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COMPUTATIONAL MODELS TO STUDY THE IMPACT OF SETTING

ADJUSTING DEVICE ON DYNAMIC PROCESSES

*Vidadi Hasan Musayev, Natig

Azerbaijan Technical University, Baku

ARTICLE INFO ABSTRACT

The developed methods and algorithms of

are presented in the paper in an example of MOP, taking into account

pumping station (PS), with a continuous regulation of operation (performance) of the PS.

Copyright © 2015 Vidadi Hasan Musayevet al.This

unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

INTRODUCTION

The STUDIES have shown that the timing of the pressure recovery in the end, as well as any points of

disconnecting the intermediate pumping stations and other disturbances, is of practical importance for the automation issues pipelines [1,2]. Calculation and examination of transients in the main pipeline with intermediate control e

stops at one of the intermediate pumping stations or pumping, including an entire pump station is enabled (disabled), is a co mathematical problem. Information about the dynamic processes at different disturbances, can prevent t

determine the performance of the remote control system for the information collection, and select the rational system of auto control.

Relevance

Due to the changes in the performance of the pumping station (PS) when it is enabled o

in the pipe changes before and after oil pumping station (OPS). The change in the pressure after the disturbance source will the performance of the next OPS. In suchproblem statement, it is important to

two adjoining sections of pipelineto OPS, moreover, at the start and end sections of the pipeline it is necessary to coordina amount of pressure change with the characteristics of related OPS [4].

meanwhile, it includes a number of specific problems awaiting solutions. Mathematical solution of the problem requiressolving the equation ofthe adjuster jointly with the equation of motion control and st

The problem statement

In [3] the analysis of the operation mode of the main pipeline with multiple adjustable intermediate pumping stations is implemented on thebase of the proposed computational models in discrete adjustment of MOPperfor

the impacts of adjusting devices on the transition processes the problem becomes much more complicated.

*Corresponding author: Vidadi Hasan Musayev, Azerbaijan Technical University, Baku

ISSN: 0975-833X

Vol.

Article History:

Received 14th September, 2015

Received in revised form 15th October, 2015

Accepted 27th November, 2015 Published online 30th December,2015

Citation: Vidadi Hasan Musayev, Natig Etibar Huseynov and Ziraddin Amirahmed Qasimov the impact of setting options of adjusting device on dynamic Processes

Keywords:

Mainoil pipeline, Distributed options, Discrete method, Adjusting device,

Initial and boundary conditions.

RESEARCH ARTICLE

COMPUTATIONAL MODELS TO STUDY THE IMPACT OF SETTING

ADJUSTING DEVICE ON DYNAMIC PROCESSES

Natig Etibar Huseynov and Ziraddin Amirahmed

Azerbaijan Technical University, Baku

ABSTRACT

The developed methods and algorithms of calculating transition processes of the main oil pipelines are presented in the paper in an example of MOP, taking into account

pumping station (PS), with a continuous regulation of operation (performance) of the PS.

This is an open access article distributed under the Creative Commons Att use, distribution, and reproduction in any medium, provided the original work is properly cited.

The STUDIES have shown that the timing of the pressure recovery in the end, as well as any points of

disconnecting the intermediate pumping stations and other disturbances, is of practical importance for the automation issues pipelines [1,2]. Calculation and examination of transients in the main pipeline with intermediate control e

stops at one of the intermediate pumping stations or pumping, including an entire pump station is enabled (disabled), is a co mathematical problem. Information about the dynamic processes at different disturbances, can prevent t

determine the performance of the remote control system for the information collection, and select the rational system of auto

Due to the changes in the performance of the pumping station (PS) when it is enabled or its separate units are disabled,the pressure in the pipe changes before and after oil pumping station (OPS). The change in the pressure after the disturbance source will the performance of the next OPS. In suchproblem statement, it is important to take into account the dynamic characteristics of the two adjoining sections of pipelineto OPS, moreover, at the start and end sections of the pipeline it is necessary to coordina amount of pressure change with the characteristics of related OPS [4]. Although this problem has not been studied enough, meanwhile, it includes a number of specific problems awaiting solutions. Mathematical solution of the problem requiressolving the equation ofthe adjuster jointly with the equation of motion control and stability of MOP.

In [3] the analysis of the operation mode of the main pipeline with multiple adjustable intermediate pumping stations is implemented on thebase of the proposed computational models in discrete adjustment of MOPperfor

the impacts of adjusting devices on the transition processes the problem becomes much more complicated.

