EM Thermal Co-Simulation
|
|
- Giles Nelson
- 6 years ago
- Views:
Transcription
1 CST STUDIO SUITE 2008 Application and Feature Tutorial EM Thermal Co-Simulation Workflow -Material Settings -Boundaries -Losses Examples 1 ube / v1.0 / 14. Sep 2007
2 Steps for EM-Thermal Co- Simulation 1. Choose Template Thermal Cosimulation to activate intersection check 2. Define thermal material properties and boundaries 3. Define E- and H-field monitors for surface and volume losses. 4. Start HF Simulation. 5. Switch to Thermal Problem Class. 6. Define Thermal Sources in CST EMS. Perform the Temperature Simulation. 2
3 Problem Type Thermal only thermal specific sources are shown in iconbar and Solve pulldown menu load loss distribution from other EM Solver 3
4 Problem Type Thermal Only problem type specific items are shown Results are always visible Currently active problemtype 4
5 Thermal Material Properties For any material (incl. background!) the correct thermal conductivity has to be defined. 5
6 Thermal Intersection check For EM Simulation PEC materials always get priority over dielectrics, when overlapping no boolean operation required However, in the thermal solver, both PEC and dielectric are typically type normal (finite thermal conductivity) and have to be intersected. The thermal interaction flag checks, if all objects are properly intersected. This flag has to be activated before EM solver starts. Template is added for conveniance. Objects 6
7 HF-Thermal coupling Thermal material properties and thermal boundary conditions may be changed without deleting HF-results. Exception: Boundary conditions that change the calculation domain (symmetries, open add space) still delete all results. 7 Fahrenheit, Celsius and Kelvin as units are supported
8 Thermal Boundaries and Symmetries In waveguide port planes as well as for magnetic Symmetry Planes, typically adiabatic should be chosen 8
9 Activate CST MWS losses as thermal sources During S-Parameter Simulations MWS monitors are normalized to 1W peak (=0.5 W rms) input power at the port. This factor allows scaling to the real applied input power. Examples: 5 W rms factor = W rms factor = mW rms factor = Applies volume and surface losses calculated by the E and H Fields from CST MWS as thermal sources. (volume loss requires E- or J-monitor, surface loss requires H-monitor) new in 2008: also losses from dispersive dielectrics and dielectric tan(delta) are considered in thermal volume losses
10 CST MWS normalization of result values 1) S-Parameter Simulations: 1W peak input power 2) Eigenmode Simulations: 1J total stored energy in mode 3) plane wave simulations: specified electric field amplitude (peak value) 4) discrete voltage or current port: specified current/voltage amplitude (peak value) simultaneous port excitations / combine results: final norming results by multiplying the given amplitudes with the above scaling (1-4) 10
11 Convection + Radiation losses Convection- and radiation-properties can be assigned to a chain of faces. Internally this is represented by a lossy surface boundary condition, which is temperature dependent. Radiated power: q R = σ (T-T back ) 4 Area with: σ = σ r σ SB σ r : Emissivity
12 Thermal HEX solver Thermal losses caused by electric currents can be used as a driving source for a thermal problem (HF + LF and Stationary currents) Stationary current field Temperature distribution 12
13 Heat Flow source values logfile 13
14 Microwave oven from Delonghi -Food model has a small variation of eps with the temperature -The results show where the food absorbed more EM-energy. - Depending on the field distribution in the cavity the hot spots can be easily identified -We thank Dr. Ruggero Roccari and Dr. Sergio Serena from Delonghi for their work on the test case 14
15 Voxel import including thermal properties Low or High Frequency losses can be used as a heat source. HUGO model automatically has electrical and thermal properties defined. 15
16 Particle Thermal coupling Trajectory Temperature 16 Particles hitting metal produce loss distribution Particles loss distribution can be used as a source for the thermal solver
17 Summary / Outlook Thermal Solver is able to read power sources from: CST MWS Monitor, calculated by T or F hex solver CST MWS - Eigenmode CST EMS - LF solver CST PS - absorbed power by hitting particles simplified user handling (materials / boundaries) near future: transient thermal solver 17
18 Outlook Transient Thermal Simulation Induction Cooker 18
Tracking. Particle In Cell. Wakefield
CST PARTICLE STUDIO STUDIO SOLVERS & APPLICATIONS 1 www.cst.com Mar-09 CST PARTICLE STUDIO Solvers Tracking Simulation of DC Particle Guns, Collectors, Magnets Tracking in static E/H fields (incl. space
More informationSupplementary Information
S1 Supplementary Information S2 Forward Backward Forward Backward Normalized to Normalized to Supplementary Figure 1 Maximum local field ratio and transmission coefficient. Maximum local field ratio (green
More informationCST EM : Examples. Chang-Kyun PARK (Ph. D. St.) Thin Films & Devices (TFD) Lab.
