International Journal of Scientific & Engineering Research, Volume 4, Issue 8, August-2013 1890

ISSN 2229-5518

Use of Artificial Neural Network for Correlation of Vapour-Liquid Equilibrium Data for

Hydrocarbon Ternary System (Ethane-n-Butane-n-Pentane)

* Daniyan, I. A.1, Adeodu, A. O.2, Omitola, O. O.3 Daniyan O. L4and Yusuff, A. S5.

(1, 2)Department of Mechanical Engineering,(3)Department of Computer Engineering,

(4) Center for Basic Space Science, University of Nigeria, Nsukka, Nigeria.

(5) Department of Chemical Engineering.

(1, 2, 3, 5)Afe Babalola University, Ado Ekiti, Ekiti State, Nigeria.




1afolabiilesanmi@yahoo.com, 2femi2001ng@yahoo.com, 3omitolasegun@yahoo.com,

(4) danomartins@hotmail.com, 5adeyinkayusuff@yahoo.com

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Abstract

In this study, existing experimental vapour-liquid equilibrium (VLE) data covering a wide range of temperature, phase composition and pressure for ethane-n-butane-n-pentane was correlated using MATLAB (Matrix Laboratory) software. To increase the reliability of correlations, neural network was trained using existing vapour-liquid equilibrium data with the aid of Levenberg Marquardt algorithm. Network parameters are fine-tuned until the output generated by simulation are checked and observed to match with pre-determined experimental V L E data. It was found that there is high degree of coherence between the chosen targets from experimental data and predicted values. This confirms that correlations and predictions of V L E data using neural network is efficient and significant.

Key words: Correlation, Levenberg Marquardt algorithm, MATLAB, Network parameters, Neural network, Simulation, Vapour-liquid equilibrium (VLE)

Word count: 126

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International Journal of Scientific & Engineering Research, Volume 4, Issue 8, August-2013 1891

ISSN 2229-5518

INTRODUCTION

Recently, many methods and approaches have been used to determine vapour-liquid equilibrium data for hydrocarbon binary, ternary and multi-components because of its relevance and great importance in chemical process industries, refining and petroleum industries. A few of these approaches are: graphical, analytical and statistical approaches. However, it was found that the correlation with these approaches were not so accurate as expected and in some cases it proved quite difficult to correlate unfamiliar data and operating conditions. Due to these frustrating efforts, artificial neural network (ANN) or machine learning algorithm (embedded in the MATLAB) comprising of a large number of highly interconnected processing elements (neurons) was developed for correlating vapour-liquid equilibrium data because it can reason more dynamically like the human brain, follow trend, capable of self training and can organize both enormous, familiar and unfamiliar data.
Vapour liquid equilibrium (abbreviation VLE) is a state where liquid and its vapour (gas phase) are in equilibrium: a condition or a state where the rate of evaporation (liquid becoming vapour) is equal to the rate of condensation (vapour becoming liquid), under specific conditions where no net vapour liquid inter-conversion intervenes [1]. When heat is added slowly to a closed vessel that contains liquid mixture of several components at constant pressure, the
temperature increases until a point is reached when the first bubble forms, at this point, vapour and liquid is said to be in a state of equilibrium [2]. As vapourization proceeds, the composition of the remaining liquid continually changes and hence does its vapourization temperature. A similar phenomenon occurs when a mixture of vapour is subjected to a condensation process at constant pressure, at some temperature. The first droplets of liquid form, thereafter the compositions of vapour and the condensation temperature both changes. When a liquid is heated slowly, at constant pressure, the temperature at which the first vapour bubble forms is the bubble point temperature of the liquid at a given pressure and when a gas (vapour) is cooled slowly at constant pressure, the temperature at which the first liquid droplet forms is the dew temperature [2] [3].
When two phases are in equilibrium, vapour- liquid equilibrium data is useful in relating the composition of the liquid phase to that of the vapour phase [4].
The modeling and control of equipment for different chemical processes require the vapour- liquid equilibrium data [5] [6].
The thermodynamics of ternary phase equilibrium is based on the concept of the chemical potential. The chemical potential was introduced by Gibbs while G. N. Lewis

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International Journal of Scientific & Engineering Research, Volume 4, Issue 8, August-2013 1892

ISSN 2229-5518

proposed the idea of the quantity called fugacity,
which has a unit pressure.

