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 conο¬guration. The purpose of such a model is to study the inο¬uence of the conο¬guration 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: ππ1 ππ = π 1 πΌ πΌ (π2 − π1 ) for first channel (1) πππ = π π πΌ π πππ(π) (ππ−1 − 2ππ + ππ+1 )channelπ: (1 < π < ππ ), π πππ(π) = {πΌ, πΌπΌ} n ππ (2) ππππ = π ππ πΌ π πππ(ππ) (πππ −1 − πππ )πππ π‘πβπππππ, π πππ(ππ ) = {πΌ, πΌπΌ} ππ (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). 1 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 2 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. 3