Determination of heat transfer intensity between free streaming water film and rigid surface using thermography

Size: px
Start display at page:

Download "Determination of heat transfer intensity between free streaming water film and rigid surface using thermography"

Transcription

1 IV Conferencia Panamericana de END Buenos Aires Octubre 2007 Determination of eat transfer intensity between free ing water film and rigid surface using termograpy Ivanka Boras and Srecko Svaic Faculty of Mecanical Engineering and Naval Arcitecture Ivana Lucica 5, Zagreb, Croatia ivanka.boras@fsb.r Mirela Susa Department of Electrical and Computer Engineering Université Laval, Quebec, G1K7P4, Canada Abstract Te goal of te researc was to find te relation for determining te eat transfer coefficient between a free ing water film and metal corrugated surface. Te relation between relevant parameters wic determine te eat transfer coefficient as been obtained by means of Wilson-plot metod using data from te measurement. 1. Introduction Te open plate eat excanger (OPHE) consists of two plates welded togeter so tat one is flowing between plates and anoter one over te outer surface of upper plate. Te aim of suc eat excanger design is to enable te eat excange between outer wic could be waste dirty water and inner. Te OPHE are often used for eat recovery purposes in laundries, paper industries etc. Te main problem in termodynamical calculation of suc type of eat excanger is determination of te eat transfer coefficient on outer side. Because te plates are always inclined to te orizontal plane and outer surface is corrugated to ensure better eat transfer te standard relations for flat plate could not be used. Te paper presents te results of te researc done on te one plate of OPHE wit te aim to find te relation for eat transfer coefficient between ing film and plate. Te IR termograpy was used for measurements of temperature distribution on water film ing over te outer plate surface 2. Te problem Te open plate eat excanger is aimed for eat excange between ot waste water and cold fres water. Waste water flows over te outer (upper) side of te OPHE plate in free and fres water flows inside, between te plates. OPHE are used in te case wen waste water contents particles or coagulants. Te advantage of

2 suc design is easy cleaning of te plates and module design wic enables enlargement of te unit. Te upper side of OPHE plate is corrugated to improve te eat excange between te free of waste water and te plate. Te OPHE plates are inclined (5 º) to orizontal plane to ensure te free ing by means of gravity. Wile te equations for calculating te eat transfer coefficient inside te plates could be found in literature, te relation for te calculation of eat transfer coefficient on te outer side became a problem. Te goal of te researc was to find te relation for te eat transfer coefficient on te outer side of te OPHE plate. Te single plate of OPHE used in experiment is sown in figure 1 and te detail of corrugated upper surface in figure 2. Figure 1. Te plate of te eat excanger 3. Te experimental rig Figure 2. Te features of upper plate Te experimental rig consists of single OPHE plate placed on a frame wit up and down container (see figure 3). Te ot waste water enters te up container and overflow on te plate. After passing te plate te water enters te down container. Te fres water s in counter flow between te plates. IV Conferencia Panamericana de END Buenos Aires Octubre

3 Figure 3. Experimental rig Te mass flow of waste (ot) and fres (cold) water are measured by weiging wile te temperatures are measured by termocouples (see figure 4). Beside te termocouples te surface temperature distribution of ot water ing over te plate was recorded by IR camera. All measurements were done in stationary state. Hot inlet Hot outlet Cold outlet Cold inlet Figure 4. Positions of termocouples and directions of ot and cold water 4. Measurements Te measurements were carried out wit mass flow of 0,1; 0,2; 0,3 and 0,4 kg/s for ot and 0,1 and 0,2 kg/s for cold. Some of te results are presented in table 1 and te related termograms are sown in figure 5. IV Conferencia Panamericana de END Buenos Aires Octubre

4 4.1 Te results of measurement using termocouples Table 1. Te results of measurement using termocouples Measurement No Hot Cold Mass flow [kg/min] 12,58 6,31 Inlet temperature [ C] 25,67 12,57 Outlet temperature [ C] 19,59 21,93 Mass flow [kg/min] 5,03 12,48 Inlet temperature [ C] 43,54 13,47 Outlet temperature [ C] 15,31 23,65 Mass flow [kg/min] 12 12,14 Inlet temperature [ C] 27,29 13,72 Outlet temperature [ C] 18,23 21,21 Mass flow [kg/min] 24,5 12,25 Inlet temperature [ C] 21,90 15,11 Outlet temperature [ C] 19,07 19, Te results of measurement using infrared camera a) Measurement No.1 IV Conferencia Panamericana de END Buenos Aires Octubre

5 b) Measurement No. 2 c) Measurement No.3 IV Conferencia Panamericana de END Buenos Aires Octubre

6 d) Measurement No.4 Figure 5. Termograms and referent temperatures Table 2. Te results of measurement; te termocouples were used for cold and infrared camera for ot Measurement No Hot Cold Mass flow [kg/min] 12,58 6,31 Inlet temperature [ C] 25,1 12,57 Outlet temperature [ C] 20,3 21,93 Mass flow [kg/min] 5,03 12,48 Inlet temperature [ C] 40,1 13,47 Outlet temperature [ C] 15,9 23,65 Mass flow [kg/min] 12 12,14 Inlet temperature [ C] 27,3 13,72 Outlet temperature [ C] 19,0 21,21 Mass flow [kg/min] 24,5 12,25 Inlet temperature [ C] 21,8 15,11 Outlet temperature [ C] 19,5 19,61 Te eat excanged between te s is calculated using relations: - for ot ( ϑ ϑ ) Φ = q c kw...(1) i o IV Conferencia Panamericana de END Buenos Aires Octubre

