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				<title level="a" type="main">Neural model of conveyor type transport system</title>
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							<persName><forename type="first">Pihnastyi</forename><surname>Oleh</surname></persName>
							<email>pihnastyi@gmail.com</email>
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								<orgName type="institution">National Technical University &quot;KPI&quot; Kharkiv</orgName>
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									<country key="UA">Ukraine</country>
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								<orgName type="institution">Kharkiv National University</orgName>
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						<title level="a" type="main">Neural model of conveyor type transport system</title>
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					<term>conveyor</term>
					<term>PDE-model</term>
					<term>distributed system</term>
					<term>transport delay</term>
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<div xmlns="http://www.tei-c.org/ns/1.0"><p>In this paper, a model of a transport conveyor system using a neural network is demonstrated. The analysis of the main parameters of modern conveyor systems is presented. The main models of the conveyor section, which are used for the design of control systems for flow parameters, are considered. The necessity of using neural networks in the design of conveyor transport control systems is substantiated. A review of conveyor models using a neural network is performed. The conditions of applicability of models using neural networks to describe conveyor systems are determined. A comparative analysis of the analytical model of the conveyor section and the model using the neural network is performed. The technique of forming a set of test data for the process of training a neural network is presented. The foundation for the formation of test data for learning neural network is an analytical model of the conveyor section. Using an analytical model allowed us to form a set of test data for transient dynamic modes of functioning of the transport system. The transport system is presented in the form of a directed graph without cycles. Analysis of the model using a neural network showed a high-quality relationship between the output flow for different conveyor sections of the transport system.</p></div>
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<div xmlns="http://www.tei-c.org/ns/1.0"><head n="1">Introduction</head><p>The transport conveyor is a complex dynamic stochastic distributed system. The transport conveyor is an integral part of the technological process at enterprises with the flow method of organizing production <ref type="bibr" target="#b0">[1]</ref>. Conveyor transport is widely used in the mining industry <ref type="bibr" target="#b1">[2]</ref><ref type="bibr" target="#b2">[3]</ref><ref type="bibr" target="#b3">[4]</ref><ref type="bibr" target="#b4">[5]</ref><ref type="bibr" target="#b5">[6]</ref>. Table <ref type="table" target="#tab_0">1</ref> shows a number of basic characteristics of conveyor-type transport systems. One way to save energy, which is necessary for the functioning of such systems, is to increase the level of congestion of the conveyor line <ref type="bibr" target="#b6">[7]</ref><ref type="bibr" target="#b7">[8]</ref><ref type="bibr" target="#b8">[9]</ref>. To reduce the energy costs required to move one ton of material along the transportation route, systems are used to control the speed of the belt or the intensity of the material at the entrance of the conveyor section from the input bunker <ref type="bibr" target="#b9">[10]</ref><ref type="bibr" target="#b10">[11]</ref><ref type="bibr" target="#b11">[12]</ref>. The effectiveness of the conveyor control system is largely determined by the model of the transport system. This fact acquires special significance when designing control systems for a transport system consisting of a large number of sections. Speed (m/sec) Capacity (t/h) From the Bu Craa mine to the coast at El Aaiún, Western Sahara, <ref type="bibr" target="#b1">[2]</ref> 128. <ref type="bibr">7 11 2000</ref> Sasol's Impumelelo project in South Africa (2015), <ref type="bibr" target="#b1">[2]</ref> 27.5 1 6.5 2400</p><p>The Henderson Coarse Ore Conveying System, the North American Continental Divide <ref type="bibr">(2000)</ref>, <ref type="bibr" target="#b2">[3,</ref><ref type="bibr" target="#b3">4]</ref> 24.0 3 12700 4.5 2270</p><p>Çöllolar Lignite Open Pit Mine, Turkey (2011), <ref type="bibr" target="#b4">[5]</ref> 17.4 26 46300 9350</p><p>From a mine in India to a cement plant in