,

Available online at http://www.journalcra.com

International Journal of Current Research Vol. 7, Issue, 12, pp.24084-24089, December, 2015

INTERNATIONAL

Vidadi Hasan Musayev, Natig Etibar Huseynov and Ziraddin Amirahmed Qasimov,2015. the impact of setting options of adjusting device on dynamic Processes”, International Journal of Current Research,

z

COMPUTATIONAL MODELS TO STUDY THE IMPACT OF SETTING OPTIONS OF

Amirahmed Qasimov

calculating transition processes of the main oil pipelines are presented in the paper in an example of MOP, taking into account adjusting devices in the pumping station (PS), with a continuous regulation of operation (performance) of the PS.

is an open access article distributed under the Creative Commons Attribution License, which permits

The STUDIES have shown that the timing of the pressure recovery in the end, as well as any points of the pipeline, after disconnecting the intermediate pumping stations and other disturbances, is of practical importance for the automation issues of pipelines [1,2]. Calculation and examination of transients in the main pipeline with intermediate control elements, when the pump stops at one of the intermediate pumping stations or pumping, including an entire pump station is enabled (disabled), is a complex mathematical problem. Information about the dynamic processes at different disturbances, can prevent the accidents, and determine the performance of the remote control system for the information collection, and select the rational system of automatic

r its separate units are disabled,the pressure in the pipe changes before and after oil pumping station (OPS). The change in the pressure after the disturbance source will affect take into account the dynamic characteristics of the two adjoining sections of pipelineto OPS, moreover, at the start and end sections of the pipeline it is necessary to coordinate the Although this problem has not been studied enough, meanwhile, it includes a number of specific problems awaiting solutions. Mathematical solution of the problem requiressolving

In [3] the analysis of the operation mode of the main pipeline with multiple adjustable intermediate pumping stations is implemented on thebase of the proposed computational models in discrete adjustment of MOPperformance. Taking into account the impacts of adjusting devices on the transition processes the problem becomes much more complicated.

INTERNATIONAL JOURNAL OF CURRENT RESEARCH

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In this context, this paper sets out the developed method and algorithm for calculating transients in MOP taking into account adjusting devices PS.

Solution method

In this work, double and discrete Laplace transform is used as the mathematical apparatus. The recurrence relations are applied in the transition from the image to the original functions [2]. Obviously, the development of calculation methods for the study of transients in MOPbecomes much more complicated during the smooth regulation of operation mode (performance) of the PS. In this case, the main pipeline should be viewed as a single system: - PS - pipeline with controller, which smoothly changes the performance of the PS [1].

Under such conditions, the problem is mathematically reduced to the solution of the equations of continuity and motion of unsteady so-called inlet and outlet sections of the main pipeline with the boundary conditions of the form as follows:

If u0(0,t)=0,

If u=1, =0 j(1,t)=J(0,t) ,j(1,t)=k4(1,t)- k5(0,t)+ k6(t), ………(1) If =1 J(1,t)=J,

Where (t) is a variable, which characterizes the relative change in the parameter with the impact of the adjusting body on the

performance of the PS, k6- defines the extent of this impact on the performance.

To solve this problem we accept zero initial conditions, and boundary conditions (1) we transfer to the operator form:

If u=0Ψ(0,s)0;

If u=1, =0j(1,s)J(0,s); ………..(2)

) ( ) , 0 ( ) , 1 ( ) , 1

( s k4Ψ s k5 s k6 s

j  

;

If =1 J s s J(1, )1 .

After the double Laplace transform the equations describing unsteady movement of fluid before and after the PS [2] in operator form are:

) , 0 ( )

,

(u s sk1 k2 sh u j s

Ψ

  

 , ……….(3)

) , 0 ( )

,

(u s ch u j s

j

, ………(4)

k s k s k s

s ch s

sh k sk

s      

 

( , )   1  2 4 (1, ) 5 (0, ) 6 ( )  (0, ) , ……….(5)

(

1

,

)

(

0

,

)

(

)

.

)

,

0

(

)

,

(

4 5 6

2 1

s

k

s

k

s

k

ch

s

sh

k

sk

s

J



……….(6)

Taking into account the boundary conditions (2), after some intermediate mathematical calculations for the functions included in (36) we get:

s J a s ch

a k

s   

5 5

4 (1, ) 1

) , 0

( 

 , ………(7)

Where , ,

2 1 5

4 10 6

4 

sh

k sk ch k a b k a a5

  

1

,

s Tu

s Tu a b10

 

  

Tu- denotes the time of the isodrom of the isodromic

adjuster; and a- as pecified speed of the servomotor; v – feed back velocity.