7 - for cold c c ( ϑ ϑ ) Φ = q c kw...(2) oc ic Table 3. Te results of calculation of te eat fluxes Measurement No. Φ c Φ termocouples Φ IR kw kw kw cold ot 1 4,119 5,327 4,21 2 8,861 9,883 8,49 3 6,343 7,580 6,68 4 3,845 4,843 3,92 It can be seen tat, using recordings by infrared camera (for ot water) a fair accordance was obtained between eat fluxes calculated for ot water and cold water, respectively. Using recordings obtained by termocouples (for ot water) te differences between eat fluxes were more empasized. 5. Calculation of eat transfer coefficients By means of overall eat transfer coefficients, calculated from measurement, and eat transfer coefficient for cold using Eq. (3), te eat transfer coefficient for ot as been determined using Eq. (4). 0,8 0,4 λ α c = 0,022 Re Pr...(3) d 1 α wall k λwall α c ekv 1 δ 1 =...(4) Using Wilson-plot metod te relation Eq. (5) for determination of eat transfer coefficient of outer can be found using data from measurements: α 0,74 1/ 3 λ = 0,524 Re Pr...(5) L Calculating te eat transfer coefficient using Eq. (5) for ot and comparing tem wit tose obtained from measurement it can be seen tat good mutual correspondence is obtained (see table 4). IV Conferencia Panamericana de END Buenos Aires Octubre

8 Table 4. Te comparison of eat transfer coefficients for ot, measurement and Eq.(5) Measurement No. α from measurement α calculated Eq.(5) W/m 2 K W/m 2 K ,7 2866, ,4 2286, ,5 2832, ,8 3376,5 6. Conclusion In te paper te application of IR termograpy in determination of eat transfer intensity as been described. Te specific profile of eat excanger's surface required an investigation for new relations for calculation of eat transfer coefficients. Te results obtained using Eq. (5) for calculation eat transfer coefficients on ot water side indicated a good correspondence wit te measurement's result. References 1. D. P. Almond, P. M. Patel, Pototermal Science and Tecnique, London, Capman & Hall, S. V. Patankar, Numerical Heat Transfer and Fluid Flow, Hemispere Publising Corporation, Mc Grow-Hill Book Co, Wasington, Gerald C. Holst, Common sense approac to termal imaging, SPIE Optical Engeenering Press, Bellingam, Wasington, USA, M. Necati Ozisik, Heat transfer: A Basic Approac, McGraw-Hill Companies, 1984 IV Conferencia Panamericana de END Buenos Aires Octubre

Determination of heat transfer intensity between free streaming water film and rigid surface using thermography

Determination of heat transfer intensity between free streaming water film and rigid surface using thermography Determination of eat transfer intensity between free ing water film and rigid surfae using termograpy Faulty of meanial engineering and naval ariteture University of Zagreb, Croatia Abstrat by S. Švaić,

More information

Simulation and verification of a plate heat exchanger with a built-in tap water accumulator

Simulation and verification of a plate heat exchanger with a built-in tap water accumulator Simulation and verification of a plate eat excanger wit a built-in tap water accumulator Anders Eriksson Abstract In order to test and verify a compact brazed eat excanger (CBE wit a built-in accumulation

More information

Experimental Analysis of Heat Transfer Augmentation in Double Pipe Heat Exchanger using Tangential Entry of Fluid

Experimental Analysis of Heat Transfer Augmentation in Double Pipe Heat Exchanger using Tangential Entry of Fluid ISR Journal of Mecanical & Civil Engineering (ISRJMCE) e-issn: 2278-1684,p-ISSN: 2320-334X PP 29-34 www.iosrjournals.org Experimental Analysis of Heat Transfer Augmentation in Double Pipe Heat Excanger

More information

CFD Analysis and Optimization of Heat Transfer in Double Pipe Heat Exchanger with Helical-Tap Inserts at Annulus of Inner Pipe

CFD Analysis and Optimization of Heat Transfer in Double Pipe Heat Exchanger with Helical-Tap Inserts at Annulus of Inner Pipe IOR Journal Mecanical and Civil Engineering (IOR-JMCE) e-in: 2278-1684,p-IN: 2320-334X, Volume 13, Issue 3 Ver. VII (May- Jun. 2016), PP 17-22 www.iosrjournals.org CFD Analysis and Optimization Heat Transfer

More information

Elmahdy, A.H.; Haddad, K. NRCC-43378

Elmahdy, A.H.; Haddad, K. NRCC-43378 Experimental procedure and uncertainty analysis of a guarded otbox metod to determine te termal transmission coefficient of skyligts and sloped glazing Elmady, A.H.; Haddad, K. NRCC-43378 A version of

More information

The entransy dissipation minimization principle under given heat duty and heat transfer area conditions

The entransy dissipation minimization principle under given heat duty and heat transfer area conditions Article Engineering Termopysics July 2011 Vol.56 No.19: 2071 2076 doi: 10.1007/s11434-010-4189-x SPECIAL TOPICS: Te entransy dissipation minimization principle under given eat duty and eat transfer area

More information

Application of control volume numerical method in thermographic analysis of relative material loss

Application of control volume numerical method in thermographic analysis of relative material loss Application of control volume numerical method in thermographic analysis of relative material loss Faculty of mechanical engineering and naval architecture University of Zagreb, Croatia by S. Švaić and

More information

Fundamentals of Heat Transfer Muhammad Rashid Usman

Fundamentals of Heat Transfer Muhammad Rashid Usman Fundamentals of Heat Transfer Muammad Rasid Usman Institute of Cemical Engineering and Tecnology University of te Punjab, Laore. Figure taken from: ttp://eatexcanger-design.com/20/0/06/eat-excangers-6/

More information

Section A 01. (12 M) (s 2 s 3 ) = 313 s 2 = s 1, h 3 = h 4 (s 1 s 3 ) = kj/kgk. = kj/kgk. 313 (s 3 s 4f ) = ln

Section A 01. (12 M) (s 2 s 3 ) = 313 s 2 = s 1, h 3 = h 4 (s 1 s 3 ) = kj/kgk. = kj/kgk. 313 (s 3 s 4f ) = ln 0. (a) Sol: Section A A refrigerator macine uses R- as te working fluid. Te temperature of R- in te evaporator coil is 5C, and te gas leaves te compressor as dry saturated at a temperature of 40C. Te mean

More information

Use of fin analysis for determination of thermal conductivity of material

Use of fin analysis for determination of thermal conductivity of material RESEARCH ARTICLE OPEN ACCESS Use of fin analysis for determination of termal conductivity of material Nea Sanjay Babar 1, Saloni Suas Desmuk 2,Sarayu Dattatray Gogare 3, Snea Barat Bansude 4,Pradyumna