Bangladesh (2005), <ref type="bibr" target="#b1">[2]</ref> 16.5 1 6.5</p><p>Neyveli Lignite Corp., India (2007), <ref type="bibr" target="#b4">[5]</ref> 14.0 8 2520 5.4 Open Cast Mine Reichwalde, Germany (2010), <ref type="bibr" target="#b4">[5]</ref> 13.5 6 19350 5.5 6000</p><p>Coarse ore conveyor system Minera Los Pelambres, Chile (1998), <ref type="bibr" target="#b4">[5]</ref> 12.7 3 25000 8700 Tianjin China Port Authority, China (2005) <ref type="bibr" target="#b5">[6]</ref> 8.98 1 4x 1500</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head n="5.6">6000</head><p>Baumgartner Tunnel, the Metropolitan St. Louis (Missouri) , USA <ref type="bibr" target="#b5">[6]</ref> 6. <ref type="bibr">18 2.54 200</ref> Barcelona Tunnel (the Metro (Train) Extension Project), Spain (2005) <ref type="bibr" target="#b5">[6]</ref> 4.71 1 3.5 1500</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head>2</head></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head>Literature review</head><p>To build the models on which the systems for controlling the speed of the belt or the intensity of material input at the entrance of the conveyor section from the input bunker are based, use the finite element method <ref type="bibr" target="#b12">[13]</ref><ref type="bibr" target="#b13">[14]</ref><ref type="bibr" target="#b14">[15]</ref><ref type="bibr" target="#b15">[16]</ref><ref type="bibr" target="#b16">[17]</ref><ref type="bibr" target="#b17">[18]</ref>; finite difference method <ref type="bibr" target="#b17">[18,</ref><ref type="bibr" target="#b18">19]</ref>; Lagrange method <ref type="bibr" target="#b18">[19]</ref>; a method using the aggregated equation of state <ref type="bibr" target="#b19">[20]</ref>; system dynamics method <ref type="bibr" target="#b9">[10]</ref>; multiple regression method <ref type="bibr" target="#b25">[26]</ref><ref type="bibr" target="#b26">[27]</ref><ref type="bibr" target="#b27">[28]</ref>. Most often used in models for calculating flow parameters a finite element method. This method allows you to determine the value of the flow parameters of the conveyor section for dynamic transient conditions, taking into account the distribution of material along the transportation route. The finite element method, before the advent of the analytical model (PiKh-model) of the conveyor-type transport system <ref type="bibr" target="#b11">[12]</ref>, was perhaps the main method used by researchers to construct the conveyor model. The use of neural network methods and multiple regression methods to describe flow parameters was less promising than the finite element method. One of the reasons is that the researchers focused on modelling a single section of the conveyor. Another, no less important reason is the lack of test data in the right amount for training a neural network or for building a regression model. When considering a model of a transport system, which consists of a large number of separate conveyor sections, the use of the finite element method is unreasonable even when modelling a transport system consisting of several dozen separate sections. A good tool, in this case, is the PiKh-con-veyor system model. In this case, a separate model is built for each separate section. Combining sections into a common system leads to a system of equations <ref type="bibr" target="#b28">[29,</ref><ref type="bibr" target="#b29">30]</ref>. In the event that a separate section does not include an accumulating bunker, the number of equations of the system is equal to the number of sections. In <ref type="bibr" target="#b28">[29]</ref>, a model of a conveyor system consisting of 2 sections is presented. In <ref type="bibr" target="#b29">[30]</ref>, the principles of constructing a model of the main conveyor are considered.</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head n="3">Formal problem statement</head><p>If the transport system is a conveyor <ref type="bibr" target="#b30">[31]</ref>, which consists of tens or even hundreds of separate sections, and each section has a system for controlling the rate of material input from the input bunker and a belt speed control system, then using analytical models can be associated with significant difficulties. In this case, the application of methods using the neural network and multiple regression methods is of scientific and practical interest for solving the problem. The more the number of sections in the transport system, the stronger the interest of researchers in applying methods using the neural network and multiple regression methods. In this regard, in this work, we will pay attention to constructing a model of an assembly line using a neural network.