Topology Optimization of an Actively Cooled Electronics Section for Downhole Tools
|
|
- Ashley Bryan
- 5 years ago
- Views:
Transcription
1 Topology Optimization of an Actively Cooled Electronics Section for Downhole Tools S. Soprani*, J. H. K. Haertel, B. S. Lazarov, O. Sigmund, K. Engelbrecht
2 Table of contents Introduction Method and COMSOL model Analysis of the results Choice of the final design Conclusions November October 2014
3 Introduction Topology Optimization: mathematical approach that optimizes the material layout within a given design space and boundary conditions November October 2014
4 Introduction Downhole Tool: cylindrical robotic tool used to increase or restore the production of oil and gas wells (well cleaning, pipe cutting, installation of valves). I feed Q TEC - Thermoelectric (Peltier) cooler: upgrade the maximum operating temperature from 175 C to 200 C November October 2014
5 Problem formulation Metallic housing (o.d. 80mm) Optimizable chassis TEC Heat spreader + soft thermal pad Design Criteria: Use aluminum to enhance Axial thesection cooler s of heat the downhole rejection tool s the implemented well. geometry. Structural chassis (o.d. 60mm) T-sensitive electronics (PCB) Use thermal insulation to protect the cooled electronics. Optimize the distribution of aluminum-thermal insulation within the chassis Minimize the average PCB temperature November October 2014
6 Governing equations Heat conduction k T = Q source (1) Modified heat conduction JST k T = Q JouleHeating (2) Convective heat flux (T fluid, h) TEC feed current I feed Boundary conditions Thermal insulation Thermal (contact) resistance Heat source (1 W) November October 2014
7 Topology Optimization Implementation (SIMP method) minimize: f obj T, ρ design = 1 A PCB Ω PCB T dω PCB (3) constraints: 0 ρ design 1 (4) ρ design Density filter f(r) ρ Projection function p(η,β) ρ interpolation function: k SIMP = k ins + k Al k ins ρ p (5) November October 2014
8 Simulation results interpolation function: k SIMP = k ins + k Al k ins ρ p (5) p(η,β = 1) p(η,β = 8) I feed = 4 A h = 50 Wm -2 K November October 2014
9 Simulation results T fluid = 200 C h = 25, 50, 100, 500 Wm -2 K -1 I feed = 1, 2, 3, 4 A ρ optimized distribution I feed = 2 A h = 100 Wm -2 K -1 ρ optimized distribution I feed = 4 A h = 50 Wm -2 K -1 Aluminum Insulator Design 1 Design 2 Low I feed / High h High I feed / Low h Aluminum pad length grows with I feed and decreases with h. Aluminum layer thickness grows with I feed and decreases with h November October 2014
10 Choice of the final design Axial section of the finally chosen design. h (Wm -2 K -1 ) Opt - 1A T PCB ( C) Design - 1A T PCB ( C) ΔT (K) h (Wm -2 K -1 ) Opt - 2A T PCB ( C) Design - 2A T PCB ( C) ΔT (K) h (Wm -2 K -1 ) Opt - 3A T PCB ( C) Design - 3A T PCB ( C) ΔT (K) h (Wm -2 K -1 ) Opt - 4A T PCB ( C) Design - 4A T PCB ( C) ΔT (K) ΔT = T PCB,design - T PCB,Opt November October 2014
11 Conclusions The topology optimization (SIMP) approach supported the development of a chassis for actively cooled downhole electronics. Two main design concepts were found and analyzed. A parametric study evaluated the sensitivity of the optimized topologies to the boundary conditions. The final design was defined according to the optimization results and proved to perform very closely to the optimized systems November October 2014
12 Thank you for the attention November October 2014
13 Extra slides November October 2014
14 COMSOL Multiphysics representation of the longitudinal section of the downhole tool (left side) and particular of the TEC device with the two plates and the semiconducting material layer highlighted in blue (right side) November October 2014
15 Governing equations Heat conduction k T = Q source (1) Modified heat conduction JST k T = Q JouleHeating (2) Convective heat flux (T fluid, h) TEC feed current I feed Boundary conditions Thermal insulation Thermal (contact) resistance Heat source (1 W) November October 2014
16 Cross-Check analysis Evaluate the performance of the optimized designs at different boundary conditions The optimization process is negligibly sensitive to the well fluid convection regime, at a given I feed. The TEC feed current influences significantly the optimized design. But we can control it! An optimal feed current I feed,opt was found. I feed,opt varies with h and ranges between 2 and 3 A November October 2014
