developed, and parametric studies are conducted with the model. Based on the parameter study results, a dehumidification performance diagram is propos

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Evaluation of A Plate Desiccant Outdoor Air-conditioning System Utilizing Cogenerated Hot Water Using A Numerical Model T. Baba 1, B. Park 1 1, *1, and T. Nagai 1 Department of Architecture, Tokyo University of Science, Niijuku, Tokyo, 125-8585, Japan ABSTRACT Desiccant-based outdoor air systems have the potential to save energy and exhibits good performance in controlling the humidity in buildings. Recently, the plate type desiccant system has been proposed. There is a lack of research about its optimal design method and system performance. The aim of this study is to propose the plate type desiccant system utilizing cogenerated hot water. A dehumidification performance diagram is proposed based on a parameter study. This diagram can be referenced for system design. KEYWORDS Desiccant, Numerical model, Performance analysis, Cogeneration INTRODUCTION Desiccant air-conditioning systems are considered to treat latent heat load efficiently by using adsorbent. A rotor type desiccant is a popular type that uses rotor covered with solid desiccant material. It can lower the air humidity ratio constantly. The rotor type desiccant system however requires high temperature to regenerate the desiccant rotor and therefore has high energy consumption. Recently, the desiccant system has been proposed that uses square plates covered with solid desiccant materials (Rang, Xiao-Hua and Yi 213). Previous studies on the heat-pump driven plate type desiccant outdoor air processor reported that the desiccant regeneration temperature (5 ) was low enough to operate. In addition, this system showed a high dehumidification performance by combining several stages. The desiccant materials, sectional area and thickness of the plates, flow rate through the system, and available heat source have however not been studied in detail. The aim of this study is therefore to evaluate the performance of the plate type desiccant outdoor air-conditioning system. A numerical model of the plate type desiccant system is * Corresponding author email: nagai@rs.tus.ac.jp 878

developed, and parametric studies are conducted with the model. Based on the parameter study results, a dehumidification performance diagram is proposed. A scheme of the plate desiccant system is shown in Fig 1.This system composed of two air flow channel, one to process the air and another to regenerate the desiccant plate. A pair of desiccant plates change positions between the two air channels, and process the air continuously. The system utilizes cogenerated hot water and cool water from a cooling tower. OA Cool and dehumidify Desiccant plate SA RA RA Cold water (26 ) Hot water (6 ) Heat and regenerate Cooling coil Heating coil Figure 1. The desiccant air-conditioning system of this study Numerical Model The scheme of the numerical model that is used in this study shown in Fig.2. Heat and moisture exchange between air and desiccant materials is calculated for each microcell defined over desiccant plate. The microcells are linked in a line, with the outlet air state of one cell being the inlet air state of next cell. The numerical model makes the following assumptions. Heat and water content distribution in the sectional area of the plate are neglected. The pressure drop of the airflow through the channel is neglected. The correlation between the humidity ratio on the desiccant s surface and the water content of the adsorptive follows the adsorption isotherm of the desiccant materials. Exchange of heat and vapor Figure 2. Modeling of desiccant plate 879

Heat and moisture equation Heat and moisture exchange are calculated by equations (1-4) which are based on the combined heat and moisture transfer theory (Momoi et al. 26). The heat equation of the air through the cell is: εc a ρ a T a t = εuc aρ a T a x αs d(t a.ave T d ) (1) The moisture equation of the air is: ερ a X a t = εuρ a X a x α S d(x a.ave X b ) (2) The heat equation of the desiccant material in the cell is: (1 ε)c d ρ d T d t = Lα S d (X a.ave X b ) + αs d (T a.ave T d ) (3) The moisture equation of the desiccant in the cell is: (1 ε)ρ d w t = α S d (X a.ave X b ) (4) The correlation between humidity ratio on the surface of the desiccant materials and the water content in the desiccant materials is: w = f(x b, T d ) X b = g(w, T d ) (5) Equation (5) defines the adsorption isotherm of desiccant materials. Fig.3 shows the adsorption isotherm of silica gel and zeolite. Equation (5) calculates the humidity ratio on the desiccant surface from the water content at equilibrium. Approximations that are obtained from the adsorption isotherm are shown in Tables 1 and 2. 88