More information

Chapter 4 Optimal Design

Chapter 4 Optimal Design 4- Capter 4 Optimal Design e optimum design of termoelectric devices (termoelectric generator and cooler) in conjunction wit eat sins was developed using dimensional analysis. ew dimensionless groups were

More information

Optimization of flat tubular molten salt receivers

Optimization of flat tubular molten salt receivers Optimization of flat tubular molten salt receivers Meige Zeng, Jon Pye Researc Scool of Engineering, Australian National University, Canberra, Australia Abstract E-mail: meige.zeng@anu.edu.au, jon.pye@anu.edu.au

More information

Chapters 19 & 20 Heat and the First Law of Thermodynamics

Chapters 19 & 20 Heat and the First Law of Thermodynamics Capters 19 & 20 Heat and te First Law of Termodynamics Te Zerot Law of Termodynamics Te First Law of Termodynamics Termal Processes Te Second Law of Termodynamics Heat Engines and te Carnot Cycle Refrigerators,

More information

The development of contact and noncontact technique to study the heat dissipation in metals under loading

The development of contact and noncontact technique to study the heat dissipation in metals under loading Te development of contact and noncontact tecnique to study te eat dissipation in metals under loading More info about tis article: ttp://www.ndt.net/?id=73 Abstract * ICMM UB RAS, Ac. Koroleva Str., 63

More information

Heat Transfer/Heat Exchanger

Heat Transfer/Heat Exchanger Heat ransfer/heat Excanger How is te eat transfer? Mecanism of Convection Applications. Mean fluid Velocity and Boundary and teir effect on te rate of eat transfer. Fundamental equation of eat transfer

More information

Exam in Fluid Mechanics SG2214

Exam in Fluid Mechanics SG2214 Exam in Fluid Mecanics G2214 Final exam for te course G2214 23/10 2008 Examiner: Anders Dalkild Te point value of eac question is given in parentesis and you need more tan 20 points to pass te course including

More information

Given: Hot fluid oil, Cold fluid - water (T 1, T 2 ) (t 1, t 2 ) Water

Given: Hot fluid oil, Cold fluid - water (T 1, T 2 ) (t 1, t 2 ) Water . In a counter flow double pipe eat excanger, oil is cooled fro 85 to 55 by water entering at 5. Te ass flow rate of oil is 9,800 kg/ and specific eat f oil is 000 J/kg K. Te ass flow rate of water is

More information

Numerical analysis of a free piston problem

Numerical analysis of a free piston problem MATHEMATICAL COMMUNICATIONS 573 Mat. Commun., Vol. 15, No. 2, pp. 573-585 (2010) Numerical analysis of a free piston problem Boris Mua 1 and Zvonimir Tutek 1, 1 Department of Matematics, University of

More information

Performance Prediction of Commercial Thermoelectric Cooler. Modules using the Effective Material Properties

Performance Prediction of Commercial Thermoelectric Cooler. Modules using the Effective Material Properties Performance Prediction of Commercial ermoelectric Cooler Modules using te Effective Material Properties HoSung Lee, Alaa M. Attar, Sean L. Weera Mecanical and Aerospace Engineering, Western Micigan University,

More information

Effects of Radiation on Unsteady Couette Flow between Two Vertical Parallel Plates with Ramped Wall Temperature

Effects of Radiation on Unsteady Couette Flow between Two Vertical Parallel Plates with Ramped Wall Temperature Volume 39 No. February 01 Effects of Radiation on Unsteady Couette Flow between Two Vertical Parallel Plates wit Ramped Wall Temperature S. Das Department of Matematics University of Gour Banga Malda 73

More information

Work and Energy. Introduction. Work. PHY energy - J. Hedberg

Work and Energy. Introduction. Work. PHY energy - J. Hedberg Work and Energy PHY 207 - energy - J. Hedberg - 2017 1. Introduction 2. Work 3. Kinetic Energy 4. Potential Energy 5. Conservation of Mecanical Energy 6. Ex: Te Loop te Loop 7. Conservative and Non-conservative

More information

Handling Missing Data on Asymmetric Distribution

Handling Missing Data on Asymmetric Distribution International Matematical Forum, Vol. 8, 03, no. 4, 53-65 Handling Missing Data on Asymmetric Distribution Amad M. H. Al-Kazale Department of Matematics, Faculty of Science Al-albayt University, Al-Mafraq-Jordan

More information

Lecture 10: Carnot theorem

Lecture 10: Carnot theorem ecture 0: Carnot teorem Feb 7, 005 Equivalence of Kelvin and Clausius formulations ast time we learned tat te Second aw can be formulated in two ways. e Kelvin formulation: No process is possible wose

More information

CFD calculation of convective heat transfer coefficients and validation Part I: Laminar flow Neale, A.; Derome, D.; Blocken, B.; Carmeliet, J.E.

CFD calculation of convective heat transfer coefficients and validation Part I: Laminar flow Neale, A.; Derome, D.; Blocken, B.; Carmeliet, J.E. CFD calculation of convective eat transfer coefficients and validation Part I: Laminar flow Neale, A.; Derome, D.; Blocken, B.; Carmeliet, J.E. Publised in: IEA Annex 41 working meeting, Kyoto, Japan Publised:

More information

CFD calculation of convective heat transfer coefficients and validation Part I: Laminar flow. Annex 41 Kyoto, April 3 rd to 5 th, 2006

CFD calculation of convective heat transfer coefficients and validation Part I: Laminar flow. Annex 41 Kyoto, April 3 rd to 5 th, 2006 CFD calculation of convective eat transfer coefficients and validation Part I: Laminar flow Annex 41 Kyoto, April 3 rd to 5 t, 2006 Adam Neale 1, Dominique Derome 1, Bert Blocken 2 and Jan Carmeliet 2,3

More information

Numerical Differentiation

Numerical Differentiation Numerical Differentiation Finite Difference Formulas for te first derivative (Using Taylor Expansion tecnique) (section 8.3.) Suppose tat f() = g() is a function of te variable, and tat as 0 te function

More information

Lecture 3 Heat Exchangers

Lecture 3 Heat Exchangers L3 Leture 3 Heat Exangers Heat Exangers. Heat Exangers Transfer eat from one fluid to anoter. Want to imise neessary ardware. Examples: boilers, ondensors, ar radiator, air-onditioning oils, uman body.

