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Thursday, 9 December 2010
08.00 – 09.00 Registration SABUGA ITB09.00 – 10.00 Opening Ceremony
- Report from the Chairman- Speech by President of ASHRAE Indonesia Chapter- Speech by President of ASHRAE Regional XIII- Opening Speech by Rector ITB
Opening the event and official visit to the Exhibition Booth
10.00 – 10.30 Coffee Break 10.30 – 11.00 Keynote Lecture 1: Prof. Akinori Furukawa (JAPAN) Auditorium
Chairman: Prof. Hyomin Jeong 11.15 – 12.30 Technical Session 1-1 Technical Session Rooms12.30 – 13.30 Lunch 13.30 – 14.00 Keynote Lecture 2: DAIKINAIRCON Auditorium
Chairman: President ASHRAE Indonesia Chapter
14.15 – 16.00 Technical Session 1-2 Technical Session Rooms16.00 – 16.30 Coffee Break 19.00 – 21.00 Welcoming Dinner Maxi’s Resto, Bandung
Technical session Schedule
Session 1.1Room 1 (Renewable Engineering)Chairman: Dr. Priyono SutiknoCo-Chair: Dr. Yali GuoTime Paper Title Author Paper no11.15 – 11.30 Portable Solar Water Heater
Abdurrachim, E. Maulana 1
11.30 – 11.45 Evaluation of the Thermal Environment of Large space installed AHU using Solar heating system
Eun Jang,B Y Ha, D-G Kim, J-S Kum, Y-H Chung, J-P Myeong
11
11.45 – 12.00 The Influence of Pinch Temperatures on Geothermal Power Plant Performance
Ari D Pasek, T A F Soelaiman, J Gozali, C Gunawan
82
Room 2 (Heat Transfer, Fluid, and Thermal Engineering)Chairman: Dr. Nathanael P TandianCo-Chair: Dr. Xiaohua LiuTime Paper Title Author Paper no
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11.15 – 11.30 Experiment of Absorption Heat Transfer Performance Enhancement for Binary Nanoemulsion
Jin Ki Lee
17
11.30 – 11.45 CFD analysis of Flow Phenomena in Shell and Tube Exchanger
Yonghan Shin,H Jeong, H S Chung
78
11.45 – 12.00 Investigation and Evaluation Steam Generator Performance of the Steam Power Plant, Tello Makassar with Energy and Exergy Analysis
S Himran,M Palaboran, E S Piarah
79
12.00 – 12.15 Experimental study on turbulence and pressure characteristics about heat transfer enhancement creating artificial roughness
Md. Julker Nine,G H Lee, H S Chung, H M Jeong
73
12.15 – 12.30 Multi-phase analysis on effect of Brownian motion in heat transfer of H2O-Cu Nanofluid using LBM
Kui Ming Li
141
Room 3 (Energy and Alternative Energy)Chairman: Prof. Hanshik ChungCo-Chair: Dr. Yuli S IndartonoTime Paper Title Author last name Paper no11.15 – 11.30 Study on Strength of Artificially Methane Hydrate-
Bearing Sediments Containing Various Volumetric Methane Hydrate Content
Feng Yu, Y song, W Liu, Y Li, R Wang, X Nie
50
11.30 – 11.45 Study on Memory effect of Structure I and II Hydrates
Yongchen Song, C Guo, J Zhao, K Xue, C Cheng, Y Song, Y Liu, Y Zhang
51
11.45 – 12.00 MRI study of the Structure of Tetrahydrofuran Hydrate in Porous Media
Chuan-Xiao Cheng,Lei Yao, Yi-Ming Zhu, J-F Zhao, K-H Xue, Y-C Song
64
12.00 – 12.15 Experimental Study of Utilization of Air Condition as Water Heater
Ika Yuliyani,Abdurrachim, Jooned Hendrarsakti
145
Room 4 (CO2 Reduction and Low Carbon Technologies; Environmental Engineering)
Chairman: Prof. Hyomin JeongCo-Chair: Dr. Jooned HendrarsaktiTime Paper Title Author Paper no11.15 – 11.30 Visualization of CO2 flooding n-decane in porous
media using NMR imaging
Yongchen Song,Y Zhao, Y Liu, L Jiang, N Zhu
63
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11.30 – 11.45 MRI Measurement of Minimum Miscibility Pressure for CO2/n-decane system at Reservoir Temperature
Ningjun Zhu,Y Song, Y Liu, Y Zhao, L Ji
65
11.45 – 12.00 Decomposition Analysis On Industrial Energy-related CO2 Emissions In China
Miao Li,H Mu, M Li, X Kang, M Zhang
106
Session 1.2Room 1 (Heat Transfer, Fluid, and Thermal Engineering)Chairman: Prof. Dr. Syukri HimranCo-Chair: Prof. Yongchen Son14.15 – 14.30 Comparison of System Performance on Hot-gas
Bypass and Capacity Control in an Oil Cooler for Machine Tools
Kim Sang Ho
14
14.30 – 14.45 Numerical Investigation of the Partition Characteristics for the Condensation X-Shock
Yong Yang,S Shen, W Bi
62
14.45 – 15.00 Boiling Mapping for Cooling Process in Annulus Narrow Gap Base on Initial Temperature Variation
Mulya Juarsa,R Koestoer, A R Antariksawan, Indarto, B Riyono, Nandy Putra
114
15.00 – 15.15 Research of Fluid Flow on a Welding Region for the Shape of Shield Gas Nozzle
Yoon Hwan Choi
140
15.15 – 15.30 A Study on Heat Transfer and Flow Characteristics of Bubble Jet Loop Heat Pipe.