</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head n="4">Conveyor section model</head><p>To describe the conveyor section (Fig. <ref type="figure" target="#fig_0">1</ref>) let us use the classic dynamic distributed model of the conveyor in a dimensionless form (PiKh-model) <ref type="bibr" target="#b11">[12]</ref>:</p><formula xml:id="formula_0">  ) ( ) ( ) ( ) ( 0 0                    , g ,<label>(1)</label></formula><formula xml:id="formula_1">) ( ) ( H ) 0 ( 0       , .<label>(2)</label></formula><p>The state of the flow parameters of the conveyor line at a point in time t at the point of the transport route with the coordinate S is described by dimensionless variables:  Equation (1) with initial conditions (2) corresponds to the solution <ref type="bibr" target="#b11">[12]</ref>:</p><formula xml:id="formula_2">d T t /   , d S S /   ,<label>(3)</label></formula><formula xml:id="formula_3">    / ) ( ) ( 0 0 S t, χ ,   ,    / ) ( ) ( S   ,<label>(4)</label></formula><formula xml:id="formula_4">  d d S T t ) ( ) (    ,   d d b b S T t ) ( ) (    ,   d d S T max max   , (<label>5</label></formula><formula xml:id="formula_5">) d d S T t a g / ) ( ) (   ,   ) ( / ), ( max t a (t) S     , ) ( ) ( S S d     , ) ( ) ( S H H   ,<label>(6)</label></formula><formula xml:id="formula_6">    ) ( ) ( ) ( 0 1 S t, χ t a S t, χ  ,   d d S T t ) ( ) (    , max 0     (t) ,<label>( 7 )</label></formula><formula xml:id="formula_7">      )) ( ( )) ( ( H )) ) ( (<label>(</label></formula><formula xml:id="formula_8">)) ) ( ( ( ) ( ) ( 1 1 0                 G G G G g G G G H H ,           (8)   0 0 0 1 / ) ( ) ( g , g ,             ,       d g G   0 ) ( .<label>(9)</label></formula><p>The system of equations ( <ref type="formula">8</ref>), ( <ref type="formula" target="#formula_8">9</ref>) determines the behaviour of the flow parameters of the conveyor. The linear density of the material along the transport route ) ( 0    , at an arbitrary point in time  can be determined if the intensity ) (</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head></head><p>of the rock entering the conveyor line entrance and the speed of the conveyor belt ) ( g are known.</p><p>The linear density of the material </p><formula xml:id="formula_9">) 1 ( 0 ,   and the material flow ) 1 ( 1 ,   at the output from the transport conveyor system 1   is determined by the expressions                ; 0 1 ) ( )), ( 1 ( ; 0 1 ) ( , )) 1 ) ( (<label>(</label></formula><formula xml:id="formula_10">)) 1 ) ( ( ( ) 1 ( 1 1 0          G G G G G g G G , ) ( ) 1 ( ) 1 ( 0 1      g , ,  . (<label>10</label></formula><formula xml:id="formula_11">    ) 0 ( ) ( / ) ( ) ( 0 0 , g ,              , tr    ,          ) ( 1 G G . (<label>12</label></formula><formula xml:id="formula_12">)</formula><p>If we introduce a definition for the delay time</p><formula xml:id="formula_13">       </formula><p>, then expression (13) can be represented as follows</p><formula xml:id="formula_14">) 0 ( ) ( ) ( ) ( 0 0 , g ,                       . (<label>13</label></formula><formula xml:id="formula_15">)</formula><p>The delay time </p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head></head><p>, the expression <ref type="bibr" target="#b13">(14)</ref> determines the relationship between the linear density of the material at the input and output. The value of the linear density at the output is equal to the value of the linear density at the input with a delay 1   .</p><formula xml:id="formula_16">) 0 ( ) 0 ( ) ( ) ( ) 1 ( 1 0 1 0 1 1 0 , , g ,                      , tr    ,</formula></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head>5</head><p>Conveyor section model using a neural network.</p><p>The system of equations ( <ref type="formula">8</ref> </p><formula xml:id="formula_17">  m m m m G G        ) ( 1 ,        d g G m m m   0 ) ( . (<label>15</label></formula><formula xml:id="formula_18">)</formula><p>If the transport system consists of a large number M of individual sections, then it is required to solve the M-equations ( <ref type="formula">8</ref>), <ref type="bibr" target="#b8">(9)</ref>. Additional restrictions are imposed due to the complexity of constructing an analytical system of equations that determines the flow of material from the place of production to the place of processing [32, Fig. <ref type="figure" target="#fig_0">1</ref> and Fig. <ref type="figure">2</ref>]. Therefore, with a large number M of individual sections, it is advisable to build aggregated models of transport systems. One of the approaches to designing aggregated models of conveyor transport systems is the use of neural networks <ref type="bibr" target="#b31">[32]</ref><ref type="bibr" target="#b32">[33]</ref><ref type="bibr" target="#b33">[34]</ref><ref