CST Advanced Training 2004 @ Daedeok Convention Town (2004.03.24) CST EM : Examples TM EM Studio TM Chang-Kyun PARK (Ph. D. St.) E-mail: ckpark@ihanyang.ac.kr Thin Films & Devices (TFD) Lab. Dept. of Electrical
More informationTemperature and Heat 4.1. Temperature depends on particle movement Energy flows from warmer to cooler objects. 4.3
Temperature and Heat NEW the BIG idea Heat is a flow of energy due to temperature differences. 4.1 Temperature depends on particle movement. 4.2 Energy flows from warmer to cooler objects. 4.3 The transfer
More informationSimulation of Secondary Electron Emission with CST PARTICLE STUDIO
Simulation of Secondary Electron Emission with CST PARTICLE STUDIO Frank Hamme, Ulrich Becker and Peter Hammes Computer Simulation Technology GmbH, 3 October 2006 Outline CST Particle Studio Secondary
More informationFrequency and time domain analysis of trapped modes in the CERN Proton Synchrotron
Frequency and time domain analysis of trapped modes in the CERN Proton Synchrotron Serena Persichelli CERN Impedance and collective effects BE-ABP-ICE Abstract The term trapped mode refers to a resonance
More informationKey-Holes Magnetron Design and Multiphysics Simulation
Key-Holes Magnetron Design and Multiphysics Simulation A. Leggieri* 1, F. Di Paolo 1, and D. Passi 1 1 Department of Electronic Engineering, University of Rome Tor Vergata, Italy *A. Leggieri: Department
More informationIntermediate Algebra Section 9.1 Composite Functions and Inverse Functions
Intermediate Algebra Section 9. Composite Functions and Inverse Functions We have added, subtracted, multiplied, and divided functions in previous chapters. Another way to combine functions is called composite
More informationElectromagnetics and Electric Machines Stefan Holst, CD-adapco
Electromagnetics and Electric Machines Stefan Holst, CD-adapco Overview Electric machines intro Designing electric machines with SPEED Links to STAR-CCM+ for thermal modeling Electromagnetics in STAR-CCM+
More informationProgress on the Design of a High Power S-Band MTM Microwave Source
Progress on the Design of a High Power S-Band MTM Microwave Source CST PIC Simulations MURI TELECON September 6 th, 2013 Jason S. Hummelt #2 Introduction Outline Metamaterial (MTM) circuit design CST PIC
More informationChapter 22. Induction
Chapter 22 Induction Induced emf A current can be produced by a changing magnetic field First shown in an experiment by Michael Faraday A primary coil is connected to a battery A secondary coil is connected
More informationModeling of a 2D Integrating Cell using CST Microwave Studio
Modeling of a 2D Integrating Cell using CST Microwave Studio Lena Simone Fohrmann, Gerrit Sommer, Alexander Yu. Petrov, Manfred Eich, CST European User Conference 2015 1 Many gases exhibit absorption lines
More informationMultiphysics Simulation of a Monoblock Dielectric Filter
Multiphysics Simulation of a Monoblock Dielectric Filter Theunis Beukman, CST AG Overview Filter device Introduction Synthesis Optimization Multiphysics workflows High ambient temperature High input power
More informationUsing Full Wave Solvers for Practical Analysis of Capacitor Mounting Structures
Using Full Wave Solvers for Practical Analysis of Capacitor Mounting Structures Scott McMorrow, Steve Weir, Teraspeed Consulting Group LLC Fabrizio Zanella, CST of America 1 Outline o MLCC Basics o MLCC
More informationImplementational Aspects of Eigenmode Computation based on Perturbation Theory
Implementational Aspects of Eigenmode Computation based on Perturbation Theory Korinna Brackebusch Prof. Ursula van Rienen University of Rostock 11th International Computational Accelerator Physics Conference
More informationBoundary and Excitation Training February 2003