Jong Soo Kim 24
Room 2 (Computational Fluid Dynamics) Chairman: Dr. Abdurrachim Halim Co-Chair: Dr. Wang Xiaopo14.15 – 14.30
A numerical study of a plate heat exchanger with sine duct
Jong-Hyun Pyo,J-H Bong, H Cho
36
14.30 – 14.45 Numerical Simulation of the Cooling System in the Combustion Chamber of Small Liquid Rocket Engine
Romie Bura
41
14.45 – 15.00 Heating Rates of the Blunt-Fin Induced Supersonic Shock-Wave/ Boundary-Layer Interactions.
Romie Bura
42
15.00 – 15.15 Numerical Prediction of Film Distribution in Horizontal—tube Falling Film Evaporator
Qinggang Qiu,J Chen
49
15.15 – 15.30 Research on Dynamical Process of Droplet Impacting on Inclined solid Surface
Yali Guo,S Quan, S Shen, J Li
59
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15.30 – 15.45 Comparison of Numerical Results of LES for Fluid Flow and Heat Transfer in a mixing tee with Sintered Porous Medium using Volume-averaging Method with Fluid-solid Coupling Method
T Lu,Y W Wang, P F Cheng, K S Wang
60
15.45 – 16.00 Numerical analysis research of pressure distribution according to nozzle shape change of shock absorber on dual pulse shock test machine
Handry Afrianto
136
Room 3 (Refrigeration Engineering)Chairman: Prof. Dr. Kamarudin AbdullahCp-Chair: Dr. Jizu LV14.15 – 14.30 HCFC Phase out development Plan in Indonesia Ari D Pasek,
N Aumkau, M Hilman, Sulistyowati, Tridayanti
81
14.30 – 14.45 Experimental study on liquid desiccant flow rate effect’s in LiCl liquid Desiccant Dehumidification System
Fatkhur Rokhman,A Bakhtiar, C K Hwan
93
14.45 – 15.00 Development of Solid Sorption Refrigeration System for Ice-maker
Wimonnad Charrote,I M Astina, P S Darmanto
129
15.00 – 15.15 Development of Zeolite-Methanol Adsorption Freezer for Fishing Boat
L Sophal,I M Astina, P S Darmanto
130
15.15 – 15.30 Life Cycle Cost Analysis of Air Conditioning System in a Cluster of High Rise Building
S Sam On,I M Astina, P S Darmanto
131
15.30 – 15.45 Thermal Characteristics Evaluation of Vegetables Oil to be Used as Phase Change Material in Air Conditioning System
Yuli S Indartono,A Suwono, A D Pasek, D Mujahidin, I Rizal
132
15.45 – 16.00 Modeling and Prototyping a Mini Portable Thermoelectric Beverage Cooling Device
Hendi Riyanto,S Yuwono
137
Room 4 (Material Engineering for Energy Machinery; Fuel Cell and Heat Pump; Renewable Energy Management, Economics and Environmental Impact)Chairman: Prof. Yeon Won Lee Co-Chair: Dr. Yanghui Li
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14.15 – 14.30 Characteristics Analysis of Brekdown Voltage on Dielectric Transformer Oil Shell Diala B at Temperature 30oC-130oC
Wahyu Kunto Wibowo 94
14.30 – 14.45 A concept of using the dynamic power profile as a control reference for an advanced water management system on PEM fuel cell vehicle
Agung Bachtiar,F Rokhman, C K Hwang
83
14.45 – 15.00 Grey modeling & analysis of energy consumption in China based on catastrophe points
Nan Li,N Li, H Mu, S Gui, X Chen
107
15.00 – 15.15 Research Progress and Analysis of Solar Desalination Technology
Xiaohua Liu
53
POSTER SESSION:No Poster Title Author Poster No
9 Dec 2010, 11.15-12.30
1Experimental analyses on the effects of heat transfer efficiency of a heat recovery ventilation system according to the air volume ratio between supply and return flows
Taekun Lim
21
2A Study On The Pressure Loss Of Sprinkler Pipe System Hur Mansung 25
3Experimental Study On Oscillating Reburning For Nox Reduction
Chang Yeop Lee 90
4The Effect Of Reburning With Rice Husk On Nox And Thermal Characteristics In A Liquid Fuel Flame.
Huidong Shin 91
5A Study On The High Efficient Fin Model For Air-Conditioning
Sunhyeng Jo34
6Solar-Powered Water Pump : Stirling Engine Design And Performance Evaluation Of Solar Cooker
Abraham Prasetyo44
9 Dec 2010, 14.15-16.00
7A Study On Ensure Proper Flow Of Hot Water In Floor Heating Tube Authors
Hongdo Jeong 30
8A Simulation Of Impact Of Droplets On A Pipe By Using Lattice Boltzmann Method
Feifei Bi55
9Condensation Phenomenon Of Stratified Flow Inside Horizontal Tube
Rui Liu56
10Effect Of Resistance Force Of Tube Bundle On The Fluid Flow Characteristic In Evaporator With Low Reynolds Number
Hua Liu
58
11Experimental Study Of Falling Film Evaporation Heat Transfer Coefficient On Horizontal-Tube
Xingsen Mu61
12Study Of Performance Of Damper Using Electro-Rheological Fluid
Hyun Gweon Jeong70
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13A Study on the Subway Platform Thermal Environment using Natural Energy
Minsoo Kim, M-S Kim, H-R Kim, J-S Kum, D-G Kim, J-R Kim
12
14A Study on Operation Characteristics Solar system with Air-handling Unit in Large Space.