(1, ) (0, ) ( )

1 ) , 0

( k4 s k5 s k6 s

ch s

j

 

 , ………..(8)

) , 0 ( ), , 1

( ss

 - accordingly, the images of the features(u,t) (ifu=1) and(,t) (if=0) or (8), taking into account (7)

ch b k a ch

b k k S J s ch

b k a ch

ch k sk

k

s j

10 6 4

10 6 5 10

6 4

2 1

4

) , 1 ( )

, 0 (

  

 

 ………(9)

) , 1 ( s

(3)



2 4 10 6 4 10 6 5 2 1

)

,

1

(

sh

k

ch

b

k

a

ch

sh

b

k

k

k

sk

s

J

s

. ……….(10)

Using (9) and (10) in (3) for

( su, )we obtain:

u

ch

sTu

sTu

v

a

k

k

k

sk

s

J

s

u

1

1

)

,

(

1 2 5 6

1

, ………..(11)

Where characteristic equation of the system is

5 6 2

2 1 2 4 1

1

ch

sTu

sTu

v

a

k

k

ch

sh

k

sk

sh

k

-

Using (9) and (10) we obtain:

4 6 10 4 2

10 6 5

)

(

1

)

(

)

,

0

(

sh

k

ch

b

k

a

ch

b

k

k

s

J

s

j

, ………(12)

Or 1 6 5 1 1 ) , 0 (             sTu sTu v a k k s J s

j . ………(13)

Thus, taking into account (13) the equations (46) will be as follows:

u

sh

sTu

sTu

v

a

k

k

s

J

s

u

j

1

1

)

,

(

5 6

1

, ……….(14)

, 1 1 ) ,

( 5 6

2 1 4 2 1 1                                 



chsh

sTu sTu v a k k ch ch k sk sh k k sk s J

s ………..(15)

1

1

)

,

(

5 6

2 1 4 1





ch

u

ch

sTu

sTu

v

a

k

k

sh

ch

k

sk

sh

k

J

s

s

J

………(16)

If t, which corresponds to the obtained expressions =0, in the new mode of the pipeline we obtain the followings:

ycm

(

u

)

Jk

2

u

;

ycm

(

)

Jk

2 , ………..(17)

J

J

j

ycm

ycm

.

Thus, the obtained expression corresponds to the expression [2]..We can conclude that although the examined section of the pipeline is the endpoint and it is equipped with the system, which gradually changes the performance of the PS, and the size of the defined pressure value does not change.

In particular case, in the case of disturbance of inertial term in the initial equations [2]., we obtain the expression corresponding to [5].:

u

sh

sTu

sTu

v

a

k

k

k

s

J

s

u

5 6 1

1 2 1

1

1

)

,

(



, ………(18)

u

sh

sTu

sTu

v

a

k

k

s

J

s

u

j

5 6 1

1

1

1

)

,

(



, ………(19)



1 1 5 6 1 1

2 1 1 4 1 2 1

1

1

)

,

(

ch

sh

sTu

sTu

v

a

k

k

ch

ch

k

sh

k

k

s

J

s

, ………..(20)



sTu

sTu

v

a

k

k

s

sh

ch

k

sh

k

J

s

s

J

(

,

)

1

1 1 5 6

1

2 1 1 4 1

, ………(21)

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where 3 2 1

k

s

k

, 2 1

6 5 1 1 2 1 1 2 4 1

1

ch

sTu

sTu

v

a

k

k

ch

sh

k

sh

k



.

To obtain thecalculated expression of thetransient, according to the described method, the resulting equations are transformed into a discrete form, and using the convolution theorem, we obtain the calculated formulas for the required functions inthe domain of originals:

                                         

     c k D m n m k c k c k m n m k m n m k D C m n m k m n m k c k k k J n n m n m n m n m n m 4 1 4 4 0 6 0 5 0 6 0 5 4 3 1 1 2 ] [ ] [ 2 } ] [ 1 ] [ ] [ 1 ] [ ] [ 1 ] [ ] [ 1 ] [ { 2 ,    

, ] [ ] [ ] [ ] [ ] [ 1 ] [ ] [ 1 ] [ ] [ ] [ ] [ 1 0 4 1 0 4 1 0 3 3 1 4 1 2 4 2 2 4 4 1 1