Water content [kg/kgd] Water content [kg/kgd].2.15.1.5. 298K 318K 333K 363K.5.1.15.2 Humidity ratio on surface of desiccant[kg/kg'] (a) Silica gel (b) zeolite Figure 3. Adsorption isotherm of each material.25 293K.2.15 318K.1.5 333K..5.1.15.2 Humidity ratio on surface of desiccant [kg/kg'] Table 1. Approximation of the adsorption isotherm of silica gel Temperature of desiccant plate Approximation 298 K Xb =.348w* 318 K Xb =.174w* 333 K Xb =.236w* 363 K Xb =.9771w* Table 2. Approximation of the adsorption isotherm of zeolite Temperature of desiccant plate Approximation 298 K Xb =.1434w* - 7E-5 (w*<.15) Xb =.129w* +.12 (w*<.263) Xb = 3E-7w* +.43 (w*.263) 318 K Xb =.3989w* +.21 (w*<.178) Xb =.58w* +.76 (w*<.231) Xb =.183w* -.136 (w*.231) 338 K Xb = 1.175w* +.27 (w*<.195) Xb =.1431w* +.216 (w*<.1945) Xb = 1.5956w* -.2513 (w*.1945) System Parameter study Conditions Many parameters affect desiccant system s performance. Several important factors are selected based on the rotor type desiccant system study by Yamaguchi (21): Air flow rate through the system Thickness of the desiccant plate Sectional area of the desiccant plate 881

Switching period of the desiccant plate Number of stages (desiccant plates in a line) These factors are evaluated by numerical model simulations. The boundary conditions for the parameter study are showed in Table 3. The average air state in summer in Japan is adopted as the outside air condition. The cold water is assumed to be obtained from the cooling tower, and the hot water is assumed to be cogenerated. Table 4 shows the cases of the parameter study. The underlined values are the standard values of each parameter. Table 3. Boundary conditions of the numerical simulations Outside air 32,.185 kg/kg (55%RH) Return air 28,.13 kg/kg (48%RH) Cold water of heat exchanger 26,.1 kg/s Hot water of heat exchanger 6,.1 kg/s Desiccant material Zeolite Table 4. Study cases Air flow rate through system 25, 5, 1 m 3 /h Sectional area of desiccant plate.2,.5,.1,.15,.2 m 2 Thickness of desiccant plate.2,.5,.1,.15,.2 m Switching period of desiccant plate - 36 s Number of stages 1-3 RESULTS Fig.4 shows the results of the system performance as change of the air flow rate. It shows the dehumidification amount in 3,6 s for each air flow rate. With larger air flow, the total dehumidification performance is reduced, because the relative humidity of the outlet air from the cooling coil was lower. Fig.5 shows the results of the study of the sectional area of the plate. It shows the dehumidification in 3,6 s versus the sectional area (Fig.5(a)) and the dehumidification per sectional area versus the air velocity (Fig.5(b)). This indicates that when the sectional area of the plate is constant, the dehumidification was higher as air velocity is faster. Fig.6 shows the dehumidification amount in 36 s versus desiccant plate thickness. When the plate was thicker, dehumidification was higher. A thick desiccant plate can dehumidify the air moisture by a large amount of desiccant material and performance is therefore better. Fig.7 shows the investigation of the switching period of the plates. This graph shows that an optimum switching period existed. 882

dehumidification [kg/h] dehumidification [kg/h] dehumidification [kg/h] dehumidification per sectional area [kg/h m2] dehumidification [kg/h].4.38.36.34.32.3 25 5 75 1 air flow rate(m3/h) Figure 4. The results of dehumidification performance as air flow rate and air velocity.8.6.4.2...4.8.12.16.2 sectional area of desiccant plate[ m2 ] 3.5. 2. 4. 6. 8. (a) sectional area of desiccant plate (b) air velocity Figure 5. The results of dehumidification with the relation sectional area of desiccant plate and air velocity 3.8 3.75 3.7 3.65 3.6 3.55 1.4 1.2 1..8.6.4.2...5.1.15.2 thickness of desiccant plate[m] Figure 6. The effect of dehumidification performance by thickness of desiccant plate 1.8 1.75 1.7 1.65 1.6 1.55 1.5 1.45 1.4 1 2 3 4 5 switching period [s] Figure 7. The effect of dehumidification performance by switching period Multiplate system Study The parameter studies showed the basic effect of each parameter, but effect when each parameter varies simultaneously needs to be discussed. Fig.8 shows the correlation between the optimum switching period and the dehumidification performance per area of plate against air velocity for two plate thicknesses. The optimal switching period was the 883