Lim Hongseok, D-G Kim, Y-H Chung, K-O Kim, Y-H Jeong, J-S Kum
13
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Friday, 10 December 2010
08.00 – 08.30 Registration 08.30 –09.00 Keynote Lecture 2: EMERSON Auditorium
Chairman: Dr. Ari D Pasek09.00 – 09.30 Coffee Break 09.30 – 11.00 Technical Session 2-1 Technical Session Rooms11.00 – 13.00 Break and Lunch Friday Pray for Moslem13.00 – 13.40 Keynote Lecture 3:
Dr. Jongman Ha (KOREA)Dr. Xiaopo Wang (CHINA)
AuditoriumChairman: Prof. Shenqiang Shen
13.45 – 15.15 Technical Session 2-2 Technical Session Rooms15.15 – 15.45 Coffee Break 15.45 – 17.00 Technical Session 2-3 Technical Session Rooms 19.00 – 21.00 Closing Ceremony
- Closing Speech by the Governor of Province of West Java*- Farewell Dinner
* to be confirmed
Technical session Schedule
Session 2.1Room 1 (Refrigeration Engineering)Chairman: Dr. Yuli S IndartonoCo-Chair: Dr. Shenglin Quan9.30 – 9.45 Determination of Potential Energy Surface of Some
Hydrocarbon Refrigerants and Their Gas Transport Properties via Semi-Empirically Based Assessment
Wang Xiaopo, B Song, J Wu, Z Liu
2
9.45 – 10.00 Thermodynamic analysis of the refrigerant mixture R125/R1270/R152A
Wang Xiaopo,Y Wang, Z Liu
3
10.00 – 10.15 Analytical Study of Performance in a Refrigerator Truck using R404a and R744
Chiwook Myung,S Kim, H Cho
8
10.15 – 10.30 Frost pattern on a fin-tube with multiple fins for evaporator of the heat pump
Keumnam Cho
9
10.30 – 10.45 The Optimization of Operating Condition in a Single-stage Compression CO2 Cycle with Internal
Heat Exchanger
Kyungjin Bae,B Kang, H Cho
37
Room 2 (Renewable Engineering; Low Temperature Engineering; Heat Transfer)Chairman: Dr. Bambang SusiloCo-Chair: Dr. Wenzheng Chui
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9.30 – 9.45 Experimental Study of Photovoltaic Thermal (PV/T)
Rahmat Subarkah,Belyamin
38
9.45 – 10.00 Drying of granular materials in inclined pneumatic conveyor
Kamaruddin Abdullah,A S Uyun, Y Chan, Y Esye
39
10.00 – 10.15 Experimental study on the heating capacity of an inverter-driven injection heat pump adopting a scroll compressor at low ambient temperatures
Suk Bin Ko,I Choi, Y Kim
117
Room 3 (Heat Transfer, Fluid and Thermal Engineering)Chairman: Dr. Toto HardiantoCo-Chair: Dr. Seongsoo Kim9.30 – 9.45 Flow Pattern and Two Phase Flow Distribution in a
Distributor
Azridjal Aziz,A Miyara, K Tsubaki, Sugiono
45
9.45 – 10.00 10.00 – 10.15 Numerical Analysis of Turbulent flow in a channel
with periodic semi-circular ribs
Gyeonghwan Lee, J Nine, H Jeong, H S Chung
69
10.15 – 10.30 Multi-phase analysis on effect of Brownian motion in heat transfer of H2O-Cu Nanofluid using LBM
Yeon Won Lee,K M Li
101
10.30 – 10.45 Natural Convection In Vertical Converging Channel Flow: The Critical Review Experimental Study of Utilization of Air Condition as Water Heater
Jooned Hendrarsakti 144
10.45 – 11.00 Thermodynamic Study Of Generator Set Exhaust Gas Heat Recovery Using Organic Rankine Cycle With Regenerator
Prihadi S Darmanto 88
Room 4 (Marine and Ocean Engineering)Chairman: Dr. Xiahoa LiuCo-Chair: Dr. Dong Eok Kim9.30 – 9.45 Study on Mechanical Behavior of Marine Hydrate-
Bearing Sediments under Triaxial Compression
Yanghui Li,Y Li, Y Song, F Yu, W Liu, R Wang, X Nie
52
9.45 – 10.00 A Study on the Pressure Drop and Flow pattern for Demister in MED-MVC System
Pil Hwan Kim,D Choi, Y Mun, H Jeong, H S Chung
85
10.00 – 10.15 Experimental fault detection of a gearbox using acoustic emission signal
Dong Sik Gu,J G Kim, B-K Choi
110
10.15 – 10.30 Evaluation of the AE Signal caused by Fatigue Crack Growth
Jae Gu Kim,D Gu, B K Choi
111
Session 2.2
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Room 1 (Computational Fluid Dynamics)Chairman: Prof. Keumnan ChoCo-Chair: Dr. Jooned Hendrarsakti13.45 – 14.00 Computational investigation on the performance
characteristics of the Mechanical Vapour Compressor
Jusik Woo,Y Chun, H S Chung, H Jeong
71
14.00 – 14.15 Numerical Study of Multistage Centrifugal Compressor in Mechanical Vapor Compression Desalination System
Muhammad Nuim Labib,H M Jeong, H S Chung
72
14.15 – 14.30 Numerical Analysis for the flow Phenomenon change the Chevron Angle in Plate Heat Exchanger
Seong Soo Kim,Y Seong, H Jeong, H S Chung, H Jeong
75
14.30 – 14.45 Molecular Dynamics simulation on nanofluids in wall layer
Jizu L V,X Li, M Bai, W Cui
96
14.45 – 15.00 Numerical simulation of single bubble rising in viscous liquid by Lattice Boltzmann method
Ning Li,W Li, J Zuo, T Sun
116
15.00 – 15.15 Study and CFD Simulation of the Utilization of Waste Treatment Plant Gas Product as Co-Fuel of Steam in Ethanol Plant