More information

International Power, Electronics and Materials Engineering Conference (IPEMEC 2015)

International Power, Electronics and Materials Engineering Conference (IPEMEC 2015) International Power, Electronics and Materials Engineering Conference (IPEMEC 2015) Calculation of Stray Losses and Temperature Distribution in Power Transformer Using Coupled Electro-Termal Field Analysis

More information

Comment on Experimental observations of saltwater up-coning

Comment on Experimental observations of saltwater up-coning 1 Comment on Experimental observations of saltwater up-coning H. Zang 1,, D.A. Barry 2 and G.C. Hocking 3 1 Griffit Scool of Engineering, Griffit University, Gold Coast Campus, QLD 4222, Australia. Tel.:

More information

RADIATIVE VIEW FACTORS

RADIATIVE VIEW FACTORS RADIATIVE VIEW ACTORS View factor definition... View factor algebra... Wit speres... 3 Patc to a spere... 3 rontal... 3 Level... 3 Tilted... 3 Disc to frontal spere... 3 Cylinder to large spere... Cylinder

More information

Chapter 3 Thermoelectric Coolers

Chapter 3 Thermoelectric Coolers 3- Capter 3 ermoelectric Coolers Contents Capter 3 ermoelectric Coolers... 3- Contents... 3-3. deal Equations... 3-3. Maximum Parameters... 3-7 3.3 Normalized Parameters... 3-8 Example 3. ermoelectric

More information

Carnot Factor of a Vapour Power Cycle with Regenerative Extraction

Carnot Factor of a Vapour Power Cycle with Regenerative Extraction Journal of Modern Pysics, 2017, 8, 1795-1808 ttp://www.scirp.org/journal/jmp ISSN Online: 2153-120X ISSN Print: 2153-1196 arnot Factor of a Vapour Power ycle wit Regenerative Extraction Duparquet Alain

More information

8-4 P 2. = 12 kw. AIR T = const. Therefore, Q &

8-4 P 2. = 12 kw. AIR T = const. Therefore, Q & 8-4 8-4 Air i compreed teadily by a compreor. e air temperature i mataed contant by eat rejection to te urroundg. e rate o entropy cange o air i to be determed. Aumption i i a teady-low proce ce tere i

More information

DEVELOPMENT AND PERFORMANCE EVALUATION OF THERMAL CONDUCTIVITY EQUIPMENT FOR LABORATORY USES

DEVELOPMENT AND PERFORMANCE EVALUATION OF THERMAL CONDUCTIVITY EQUIPMENT FOR LABORATORY USES . Sunday Albert LAWAL,. Benjamin Iyenagbe UGHEOKE DEVELOPMENT AND PERFORMANCE EVALUATION OF THERMAL CONDUCTIVITY EQUIPMENT FOR LABORATORY USES. DEPARTMENT OF MECHANICAL ENGINEERING, FEDERAL UNIVERSITY

More information

Prediction of Oil-Water Two Phase Flow Pressure Drop by Using Homogeneous Model

Prediction of Oil-Water Two Phase Flow Pressure Drop by Using Homogeneous Model FUNDAMENTAL DAN APLIKASI TEKNIK KIMIA 008 Surabaya, 5 November 008 Prediction of Oil-Water Two Pase Flow Pressure Drop by Using Nay Zar Aung a, Triyogi Yuwono b a Department of Mecanical Engineering, Institute

More information

Study of Convective Heat Transfer through Micro Channels with Different Configurations

Study of Convective Heat Transfer through Micro Channels with Different Configurations International Journal of Current Engineering and Tecnology E-ISSN 2277 4106, P-ISSN 2347 5161 2016 INPRESSCO, All Rigts Reserved Available at ttp://inpressco.com/category/ijcet Researc Article Study of

More information

158 Calculus and Structures

158 Calculus and Structures 58 Calculus and Structures CHAPTER PROPERTIES OF DERIVATIVES AND DIFFERENTIATION BY THE EASY WAY. Calculus and Structures 59 Copyrigt Capter PROPERTIES OF DERIVATIVES. INTRODUCTION In te last capter you

More information

Development of new and validation of existing convection correlations for rooms with displacement ventilation systems

Development of new and validation of existing convection correlations for rooms with displacement ventilation systems Energy and Buildings 38 (2006) 163 173 www.elsevier.com/locate/enbuild Development of new and validation of existing convection correlations for rooms wit displacement ventilation systems Atila Novoselac

More information

T718. c Dr. Md. Zahurul Haq (BUET) HX: Energy Balance and LMTD ME 307 (2018) 2/ 21 T793

T718. c Dr. Md. Zahurul Haq (BUET) HX: Energy Balance and LMTD ME 307 (2018) 2/ 21 T793 HX: Energy Balance and LMTD Dr. Md. Zahurul Haq Professor Department of Mechanical Engineering Bangladesh University of Engineering & Technology (BUET) Dhaka-000, Bangladesh http://zahurul.buet.ac.bd/

More information

Hall Effcts Eon Unsteady MHD Free Convection Flow Over A Stretching Sheet With Variable Viscosity And Viscous Dissipation

Hall Effcts Eon Unsteady MHD Free Convection Flow Over A Stretching Sheet With Variable Viscosity And Viscous Dissipation IOSR Journal of Matematics (IOSR-JM) e-issn: 78-578, p-issn: 39-765X. Volume, Issue 4 Ver. I (Jul - Aug. 5), PP 59-67 www.iosrjournals.org Hall Effcts Eon Unsteady MHD Free Convection Flow Over A Stretcing

More information

Distribution of reynolds shear stress in steady and unsteady flows

Distribution of reynolds shear stress in steady and unsteady flows University of Wollongong Researc Online Faculty of Engineering and Information Sciences - Papers: Part A Faculty of Engineering and Information Sciences 13 Distribution of reynolds sear stress in steady

More information

Journal of Applied Science and Agriculture. The Effects Of Corrugated Geometry On Flow And Heat Transfer In Corrugated Channel Using Nanofluid