Boundary and Excitation Training February 2003 1 Why are They Critical? For most practical problems, the solution to Maxwell s equations requires a rigorous matrix approach such as the Finite Element Method
More informationASTRONOMY 161. Introduction to Solar System Astronomy. Class 9
ASTRONOMY 161 Introduction to Solar System Astronomy Class 9 Light Monday, January 29 Look, but don t touch. - Astronomers Motto Light: Key Concepts (1) Visible light is just one form of electromagnetic
More informationStudies of trapped modes in the new extraction septum of the CERN Proton Synchrotron
Studies of trapped modes in the new extraction septum of the CERN Proton Synchrotron Serena Persichelli CERN Impedance and collective effects (BE-ABP-ICE) LIU LHC Injectors Upgrade project Università di
More informationSelf-Inductance. Φ i. Self-induction. = (if flux Φ 1 through 1 loop. Tm Vs A A. Lecture 11-1
Lecture - Self-Inductance As current i through coil increases, magnetic flux through itself increases. This in turn induces back emf in the coil itself When current i is decreasing, emf is induced again
More informationLimitations of the Leap-Frog Scheme
Limitations of the Leap-Frog Scheme 1. Structures with high quality factor (resonators, filter,...): ω Ws frequency stored energy The quality factor Q is defined as Q= = Pv losses long decay time of resonant
More informationLecture 3: Light and Temperature
Lecture 3: Light and Temperature terrestrial radiative cooling Solar radiative warming (Light) Global Temperature atmosphere ocean land Light Temperature Different forms of energy Energy conservation energy,
More informationThermal sensitive foils in physics experiments
Thermal sensitive foils in physics experiments Zdeněk Bochníček, Pavel Konečný Department of Physical Electronics, Faculty of Science, Masaryk University, Kotlarska 2, 611 37 Brno, Czech Republic. E-mail:
More informationGeneral Appendix A Transmission Line Resonance due to Reflections (1-D Cavity Resonances)
A 1 General Appendix A Transmission Line Resonance due to Reflections (1-D Cavity Resonances) 1. Waves Propagating on a Transmission Line General A transmission line is a 1-dimensional medium which can
More informationStudy of Specific Absorption Rate (SAR) in the human head by metamaterial attachment
Study of Specific Absorption Rate (SAR) in the human head by metamaterial attachment M. T Islam 1a), M. R. I. Faruque 2b), and N. Misran 1,2c) 1 Institute of Space Science (ANGKASA), Universiti Kebangsaan
More informationCERN Accelerator School Wakefields. Prof. Dr. Ursula van Rienen, Franziska Reimann University of Rostock
CERN Accelerator School Wakefields Prof. Dr. Ursula van Rienen, Franziska Reimann University of Rostock Contents The Term Wakefield and Some First Examples Basic Concept of Wakefields Basic Definitions
More informationA Polynomial Approximation for the Prediction of Reflected Energy from Pyramidal RF Absorbers
A Polynomial Approximation for the Prediction of Reflected Energy from Pyramidal RF Absorbers Vince Rodriguez and Edwin Barry NSI-MI Technologies Suwanee, GA, USA vrodriguez@nsi-mi.com Abstract Indoor
More informationElectromagnetic-Thermal Analysis Study Based on HFSS-ANSYS Link
Syracuse University SURFACE Electrical Engineering and Computer Science Technical Reports College of Engineering and Computer Science 5-9-2011 Electromagnetic-Thermal Analysis Study Based on HFSS-ANSYS
More informationPHY3128 / PHYM203 (Electronics / Instrumentation) Transmission Lines
Transmission Lines Introduction A transmission line guides energy from one place to another. Optical fibres, waveguides, telephone lines and power cables are all electromagnetic transmission lines. are
More informationChaos Experiments. Steven M. Anlage Renato Mariz de Moraes Tom Antonsen Ed Ott. Physics Department University of Maryland, College Park