                                              n m n m n m n m n m n m m T n c k D m n m k m n m k k k c k m n m k c k D m n m k c k c k m n m k           ………(22)

where © [ ] [ ]; © [ ] [ ];

0 2 2

0 1

1

    n m n m m k m k m k m k

   

u)

λ(1

m

,

u)

λ(1

m

αT

I

(e

λ

αT

u)

λ(1

m

αT

I

(e

u)

λ(1

m

0

при

,

0

[m]

k

2 2 1 0 n u) λ(1 m m αT 2 2 0 n 0 m m αmT 5,6 1 1 1

The sign “-“ refers to the original

k

5

,and «+» to

k

6

.

In a particular case, if we neglect in the initial equations

t t) (u, j  

, the design formula (21) is as follows:

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. ] [ ]

[ ; ] [ ]

[

; 2 4

4 exp 2

] [

; 2 ] [ ; ]

[

0 6 6

0 1 5 5

6

5 4 4

1 1

 

       

        

       



  

m

m m

m

nT

m k m

k m k m

k

nT k erfc k nT

k nT

n k

nT n

k e nT n

k







Original functions j

 ,n

,

,n

,J

,n

are determined by the similar way.

All abovementioned proves that dealing with such problems with the use of the proposed method, there is no need for the decomposition of the coefficient of the expansion wave, and limiting with the first two terms, where, in fact, the systems with the distributed parameters are examined instead of the dynamics as a special case, the dynamics of the so-called balanced links. An analysis of the work shows that depending on the parameters’ values, which take into account the friction and the repetition period of the lattice function, different errors occur [2]. Apparently, the greater the friction values and the repetition period of the lattice function, the more the value of the desired parameter of the specified mode and dynamics differs from the reality.

The Figures 1 and 2 show the theoretical pressure variation curves calculated with the expression (22) corresponding to different settings of the examined adjuster caused by increasing the load at the end point. The Figure 1: 1 - the curve is obtained ifa/s=0,18,

[image:5.595.175.425.314.453.2]

Tu=25; 2- the curve is obtained ifa/s=1, Tu=25; 3 - the curve a/s=1, Tu=50; 4- the curve a/s=0,2, Tu=50.

[image:5.595.166.429.480.623.2]

Fig. 1. The theoretical curves of transients in MOP at different settings of the adjuster

Fig. 2. The theoretical curves of transients in MOP at different settings of the pressure adjuster

The graph (Fig. 1, curves 1 and 3) shows that choosing the greater values of the constant time of the adjuster and the ratio of the feedback speed controller to the specified value of the speed of the servomotor (a/s) significantly delays the transition process and leads to overshoot.

REFERENCES

Musayev Vidadi Hasan, Huseynov Natig Etibar 2015. Analysis of the Operation of the Systems with Distributed Parameters with the Adjusting System Objects International Transaction of Electrical and Computer Engineers System, 3(1), 30-33 doi: 10.12691/iteces-3-1-4

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Musayev, V.G. 2014. Dynamic processes in complex systems with distributed parameters. LAP LAMBERT Academic Publishing., 127 p.

Musayev, V.G. 2013. The development of computational models of transient processes in the systems with distributed parameters with the system adjusters. International Scientific-Technical Journal “Інформаційнітехнологіїтакомп’ютернаінженерія”, 2013, No 2, pp. 46-63.

Musayev, V.G., Huseynov, N.E., Abilov, K.A. 2011. Structural analysis of the dynamic processes in the main oil pipelines. Information technologies of modeling and control. Voronezh, No 6 (71), pp.667-674.

Zhidkova, M.A. Pipeline transportation of gas. Kiev, NaukovaDumka, 1973, 142 p. Information about the authors

Musayev Vidadi Hasan–Dr. "Computer systems and networks" Department chairman, Azerbaijan Technical University, Baku. Tel: (994 12) 5391138, e-mail:[email protected]

Huseynov Natig Etibar- Ph.D., Associate professor."Applied Informatics" Department, Azerbaijan Technical University, Baku. Tel: (994 12) 5391138,[email protected]

Qasimov Ziraddin Amirahmed - Ph.D. associate professor."Computer systems and networks" Department, Azerbaijan Technical University, Baku. Tel: (994 12) 5391138

Figure

Fig. 1. The theoretical curves of transients in MOP at different settings of the adjuster

References

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