17 R vs. well fluid convective coefficient, for different TEC feed currents. Different symbols refer to the different optimized design concepts. = Design 1, = Design 2. HTS electronics temperature vs. well fluid convective coefficient for four different systems, optimized for I feed = 2 A and h = 25, 50, 100 and 500 Wm -2 K November October 2014
18 HTS electronics temperature vs. TEC feed current for four different systems, optimized for I feed h = 25 Wm -2 K -1 (left side) and 50 Wm -2 K -1 (right side). = 1, 2, 3 and 4 A, and November October 2014
19 Characteristic curve of the finally designed electronics unit. The plot reports the performance of the cooling system as HTS electronics temperature vs. Convective coefficient and TEC feed current. The minimum HTS electronics temperatures for each operating condition are highlighted with a red line November October 2014
20 J = NI feed A tot = NI feed A tot NA leg = I feed A BiTe = J x NA leg A leg A BiTe tot J S = J S S = S x BiTe k A air A BiTe = k air + k A BiTe = k tot A air (1 x BiTe ) + k BiTe x BiTe tot σ = σ BiTe x BiTe + σ air x air = σ BiTe x BiTe (Gordon 2002) November October 2014
21 Topology Optimization Implementation (SIMP method) minimize: f obj T, ρ design = 1 A PCB Ω PCB T dω PCB (3) constraints: 0 ρ design 1 (4) r T, ρ design = 0 (5) density filter: r 2 2 ρ + ρ = ρ design (Lazarov 2011) (6) projection function: ρ i = tanh βη +tanh(β( ρ i η) tanh βη +tanh β 1 η (Wang 2011) (7) interpolation function: k SIMP = k ins + k Al k ins ρ p (8) November October 2014
22 Topology Optimization Implementation (SIMP method) projection function: ρ i = tanh βη +tanh(β( ρ i η) tanh βη +tanh β 1 η (Wang 2011) (7) November October 2014
23 Simulation results interpolation function: k SIMP = k ins + k Al k ins ρ p (5) November October 2014
24 Simulation results interpolation function: k SIMP = k ins + k Al k ins ρ p (5) November October 2014
25 Simulation results interpolation function: k SIMP = k ins + k Al k ins ρ p (5) November October 2014
26 Simulation results interpolation function: k SIMP = k ins + k Al k ins ρ p (5) November October 2014
27 Simulation results interpolation function: k SIMP = k ins + k Al k ins ρ p (5) November October 2014
28 Simulation results interpolation function: k SIMP = k ins + k Al k ins ρ p (5) November October 2014
29 Simulation results interpolation function: k SIMP = k ins + k Al k ins ρ p (5) November October 2014
30 Simulation results interpolation function: k SIMP = k ins + k Al k ins ρ p (5) November October 2014
31 Simulation results interpolation function: k SIMP = k ins + k Al k ins ρ p (5) p(η,β = 1) p(η,β = 8) November October 2014
Topology Optimization of an Actively Cooled Electronics Section for Downhole Tools
Downloaded from orbit.dtu.dk on: Apr 01, 2019 Topology Optimization of an Actively Cooled Electronics Section for Downhole Tools Soprani, Stefano; Haertel, Jan Hendrik Klaas; Lazarov, Boyan Stefanov; Sigmund,
More informationActive Cooling and Thermal Management of a Downhole Tool Electronics Section
Downloaded from orbit.dtu.dk on: Dec 09, 2017 Active Cooling and Thermal Management of a Downhole Tool Electronics Section Soprani, Stefano; Engelbrecht, Kurt; Just Nørgaard, Anders Published in: Proceedings
More informationComponent & Board Level Cooling.
> Component & Board Level Cooling www.resheji.com (C) Flomerics Ltd 2002 Section Title Components PCBs Packages Interface Materials Heat Sinks Thermoelectric Coolers Heat Pipes Printed Circuit Boards
More information11. Advanced Radiation
. Advanced adiation. Gray Surfaces The gray surface is a medium whose monochromatic emissivity ( λ does not vary with wavelength. The monochromatic emissivity is defined as the ratio of the monochromatic
More informationThermal Design of Heat Sink and Optimization of Fin Parameters
Thermal Design of Heat Sink and Optimization of Fin Parameters Srikanth. V 1, Ramesh.C.G 2 Department of Mechanical Engineering, Sir MVIT, Bangalore, India. 1 Department of Mechanical Engineering, Sir
More informationThermo-Fluid Performance of a Vapor- Chamber Finned Heat Sink
The Egyptian International Journal of Engineering Sciences and Technology Vol. 20 (July 2016) 10 24 http://www.eijest.zu.edu.eg Thermo-Fluid Performance of a Vapor- Chamber Finned Heat Sink Saeed A.A.