type="bibr" target="#b34">[35]</ref><ref type="bibr" target="#b35">[36]</ref><ref type="bibr" target="#b36">[37]</ref>. To describe the functioning of a separate conveyor section of the transport system, we use dimensionless variables ( <ref type="formula" target="#formula_3">4</ref>) -( <ref type="formula" target="#formula_6">7</ref>) of the model ( <ref type="formula" target="#formula_0">1</ref>), <ref type="bibr" target="#b1">(2)</ref>, which allow us to determine the state of the flow parameters of the individual conveyor section at a time</p><formula xml:id="formula_19"> : ) (  m is the intensity of the input flow of material; ) ( m g is conveyor belt speed; m</formula><p> is section transport route length. Let's move on to the construction of a neural network using the example of a branched transport system. As an option for analysis, we will use the structure of the transport conveyor shown in Fig. <ref type="figure">2</ref>, which consists of 8 separate sections (M = 8). It should be noted that the state of the flow parameters at the output sections (section m = 7.8) is determined by the parameters of the 4 input sections (section m = 1,2,4,5). The transport system has nodes where the material flows converge (Fig. <ref type="figure">5</ref>.a) and nodes where the material flows diverge (Fig. <ref type="figure">3</ref>). When considering, let's assume that there is no bunker control. The amount of material flow through the bunker remains unchanged. This situation is common, it represents the case when the parameters of the bunker are not controlled. In this case, the bunker at the entrance of a separate section does not contain material. For nodes in which the material flows converge, the intensity of the input material flow is determined through the parameters of the converging sections. For the case when the node contains two incoming flows and one outgoing (Fig. <ref type="figure">3</ref>), the balance relation holds:</p><formula xml:id="formula_20">) ( ) ( ) ( ) ( ) ( ) ( ) ( 2 2 2 2 2 1 1 1 1 1 3                             g g g g , (<label>16</label></formula><formula xml:id="formula_21">)   m m m m m G G                ) ( 1 . (<label>17</label></formula><formula xml:id="formula_22">)</formula><p>For nodes in which the material flows diverge, the intensity of the input material flow is also determined through the parameters of the converging sections. For the case when the node contains an incoming flow and two outgoing flows (Fig. <ref type="figure">3</ref>), the balance ratio has the form: </p><formula xml:id="formula_23">     , 0 ) ( 3    . (<label>18</label></formula><formula xml:id="formula_24">)</formula><p>Let us assume that the state of the transport system is determined at a moment in time , if at that moment in time the parameters of each individual conveyor section are determined:</p><formula xml:id="formula_25">) (  m , ) ( m g</formula><p>. When constructing an aggregated model of a conveyor transport system in the absence of control, we exclude from consideration the parameters ) (  m of the internal nodes, which can be determined through the flow parameters of the mated sections. The architecture of the neural network to build an aggregated model (Fig. <ref type="figure" target="#fig_6">4</ref>.) Let us introduce the notation for the parameters of the input layer of the neural network</p><formula xml:id="formula_26">) ( 2 3   m m x   , ) ( 1 3  m m g x   , m m x   3 , m=1..M, (<label>190</label></formula><formula xml:id="formula_27">)</formula><p>where m is the number of the conveyor section (Fig. <ref type="figure">2</ref>). For the transport system model in Fig. <ref type="figure">2</ref>, the input parameters ( <ref type="formula" target="#formula_29">20</ref>)</p><formula xml:id="formula_28">) ( 3 7    x , ) ( 6 16    x , ) ( 7 19    x , ) ( 8 22    x</formula><p>are excluded. Similarly, let us exclude the velocities for sections m=3,6 from the input layer. We introduce the notation for the parameters of the output layer</p><formula xml:id="formula_29">) ( 7 7 1 1    , y  , ) ( 8 8 1 2    , y  . (<label>20</label></formula><formula xml:id="formula_30">)</formula><p>The output parameters 1 y and 2 y correspond to the output material flow for m=7,8 sections of the transport system Fig. <ref type="figure">2</ref>. The topology of the hidden layer of the neural network for models of the conveyor section using part of the parameters (20) was considered in <ref type="bibr" target="#b33">[34]</ref>. For forecasting, one hidden layer with six nodes was used. As an activation function, the Logistic function was selected:</p><formula xml:id="formula_31">) exp( 1 ) ( bx a x f    (<label>21</label></formula><formula