Prihadi S Darmanto,M Ariefyanto
119
Room 2 (Renewable Energies)Chairman: Dr. Abdurrachim HalimCo-Chair: Dr. Chang Yeop Lee13.45 – 14.00 The Comparison between the Effects of Using Two
Plane Mirror Concentrators and that without Mirror on the Flat-Plate Collector
S Himran,B Sudia, W S Piarah
80
14.00 – 14.15 Kinetic Model of Palm Oil Transesterification to Biodiesel with Ultrasound
Bambang Susilo,La Chovia Hawa, M Bagus Hermanto
113
14.15 – 14.30 Development of Microhydro Power for Encouraging Small Scale Cofee Processing in Geumpang-Aceh
Hamdani,Irwansyah
124
14.30 – 14.45 Design and Blade Optimization of Intelligent Wind Turbine
Priyono Sutikno,D B Saepudin
127
14.45 – 15.00 Design, Simulation and Experimental of the Very Low Head Axial Water Turbine
Priyono Sutikno,I M Khalik
128
Room 3 (Energy and Alternative energy)Chairman: Prof. SutardiCo-Chair: Dr. Muhammad Nurhuda
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13.45 – 14.00 Ocean Thermal Energy Conversion (Otec) Power Plant And Its By Products Yield For Small Islands In Indonesia Seawater
Y Siahaya,L Salam
97
14.00 – 14.15 Thermodynamic Analysis of a Flash-Binary Cycle in a Geothermal Power Plant
T.A.Fauzi Soelaiman,A D Pasek, C Gunawan
100
14.15 – 14.30 The Development of Laboratory Scale Continuous Peat Torrefaction Reactor System
Haryadi,T Hardianto, A D Pasek, A Suwono
123
14.30 – 14.45 The effect of components composition of mixed municipal solid waste on torrefaction temperature and resident Time
Amrul, A Suwono, A D Pasek, T Hardianto
126
14.45 – 15.00 Triga 2000 Reactor Thermal Hydraulics Performance for 1 MW Power Condition
Rosalina Fiantini, N Nagara, P Basuki, E Umar
133
Room 4 (Heat Transfer, Fluid and Thermal Engineering)Chairman: Prof. Dr. S.H. WinotoCo-Chair: Dr. I Made Astina13.45 – 14.00 Experimental Study of Morphology on Water
Droplet Impacted onto Incline Solid Surface
Shenglin Quan, Y Guo, W Li, S Shen
67
14.00 – 14.15 Shell side Fluid Flow Phenomena of a Shell-and-Tube LNG Vaporizer
S.M. Sayeed-Bin-Asad Sayeed, Y H Shin, H S Chung, M Jeong
68
14.15 – 14.30 Molecular dynamics simulation on thermal physical properties of nanofluids
Wenzheng Cui, J LV, M Bai, X Li
92
14.30 – 14.45 Experimental investigation of high pressure steam condensation heat transfer in a vertical tube
Dong Eok Kim, K W Hwang, K H Yang, Y H Ha, G C Park, M H Kim
98
14.45 – 15.00 Experimental Investigations on the Temperature Characteristics Using Different Fill Ratio of the Loop Heat Pipe
Md.Riyad Tanshen,K Lee, H Jeong, H S Chung
74
Session 2.3Room 1 (Computational Fluid Dynamics)Chairman: Dr. Wenzheng Chui Co-Chair: Dr. Yusuf SiahayaTime Paper Title Author Paper no
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15.45 – 16.00 Numerical and Experimental Study on the Effect of Guide Vane Insertion on the Flow Characteristics in a 90º Rectangular Elbow
Sutardi,A W Wawan, N Nadia, K Puspita
5
16.00 -16.15 Numerical Analysis of Natural Convection Air Cooling on Containment of AP-1000 Reactor Model
Ari D Pasek
6
16.15 – 16.30 A numerical study of gas-liquid bubbly flow split through branching T-junctions with different internal configurations
Yang Liu,W Z Li
66
Room 2 (Heat Transfer, Fluid and Thermal Engineering)Chairman: Dr. Priyono SutiknoCo-Chair: Dr. Shenglin QuanTime Paper Title Author Paper no15.45 – 16.00 Analysis of cooling performance of EGR Cooler by
using carbon-nanofluid
Seongsoo Kim, H S Chung, H M Jeong, B H Kim, B H Lee, H Choi, J Hwang
105
16.00 -16.15 Theoretical Study of Convective Heat Transfer in a Vertical Square Sub Channel
Nathanael Tandian, E Umar, T Hardianto, A C Syuryavin,
134
16.15 – 16.30 Improvement of Cooling Tower Performance through Fan Stack Geometry Modification: Wayang Windu Geothermal Power Plant Case Study
Willy Adriansyah
135
16.30 – 16.45 Lattice-Boltzmann Simulation on Heat Transfer Performance in Microchannel With Difference Surface Characteristics
J. Chui, W. Z. Li
138
16.45 – 17.00 Study of Steam Compressed Heat Pump System on The Gas Separation Device
Ping Wang
139
Room 3 (Renewable Engineering)Chairman: Dr. Prihadi S DarmantoCo-Chair: Dr. Yali Guo Time Paper Title Author Paper no
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15.45 – 16.00 Economic Benefit Of Hybrid Nocturnal Cooling Applications Under Indonesian Climatic Condition
Kamaruddin Abdullah, I B P Gunadnya, Y A Purwanto, H T Armansyah, M A M Oktaufik, K Abdullah
40
16.00 -16.15 Solar-Powered Water Pump : Stirling Engine Design and Performance Evaluation of Solar Cooker
Abraham Prasetyo, A Prasetya, A H Prasetyo, Z A Abidin
43