More informationMultiphysics Simulation and Optimization for Thermal Management of Electronics Systems
Multiphysics Simulation and Optimization for Thermal Management of Electronics Systems Ercan M. Dede, Jaewook Lee, & Tsuyoshi Nomura Toyota Research Institute of North America Ann Arbor, MI APEC 2012 Industry
More informationPrinciples of Food and Bioprocess Engineering (FS 231) Problems on Heat Transfer
Principles of Food and Bioprocess Engineering (FS 1) Problems on Heat Transfer 1. What is the thermal conductivity of a material 8 cm thick if the temperature at one end of the product is 0 C and the temperature
More informationPHYSICAL MECHANISM OF NATURAL CONVECTION
1 NATURAL CONVECTION In this chapter, we consider natural convection, where any fluid motion occurs by natural means such as buoyancy. The fluid motion in forced convection is quite noticeable, since a
More informationMPC-D403 MPC-D404. Ultra-small Peltier Coolers. High impedance Low control current High power efficiency
MPC-D MPC-D Ultra-small Peltier Coolers High impedance Low control current High power efficiency MPC-D / D. Introduction. General description The MPC- / D micro chip-sized thermoelectric coolers (TEC)
More informationThe Influence of Channel Aspect Ratio on Performance of Optimized Thermal-Fluid Structures
Excerpt from the Proceedings of the COMSOL Conference 2010 Boston The Influence of Channel Aspect Ratio on Performance of Optimized Thermal-Fluid Structures Ercan M. Dede 1* 1 Technical Research Department,
More informationNumerical Study of a High Temperature Latent Heat Storage ( C) Using NaNO 3 -KNO 3 Binary Mixture
1 Presented at the COMSOL Conference 2010 Paris Numerical Study of a High Temperature Latent Heat Storage (200-300 0 C) Using NaNO 3 -KNO 3 Binary Mixture Foong Chee Woh, 17-11-2010 2 Background 3 Background
More informationWrite Down Your NAME. Circle Your DIVISION. Div. 1 Div. 2 Div. 3 Div.4 8:30 am 9:30 pm 12:30 pm 3:30 pm Han Xu Ruan Pan
Write Down Your NAME, Last First Circle Your DIVISION Div. 1 Div. 2 Div. 3 Div.4 8:30 am 9:30 pm 12:30 pm 3:30 pm Han Xu Ruan Pan ME315 Heat and Mass Transfer School of Mechanical Engineering Purdue University
More informationDesign of an Automated Thermal Cycler for Long-term Phase Change Material Phase Transition Stability Studies
Design of an Automated Thermal Cycler for Long-term Phase Change Material Phase Transition Stability Studies Ali C. Kheirabadi, Dominic Groulx Dept. of Mechanical Engineering Dalhousie University Thermal
More informationENSC 388. Assignment #8
ENSC 388 Assignment #8 Assignment date: Wednesday Nov. 11, 2009 Due date: Wednesday Nov. 18, 2009 Problem 1 A 3-mm-thick panel of aluminum alloy (k = 177 W/m K, c = 875 J/kg K, and ρ = 2770 kg/m³) is finished
More informationN. Lemcoff 1 and S.Wyatt 2. Rensselaer Polytechnic Institute Hartford. Alstom Power
N. Lemcoff 1 and S.Wyatt 2 1 Rensselaer Polytechnic Institute Hartford 2 Alstom Power Excerpt from the Proceedings of the 2012 COMSOL Conference in Boston Background Central solar receiver steam generators
More informationModeling a Catalytic Converter in Comsol Multiphysics
Modeling a Catalytic Converter in Comsol Multiphysics By Jacob Harding December 10 th, 2007 Chem E 499 Problem The goal of this project was to develop a model of a catalytic converter in Comsol Multiphysics.
More informationMECH 375, Heat Transfer Handout #5: Unsteady Conduction
1 MECH 375, Heat Transfer Handout #5: Unsteady Conduction Amir Maleki, Fall 2018 2 T H I S PA P E R P R O P O S E D A C A N C E R T R E AT M E N T T H AT U S E S N A N O PA R T I - C L E S W I T H T U
More informationSupplementary Information for On-chip cooling by superlattice based thin-film thermoelectrics
Supplementary Information for On-chip cooling by superlattice based thin-film thermoelectrics Table S1 Comparison of cooling performance of various thermoelectric (TE) materials and device architectures
More informationOPTIMIZATION of the GEOMETRY & MATERIAL of SOLAR WATER HEATERS.
OPTIMIZATION of the GEOMETRY & MATERIAL of SOLAR WATER HEATERS. FLAT PLATE COLLECTORS ABSORBER PLATES OPTIMIZATION OF GEOMETRY SELECTIVE SURFACES METHODS OF TESTING TO DETERMINE THE THERMAL PERFORMANCE
More informationUWE has obtained warranties from all depositors as to their title in the material deposited and as to their right to deposit such material.