Journal of Applied Science and Agriculture. The Effects Of Corrugated Geometry On Flow And Heat Transfer In Corrugated Channel Using Nanofluid Journal o Applied Science and Agriculture, 9() February 04, Pages: 408-47 AENSI Journals Journal o Applied Science and Agriculture ISSN 86-9 Journal ome page: www.aensiweb.com/jasa/index.tml Te Eects O

More information

Pre-lab Quiz/PHYS 224 Earth s Magnetic Field. Your name Lab section

Pre-lab Quiz/PHYS 224 Earth s Magnetic Field. Your name Lab section Pre-lab Quiz/PHYS 4 Eart s Magnetic Field Your name Lab section 1. Wat do you investigate in tis lab?. For a pair of Helmoltz coils described in tis manual and sown in Figure, r=.15 m, N=13, I =.4 A, wat

More information

A = h w (1) Error Analysis Physics 141

A = h w (1) Error Analysis Physics 141 Introduction In all brances of pysical science and engineering one deals constantly wit numbers wic results more or less directly from experimental observations. Experimental observations always ave inaccuracies.

More information

1 Power is transferred through a machine as shown. power input P I machine. power output P O. power loss P L. What is the efficiency of the machine?

1 Power is transferred through a machine as shown. power input P I machine. power output P O. power loss P L. What is the efficiency of the machine? 1 1 Power is transferred troug a macine as sown. power input P I macine power output P O power loss P L Wat is te efficiency of te macine? P I P L P P P O + P L I O P L P O P I 2 ir in a bicycle pump is

More information

HYDROMAGNETIC BOUNDARY LAYER MICROPOLAR FLUID FLOW OVER A STRETCHING SURFACE EMBEDDED IN A NON-DARCIAN POROUS MEDIUM WITH RADIATION

HYDROMAGNETIC BOUNDARY LAYER MICROPOLAR FLUID FLOW OVER A STRETCHING SURFACE EMBEDDED IN A NON-DARCIAN POROUS MEDIUM WITH RADIATION HYDROMAGNETIC BOUNDARY LAYER MICROPOLAR FLUID FLOW OVER A STRETCHING SURFACE EMBEDDED IN A NON-DARCIAN POROUS MEDIUM WITH RADIATION MOSTAFA A. A. MAHMOUD, MAHMOUD ABD-ELATY MAHMOUD, AND SHIMAA E. WAHEED

More information

De-Coupler Design for an Interacting Tanks System

De-Coupler Design for an Interacting Tanks System IOSR Journal of Electrical and Electronics Engineering (IOSR-JEEE) e-issn: 2278-1676,p-ISSN: 2320-3331, Volume 7, Issue 3 (Sep. - Oct. 2013), PP 77-81 De-Coupler Design for an Interacting Tanks System

More information

Hydraulic validation of the LHC cold mass heat exchanger tube.

Hydraulic validation of the LHC cold mass heat exchanger tube. Hydraulic validation o te LHC cold mass eat excanger tube. LHC Project Note 155 1998-07-22 (pilippe.provenaz@cern.c) Pilippe PROVENAZ / LHC-ACR Division Summary Te knowledge o te elium mass low vs. te

More information

Journal of Engineering Science and Technology Review 5 (4) (2012) Special Issue on Renewable Energy Systems.

Journal of Engineering Science and Technology Review 5 (4) (2012) Special Issue on Renewable Energy Systems. Jestr Journal of Engineering Science and ecnology eview 5 (4) (0) 56-65 Special Issue on enewable Energy Systems esearc Article JONA OF Engineering Science and ecnology eview www.jestr.org An Effective

More information

Journal of Chemical and Pharmaceutical Research, 2013, 5(12): Research Article

Journal of Chemical and Pharmaceutical Research, 2013, 5(12): Research Article Available online.jocpr.com Journal of emical and Parmaceutical Researc, 013, 5(1):55-531 Researc Article ISSN : 0975-7384 ODEN(USA) : JPR5 Performance and empirical models of a eat pump ater eater system

More information

Velocity distribution in non-uniform/unsteady flows and the validity of log law

Velocity distribution in non-uniform/unsteady flows and the validity of log law University of Wollongong Researc Online Faculty of Engineering and Information Sciences - Papers: Part A Faculty of Engineering and Information Sciences 3 Velocity distribution in non-uniform/unsteady

More information

Desalination by vacuum membrane distillation: sensitivity analysis

Desalination by vacuum membrane distillation: sensitivity analysis Separation and Purification Tecnology 33 (2003) 75/87 www.elsevier.com/locate/seppur Desalination by vacuum membrane distillation: sensitivity analysis Fawzi Banat *, Fami Abu Al-Rub, Kalid Bani-Melem

More information

Department of Mechanical Engineering, Azarbaijan Shahid Madani University, Tabriz, Iran b

Department of Mechanical Engineering, Azarbaijan Shahid Madani University, Tabriz, Iran b THERMAL SCIENCE, Year 2016, Vol. 20, No. 2, pp. 505-516 505 EXPERIMENTAL INVESTIGATION ON FLOW AND HEAT TRANSFER FOR COOLING FLUSH-MOUNTED RIBBONS IN A CHANNEL Application of an Electroydrodinamics Active

More information

Investigation of Heat Transfer on Smooth and Enhanced Tube in Heat Exchanger

Investigation of Heat Transfer on Smooth and Enhanced Tube in Heat Exchanger International Journal of Current Engineering and Technology E-ISSN 2277 4106, P-ISSN 2347 5161 2015INPRESSCO, All Rights Reserved Available at http://inpressco.com/category/ijcet Research Article Investigation

More information

Brazilian Journal of Physics, vol. 29, no. 1, March, Ensemble and their Parameter Dierentiation. A. K. Rajagopal. Naval Research Laboratory,

Brazilian Journal of Physics, vol. 29, no. 1, March, Ensemble and their Parameter Dierentiation. A. K. Rajagopal. Naval Research Laboratory, Brazilian Journal of Pysics, vol. 29, no. 1, Marc, 1999 61 Fractional Powers of Operators of sallis Ensemble and teir Parameter Dierentiation A. K. Rajagopal Naval Researc Laboratory, Wasington D. C. 2375-532,