16.15 – 16.30 Enhancing the efficiency of biomass stove by using radiant waste heat for pre-heating
Muhammad Nurhuda, T Baolun
47
16.30 – 16.45 Performace of A Shrouded Wind Turbine: A Preliminary Study
S H Winoto
48
Room 4 (HVAC System)Chairman: Prof. Jong Soo KimCo-Chair: Dr. Toto HardiantoTime Paper Title Author Paper no15.45 – 16.00 A study on the vertical sectional exhaust
characteristics from kitchens using a vertical shaft
Byeong Kwon Yi
89
16.00 -16.15 A Study on the Thermal Conductivity of Heat Exchangers on the Geothermal Heat Pump System
Chenkuan Park, H Jeong, Y-H Lee, H Jeong, H Chung
28
16.15 – 16.30 System Sizing Commissioning and Balancing in a Constant-Primary Variable-Secondary Pumping Scheme of a Central Cooling System
Egi Al-GhifariWilly Adriansyah, I Made Astina, Prihadi Setyo Darmanto
143
POSTER SESSION:10 Dec 2010, 09.30-11.00
15Comparison Of Cyanide Degrading Enzymes Expressed From Genes Of Fungal Origin
Sunghyun Kwon76
16Study On Fresh Water Generation System With Low Pressure Evaporation By Experiment
Supriyanto Wibowo77
17Thermal And Economic Analysis On Green House Effect (Ghe) Of Solar Rotary Dryer For Drying The Agricultural Product
Ropiudin Ropi
87
18A World Trend Of New•Renewable Energy Policy And Patent Analysis Waste Heat Recovery System
Churl Pyo Kim27
19A Study Of Refrigeration Cycle Depending On Changes In Evaporator Fan Motor (EFM) Temperature Control And Load
Chang Myung Seo
29
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20Performance Analysis Of A R744-R404A Cascade Refrigeration System With Internal Heat Exchanger
Min-ju Jeong95
21The Characteristics on the Capacity Control of Inverter Type in an Industrial Water Cooler
Hyun-Woo Kim 16
10 Dec 2010, 13.45-15.15
22A Study On The Pressure Loss Of Sprinkler Pipe System Hur Mansung 102
23A Study Of Silencer To Decrease Noise For Tank Gun Hyun Mo Jung 103
24CFD Simulation Of The Permeability Cylinder Using Porous Boundary Condition
Kyujin Shim104
25Microstructural Characterization And Vickers Hardness Of Al2O3 Fiber-Reinforced Al Alloy Metal Matrix Composites Processed By Low-Pressure Infiltration
Hua Wei Rong
109
26Composition Design And Mechanical Properties Of BCC Ti Solid Solution Alloys With Low Young’s Modulus.
Kelimu Tulugan112
27Direct Numerical Simulation Of Single Bubble Rising In Viscous Liquid
Aiming Yuan115
28Comparison of Performance on the Natural Gas Liquefaction Process using Intercooler
Jin Woo Kwag 20
29Compare of Thermal Comfort Sensation between Elder’s and Young’s from Indoor Thermal Environment in Cooling
Ha Byeong-Yong, D G Kim, J-S Kum, Y-H Chung, D-S Kim
10
10 Dec 2010, 15.45-17.00
30Micromechanical Analysis Of Uni-Directional Carbon/Epoxy Composites
Hong Gun Kim118
31A Study On The High Quality Drying Products Of Sea Foods By The New Drying Technology
Kyong-Suk Kim 120
32A Study On The Effect Of Automobile Engine Performance By Using Carbon Nano Colloid Cooling Water
Bohan Kim 26
33Prediction Of Cement Demand And Energy Consumption In China
Yong Yang 122
34Electromagnetic Induction Heating For Recovery Unconventional Reservoirs
Pramana142
35Optimization of Thermosyphon Inserted Vacuum Tube Type Solar Heat Collector
Soonchang Yang 22
36The Effects of Air Bubbles to Decrease the Fouling of the Plate Heat Exchanger
Baek Seung Moon, W-S Seol, T-S Oh, J-I Yoon
46
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ICCHT2010 - 5th International Conference on Cooling and Heating Technologies. Bandung, Indonesia
9- 11 December 2010
130- 1
Development of Zeolite-Methanol Adsorption Freezer for
Fishing Boat
L. Sophal1,2, I M. Astina3, P.S. Daramanto3
1Department of Mechanical and Industrial Engineering, Institute of Technology
of Cambodia 2Student of Institut Tecknologi Bandung, Indonesia
E-mail: [email protected]
3 Faculty of Mechanical and Aerospace Engineering, Institut Teknologi Bandung,
Jalan Ganesha 10, Bandung 40132 West Java, Indonesia
ABSTRACT: Vapour compression refrigeration system using chlorofluorocarbons
is harmful to the environment and destructive to the ozone layer. It also consumes
more energy than others energy consumption utilities. This concerns lead to the
development of solid sorption refrigeration system which is environmentally
friendly and could be driven by low waste heat energy. Due to the availability of
waste heat from fishing boat, adsorption system has been proposed to be an
alternative refrigeration system on the boat. Meanwhile, various kinds of
adsorbent-adsorbate pairs have been developed. The most common pairs are silica
gel-water, activated carbon-ammonia, and activated carbon-methanol pairs.