Hughes, T. and Weerasinghe, R. (2015) CFD modelling of thermal management in downhole tools. In: UK HTC 2015, Edinburgh, Scotland, UK, 7-8 September 2015. Available from: http://eprints.uwe.ac.uk/28777
More informationCOVENANT UNIVERSITY NIGERIA TUTORIAL KIT OMEGA SEMESTER PROGRAMME: MECHANICAL ENGINEERING
COVENANT UNIVERSITY NIGERIA TUTORIAL KIT OMEGA SEMESTER PROGRAMME: MECHANICAL ENGINEERING COURSE: MCE 524 DISCLAIMER The contents of this document are intended for practice and leaning purposes at the
More informationUNIVERSITY OF WATERLOO. ECE 309 Thermodynamics and Heat Transfer. Final Examination Spring 1997
UNIVERSITY OF WATERLOO DEPARTMENT OF ELECTRICAL ENGINEERING ECE 309 Thermodynamics and Heat Transfer Final Examination Spring 1997 M.M. Yovanovich August 5, 1997 9:00 A.M.-12:00 Noon NOTE: 1. Open book
More informationThermal Unit Operation (ChEg3113)
Thermal Unit Operation (ChEg3113) Lecture 3- Examples on problems having different heat transfer modes Instructor: Mr. Tedla Yeshitila (M.Sc.) Today Review Examples Multimode heat transfer Heat exchanger
More informationNumerical Heat and Mass Transfer
Master Degree in Mechanical Engineering Numerical Heat and Mass Transfer 03 Finned Surfaces Fausto Arpino f.arpino@unicas.it Outline Introduction Straight fin with constant circular cross section Long
More informationHEAT TRANSFER. Mechanisms of Heat Transfer: (1) Conduction
HEAT TRANSFER Mechanisms of Heat Transfer: (1) Conduction where Q is the amount of heat, Btu, transferred in time t, h k is the thermal conductivity, Btu/[h ft 2 ( o F/ft)] A is the area of heat transfer
More informationIf there is convective heat transfer from outer surface to fluid maintained at T W.
Heat Transfer 1. What are the different modes of heat transfer? Explain with examples. 2. State Fourier s Law of heat conduction? Write some of their applications. 3. State the effect of variation of temperature
More informationIntroduction to Heat and Mass Transfer. Week 5
Introduction to Heat and Mass Transfer Week 5 Critical Resistance Thermal resistances due to conduction and convection in radial systems behave differently Depending on application, we want to either maximize
More informationPotential use of Thermoelectric Generator Device for Air Conditioning System
Potential use of Thermoelectric Generator Device for Air Conditioning System Pedro M. Peralta Trinidad 1, Gerardo Carbajal 1 1 Universidad del Turabo, Puerto Rico, pperalta.engi@gmail.com, gcarbajal1@suagm.edu
More informationThermoelectric heat pump for heating and cooling in building services with low thermal power (Peltier_Heat_Pump)
Highlights der Energieforschung / 22.6.2016 / Wien Thermoelectric heat pump for heating and cooling in building services with low thermal power (Peltier_Heat_Pump) Stutterecker, Aschauer + Projektteam
More information1. Nusselt number and Biot number are computed in a similar manner (=hd/k). What are the differences between them? When and why are each of them used?
1. Nusselt number and Biot number are computed in a similar manner (=hd/k). What are the differences between them? When and why are each of them used?. During unsteady state heat transfer, can the temperature
More informationHEAT TRANSFER THERMAL MANAGEMENT OF ELECTRONICS YOUNES SHABANY. C\ CRC Press W / Taylor Si Francis Group Boca Raton London New York
HEAT TRANSFER THERMAL MANAGEMENT OF ELECTRONICS YOUNES SHABANY C\ CRC Press W / Taylor Si Francis Group Boca Raton London New York CRC Press is an imprint of the Taylor & Francis Group, an informa business
More informationHEAT TRANSFER FROM FINNED SURFACES
Fundamentals of Thermal-Fluid Sciences, 3rd Edition Yunus A. Cengel, Robert H. Turner, John M. Cimbala McGraw-Hill, 2008 HEAT TRANSFER FROM FINNED SURFACES Mehmet Kanoglu Copyright The McGraw-Hill Companies,
More informationConduction Heat Transfer. Fourier Law of Heat Conduction. x=l Q x+ Dx. insulated x+ Dx. x x. x=0 Q x A
Conduction Heat Transfer Reading Problems 10-1 10-6 10-20, 10-48, 10-59, 10-70, 10-75, 10-92 10-117, 10-123, 10-151, 10-156, 10-162 11-1 11-2 11-14, 11-20, 11-36, 11-41, 11-46, 11-53, 11-104 Fourier Law
More informationAvailable online at ScienceDirect. Energy Procedia 75 (2015 ) Multiphysics Simulations of a Thermoelectric Generator
Available online at www.sciencedirect.com ScienceDirect Energy Procedia 75 (2015 ) 633 638 The 7 th International Conference on Applied Energy ICAE2015 Multiphysics Simulations of a Thermoelectric Generator
More informationELEC9712 High Voltage Systems. 1.2 Heat transfer from electrical equipment
ELEC9712 High Voltage Systems 1.2 Heat transfer from electrical equipment The basic equation governing heat transfer in an item of electrical equipment is the following incremental balance equation, with
More informationAnalysis of the Cooling Design in Electrical Transformer
Analysis of the Cooling Design in Electrical Transformer Joel de Almeida Mendes E-mail: joeldealmeidamendes@hotmail.com Abstract This work presents the application of a CFD code Fluent to simulate the
More informationINTRODUCTION TO FLUID MECHANICS June 27, 2013
INTRODUCTION TO FLUID MECHANICS June 27, 2013 PROBLEM 3 (1 hour) A perfect liquid of constant density ρ and constant viscosity µ fills the space between two infinite parallel walls separated by a distance
More informationPeltier Application Note