F v Φ = i yi P

(3)

Since, in a mixture of ideal gases, the fugacity of
each component is equal to its partial pressure.
The activity coefficient γ on the other hand
Physically, it is convenient to think of the
relates the liquid phase fugacity

Fi L

to the
fugacity as thermodynamic pressure, in real
liquid phase mole fraction xi
and to the
mixtures, the fugacity can be considered as a partial pressure which is corrected for non-ideal
standard state fugacity

Fi L

Fi01 as

behavior. Fugacity Fi
is related to partial

γ i = 01

xi Fi

(4)

pressure of a system when the system
approaches or behaves like an ideal situation. Thus,
Combining equations 3 and 4, the equation for any component i becomes:

Fi

yi P

as p-------0 (1)

Fi = Fi

01

(5); and

Pressure is low and approaches zero

Φi yi P = γ i xi Fi

(6)

yi = mole

fraction of component i in the

The relation between fugacity coefficient Φ and activity coefficient γ is may be given as

vapour phase

P = total

pressure

Φi yi P = γ i xi Pi

(7)

For two phases which are at the same temperature, the equation of equilibrium for
For non ideal gas and liquid solution

Sat Sat

each component is expressed in terms of

Φi yi P = γ i xi Pi

Φ (8)

fugacity Fi as

Fi = FL

(2)

Equation 7 reduces to

yi P = xi Pi

(9)

Thus, fugacity coefficient Φ relates the vapour phase fugacity F V to vapour phase mole fraction
yi and total pressure P by

Pi = vapour

Pp = Partial

pressure

pressure

P Sat is the saturation vapour pressure of pure

component i

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International Journal of Scientific & Engineering Research, Volume 4, Issue 8, August-2013 1893

ISSN 2229-5518

Φ Sat

is the fugacity coefficient at saturation of

[7], [8], [9], [10], [11], and [12], have all
reported the correlation of vapour-liquid

pure component i

but

yi P = Pp

Equation 9 becomes

Pp = xi P1

(10)

(11)

equilibrium data for binary systems while [13] have shown how NRTL equation can be used to correlate vapour-liquid equilibrium data for ternary systems. In this work, MATLAB, software with neural network conditions was used to correlate experimental vapour-liquid equilibrium data with the aid of Levenberg
Marquardt algorithm employed to train the set of
Activity coefficient is related to molar Gibb’s energy by:
data. The Levenberg Marquardt algorithm is one of the best training rules designed to approach network speed [14], cited by [8]. Neural

T i i

(12)

network is an interconnected group akin to the

n G E = RT n ln γ

i

vast network of neuron in the human brain. It is

RT ln γ

 ∂(nG E ) 

=

an information processing paradigm that is

i

 ∂ni

T ,P ,n ≠1

(13)

inspired by the way biological system neurons such as the brain process information [15]. The

E E

ln G

1  ∂(nG ) 

artificial neural network is a model based on

γ i =

RT

where

= 

RT

ni

T ,P ,n ≠1

(14)

some experimental results that is proposed to predict the required data because of avoiding more experiments. [8]. In the course of data

R is the ideal gas constant and T is temperature

correlation, neural network provides a network which organizes and provides good pattern for
vapour- liquid equilibrium data.

Table 1.0: Experimental vapour-liquid equilibrium data for the ethane-n-butane-pentane ternary system

Source: [16], [17]

Pressure

(kPa)

Ethane

vapour mole

Butane

vapour mole

Pentane

vapour mole

Ethane

liquid mole

Butane

liquid mole

Pentane

liquid mole

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International Journal of Scientific & Engineering Research, Volume 4, Issue 8, August-2013 1894

ISSN 2229-5518

fraction

(y2 )

fraction

(y4 )

fraction

(y5 )

fraction

(x2 )

fraction

(x4 )

fraction

(x5 )

2444.3

0.846

O.102

0.052

0.517

0.274

0.209

2855.2

0.875

0.086

0.039

0.602

0.229

0.169

3026.2

0.860

0.077

0.037

0.713

0.175

0.112

3271.5

0.882

0.081

0.037

0.765

0.144

0.091

3386.0

0.872

0.085

0.043

0.794

0.128

0.078

2111.7

0.828

0.149

0.023

0.510

0.378

0.112

2507.8

0.852

0.122

0.020

0.599

0.312

0.089

2903.0

0.871

0.111

0.018

0.690

0.245

0.065

3146.4

0.871

0.110

0.019

0.740

0.208

0.052

3349.46

0.865

0.115

0.020

0.788

0.170

0.042

2164.2

0.893

0.046

0.061

0.560

0.131

0.309

2254.2

0.898

0.043

0.059

0.064

0.113

0.246

2923.7

0.904

0.041

0.055

0.718

0.093

0.246

3316.6

0.911

0.041

0.051

0.793

0.076

0.131

3439.6

0.910

0.038

0.052

0.823

0.068

0.109

3517.5

0.904

0.041

0.055

0.836

0.061

0.103

RESULTS AND DISCUSSION


Fig.1.0: Performance Trainlm Graph Fig.3.0: Output-target Graph (Ethane)