In order to make the system more compact, the heat transfer flux in and out of
the adsorbent must be high. Therefore, a compact heat exchanger shell and tube is
proposed to work as a generator. A zeolite-methanol is selected as adsorbent-
adsorbate pair. Zeolite is coated on the tube inside of the heat exchanger. The heat
transfer in the generator is calculated. The highest rate of the heat transfer is 268.23
W/m2∙K when the heating temperature of water is 100
oC and the water mass flow
rate is 0.5 kg/s.
Keywords: adsorption, generator, adsorbent-adsorbate, coating
NOMENCLATURE
A-F points on the Clapeyron diagram
Cp specific heat of at constant pressure [kJ/kg∙K]
D diameter of tube [m]
H heat of adsorption/desorption [kJ/kg]
h heat transfer coefficient [kW/ m2∙K]
k thermal conductivity [kW/m∙K]
L 𝑳 latent heat [kJ/kg]; length of heat exchanger [m]
m𝒎 mass [kg]
ICCHT2010 - 5th International Conference on Cooling and Heating Technologies. Bandung, Indonesia
9- 11 December 2010
130- 2
Nu Nusselt number
Pr Prandtl number
q heat input out per unit mass of adsorbent [kJ]
r radius of tube
Re 𝑹𝒆 Reynolds number
T temperature [K]
U overall heat transfer coefficient [kW/ m2∙K]
x0 adsorption capacity at T=Ts𝑻𝒃𝒆𝒅 = 𝑻𝒔
x adsorption/desorption capacity
thickness of zeolite layer
n,y,w constants
Subscript
1-9 points on the Clapeyron diagram
ad adsorption
al aluminium
bed adsorbent bed
de desorption
c condenser
e evaporator
m methanol
mi middle
sat saturation
t tube
z zeolite
1. INTRODUCTION
Refrigeration has applications embracing a huge range of fields in which we all
encounter in our daily lives and therefore plays an essential role in sustainable development.
Unfortunately, the common refrigerants such as CFCs and HCHCs refrigerant have the global
warming potential and thus contribute to the greenhouse effect. The discovery of ozone
depletion caused by those refrigerants led to the Montreal Protocol, which schedule to phase
out CFCs by the end of 1995, HCHCs by the end of 2030. Furthermore, refrigeration systems
are used in various sectors and they are the primary of energy consumption. With the
increasing of energy consumption worldwide, it is becoming more urgent to find way of using
the energy resources as efficiently as possible. Thus, machine that can recover waste heat at
low temperature level, such as adsorption machine, can be an interesting alternative for a wiser
energy management.
Sine the interest in adsorption systems was renewed in the last 20 years, the COP and SCP
of these systems greatly increased due to the works of several research groups. Wang and
Olivera [1] have conducted a study of adsorption refrigeration. They showed that consolidated
compound adsorbents have shown their potential to increase cooling performance of the
adsorption refrigeration system and the COP is 0.4 for evaporating temperature is -15.
Jribi et al [2] studied about the performance of a two-stage activated carbon-CO2 adsorption
system. The adsorption uptake is carried out for the temperature range from -18 to 80oC. The
ICCHT2010 - 5th International Conference on Cooling and Heating Technologies. Bandung, Indonesia
9- 11 December 2010
130- 3
maximum COP is 0.16 for the evaporator and desorption temperature of 15oC and 80
oC,
respectively. To improve the over performance of adsorption refrigeration system, different
construction of bed have been designed [3, 4]. Waszkiewicz et al. [11] reviewed an adsorption
refrigeration system using zeolite and methanol. The analysis confirms that large changes on
COP are possible. Typical estimates are 0.535 for a single bed cycle and around 0.935 for a
twin bed cycle.
In this work we present the analysis of a novel twin bed adsorption system. By using two
beds, heat rejected from the first bed can be recuperated and used to regenerate the second, the
limitation of mass and heat transfer is diminished. The design is based on the technology of
coating zeolite paste on substrate [5, 6].
2. WORKING PRINCIPLE OF ADSORPTION SYSTEM
Physical adsorption: Adsorbent (solid) has physically high porous structures with surface–
volume that can catch and hold refrigerants (vapor). When saturated, it can be regenerated
simply by heating.
