to move the conveyor belt with the material
is determined by the expression:
1
  ( ) =  ( ) ( ),  ( ) = ∫ (2 0 + 2 0 +  0( ,  )) (
        <xref ref-type="bibr" rid="ref12">12</xref>
        )
      </p>
      <p>0</p>
      <p>
        The obtained expressions (
        <xref ref-type="bibr" rid="ref10">10</xref>
        ), (
        <xref ref-type="bibr" rid="ref11">11</xref>
        ) are used to determine the optimal control algorithm of
the conveyor belt speed.
      </p>
    </sec>
    <sec id="sec-4">
      <title>4. Optimal belt speed control</title>
      <sec id="sec-4-1">
        <title>4.1. Statement of the control problem</title>
        <p>The optimal control problem of the conveyor belt speed is formulated as follows: To determine
the modes of switching the conveyor belt speed during a period of time  = [0,  24] with the
value of the price coeficients of the cost of electricity  ( ) (Figure 1, Figure 2, Figure3) with
stepwise the speed belt control  ( ) =  ( ) = ( 1,  2), 0 &lt;  1 &lt;  2 &lt; ∞,   =  , which leads
to a minimum of functional:
with diferential connections
∫0
1
 (0) = 2( 0 +  0 ) + ∫  ( ) ,
0
and limitation on the total amount of energy consumed per day ( = [0,  24])
 ( ) ( )
=  = ,</p>
        <p>( ) = ( 1,  2).</p>
        <p>∫0</p>
        <p>
          The equation (
          <xref ref-type="bibr" rid="ref13">13</xref>
          ) is written taking into account dependence (
          <xref ref-type="bibr" rid="ref10">10</xref>
          ) for the material output
lfow. The choice of the stepped control mode is due to its prevalence in the control of transport
systems [28, 29, 30, 31]. The equation (
          <xref ref-type="bibr" rid="ref14">14</xref>
          ) can be replaced by the diferential equation
 = (  −  ( )) ( ) ( ) +   ( 1( ) −  1( − △ 1)
 ( )
 ( − △  1)
        </p>
        <p>),
 

= −</p>
        <p>= 0,
  = ( ( ) −   ) ( )  ( 24) = 0. (19)</p>
        <p>
          From thr equation (18) follows   =   =  For a two-stage control mode  ( ) = ( 1,  2)
[31] 0 &lt;  1 &lt;  2 &lt; ∞ the optimal belt speed corresponds to the maximum value of the Hamilton
function (16). Switching points of control modes are determined by solving equations (
          <xref ref-type="bibr" rid="ref13">13</xref>
          ), (
          <xref ref-type="bibr" rid="ref15">15</xref>
          ),
(17) and (18).
        </p>
      </sec>
      <sec id="sec-4-2">
        <title>4.2. Selecting the range of the parameters</title>
        <p>1 = 1(
belt speed:
For quantitative calculations, let us take the values of the characteristic time and the
characteristic length as values   = 1(ℎ ),   = 20.5( ). The choice of the value of the characteristic
time   allows you to conveniently display the change in parameters during the day  ∈ [0; 24],
and the choice of the value of the characteristic length corresponds to the consideration of
extended transport conveyors (Sasol – Shondoni Overland [18] (20.5 km single flight overland
conveyor with multiple horizontal curves). Then the control modes  ( ) = ( 1,  2) , at the speed
/ ),  1 = 5( / ) will correspond to dimensionless values of the</p>
        <p>
          For values of the specific mass of the belt  0 and the linear load from rotating parts  0 ,
( 0 +  0 ) = 0.2 mass  ( ) (
          <xref ref-type="bibr" rid="ref11">11</xref>
          ), (
          <xref ref-type="bibr" rid="ref13">13</xref>
          ) will vary in the range
1.69 = 24 1 1 =  1 ≤  ≤  2 = 24 2 2 = 29.50.
        </p>
        <p>The condition for the inadmissibility of exceeding the maximum permissible specific load
from the incoming material on the conveyor belt can be written as
(23)
 1( )
 ( ) ≤ [ ]0 .</p>
        <p>This condition imposes a limitation on the maximum value of the input flow at the current
belt speed  ( )
(24)
 1( )</p>
        <p>≤  ( ).</p>
        <p>[ ]0</p>
        <p>
          If inequality (24) is satisfied, there will be no excess of the maximum permissible belt load.
Using dimensionless notation (
          <xref ref-type="bibr" rid="ref7">7</xref>
          ), condition (24) can be written as follows:
 1( ) ≤  ( ) ≤  2 = 0.878,
(25)
(26)
(28)
 1( ) =  1( )   ≤  ( ),  ( ) = ( 1,  2). (27)
        </p>
        <p>[ ]0</p>
        <p>The condition (25) allows us to carry out an important conclusion: if for any moment of time
the inequality</p>
        <p>1 ≤  1( ) ≤  2.</p>
        <p>then the transport section will operate only in speed mode  ( ) =  2, without switching
speed modes.</p>
        <p>The equation (18) provides a boundary range for</p>
        <p>≤   ≤   ,   ≤  ( ) ≤   .</p>
        <p>
          Conditions (19)–(21), (25)–(28) determine the existence of a solution to the system of equations
(
          <xref ref-type="bibr" rid="ref13">13</xref>
          ), (
          <xref ref-type="bibr" rid="ref15">15</xref>
          )–(18).
