310715184743abstractSusChemE2015

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SusChemE 2015
International Conference on Sustainable Chemistry & Engineering
October 8-9, 2015, Hotel Lalit, Mumbai
MODELING AND SIMULATION OF PLATE HEAT EXCHANGERS WITH
GENERALIZED CONFIGURATION
Faizan Ahmad1, Sadaf Zaidi1
1
Department of Chemical Engineering, Z.H.C.E.T, Aligarh Muslim University, Aligarh- 202002, India
E-mail: f4faizahmad1989@gmail.com, sadaf63in@yahoo.com.
1. Introduction
The aim of this work is to develop a plate heat exchanger (PHE) modeling framework that is suitable for any configuration.
The purpose of such a model is to study the influence of the configuration on the exchanger performance. The model
equations are solved by a numerical simulation program in MATLAB 7.0.1 based on the R-K 4 numerical approach. The
program act’s as an ‘experimental’ tool to examine the combined effect of most of the geometrical parameters on the
operation of PHE, particularly the momentum and heat transfer rates. The results are compared with those obtained by Gut
and Pinto [1], who used second order centered finite difference method adopted for sugar solution system.
2. Material and Methods:
In this work, a configuration characterization of the PHE is presented by using the six simple parameters, which are used to
define the geometry of the PHE. The model equations based on some simplified assumptions are derived with the use of the
energy balance equations, which yield a set of ordinary differential equations (ODEs). The fluid inside a channel exchanges
heat with the fluid in the neighbouring channels through the thin metal plates, as shown in Fig.1.
On applying the energy balance on the differential element “control volume” as shown in Fig.1 in the direction of flow of
fluid, the following equations are obtained:
π‘‘πœƒ1
π‘‘πœ‚
= 𝑠1 𝛼 𝐼 (πœƒ2 − πœƒ1 ) for first channel
(1)
π‘‘πœƒπ‘–
= 𝑠𝑖 𝛼 𝑠𝑖𝑑𝑒(𝑖) (πœƒπ‘–−1 − 2πœƒπ‘– + πœƒπ‘–+1 )channel𝑖: (1 < 𝑖 < 𝑁𝑐 ), 𝑠𝑖𝑑𝑒(𝑖) = {𝐼, 𝐼𝐼} n
π‘‘πœ‚
(2)
π‘‘πœƒπ‘π‘
= 𝑠𝑁𝑐 𝛼 𝑠𝑖𝑑𝑒(𝑁𝑐) (πœƒπ‘π‘ −1 − πœƒπ‘π‘ )π‘™π‘Žπ‘ π‘‘π‘β„Žπ‘Žπ‘›π‘›π‘’π‘™, 𝑠𝑖𝑑𝑒(𝑁𝑐 ) = {𝐼, 𝐼𝐼}
π‘‘πœ‚
(3)
The equations 1, 2 and 3 are linear ODE(s) which can be solved analytically or by any numerical method. In this study RK4 order numerical method is used.
3. Results and Discussion:
The results obtained by the simulation program (Fig.2) for the general model of the PHE for the given inputs are compared
with those obtained by Gut and Pinto [1] (Fig. 3), who used a second order centred finite difference method adopted for
sugar solution system. The results of this work are close to that obtained by Gut and Pinto [1]. The variation of the
temperature with respect to the height of the plate shows almost the same trends as obtained by Gut and Pinto [1]. To
understand the trend of temperature profiles, the program in this work has been run for 7 channels. Here the configuration
has been taken in which hot fluid is flowing in side (I) and cold fluid in side (II).
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SusChemE 2015
International Conference on Sustainable Chemistry & Engineering
October 8-9, 2015, Hotel Lalit, Mumbai
The small deviation from the results of Gut and Pinto [1] may be attributed to the fact that the present model has used 7
channels whereas in [1] 36 channels have been used. Moreover, the numerical methods used for solving the two models are
also different.
Figure 1: Control volume for derivation of energy balance in an upward flow channel.
35
side I, 1st pass
30
theta 1
theta 2
thata 3
theta 4
theta 5
theta 6
theta 7
T(oC)
25
side I, 2nd pass
20
15
10
side II, 2st pass
5
side II, 1st pass
0
0
0.2
0.4 η
0.6
0.8
1
Figure 2: Simulated results for PHE by RK-4 numerical approach
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SusChemE 2015
International Conference on Sustainable Chemistry & Engineering
October 8-9, 2015, Hotel Lalit, Mumbai
Figure 3: simulated results by Gut and Pinto
4. Conclusions:
In the present a model has been developed to study the performance of PHE. The simulation results have been compared
with those obtained by Gut and Pinto [1]. The program developed in this study is an important tool for studying the
influence of the configuration on the exchanger performance. Further, an optimization method can be developed for a
rigorous configuration selection for PHE.
References:
[1] Gut, J.A.W., Pinto, J.M, “International Journal of Heat and Mass Transfer”, 46 (2003) 2571–2585.
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