Chaos Experiments Steven M. Anlage Renato Mariz de Moraes Tom Antonsen Ed Ott Physics Department University of Maryland, College Park MURI Review Meeting 8 June, 2002 Chaos Experiments Two Approaches Classical
More informationModeling the Effect of Headspace Steam on Microwave Heating Performance of Mashed Potato
Modeling the Effect of Headspace Steam on Microwave Heating Performance of Mashed Potato J. Chen, K. Pitchai, D. Jones, J. Subbiah University of Nebraska Lincoln October 9 th, 2014 Session : Electromagnetic
More informationName Date Class. Electromagnetic Spectrum. Colors
b e n c h m a r k t e s t : p h y s i c a l s c i e n c e Multiple Choice Directions: Use the diagram below to answer question 1. Electromagnetic Spectrum Radio waves A B C D Gamma rays Long Wavelength
More informationPreview of Period 4: Transfer of Thermal Energy
Preview of Period 4: Transfer of Thermal Energy 4.1 Temperature and Thermal Energy How is temperature measured? What temperature scales are used? 4.2 How is Thermal Energy Transferred? How do conduction,
More informationLUMPED EQUIVALENT MODELS OF COMPLEX RF STRUCTURES
LUMPED EQUIVALENT MODELS O COMPLEX R STRUCTURES T lisgen, J Heller, U van Rienen, Universität Rostock, IAE, IE, 1859 Rostock, Germany Abstract The prediction of R properties of complex accelerating structures
More informationElectrical Package Design TKK 2009 Lecture 2
Electrical Package Design TKK 2009 Lecture 2 James E. Morris Dept of Electrical & Computer Engineering Portland State University i Electrical Package Design Lecture topics A: Introduction CMOS; R, L, &
More informationCoupling Impedance of Ferrite Devices Description of Simulation Approach
Coupling Impedance of Ferrite Devices Description of Simulation Approach 09 May 2012 TU Darmstadt Fachbereich 18 Institut Theorie Elektromagnetischer Felder Uwe Niedermayer 1 Content Coupling Impedance
More informationChapter 5 Light and Matter
Chapter 5 Light and Matter Stars and galaxies are too far for us to send a spacecraft or to visit (in our lifetimes). All we can receive from them is light But there is much we can learn (composition,
More informationBeam dynamics studies for PITZ using a 3D full-wave Lienard-Wiechert PP code
Beam dynamics studies for PITZ using a 3D full-wave Lienard-Wiechert PP code Y. Chen, E. Gjonaj, H. De Gersem, T. Weiland TEMF, Technische Universität Darmstadt, Germany DESY-TEMF Collaboration Meeting
More informationA Time Domain Approach to Power Integrity for Printed Circuit Boards
A Time Domain Approach to Power Integrity for Printed Circuit Boards N. L. Mattey 1*, G. Edwards 2 and R. J. Hood 2 1 Electrical & Optical Systems Research Division, Faculty of Engineering, University
More informationElectromagnetic Radiation. Physical Principles of Remote Sensing
Electromagnetic Radiation Physical Principles of Remote Sensing Outline for 4/3/2003 Properties of electromagnetic radiation The electromagnetic spectrum Spectral emissivity Radiant temperature vs. kinematic
More informationTransformers. slide 1
Transformers an alternating emf V1 through the primary coil causes an oscillating magnetic flux through the secondary coil and, hence, an induced emf V2. The induced emf of the secondary coil is delivered
More informationParameter Study and Coupled S-Parameter Calculations of Superconducting RF Cavities
Parameter Study and Coupled S-Parameter Calculations of Superconducting RF Cavities Tomasz Galek, Thomas Flisgen, Korinna Brackebusch, Kai Papke and Ursula van Rienen CST European User Conference 24.05.2012,
More informationChapters 16 Temperature and Heat