Peltier Application Note Early 19th century scientists, Thomas Seebeck and Jean Peltier, first discovered the phenomena that are the basis for today s thermoelectric industry. Seebeck found that if you
More informationSIMULATION OF HEAT TRANSFER AND ELECTROMAGNETIC FIELDS OF PROTECTED MICROCOMPUTERS
281 Simulation of heat transfer and electromagnetic fields of protected microcomputers SIMULATION OF HEAT TRANSFER AND ELECTROMAGNETIC FIELDS OF PROTECTED MICROCOMPUTERS J. Lakatoš, J. untala, A. Kondelová
More informationNatural Convection from Horizontal Rectangular Fin Arrays within Perforated Chassis
Proceedings of the 2 nd International Conference on Fluid Flow, Heat and Mass Transfer Ottawa, Ontario, Canada, April 30 May 1, 2015 Paper No. 146 Natural Convection from Horizontal Rectangular Fin Arrays
More informationAnalysisofElectroThermalCharacteristicsofaConductiveLayerwithCracksandHoles
Global Journal of Researches in Engineering Mechanical and Mechanics Engineering Volume 14 Issue 1 Version 1.0 Type: Double Blind Peer Reviewed International Research Journal Publisher: Global Journals
More informationDesign of an Automated Thermal Cycler for Long-term Phase Change Material Phase Transition Stability Studies
Design of an Automated Thermal Cycler for Long-term Phase Change Material Phase Transition Stability Studies A. C. Kheirabadi, D. Groulx * Laboratory of Applied Multiphase Thermal Engineering (LAMTE),
More informationPHYSICAL MECHANISM OF CONVECTION
Tue 8:54:24 AM Slide Nr. 0 of 33 Slides PHYSICAL MECHANISM OF CONVECTION Heat transfer through a fluid is by convection in the presence of bulk fluid motion and by conduction in the absence of it. Chapter
More informationUniversity of New Mexico Mechanical Engineering Spring 2012 PhD qualifying examination Heat Transfer
University of New Mexico Mechanical Engineering Spring 2012 PhD qualifying examination Heat Transfer Closed book. Formula sheet and calculator are allowed, but not cell phones, computers or any other wireless
More informationChapter 3 Steady-State, ne- mens onal C on uction
Chapter 3 Steady-State, One-Dimensional i Conduction 3.1 The Plane Wall 3.1.1 Temperature Distribution For one-dimensional, steady-state conduction in a plane wall with no heat generation, the differential
More informationPrinciples of Food and Bioprocess Engineering (FS 231) Exam 2 Part A -- Closed Book (50 points)
Principles of Food and Bioprocess Engineering (FS 231) Exam 2 Part A -- Closed Book (50 points) 1. Are the following statements true or false? (20 points) a. Thermal conductivity of a substance is a measure
More informationPossibilities of Using COMSOL Software in Physics
ALEKSANDRAS STULGINSKIS UNIVERSITY Possibilities of Using COMSOL Software in Physics Jolita Sakaliūnienė 1 Overview Requirement of study quality Student motivation COMSOL software Composition of COMSOL
More informationMODEL: WB009GMFI19HLD (120V) Wall Mount DC Inverter Fan Coil Unit 9,000 BTUH
MODEL: WB009GMFI19HLD (120V) Wall Mount DC Inverter Fan Coil Unit 9,000 BTUH No. Part Name Quantity BOM code List Price Remark 1 Panel assembly 1 201132890609 2 Air filter 2 201132890704 5 Display box
More informationMECHANISM BEHIND FREE /NATURAL CONVECTION
CONVECTIVE HEAT TRANSFER By: Prof K. M. Joshi, Assi. Professor, MED, SSAS Institute of Technology, Surat. MECHANISM BEHIND FREE /NATURAL CONVECTION The stagnate layer of fluid in immediate vicinity of
More informationChapter 7: Natural Convection
7-1 Introduction 7- The Grashof Number 7-3 Natural Convection over Surfaces 7-4 Natural Convection Inside Enclosures 7-5 Similarity Solution 7-6 Integral Method 7-7 Combined Natural and Forced Convection
More informationTRANSIENT HEAT CONDUCTION
TRANSIENT HEAT CONDUCTION Many heat conduction problems encountered in engineering applications involve time as in independent variable. This is transient or Unsteady State Heat Conduction. The goal of
More informationChapter 3: Fundamentals of Mechanics and Heat. 1/11/00 Electromechanical Dynamics 1
Chapter 3: Fundamentals of Mechanics and Heat 1/11/00 Electromechanical Dynamics 1 Force Linear acceleration of an object is proportional to the applied force: F = m a x(t) F = force acting on an object
More informationMicro Cooling of SQUID Sensor
Excerpt from the Proceedings of the COMSOL Conference 2008 Hannover Micro Cooling of SQUID Sensor B.Ottosson *,1, Y. Jouahri 2, C. Rusu 1 and P. Enoksson 3 1 Imego AB, SE-400 14 Gothenburg, Sweden, 2 Mechanical
More informationHEAT TRANSFER BY CONVECTION. Dr. Şaziye Balku 1
HEAT TRANSFER BY CONVECTION Dr. Şaziye Balku 1 CONDUCTION Mechanism of heat transfer through a solid or fluid in the absence any fluid motion. CONVECTION Mechanism of heat transfer through a fluid in the
More informationComparative assessment of a temperature distribution into different CPU coolers
Comparative assessment of a temperature distribution into different CPU coolers DUMITRU CAZACU Electrical Engineering Department University of Pitesti 1 Targul din vale, 110040, Pitesti, jud Arges ROMANIA
More informationHow thermal management affects your product and business
#1 Thermal management How thermal management affects your product and business White paper Thermal management #1 Nolato 2 of 11 Fundamental all electronics generate heat All electronic devices and circuitry
More informationFIND: (a) Sketch temperature distribution, T(x,t), (b) Sketch the heat flux at the outer surface, q L,t as a function of time.