(29)
        </p>
      </sec>
    </sec>
    <sec id="sec-5">
      <title>5. Analysis of results</title>
      <p>
        Let us consider the construction of a schedule for switching the belt speed modes for the tarif
coeficients Ukraine – TOU periods (Figure 2), when the intensity of the material input flow is
constant  1( ) = 0.15 with daily energy consumption  = 6.5 (
        <xref ref-type="bibr" rid="ref14">14</xref>
        ), (22). The selected value of the
intensity of the input flow  1( ) in accordance with inequality (26) allows the transport system
to operate in a two-speed mode  ( ) = (0.176, 0.878) (19). An increase in belt speed  ( ) leads
to an increase in the power consumption of the transport system   ( ) (
        <xref ref-type="bibr" rid="ref11">11</xref>
        ). The connection
between the belt speed and the linear density of the material along the transport route (and, as a
consequence, the connection between the belt speed and mass) is a characteristic feature of the
transport systems functioning. The next feature is that the conveyor belt is an accumulator of
the material incoming the section input. Constraint (23) does not allow to allow both the excess
of the specific density  0( ,  ) and the overflow of the accumulator. The presence of an upper
and a lower limit for the material amount (20) in the accumulator for a suficiently long period
of operation of the transport system determines the ratio between the average intensity of the
incoming flow and the average power consumption of the transport system for the period under
consideration. An increase in the value of the intensity  1( ) of the incoming material over a
suficiently long time period leads to an increase in the power consumption of the transport
system. These features significantly complicate the synthesis of the optimal control algorithms
of the flow parameters of the transport system. In order to simplify the qualitative analysis in
this paper, a constant value for the intensity of the incoming flow is taken  1( ).
      </p>
      <p>
        The solution of equations (
        <xref ref-type="bibr" rid="ref15">15</xref>
        ), (18) for the parameters   ( ) and   ( ) are presented in Figure
4. The parameter   ( ) determines the amount of energy used by the transport system during
the period of the time [0,  ], satisfies the conditions (
        <xref ref-type="bibr" rid="ref15">15</xref>
        ) for the initial and final moments of the
time. The quasi-linear dependence of energy consumption   ( ) as a function of time indicates
a quasi-stationary value of the power consumption of the transport system with a variable
value of the transport delay △ 1( ).
      </p>
      <p>
        The quasi-stationary change in the amount of energy consumed by the transport system
is explained by the considered feature, which is characteristic of a conveyor-type transport
system (
        <xref ref-type="bibr" rid="ref8">8</xref>
        ).
      </p>
      <p>The belt speed regulation modes  ( ) = ( 1,  2) for tarif coeficient values   ( ) = (0.35, 1.8)
are shown in Figure 5. The value of the tarif coeficient   = 1.8 corresponds to the minimum
belt speed  1. There are several switching points of the speed mode for the tarif coeficient
  = 0.35. The belt speed switching modes on the interval  ∈ [0.0; 1.0] are related to the type of
(30)
function (21), which determines the initial distribution of material along the route. The points
of the belt speed switching for the interval  ∈ [4.0; 5.0] are repeated points of the belt speed
switching for the interval  ∈ [0.0; 1.0] with a shift along the time scale equal to the value of
the transport delay △ 1(4.0) = 3.711 (Figure 4). With a uniform distribution of material at the
initial moment of time</p>
      <p>
        ( ) =  0(
        <xref ref-type="bibr" rid="ref1 ref12">12, 1</xref>
        ) = 0.8523,
there are no the speed modes switching points in the interval  ∈ [0.0; 5.0] (Figure 6), which
leads to a decrease in the value of the power consumption of the transport system.
(31)
  ( ) = (0.35, 1.8) at  ( ) = 0.5 +
  ( ) = (0.35, 1.8) at  ( ) = 0.8523
      </p>
      <p>The density of the material  0( , 0) at the input to the conveyor section is shown in Figure 7
and corresponds to the condition
 0( , 0) =
.</p>
      <p>(32)</p>
      <p>The speed modes switching points correspond to the density jumps of the material  0( , 0)
at the input to the section. The mass  ( ) of the belt with the material correlates with the
transport delay function △ 1( ). For times when the transport delay is high, the mass of the
belt with the load being moved also has high values (Figure 4, Figure 7). An increase in the
transport delay leads to an increase in the mass of material on the belt.</p>
    </sec>
    <sec id="sec-6">
      <title>6. Conclusions</title>
      <p>The article deals with the problem of synthesis of the optimal belt speed control algorithms for
a distributed conveyor-type transport system. A method for constructing an algorithm based
on the Pontryagin maximum principle with the use of an analytical PiKh–model for a conveyor
section is proposed. The use of the Pontryagin maximum principle in conjunction with the
analytical PiKh–model allows providing acceptable accuracy for calculating the switching points
of speed modes. The software for the synthesis of algorithms for optimal discrete control of
the belt speed has been developed and used for analysing the belt conveyor flow parameters.
The influence of the initial distribution of the material on the choice of modes for controlling
the belt speed is demonstrated. The relationship between the transport delay for a conveyor
system and the mass of material that moves with the belt is presented.</p>
      <p>The originality and novelty of the obtained results consist in improving the analytical model
by including additional parameters that characterize the state of the transport system at an
arbitrary moment in time (the total material mass and the power consumption of the transport
system). This made it possible to form a new criterion for the quality of control based on
Time-Of-Use tarifs. When synthesizing the optimal control algorithm, additional diferential
connections were added that determine the change in the mass of the material being moved
and the power consumption of the transport system required to move the material.</p>
      <p>The prospect of further research is the determination of algorithms for the belt speed optimal
control for the time interval when the influence of the initial conditions of material distribution
becomes insignificant.
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