More information

A MONTE CARLO ANALYSIS OF THE EFFECTS OF COVARIANCE ON PROPAGATED UNCERTAINTIES

A MONTE CARLO ANALYSIS OF THE EFFECTS OF COVARIANCE ON PROPAGATED UNCERTAINTIES A MONTE CARLO ANALYSIS OF THE EFFECTS OF COVARIANCE ON PROPAGATED UNCERTAINTIES Ronald Ainswort Hart Scientific, American Fork UT, USA ABSTRACT Reports of calibration typically provide total combined uncertainties

More information

AN ANALYSIS OF AMPLITUDE AND PERIOD OF ALTERNATING ICE LOADS ON CONICAL STRUCTURES

AN ANALYSIS OF AMPLITUDE AND PERIOD OF ALTERNATING ICE LOADS ON CONICAL STRUCTURES Ice in te Environment: Proceedings of te 1t IAHR International Symposium on Ice Dunedin, New Zealand, nd t December International Association of Hydraulic Engineering and Researc AN ANALYSIS OF AMPLITUDE

More information

Theoretical Analysis of Flow Characteristics and Bearing Load for Mass-produced External Gear Pump

Theoretical Analysis of Flow Characteristics and Bearing Load for Mass-produced External Gear Pump TECHNICAL PAPE Teoretical Analysis of Flow Caracteristics and Bearing Load for Mass-produced External Gear Pump N. YOSHIDA Tis paper presents teoretical equations for calculating pump flow rate and bearing

More information

Examination Heat Transfer

Examination Heat Transfer Examination Heat Transfer code: 4B680 date: June 13, 2008 time: 14.00-17.00 Note: There are 4 questions in total. The first one consists of independent subquestions. If possible and necessary, guide numbers

More information

Thermodynamics Lecture Series

Thermodynamics Lecture Series Termodynamics Lecture Series Ideal Ranke Cycle Te Practical Cycle Applied Sciences Education Researc Group (ASERG) Faculty of Applied Sciences Universiti Teknologi MARA email: drjjlanita@otmail.com ttp://www5.uitm.edu.my/faculties/fsg/drjj1.tml

More information

CHAPTER 7 NUMERICAL MODELLING OF A SPIRAL HEAT EXCHANGER USING CFD TECHNIQUE

CHAPTER 7 NUMERICAL MODELLING OF A SPIRAL HEAT EXCHANGER USING CFD TECHNIQUE CHAPTER 7 NUMERICAL MODELLING OF A SPIRAL HEAT EXCHANGER USING CFD TECHNIQUE In this chapter, the governing equations for the proposed numerical model with discretisation methods are presented. Spiral

More information

Flow of a Rarefied Gas between Parallel and Almost Parallel Plates

Flow of a Rarefied Gas between Parallel and Almost Parallel Plates Flow of a Rarefied Gas between Parallel and Almost Parallel Plates Carlo Cercignani, Maria Lampis and Silvia Lorenzani Dipartimento di Matematica, Politecnico di Milano, Milano, Italy 033 Abstract. Rarefied

More information

SENSITIVITY ANALYSIS FOR COUNTER FLOW COOLING TOWER- PART I, EXIT COLD WATER TEMPERATURE

SENSITIVITY ANALYSIS FOR COUNTER FLOW COOLING TOWER- PART I, EXIT COLD WATER TEMPERATURE SENSITIVITY ANALYSIS FOR COUNTER FLOW COOLING TOWER- PART I, EXIT COLD WATER TEMPERATURE *Citranjan Agaral Department of Mecanical Engineering, College of Tecnology and Engineering, Maarana Pratap Univerity

More information

Circle one: School of Mechanical Engineering Purdue University ME315 Heat and Mass Transfer. Exam #2. April 3, 2014

Circle one: School of Mechanical Engineering Purdue University ME315 Heat and Mass Transfer. Exam #2. April 3, 2014 Circle one: Div. 1 (12:30 pm, Prof. Choi) Div. 2 (9:30 am, Prof. Xu) School of Mechanical Engineering Purdue University ME315 Heat and Mass Transfer Exam #2 April 3, 2014 Instructions: Write your name

More information

The Effect of Mass Flow Rate on the Effectiveness of Plate Heat Exchanger

The Effect of Mass Flow Rate on the Effectiveness of Plate Heat Exchanger The Effect of Mass Flow Rate on the of Plate Heat Exchanger Wasi ur rahman Department of Chemical Engineering, Zakir Husain College of Engineering and Technology, Aligarh Muslim University, Aligarh 222,

More information

Why gravity is not an entropic force

Why gravity is not an entropic force Wy gravity is not an entropic force San Gao Unit for History and Pilosopy of Science & Centre for Time, SOPHI, University of Sydney Email: sgao7319@uni.sydney.edu.au Te remarkable connections between gravity

More information

Dedicated to the 70th birthday of Professor Lin Qun

Dedicated to the 70th birthday of Professor Lin Qun Journal of Computational Matematics, Vol.4, No.3, 6, 4 44. ACCELERATION METHODS OF NONLINEAR ITERATION FOR NONLINEAR PARABOLIC EQUATIONS Guang-wei Yuan Xu-deng Hang Laboratory of Computational Pysics,

More information

DYNAMIC MODELING OF ORGANIC RANKINE CYCLE (ORC) SYSTEM FOR FAULT DIAGNOSIS AND CONTROL SYSTEM DESIGN

DYNAMIC MODELING OF ORGANIC RANKINE CYCLE (ORC) SYSTEM FOR FAULT DIAGNOSIS AND CONTROL SYSTEM DESIGN DYNAMIC MODELING OF ORGANIC RANKINE CYCLE (ORC SYSTEM FOR FAULT DIAGNOSIS AND CONTROL SYSTEM DESIGN Sungjin Coi and Susan Krumdieck University of Canterbury, Private Bag 48, Cristcurc 84 New Zealand sungjin.coi@pg.canterbury.ac.nz

More information

Grade: 11 International Physics Olympiad Qualifier Set: 2

Grade: 11 International Physics Olympiad Qualifier Set: 2 Grade: 11 International Pysics Olympiad Qualifier Set: 2 --------------------------------------------------------------------------------------------------------------- Max Marks: 60 Test ID: 12111 Time