PROBLEM 5.1 NOWN: Electrical heater attached to backside of plate while front surface is exposed to convection process (T,h); initially plate is at a uniform temperature of the ambient air and suddenly
More informationSimplifying a model of short subsequent sections containing a common detailed cross-section.
Excerpt from the Proceedings of the COMSOL Conference 010 Paris Simplifying a model of short subsequent sections containing a common detailed cross-section. J. Krah Aker Solutions Snar yveien 36, 1364
More informationSimulation of Free Convection with Conjugate Heat Transfer
Simulation of Free Convection with Conjugate Heat Transfer Hong Xu, Chokri Guetari, Kurt Svihla ANSYS, Inc. Abstract This study focuses on free convective and conjugate heat transfer in a naturally ventilated,
More informationRadiant Heating Panel Thermal Analysis. Prepared by Tim Fleury Harvard Thermal, Inc. October 7, 2003
Radiant Heating Panel Thermal Analysis Prepared by Tim Fleury Harvard Thermal, Inc. October 7, 2003 Analysis Objective Perform a thermal test on a small sample of the concrete to determine the Thermal
More informationFeatures of Uni-Thermo
Pelti ier Device in the 21st Uni-Thermo Century Hi eliability NTENTS Comparison with a Conventional Peltier Device. The Result of Operating Reliability Test Peltier Device Uni-Thermo Quality Chart Peltier
More informationNumerical Investigation on The Convective Heat Transfer Enhancement in Coiled Tubes
Numerical Investigation on The Convective Heat Transfer Enhancement in Coiled Tubes Luca Cattani Department of Industrial Engineering - University of Parma Excerpt from the Proceedings of the 2012 COMSOL
More informationNEEDS Thermoelectric Compact Model Documentation Version 1.0.0
NEEDS Thermoelectric Compact Model Documentation Version 1.0.0 Published on August 31, 2015 Introduction The NEEDS thermoelectric compact model (TEsegment.va) describes a homogeneous segment of thermoelectric
More informationTopology Optimization Formulations for Circuit Board Heat Spreader Design
Topology Optimization Formulations for Circuit Board Heat Spreader Design Danny J. Lohan and James T. Allison University of Illinois at Urbana-Champaign, Urbana, Illinois, 68, USA Ercan M. Dede Toyota
More informationChapter 3: Steady Heat Conduction. Dr Ali Jawarneh Department of Mechanical Engineering Hashemite University
Chapter 3: Steady Heat Conduction Dr Ali Jawarneh Department of Mechanical Engineering Hashemite University Objectives When you finish studying this chapter, you should be able to: Understand the concept
More informationSimulation and Experimental Validation of Induction Heating of MS Tube for Elevated Temperature NDT Application.
Simulation and Experimental Validation of Induction Heating of MS Tube for Elevated Temperature NDT Application. B. Patidar, M.M.Hussain, Sanjoy Das, D Mukherjee, A.P. Tiwari Bhabha Atomic Research Centre,
More informationThermodynamics 1. Lecture 7: Heat transfer Open systems. Bendiks Jan Boersma Thijs Vlugt Theo Woudstra. March 1, 2010.
hermodynamics Lecture 7: Heat transfer Open systems Bendiks Jan Boersma hijs Vlugt heo Woudstra March, 00 Energy echnology Summary lecture 6 Poisson relation efficiency of a two-stroke IC engine (Otto
More informationTESTING THERMOELECTRIC GENERATORS. Introduction. Test Considerations. Application Note n by Thermoelectric Conversion Systems Limited (TCS)
TESTING THERMOELECTRIC GENERATORS Application Note n. 2901 by Thermoelectric Conversion Systems Limited (TCS) Introduction Testing the performance of thermoelectric devices in not straightforward for a
More informationTHERMAL ANALYSIS AND OPTIMIZATION OF THERMAL PAD THICKNESS FOR TRANSISTOR MOUNTING IN FOR CPU S
ISSN Number (online): 2455-4650 THERMAL ANALYSIS AND OPTIMIZATION OF THERMAL PAD THICKNESS FOR TRANSISTOR MOUNTING IN FOR CPU S S. Balakrishnan *, M. Manikandan *Corresponding Author Department of Mechanical
More informationChapter 1: 20, 23, 35, 41, 68, 71, 76, 77, 80, 85, 90, 101, 103 and 104.