xml:id="formula_32">)</formula><p>Weights are initialized with random values. In <ref type="bibr" target="#b32">[33]</ref>, a 4-20-1 conveyor system model was considered to study the dependence of the output material flow on 4 input parameters, among which an important parameter is</p><formula xml:id="formula_33">) ( m g</formula><p>. The inner layer contains 20 nodes. In <ref type="bibr" target="#b34">[35]</ref>, the topology of a neural network of the form</p><formula xml:id="formula_34">( 1 m -2 m -14)=   14 9 4   was considered, where 1 2 1 2   m m</formula><p>is the number of hidden layers;</p><formula xml:id="formula_35">4 1  m</formula><p>is the number of nodes in the input layer. In this paper, let's focus on the topology 9-3-2. This architecture corresponds to the transport system model of 4 sections with parameters ( <ref type="formula" target="#formula_29">20</ref>)</p><formula xml:id="formula_36">) ( 2 3   m m x   , ) ( 1 3  m m g x  </formula><p>and one node whose value is one. The hidden layer contains 3 nodes. The output layer contains 2 nodes <ref type="bibr" target="#b20">(21)</ref>. The activation function has the form <ref type="bibr" target="#b21">(22)</ref>. The length of the conveyor is different.</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head n="6">Preparation of test data</head><p>As noted above, for existing transport systems it is almost impossible to obtain complete experimental data for training a neural network for transient modes. For training of the neural network, test data is required that contain a wide range of values. However, the functioning of the transport system in such a range of flow parameters is associated with high energy costs. Additionally, the lengths of the sections of the existing transport system are defined and cannot be changed. In this regard, let's use the PiKh -model ( <ref type="formula" target="#formula_0">1</ref>), ( <ref type="formula" target="#formula_1">2</ref>) <ref type="bibr" target="#b11">[12]</ref> to prepare the test data, which allows us to construct an exact solution that determines the state of the flow parameters of the transport system. Let us believe that the intensity of the material flow ) (  m to the input of the m-th non-node section of the conveyor and the belt speed ) (t a m m-th section is known:</p><formula xml:id="formula_37">  m a m a m m m t a a t a 1 0 sin ) (      ,<label>(22)</label></formula><formula xml:id="formula_38">a m a T m   , 4   m m a  , 8 3 0 1 0 m a a a m m    ,<label>(23)</label></formula><formula xml:id="formula_39">  m m m m m t t 1 0 sin ) (           ,<label>(24)</label></formula><formula xml:id="formula_40">    T m m  , 4    m m   , 8 3 0 1 0 m m m       ,<label>(25)</label></formula><p>at the initial linear density along the route of the conveyor section</p><formula xml:id="formula_41">  m m m m m S k t 1 0 sin ) (         ,<label>(26) 4 </label></formula><formula xml:id="formula_42"> m m   , 8 3 0 1 0 m m m       .<label>(27)</label></formula><p>To go to dimensionless coordinates, we choose the characteristic size d S , the charac- teristic process time d T for the transport system</p><formula xml:id="formula_43">6 S S d  , 6 T T d  . (<label>28</label></formula><formula xml:id="formula_44">)</formula><p>The choice of characteristic quantities is arbitrary and is used to select the scale of the scale for measuring system parameters for conducting a numerical experiment. We assume that the 6th section will be one of the most loaded elements of the system, or at least for a functioning transport system this section will be in operation for maximum time. To simplify the dependencies</p><formula xml:id="formula_45">) (  m , ) (t a m , ) (t m </formula><p>, used to form test data, we assume</p><formula xml:id="formula_46">d a T T  , d T T   , d S S   . (<label>29</label></formula><formula xml:id="formula_47">)</formula><p>Let us also introduce the characteristic flow of material in the network </p><formula xml:id="formula_48">d T t /   , d m d m d S S /   , (<label>30</label></formula><formula xml:id="formula_49">) d d m m m S T a g g 0 1 0   , kh m m m     0 1 0   , d d kh m m m T S 0 1 0       ,<label>(31)</label></formula><formula xml:id="formula_50">          4 sin ) ( ) ( 1 0    m m g g S T t a g m m d d m m ,<label>(32)</label></formula><formula xml:id="formula_51">           4 sin ) ( ) ( 1 0        m m S T t m m d d m m , (<label>33</label></formula><formula xml:id="formula_52">)             4 sin ) ( ) ( 1 0      m m t t m m m m . (<label>34</label></formula><formula xml:id="formula_53">)</formula><p>Since the choice d T is arbitrary, the parameter d T is defined in such a way that equality</p><formula