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International Journal of Scientific & Engineering Research, Volume 4, Issue 8, August-2013 1895

ISSN 2229-5518


Fig. 2.0: Regression Graph Fig. 4.0: Output-target Graph (Butaane)

Fig. 5.0: Output-target Graph (Pentane)

Table 2.0: Table showing liquid mole fraction and temperature values from experimental data (target)

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International Journal of Scientific & Engineering Research, Volume 4, Issue 8, August-2013 1896

ISSN 2229-5518

Table 3.0: Table showing predicted values of liquid mole fraction and pressure with the use of Artificial Neural Network (A N N)

Ethane

(x2 )

Butane

(x4 )

Pentane

(x5 )

Temperat ure (K)

0.5173

0.2738

0.2091

338.5500

0.6029

0.2290

0.1690

338.5550

0.7127

0.1734

0.1122

338.5551

0.7649

0.1450

0.0900

338.5551

0.7957

0.1284

0.0780

338.5549

0.5104

0.3776

0.1121

338.5550

0.5980

0.3121

0.0890

338.5552

0.6857

0.2443

0.0652

338.5551

0.7426

0.2060

0.0520

338.5550

0.7866

0.1708

0.0422

338.5550

0.5653

0.1310

0.3090

338.5551

0.6400

0.1131

0.2455

338.5500

0.7105

0.0920

0.2460

338.5500

0.7942

0.0762

0.1314

338.5500

0.8266

0.0667

0.1090

338.5550

0.8349

0.0617

0.1033

338.5549

Simulation takes the network input P and the network object and returns the network output a. In this work, the simulation is repeated as a loop. In the loop, the model is run for specific time, parameter changed and model run again. This was repeated until the correlation was completed and the simulation was completed when the target was met after 104 iterative processes. This is shown in Fig. 1.0, with the trainlm line (performance goal line) touching the target line.
The small value of the mean square error (M S E) as shown in Fig. 1.0 is an indication that the developed network has efficiently trained the data and that the output (predicted values) are not far from the target. Comparing table 2.0 and
3.0, the output (predicted values) of liquid phase compositions and temperature gives set of data that is close to the target (experimental liquid phase compositions and temperature data).
From Fig. 2.0, 3.0, 4.0 and 5.0 (regression and output-target) graphs, deviations of data points from the line of best fit is negligible which indicates that there is high degree of correlation between predicted values and experimental data. Correlation coefficient R will be significant when the indices given by [i, j] in the P matrix is less or equal to 0.05. Correlation coefficient R in Fig. 2.0 (Regression graph) is 1, which means there is 100% correlation between the predicted and experimental vapour-liquid equilibrium data: an indication that the developed neural network is highly efficient. The value of R in Fig. 3.0, 4.0 and 5.0 is given as 0.99949,
0.99879 and 0.99919 respectively meaning that there is 99.949%, 99.879% and 99.919% correlation between output and the set target for ethane-butane-pentane ternary system. It also confirms that there is good correlation between the input, target and output parameter.
From the experimental data, the values of pressure and vapour phase composition of the ternary system were given as input to the network while the target was taken to be the

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International Journal of Scientific & Engineering Research, Volume 4, Issue 8, August-2013 1897

ISSN 2229-5518

respective temperatures and liquid phase composition.
Comparing table 2.0 and 3.0, the output (predicted values) of liquid phase compositions and temperature gives set of data that is close to the target (experimental liquid phase compositions and temperature data).
Vapour mole fraction of ethane, butane and pentane picked at random at a particular pressure, [0.865; 0.115; 0.020; 3349.46], were given as input to the trained network which predicted its equivalent composition of the liquid phase and temperature as [0.7881; 0.1699;
0.0420; 3380.55]. These values agree with the experimental data.

CONCLUSIONS AND RECOMMENDATIONS

Neural network was successfully used to correlate vapour-liquid equilibrium data for hydrocarbon ternary systems (ethane-n-butane- n-pentane). The network was highly efficient and suitable for training the experimental data because the set target and performance goal was met. The accuracy of prediction of neural network increases when the network is iteratively trained. For the ternary systems, mean square errors are negligible and predicted values were very close to the targets. In addition, good correlation results for hydrocarbon ternary systems were achieved as correlation coefficient
is close to 1 for each of the system. A successful
validation test evidenced in the corresponding predicted values of liquid phase compositions and its equivalent vapour phase compositions also indicates that the predictive capability of the network is highly efficient. All these confirmed conclusively that neural network is a viable tool for the correlation of vapour-liquid equilibrium data for hydrocarbon ternary system.
Research work can however be extended to other ternary systems like alcohol.

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International Journal of Scientific & Engineering Research, Volume 4, Issue 8, August-2013 1898

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