dehumidification per sectional areaof desiccant plate [kg/hr.m2] dehumidification per sectional areaof desiccant plate [kg/hr.m2] dehumidification per sectional areaof desiccant plate [kg/hr.m2] dehumidification per sectional areaof desiccant plate [kg/hr.m2] period the best dehumidification. When the air velocity is faster, the optimal switching period is shorter. This means that much air flow can be processed in a short time. The system had limited potential with a single desiccant plate, but its performance could be improved by combining several plates in a line. Fig.9 shows the results of simulations of single to triple stage plate desiccant systems. This indicates that multiplate systems improved performance without raising the hot water temperature. 7 6 5 4 3 2 1 dehumidification per sectional areaof desiccant plate [kg/hr.m2] y = 9.14ln(x) + 14.162 y = 365.42x-1.13 5 1 15 2 16 12 8 4 dehumidification per sectional areaof desiccant plate [kg/hr.m2] 7 2 6 16 5 4 3 y = 15.858ln(x) + 17.637 12 8 2 1 y = 749.6x -1.145 4 5 1 15 (a) Thickness of desiccant plate.5m (b) Thickness of desiccant plate.1m Figure 8. The result of parameter studies single stage double stage triple stage 12 8 1 6 8 6 4 4 2 2 1 2 3 4 5 single stage double stage triple stage 12 8 1 6 8 6 4 4 2 2 1 2 3 4 5 (a)thickness of desiccant plate.5m (b)thickness of desiccant plate.1m Figure 9. The integrated dehumidification performance diagram CONCLUSION A numerical model of the plate type desiccant system has been proposed, and performance analysis was conducted assuming that cold water was obtained from a cooling tower and hot water was cogenerated. A parameter study defined the effect of each parameter on dehumidification performance. All results were integrated in the dehumidification performance diagram (Fig.9). This diagram can be used as reference for system design. For example, the thickness and area of the desiccant plate, the switching period, and number of stages that achieve required dehumidification performance can be designed. The pressure drop and heat distribution on the surface of the desiccant plate, etc., should 884

be investigated in future. Model experiments should be conducted to build a more precise numerical model. Furthermore, a feasibility study has to be conducted with the numerical model. It is important to study from the point of view of air process performance and energy consumption. ACKNOWLEDGEMENTS This work was supported by JSPS KAKENHI Grant Number 2682249. REFERENCES Rang, T., Xiao-Hua, L. and Yi. J. 213. Performance analysis of a new kind of heat pumpdriven outdoor air processor using solid desiccant, Renewable Energy 57, pp11-11 Momoi, Y., Yoshie, R., Satake, A., Yoshino, H. 26. Numerical Simulation of Moisture Adsorption-Desorption for Desiccant Dehumidifier, Part 4 Calculation Dehumidification Coefficient of Desiccant Rotor, Proceedings of the Society of Heating, Air-Conditioning and Sanitary Engineers of Japan 26. Yamaguchi, S. 21. Numerical and Experimental Performance Evaluation for Silica Gel Desiccant Wheel, Waseda University (Japan). Symbols t Time [s] ε Prorosity of porous solid [-] Ca Specific heat at constant pressure of air [J/kg K] Cd Specific heat of desiccant [J/kg K] ρa Density of humid air [kg/m 3 ] ρd Density of desiccant [kg/m 3 ] α Heat diffusivity [W/m 2 K] α Mass diffusivity [kg/m2 s kg/kg(da)] Sd Surface area per volume [m 2 /m 3 ] L Latent heat [J/kg] Ta Temperature of air [ ] Td Temperature of desiccant [ ] Xa Absolute humidity ratio of air [kg/kg(da)] Xb Absolute humidity of surface of desiccant [kg/kg(da)] W Water content of desiccant [kg/kgd] W* Water content at equilibrium of desiccant [kg/kgd] u Velocity of air [m/s] Average value in the cell ave 885