xml:id="formula_54">d d S T a / 1 0  ,<label>(35)</label></formula><p>then dimensionless coefficients can be written as</p><formula xml:id="formula_55">8 3 0 m g m   ,<label>24</label></formula><formula xml:id="formula_56">3 0 m m    ,<label>24</label></formula><formula xml:id="formula_57">3 0 0 0 0 m a m      . (<label>36</label></formula><formula xml:id="formula_58">)</formula><p>For training the neural network, test data were used <ref type="bibr" target="#b37">[38]</ref>. Test data was generated on the foundation of the model ( <ref type="formula" target="#formula_0">1</ref>) -( <ref type="formula" target="#formula_6">7</ref>) <ref type="bibr" target="#b11">[12]</ref> in accordance with the scheme of the transport system of Fig. <ref type="figure">3</ref> and the architecture of the neural network shown in Fig. <ref type="figure" target="#fig_6">4</ref>. Test data is based on an analytical model (PiKh-model). The parameters of the analytical model correspond to conditions ( <ref type="formula" target="#formula_38">23</ref>)- <ref type="bibr" target="#b36">(37)</ref>.</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head>Analysis of the results</head><p>Fig. <ref type="figure">5</ref> shows the output flow of section 8 of the transport system (Fig. <ref type="figure">2</ref>, Fig. <ref type="figure" target="#fig_6">4</ref>) for the analytical model and the neural network model. The calculation of the parameters of the output flow for the neural network model is performed for the number of epochs equal to 300,000 and the learning coefficient</p><formula xml:id="formula_59">5 10    E W W n k j n k j      , , 1 , , ,     m N m m m y z E 1 2 ) ( 2 1 , (<label>37</label></formula><formula xml:id="formula_60">)</formula><p>where the updated weight value  Repetition is carried out with some delay (Fig. <ref type="figure">7</ref>). The delay value is the value 15 . 1 68   ( Fig. <ref type="figure">7</ref>) <ref type="bibr" target="#b37">[38]</ref>. This value can also be calculated using the test data table <ref type="bibr" target="#b37">[38]</ref>. On the other hand, using test data, let's calculate the average delay for section 6 and section 8. Material that leaves section 3 should go through section 6 and section 8 until it reaches the output of section 8 of the transport system. Thus, it should be assumed that the delay between the value of the material flow in section 6 and in section 8 is ).The offset of the output flow of section 8 is shown in Fig. <ref type="figure">8</ref>.</p><p>The developed model of a transport system using the neural network opens up new prospects for the design of control systems for a multi-section conveyor. Also, one of the differences between this work and works <ref type="bibr" target="#b20">[21]</ref><ref type="bibr" target="#b21">[22]</ref><ref type="bibr" target="#b22">[23]</ref><ref type="bibr" target="#b23">[24]</ref><ref type="bibr" target="#b24">[25]</ref> is that a new method of data preparation for training a neural network is proposed. This allows you to significantly expand the field of study of the behaviour of the parameters of the transport system for various established operating modes of individual sections. A separate area of further research is the definition of similarity criteria for transport systems. Such an approach will make it possible to determine the basic models for various operating modes of the transport conveyor and to study in detail the characteristics of the flow of the material for individual sections.</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head n="8">Conclusion</head><p>A model of a conveyor transport system using a neural network is one of the tools for research a transport system with a large number of separate sections. The advent of the analytical PiKh-model <ref type="bibr" target="#b11">[12]</ref> made it possible to generate test data that are necessary for training a neural network. The lack of a test data set is one of the problems that impede the process of constructing neural models. In many cases, the formation of a set of test data in the required range of parameter changes is an insurmountable obstacle. In this regard, an important result of this work is the development of a method for generating a set of test data for training a neural network that simulates conveyor-type transport systems. A distinctive feature of the modelling of transport systems is that they are complex dynamic distributed systems in which the signal propagates with a delay. And this article presents the first results of constructing a neural model on the foundation of an analytical model. Using the simple architecture of a neural network (9-3-2) as an example, a qualitative relationship between the output flows of the material of different sections is shown. The qualitative relationship between the output flow parameters of section 3 and section 8 is shown. A quantitative assessment of the estimated time of movement of the material through the sections of the transport system is given.