There are three main components in the system: a generator, a condenser and an evaporator.
The generator is capable to adsorb and desorb vapor refrigerant when it is being cooled and
heated, respectively. The generator works as a thermal compressor by adsorbing refrigerant at
the evaporating pressure and desorb the adsorbed refrigerant at the condensing pressure. The
high pressure refrigerant leaving from the generator will be condensed in the condenser by
isobaric process. The liquid refrigerant at high pressure leaves the condenser and expanses to
evaporating pressure so that the refrigerant evaporates in the evaporator where the cooling
effect take place. The evaporating vapor refrigerant will be adsorbed in the adsorbent surface
volume and then desorbed again to complete a cycle in the adsorption process. The process is
intermittent for a single generator system because the adsorbent in the generator have to be
cooled in adsorption process and heated in desorption process at different time. Multiple
adsorbent beds are required for continuous operation [7].
3. ADSORBENT-ADSORBATE SELECTION
In this study zeolite-methanol is selected as the adsorbent-adsorbate pair. It is expected to
work in better coefficient of performance because the regeneration temperature is as low as 100 oC for the refrigerant to be fully generated and with this temperature does not causes methanol
to decompose. The difficulties of selecting an adsorber pair refrigerant are the limitations of
heat transfer coefficient of adsorbent and the generating temperature of the adsorbate. Various
feasibilities of adsorbent-bed design have been proposed and developed to improve the heat
transfer inside the generator. Zeolite is an adsorbent material that can be prepared for coating
on a substrate surface [3, 7].
The refrigerant is basically selected upon it heat capacity, evaporating temperatures and
pressures, environmental impact and its ability to be adsorbed on adsorber. Water is generally
not useful for high heat load. Ammonia has a more favourable specific volume but is toxic and
corrodes copper and brass fittings. Most alcohol are environmentally friendly but are
dehydrated and catalytic decomposed during desorption at 150 - 200oC. Compared to
ammonia, methanol is more compatible and less toxic. The normal boiling point of methanol is
64.7oC and the low melting point is -93.9
oC is convenient for a refrigeration of subzero
evaporating temperature. Zeolite-methanol pair was also selected by Waszkiewicz [11] and it
ICCHT2010 - 5th International Conference on Cooling and Heating Technologies. Bandung, Indonesia
9- 11 December 2010
130- 4
gives the best coefficient of performance of 0.5 for a single bed cycle [9, 10] and it can be
improved to 0.935 for a twin-bed cycle.
4. GENERATOR DESIGN
Generator is the main component of adsorption refrigeration system which dominates the
overall performance of the system. Maximizing the heat transfer coefficient is the difficulties
of generator design while adsorbent is known as a low thermal conductivity material.
Schematic diagram of a novel twin beds adsorption system is shown in the figure 1. The
system consists of two beds, a condenser, and an evaporator. The system is continuous while
one bed is cooled for adsorption and another one is heated for desorption. Periodically, V-5 is
opened to allow the beds to achieve the equilibrium.
Adsorber I
Adsorber II
Condenser
Evaporator
V-2
Expansion
valve
V-1
V-5
3
V-3
Heating/
Cooling
Heating/
Cooling
Figure 1. Schematic diagram of an adsorption system Figure 2. Cross section of generator
Figure 2 shows the cross section of a shell and tube heat exchanger (generator). The
generator is simply designed as part of the refrigeration system. The length is 0.326 m and the
shell inner diameter is 1.79 m (15.25 in). There are 103 aluminum tubes with outside diameter
of 25.4 mm (1 in) and thickness of 3 mm (0.12in). Outside surface of the tubes is coated with 2
mm thickness of zeolite 4A paste. The volume of adsorbent is 0.04 m3 which equals to 106.72
kg and it could adsorb 18.65 kg of methanol on its porous surface at the ambient temperature.
The shell side is used to maintain the methanol vapor pressure when the bed is heated. Heating
and cooling fluid is flown inside the tubes for desorption and adsorption process, respectively.
4.1.Heat transfer coefficient in the generator
The inside tube heat transfer coefficient of the generator which is coated with layer of
zeolite paste is calculated using the Dittus-Boelter equation for getting Nusselt number as
given by equation (1).
nNu PrRe023.0 5
4
(1)
Where n = 4 for heating and n = 0.3 for cooling.
Reynolds number is evaluated by equation (2)
1
ReDu
(2)
ICCHT2010 - 5th International Conference on Cooling and Heating Technologies. Bandung, Indonesia
9- 11 December 2010
130- 5
0.01 0.015 0.02 0.025 0.03 0.035 0.04180
190
200
210
220
230
240
250
260
270
Pipe inner diameter [m]
Heat
Tra
nsfe
Coeff
icie
nt
[W/m
2K
]
100 oC
80 oC
60 oC
40 oC
20 oC
20 30 40 50 60 70 80 90 100240
245
250
255
260
265
270
Hot water temperature [oC]
Heat
Tra
nsfe
Coeff
icie
nt
[W/m
2K
]
desorption
adsorption
The overall heat transfer of the generator is calculated by equation (3).
23
1
23
1
12
1
1
)/ln()/ln(1
1
hr
rrr
k
Drr
k
D
h
U
aw
(3)
Where 1
h is heat transfer coefficient inside the tubes, 2
h is the heat transfer coefficient
at shell side and 1
D is the tube inner diameter. 1
r , 2
r and 3
r are radius of inner tube, outer tube
and coated zeolite tube, respectively. Kerm method is used for calculation the heat transfer
coefficient at the shell side.