Chapter 1: 0, 3, 35, 1, 68, 71, 76, 77, 80, 85, 90, 101, 103 and 10. 1-0 The filament of a 150 W incandescent lamp is 5 cm long and has a diameter of 0.5 mm. The heat flux on the surface of the filament,
More informationTHERMAL ANALYSIS OF A SEALED BATTERY POWER SYSTEM ENCLOSURE FOR UNDERWATER OPERATIONS
THERMAL ANALYSIS OF A SEALED BATTERY POWER SYSTEM ENCLOSURE FOR UNDERWATER OPERATIONS Chiew Hay King Joel School of Engineering, Temasek Polytechnic, Singapore BATTERY POWER SYSTEM To power unmanned underwater
More informationAustralian Journal of Basic and Applied Sciences. Numerical Investigation of Flow Boiling in Double-Layer Microchannel Heat Sink
AENSI Journals Australian Journal of Basic and Applied Sciences ISSN:1991-8178 Journal home page: www.ajbasweb.com Numerical Investigation of Flow Boiling in Double-Layer Microchannel Heat Sink Shugata
More informationNumerical Analysis and Optimization of Thermal Performance of LED Filament Light Bulb
2017 IEEE 67th Electronic Components and echnology Conference Numerical Analysis and Optimization of hermal Performance of LED Filament Light Bulb Jie Liu 1, Chunlin Xu 2, Huai Zheng 1, *, and Sheng Liu
More informationFinite-Element Evaluation of Thermal Response Tests Performed on U-Tube Borehole Heat Exchangers
Excerpt from the Proceedings of the COMSOL Conference 2008 Hannover Finite-Element Evaluation of Thermal Response Tests Performed on U-Tube Borehole Heat Exchangers E. Zanchini,1 and T. Terlizzese 1 1
More informationThermal Management In Microelectronic Circuits
Thermal Management In Microelectronic Circuits Prakash Bhartia*, C.M., Ph.D., F.R.S.C. Natel Engineering Co., Inc. 9340 Owensmouth Avenue Chatsworth, CA 91311-6915 Phone: (818) 734-6500 www.natelengr.com
More informationThermal Interface Material Performance Measurement
Thermal Interface Material Performance Measurement Long Win Science & Technology Co., Ltd. www.longwin.com longwin@longwin.com 886-3-4643221 886-3-4986875 2007/07/16 Contents 1. Introduction Heat Transfer
More informationConduction Heat Transfer. Fourier Law of Heat Conduction. Thermal Resistance Networks. Resistances in Series. x=l Q x+ Dx. insulated x+ Dx.
Conduction Heat Transfer Reading Problems 17-1 17-6 17-35, 17-57, 17-68, 17-81, 17-88, 17-110 18-1 18-2 18-14, 18-20, 18-34, 18-52, 18-80, 18-104 Fourier Law of Heat Conduction insulated x+ Dx x=l Q x+
More informationEYP-DFB TOC03-000x
Version 0.93 2009-05-06 page 1 from 5 General Product Information Product Application 1083 nm DFB Laser with hermetic TO Housing Spectroscopy Monitor Diode, Thermoelectric Cooler and Thermistor He Polarization
More informationq x = k T 1 T 2 Q = k T 1 T / 12
Conductive oss through a Window Pane q T T 1 Examine the simple one-dimensional conduction problem as heat flow through a windowpane. The window glass thickness,, is 1/8 in. If this is the only window
More informationThe application of TIMs in the electronic industry
The application of TIMs in the electronic industry Catalog Application of TIMs Electronic system is m ore integration, the thickness of electr onic product is more and more thin Performance is getting
More informationChapter 9 NATURAL CONVECTION
Heat and Mass Transfer: Fundamentals & Applications Fourth Edition in SI Units Yunus A. Cengel, Afshin J. Ghajar McGraw-Hill, 2011 Chapter 9 NATURAL CONVECTION PM Dr Mazlan Abdul Wahid Universiti Teknologi
More informationheat transfer process where a liquid undergoes a phase change into a vapor (gas)
Two-Phase: Overview Two-Phase two-phase heat transfer describes phenomena where a change of phase (liquid/gas) occurs during and/or due to the heat transfer process two-phase heat transfer generally considers
More informationHeat Removal of a Protection Chip after Surge Pulse Tom Graf Hochschule Luzern T&A Technikumstrasse 21 CH-6048 Horw Switzerland
Heat Removal of a Protection Chip after Surge Pulse Tom Graf Hochschule Luzern T&A Technikumstrasse 21 CH-6048 Horw Switzerland 1 / 23 Abstract EMC protection elements experienced significant heating after
More informationIntroduction to Heat and Mass Transfer. Week 7
Introduction to Heat and Mass Transfer Week 7 Example Solution Technique Using either finite difference method or finite volume method, we end up with a set of simultaneous algebraic equations in terms