More information

Analysis of Heat Transfer Enhancement in Spiral Plate Heat Exchanger

Analysis of Heat Transfer Enhancement in Spiral Plate Heat Exchanger Vol. 2, No. 4 Modern Applied Science Analysis of Heat Transfer Enhancement in Spiral Plate Heat Exchanger Dr. Kaliannan Saravanan Professor & Head, Department of Chemical Engineering Kongu Engineering

More information

Announcements. Exam 4 - Review of important concepts

Announcements. Exam 4 - Review of important concepts Announcements 1. Exam 4 starts Friday! a. Available in esting Center from Friday, Dec 7 (opening time), up to Monday, Dec 10 at 4:00 pm. i. Late fee if you start your exam after 4 pm b. Covers C. 9-1 (up

More information

Lecture 38: Vapor-compression refrigeration systems

Lecture 38: Vapor-compression refrigeration systems ME 200 Termodynamics I Lecture 38: Vapor-compression refrigeration systems Yong Li Sangai Jiao Tong University Institute of Refrigeration and Cryogenics 800 Dong Cuan Road Sangai, 200240, P. R. Cina Email

More information

Chapter 11: Heat Exchangers. Dr Ali Jawarneh Department of Mechanical Engineering Hashemite University

Chapter 11: Heat Exchangers. Dr Ali Jawarneh Department of Mechanical Engineering Hashemite University Chapter 11: Heat Exchangers Dr Ali Jawarneh Department of Mechanical Engineering Hashemite University Objectives When you finish studying this chapter, you should be able to: Recognize numerous types of

More information

Technology-Independent Design of Neurocomputers: The Universal Field Computer 1

Technology-Independent Design of Neurocomputers: The Universal Field Computer 1 Tecnology-Independent Design of Neurocomputers: Te Universal Field Computer 1 Abstract Bruce J. MacLennan Computer Science Department Naval Postgraduate Scool Monterey, CA 9393 We argue tat AI is moving

More information

Heat Transfer and MHD Boundary Layer Flow over a Rotating Disk

Heat Transfer and MHD Boundary Layer Flow over a Rotating Disk J. Basic. Appl. Sci. Res., 4()37-33, 4 4, TextRoad Publication ISSN 9-434 Journal of Basic and Applied Scientific Researc www.textroad.com Heat Transfer and MHD Boundary Layer Flow over a Rotating Disk

More information

232 Calculus and Structures

232 Calculus and Structures 3 Calculus and Structures CHAPTER 17 JUSTIFICATION OF THE AREA AND SLOPE METHODS FOR EVALUATING BEAMS Calculus and Structures 33 Copyrigt Capter 17 JUSTIFICATION OF THE AREA AND SLOPE METHODS 17.1 THE

More information

The derivative function

The derivative function Roberto s Notes on Differential Calculus Capter : Definition of derivative Section Te derivative function Wat you need to know already: f is at a point on its grap and ow to compute it. Wat te derivative

More information

DESIGN AND EXPERIMENTAL ANALYSIS OF SHELL AND TUBE HEAT EXCHANGER (U-TUBE)

DESIGN AND EXPERIMENTAL ANALYSIS OF SHELL AND TUBE HEAT EXCHANGER (U-TUBE) DESIGN AND EXPERIMENTAL ANALYSIS OF SHELL AND TUBE HEAT EXCHANGER (U-TUBE) Divyesh B. Patel 1, Jayesh R. Parekh 2 Assistant professor, Mechanical Department, SNPIT&RC, Umrakh, Gujarat, India 1 Assistant

More information

1. Introduction. We consider the model problem: seeking an unknown function u satisfying

1. Introduction. We consider the model problem: seeking an unknown function u satisfying A DISCONTINUOUS LEAST-SQUARES FINITE ELEMENT METHOD FOR SECOND ORDER ELLIPTIC EQUATIONS XIU YE AND SHANGYOU ZHANG Abstract In tis paper, a discontinuous least-squares (DLS) finite element metod is introduced

More information

Experimental Validation of Cooperative Formation Control with Collision Avoidance for a Multi-UAV System

Experimental Validation of Cooperative Formation Control with Collision Avoidance for a Multi-UAV System Proceedings of te 6t International Conference on Automation, Robotics and Applications, Feb 17-19, 2015, Queenstown, New Zealand Experimental Validation of Cooperative Formation Control wit Collision Avoidance

More information

Physics 121, April 1, Equilibrium. Physics 121. April 1, Physics 121. April 1, Course Information. Discussion of Exam # 2

Physics 121, April 1, Equilibrium. Physics 121. April 1, Physics 121. April 1, Course Information. Discussion of Exam # 2 Pysics 121, April 1, 2008. Pysics 121. April 1, 2008. Course Information Discussion of Exam # 2 Topics to be discussed today: Requirements for Equilibrium Gravitational Equilibrium Sample problems Pysics

More information

(4.2) -Richardson Extrapolation

(4.2) -Richardson Extrapolation (.) -Ricardson Extrapolation. Small-O Notation: Recall tat te big-o notation used to define te rate of convergence in Section.: Suppose tat lim G 0 and lim F L. Te function F is said to converge to L as

More information

CHAPTER 18 MOTION IN A CIRCLE

CHAPTER 18 MOTION IN A CIRCLE EXERCISE, Pae 6 CHAPTER 8 MOTION IN A CIRCLE. A locomotive travels around a curve of 0 m radius. If te orizontal trust on te outer rail is of te locomotive weit, determine te speed of te locomotive. Te

More information

c Dr. Md. Zahurul Haq (BUET) Heat Exchangers: Rating & Sizing - I ME 307 (2017) 2 / 32 T666

c Dr. Md. Zahurul Haq (BUET) Heat Exchangers: Rating & Sizing - I ME 307 (2017) 2 / 32 T666 Heat Exchanger: Rating & Sizing Heat Exchangers: Rating & Sizing - I Dr. Md. Zahurul Haq Professor Department of Mechanical Engineering Bangladesh University of Engineering & Technology (BUET) Dhaka-000,

More information

Wind Turbine Micrositing: Comparison of Finite Difference Method and Computational Fluid Dynamics