The total volume of zeolite is calculated from equation (4)
)(2 zzz
DNLV (4)
and the mas of zeolite is
zzzVm (5)
If the velocity of the water is 0.02 m/s, the heat transfer coefficient of water can be
calculated for heating and cooling at different temperature. The results are graphically
represented in figures 3. The expected heat transfer coefficient is high for higher water
temperature and low for the increasing tube diameter. Another prediction of the heat transfer
with water temperature is shown in figure 4. It was plotted for a fixed tube inner diameter of
0.01 m.
Figure 3. The variation of heat transfer coefficient Figure 4. The variation of heat transfer coefficient with tube diameter and the water temperature for with water temperature at tube diameter 0.01 m. adsorption and regeneration
4.2.The limitation of adsorption capacity
The figures 7 and 8 show the capacity of adsorption and desorption which limit the
evaporating temperature for the cooling effect. The calculation is based on adsorption capacity
x which is calculated by using the Dubinin-Astakhov (D-A) equation as given in equation (6).
w
sat
bed
T
Tyxx 1exp
0 (6)
ICCHT2010 - 5th International Conference on Cooling and Heating Technologies. Bandung, Indonesia
9- 11 December 2010
130- 6
-50 0 50 100 1500
0.02
0.04
0.06
0.08
0.1
0.12
0.14
0.16
0.18
Temperature
Adsorp
tion c
apacity
Xad
Xde
-50 -40 -30 -20 -10 0 10 20 30-0.02
0
0.02
0.04
0.06
0.08
0.1
0.12
0.14
0.16
0.18
Temperature
Adsorp
tion c
apacity d
iffe
rence (
Xad-X
de)
Xad-Xde
Where y and w are the constants of zeolite-methanol pair.
Quantity of adsorbed methanol increases with higher saturation temperature during adsorption
and decreases with higher generating temperature during desorption as shown in figur5. It
means that the higher saturation and generating temperature, the larger quantity of methanol
circulate in the system. For adsorption temperature is 35oC and desorption temperature is 90, it
is impossible to set the evaporating temperature lower than -20oC as confirm in figure 6.
Figure 5. The variation of adsorption capacity with Figure 6. Variation of adsorption capacity adsorbent temperature difference
5. MATHEMATICAL MODEL FOR TWIN BEDS ADSORPTION
The conditions of adsorber for twin beds cycle is presented in figure 7. The process (1-2-3-
4) presents the adsorber cycle for a single bed system and the process (1-5-6-7) and (6-6-3-9)
presents the adsorber cycle for a twin beds system.
Figure 7. Clapeyron diagram of a twin beds cycle
Initially, some assumptions of the middle point between the two beds are made for the
calculation of twin beds adsorption cycle. The middle adsorption capacity of the adsorbent and
the saturation temperature are
%4.62
dead
mi
xxx and C66.27
o
,
misatT .
ICCHT2010 - 5th International Conference on Cooling and Heating Technologies. Bandung, Indonesia
9- 11 December 2010
130- 7
The COP of the twin beds system is defined by
8368
71
qCOP
(8)
Where68
q , 83
q and 71
q are the heating quantity per unit mass of adsorbent. They are
defined by equations (9), (10) and (11), respectively.
dTxccq
T
T
admvzp
8
6
)(,,68
(9)
ad
de
x
x
T
T
mpzpHdxdTxccq
3
8
)(,,83
(10)
Where H is defined as desorption heat and x can be calculate from Dubinin Astakhov
equation as given in equation (6).
The heat capacity of for the isobaric process from point 7 to 1 is defined by equation (11).
ad
de
ad
de
x
x
emp
x
x
T
T
mpzpdxTTcHdxdTxccq )()(
1,,,71
1
7
(11)
5.4.Calculation result
For zeolite-methanol, with Dubinin-Astakhov equation the results were calculated which
shown in the table 1. There upon, the COP for twin beds cycle was found to be 0.652.
Table 1. End point of the ideal twin beds cycle
Position
in the
diagram
Saturation
temperature
Tsat [oC]
System
temperature
T [oC]
Refrigeration
concentration
X
1 -10 30 0.1106
5 10 53 0.1106
6 10 59.4 0.0780
7 -10 54 0.0780
8 30 83 0.0780
3 30 90 0.0450
9 10 88.8 0.0450
6. CONCLUSION
All the work presented here shows the importance of properly designing parts the adsorption
refrigeration system, mainly the bed. The evaluation has shown that the system has a potential
to be manufactured as compact system which suitable for domestic uses as it has a high system
performance. The COP of the system is 0.652 which is around a double COP compared to a
single bed cycle. Somehow, there are some points that should be more studied such as the
following:
Adsorbent-adsorbate pair should be more studied to suit the refrigeration system of lower
evaporating temperature such as freezer, for which temperature need to be lower than -20oC.
ICCHT2010 - 5th International Conference on Cooling and Heating Technologies. Bandung, Indonesia
9- 11 December 2010
130- 8
Shell and tube heat exchanger coated with zeolite paste is an interesting method and needs
further study to improve heat and mass transfer in the system.
Double twin beds system is also interesting to be studied as it is capable to recover heat in
the system and it can be operated continuously.
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