More informationSensitivity Estimation of Permanent Magnet Flowmeter
Excerpt from the Proceedings of the COMSOL Conference 2009 Bangalore Sensitivity Estimation of Permanent Magnet Flowmeter Vijay Sharma, S.K.Dash, G.Vijaykumar, B.K.Nashine, B. Krishnakumar, P. Kalyanasundaram,
More informationComparing 2-D Conduction Experiments with Simulation
Comparing 2-D Conduction Experiments with Simulation Introduction Simulation techniques are often used in industry as a beneficial part in the development process whether an engineer or scientist is designing
More information3. LED THERMAL. a) b) 3.1. Introduction Heat transfer introduction LED ACADEMY/LED THERMAL
3. LED THERMAL 3.1. Introduction An LED is an electronic device that lights up when electricity is passed through. They are used as indicators in many devices and increasingly used for other lighting purposes
More information2 Navier-Stokes Equations
1 Integral analysis 1. Water enters a pipe bend horizontally with a uniform velocity, u 1 = 5 m/s. The pipe is bended at 90 so that the water leaves it vertically downwards. The input diameter d 1 = 0.1
More informationThermal Management of Downhole Measuring Tools Using Thermoelectric Cooling; A Numerical and Experimental Investigation
Thermal Management of Downhole Measuring Tools Using Thermoelectric Cooling; A Numerical and Experimental Investigation Weerasinghe S.R.* and Hughes T.P. *Author for correspondence Department of Engineering
More informationThermoelectric Cooling in Downhole Measuring Tools
Thermoelectric Cooling in Downhole Measuring Tools Rohitha Weerasinghe University of the West of England, Bristol, UK ABSTRACT: Thermoelectric cooling is a highly effective and a novel technique used for
More informationPhone: , For Educational Use. SOFTbank E-Book Center, Tehran. Fundamentals of Heat Transfer. René Reyes Mazzoco
8 Fundamentals of Heat Transfer René Reyes Mazzoco Universidad de las Américas Puebla, Cholula, Mexico 1 HEAT TRANSFER MECHANISMS 1.1 Conduction Conduction heat transfer is explained through the molecular
More informationEXPLODED DIAGRAM - PARTS VIEW
Power Supply Sales Model: KSIL018-H216-I 208-230V~ / 1ph / 60Hz EXPLODED DIAGRAM - PARTS VIEW This information is to be used by qualify AC technicians only KSIL1816- Drawing No. D2IL16181301 Above information
More informationME 331 Homework Assignment #6
ME 33 Homework Assignment #6 Problem Statement: ater at 30 o C flows through a long.85 cm diameter tube at a mass flow rate of 0.020 kg/s. Find: The mean velocity (u m ), maximum velocity (u MAX ), and
More informationA NUMERICAL APPROACH FOR ESTIMATING THE ENTROPY GENERATION IN FLAT HEAT PIPES
A NUMERICAL APPROACH FOR ESTIMATING THE ENTROPY GENERATION IN FLAT HEAT PIPES Dr. Mahesh Kumar. P Department of Mechanical Engineering Govt College of Engineering, Kannur Parassinikkadavu (P.O), Kannur,
More informationMitigating Semiconductor Hotspots
Mitigating Semiconductor Hotspots The Heat is On: Thermal Management in Microelectronics February 15, 2007 Seri Lee, Ph.D. (919) 485-5509 slee@nextremethermal.com www.nextremethermal.com 1 Agenda Motivation
More informationExperimental Analysis of Wire Sandwiched Micro Heat Pipes
Experimental Analysis of Wire Sandwiched Micro Heat Pipes Rag, R. L. Department of Mechanical Engineering, John Cox Memorial CSI Institute of Technology, Thiruvananthapuram 695 011, India Abstract Micro
More informationEXPERIMENTAL ANALYSIS OF R-134a FLOW CONDENSATION IN A SMOOTH TUBE
HEFAT2012 9 th International Conference on Heat Transfer, Fluid Mechanics and Thermodynamics 16 18 July 2012 Malta EXPERIMENTAL ANALYSIS OF R-134a FLOW CONDENSATION IN A SMOOTH TUBE Bastos S., Fernández-Seara
More informationThermal engineering with QuickField
Thermal engineering with QuickField Vladimir Podnos Director of marketing and support, Tera Analysis Ltd. Thermal problems in QuickField Sergey Ionin Support engineer, Tera Analysis Ltd. Basics of the
More informationMYcsvtu Notes HEAT TRANSFER BY CONVECTION
www.mycsvtunotes.in HEAT TRANSFER BY CONVECTION CONDUCTION Mechanism of heat transfer through a solid or fluid in the absence any fluid motion. CONVECTION Mechanism of heat transfer through a fluid in
More information