Wind Turbine Micrositing: Comparison of Finite Difference Method and Computational Fluid Dynamics IJCSI International Journal of Computer Science Issues, Vol. 9, Issue 1, No 1, January 01 ISSN (Online): 169-081 www.ijcsi.org 7 Wind Turbine Micrositing: Comparison of Finite Difference Metod and Computational

More information

Introduction to Heat and Mass Transfer

Introduction to Heat and Mass Transfer Introduction to Heat and Mass Transfer Week 16 Merry X mas! Happy New Year 2019! Final Exam When? Thursday, January 10th What time? 3:10-5 pm Where? 91203 What? Lecture materials from Week 1 to 16 (before

More information

INTRODUCTION DEFINITION OF FLUID. U p F FLUID IS A SUBSTANCE THAT CAN NOT SUPPORT SHEAR FORCES OF ANY MAGNITUDE WITHOUT CONTINUOUS DEFORMATION

INTRODUCTION DEFINITION OF FLUID. U p F FLUID IS A SUBSTANCE THAT CAN NOT SUPPORT SHEAR FORCES OF ANY MAGNITUDE WITHOUT CONTINUOUS DEFORMATION INTRODUCTION DEFINITION OF FLUID plate solid F at t = 0 t > 0 = F/A plate U p F fluid t 0 t 1 t 2 t 3 FLUID IS A SUBSTANCE THAT CAN NOT SUPPORT SHEAR FORCES OF ANY MAGNITUDE WITHOUT CONTINUOUS DEFORMATION

More information

Thermal Bending of Circular Plates for Non-axisymmetrical Problems

Thermal Bending of Circular Plates for Non-axisymmetrical Problems Copyrigt 2 Tec Science Press SL, vol.4, no.2, pp.5-2, 2 Termal Bending of Circular Plates for Non-axisymmetrical Problems Dong Zengzu Peng Weiong and Li Suncai Abstract: Due to te complexity of termal

More information

The Vorticity Equation in a Rotating Stratified Fluid

The Vorticity Equation in a Rotating Stratified Fluid Capter 7 Te Vorticity Equation in a Rotating Stratified Fluid Te vorticity equation for a rotating, stratified, viscous fluid Te vorticity equation in one form or anoter and its interpretation provide

More information

Falling liquid films: wave patterns and thermocapillary effects

Falling liquid films: wave patterns and thermocapillary effects Falling liquid films: wave patterns and termocapillary effects Benoit Sceid Cimie-Pysique E.P., Université Libre de Bruxelles C.P. 65/6 Avenue F.D. Roosevelt, 50-50 Bruxelles - BELGIUM E-mail: bsceid@ulb.ac.be

More information

Chapter 2 Ising Model for Ferromagnetism

Chapter 2 Ising Model for Ferromagnetism Capter Ising Model for Ferromagnetism Abstract Tis capter presents te Ising model for ferromagnetism, wic is a standard simple model of a pase transition. Using te approximation of mean-field teory, te

More information

Finite Element Analysis of J-Integral for Surface Cracks in Round Bars under Combined Mode I Loading

Finite Element Analysis of J-Integral for Surface Cracks in Round Bars under Combined Mode I Loading nternational Journal of ntegrated Engineering, Vol. 9 No. 2 (207) p. -8 Finite Element Analysis of J-ntegral for Surface Cracks in Round Bars under Combined Mode Loading A.E smail, A.K Ariffin 2, S. Abdulla

More information

Coolant. Circuits Chip

Coolant. Circuits Chip 1) A square isothermal chip is of width w=5 mm on a side and is mounted in a subtrate such that its side and back surfaces are well insulated, while the front surface is exposed to the flow of a coolant

More information

Derivative as Instantaneous Rate of Change

Derivative as Instantaneous Rate of Change 43 Derivative as Instantaneous Rate of Cange Consider a function tat describes te position of a racecar moving in a straigt line away from some starting point Let y s t suc tat t represents te time in

More information

Heat Transfer Convection

Heat Transfer Convection Heat ransfer Convection Previous lectures conduction: heat transfer without fluid motion oday (textbook nearly 00 pages) Convection: heat transfer with fluid motion Research methods different Natural Convection

More information

HOW TO DEAL WITH FFT SAMPLING INFLUENCES ON ADEV CALCULATIONS

HOW TO DEAL WITH FFT SAMPLING INFLUENCES ON ADEV CALCULATIONS HOW TO DEAL WITH FFT SAMPLING INFLUENCES ON ADEV CALCULATIONS Po-Ceng Cang National Standard Time & Frequency Lab., TL, Taiwan 1, Lane 551, Min-Tsu Road, Sec. 5, Yang-Mei, Taoyuan, Taiwan 36 Tel: 886 3

More information

New Fourth Order Quartic Spline Method for Solving Second Order Boundary Value Problems

New Fourth Order Quartic Spline Method for Solving Second Order Boundary Value Problems MATEMATIKA, 2015, Volume 31, Number 2, 149 157 c UTM Centre for Industrial Applied Matematics New Fourt Order Quartic Spline Metod for Solving Second Order Boundary Value Problems 1 Osama Ala yed, 2 Te

More information

Axial profiles of heat transfer coefficients in a liquid film evaporator

Axial profiles of heat transfer coefficients in a liquid film evaporator Axial profiles of heat transfer coefficients in a liquid film evaporator Pavel Timár, Ján Stopka, Vladimír Báleš Department of Chemical and Biochemical Engineering, Faculty of Chemical and Food Technology,

More information

ONSET OF NUCLEATE BOILING AND CRITICAL HEAT FLUX WITH BOILING WATER IN MICROCHANNELS

ONSET OF NUCLEATE BOILING AND CRITICAL HEAT FLUX WITH BOILING WATER IN MICROCHANNELS International Journal of Microscale and Nanoscale Termal ISSN: 1949-4955 Volume 4, Number 1 Nova Science Publisers, Inc. ONSET OF NUCLEATE BOILING AND CRITICAL HEAT FLUX WITH BOILING WATER IN MICROCHANNELS

More information

106 PHYS - CH6 - Part2

106 PHYS - CH6 - Part2 106 PHYS - CH6 - Part Conservative Forces (a) A force is conservative if work one by tat force acting on a particle moving between points is inepenent of te pat te particle takes between te two points

More information