</p></div><figure xmlns="http://www.tei-c.org/ns/1.0" xml:id="fig_0"><head>1 </head><label>1</label><figDesc>where d S is length of the conveyor line; d T is the characteristic time of the passage of the material along the transport route;    is the linear density of material distribution and material flow at a point in time t at the point of the transport route with the coordinate the limit value of the linear density of the material for the analyzed conveyor section; is the output flow of material from the bunker to the input of the con- veyor section, limited by max  is the predicted output flow of the material from the conveyor section;  </figDesc></figure>
<figure xmlns="http://www.tei-c.org/ns/1.0" xml:id="fig_1"><head>Fig. 1 .</head><label>1</label><figDesc>Fig. 1. Schematic diagram of the conveyor line [2]</figDesc><graphic coords="4,144.24,308.76,306.76,100.56" type="bitmap" /></figure>
<figure xmlns="http://www.tei-c.org/ns/1.0" xml:id="fig_2"><head></head><label></label><figDesc>the material flow at the exit from the transport system is determined by the type of expression of the linear density of the material ) (  at the initial time 0  . The linear density of the material ) ( 0    , at an arbitrary point  at the time tr    is related to the linear density of the material ) the input of the transport system at the time</figDesc></figure>
<figure xmlns="http://www.tei-c.org/ns/1.0" xml:id="fig_3"><head></head><label></label><figDesc>of time during which the element of material received at the entrance of the transport system at a time   passes the path along the transportation route equal to  . When 1 </figDesc></figure>
<figure xmlns="http://www.tei-c.org/ns/1.0" xml:id="fig_4"><head></head><label></label><figDesc>),<ref type="bibr" target="#b8">(9)</ref> determines the linear density of the material along the transportation route and allows you to calculate the material flow at an arbitrary location of the transport path of a separate conveyor section. At a constant speed of movement of the conveyor belt, the expression determining the linear density of the material speed of the belt is not constant in time, then to calculate the flow parameters of the conveyor transport system, it is necessary to determine the value of the delay timem   for each m-th section from the equation</figDesc></figure>
<figure xmlns="http://www.tei-c.org/ns/1.0" xml:id="fig_5"><head>Fig. 2 .Fig. 3 .</head><label>23</label><figDesc>Fig. 2. Diagram of a branched conveyor transport route</figDesc><graphic coords="7,124.68,182.28,345.84,225.00" type="bitmap" /></figure>
<figure xmlns="http://www.tei-c.org/ns/1.0" xml:id="fig_6"><head>Fig. 4 .</head><label>4</label><figDesc>Fig. 4. Neural network architecture</figDesc><graphic coords="8,188.52,309.24,218.16,200.28" type="bitmap" /></figure>
<figure xmlns="http://www.tei-c.org/ns/1.0" xml:id="fig_7"><head></head><label></label><figDesc>characteristic flow is equal to the sum of the average values m 0  of the non-nodal sections. It should be noted that the choice of characteristic values is arbitrary and also determines the scale of the variables m 0  of the problem under consideration. Taking into account (30), should write</figDesc></figure>
<figure xmlns="http://www.tei-c.org/ns/1.0" xml:id="fig_8"><head></head><label></label><figDesc>the m N parameters of the output layer between the test data m z and the values m y of the neural network model (Fig.4). To analyze the process of training a neural network, data from a test run comes in a strictly specified order. This allows for multiple repetitions of training</figDesc></figure>
<figure xmlns="http://www.tei-c.org/ns/1.0" xml:id="fig_9"><head>Fig. 5 .Fig. 6 .Fig. 7 .Fig. 8 .</head><label>5678</label><figDesc>Fig. 5. The value of the output flow of section 8, calculated using the analytical model (8, output) and the neural network model (8, outputA)</figDesc><graphic coords="11,125.28,362.28,344.64,116.04" type="bitmap" /></figure>
<figure xmlns="http://www.tei-c.org/ns/1.0" type="table" xml:id="tab_0"><head>Table 1 .</head><label>1</label><figDesc>Characteristics of long-ranged conveyor transport system</figDesc><table><row><cell>Сonveyor name</cell><cell>Length</cell><cell>sections Power</cell></row><row><cell></cell><cell>(km)</cell><cell>(kW)</cell></row></table></figure>
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