Chapters 16 Temperature and Heat 1 Overview of Chapter 16 Temperature and the Zeroth Law of Thermodynamics Temperature Scales Thermal Expansion Heat and Mechanical Work Specific Heat Conduction, Convection,
More informationEM Simulations using the PEEC Method - Case Studies in Power Electronics
EM Simulations using the PEEC Method - Case Studies in Power Electronics Andreas Müsing Swiss Federal Institute of Technology (ETH) Zürich Power Electronic Systems www.pes.ee.ethz.ch 1 Outline Motivation:
More informationReduction of Simulation Times for High-Q Structures Using the Resonance Equation
Progress In Electromagnetics Research M, Vol. 44, 149 160, 2015 Reduction of Simulation Times for High-Q Structures Using the Resonance Equation Thomas Wesley Hall 1, 2, *, Prabhakar Bandaru 2, and Daniel
More informationBernoulli s Principle. Application: Lift. Bernoulli s Principle. Main Points 3/13/15. Demo: Blowing on a sheet of paper
Bernoulli s Principle Demo: Blowing on a sheet of paper Where the speed of a fluid increases, internal pressure in the fluid decreases. Due to continuous flow of a fluid: what goes in must come out! Fluid
More informationB 2 = ɛ o. E o B o. B 2 = 1 µ o. E B. Note that the direction of the vector S gives the direction of propagation of the wave.
Physics 33 : Chapter 31 Examples : Electromagnetic Waves Maxwell s equations relate electric and magnetic fields in fairly complex ways, involving space and time derivatives of each other. Combining these
More informationNovel concept for pulse compression via structured spatial energy distribution
arxiv: [physics.optics] 8 October 013 V. A. amma, A. Figotin, F. Capolino, Novel concept for pulse compression, Oct. 013 Novel concept for pulse compression via structured spatial energy distribution Venkata
More information3D Electromagnetic Field Simulation in Microwave Ovens: a Tool to Control Thermal Runaway
Excerpt from the Proceedings of the COMSOL Conference 010 Paris 3D Electromagnetic Field Simulation in Microwave Ovens: a Tool to Control Thermal Runaway T. Santos 1,,*, L. C. Costa 1,, M. Valente 1,,
More information8.5 - Energy. Energy The property of an object or system that enables it to do work. Energy is measured in Joules (J).
Work Work The process of moving an object by applying a force. Work = Force x displacement. Work is measured in Joules (J) or Newton-meters (Nm). W = Fd Example: To prove his strength, a weightlifter pushes
More informationThermal Analysis & Design Improvement of an Internal Air-Cooled Electric Machine Dr. James R. Dorris Application Specialist, CD-adapco
Thermal Analysis & Design Improvement of an Internal Air-Cooled Electric Machine Dr. James R. Dorris Application Specialist, CD-adapco Thermal Analysis of Electric Machines Motivation Thermal challenges
More informationKeywords: Electric Machines, Rotating Machinery, Stator faults, Fault tolerant control, Field Weakening, Anisotropy, Dual rotor, 3D modeling
Analysis of Electromagnetic Behavior of Permanent Magnetized Electrical Machines in Fault Modes M. U. Hassan 1, R. Nilssen 1, A. Røkke 2 1. Department of Electrical Power Engineering, Norwegian University
More informationElectromagnetics in COMSOL Multiphysics is extended by add-on Modules
AC/DC Module Electromagnetics in COMSOL Multiphysics is extended by add-on Modules 1) Start Here 2) Add Modules based upon your needs 3) Additional Modules extend the physics you can address 4) Interface
More informationCoupled Electromagnetics- Multiphase Porous Media Model for Microwave Combination Heating
Presented at the COMSOL Conference 2008 Boston Coupled Electromagnetics- Multiphase Porous Media Model for Microwave Combination Heating Vineet Rakesh and Ashim Datta Biological & Environmental Engineering
More informationDesign and numerical simulation of thermionic electron gun
Design and numerical simulation of thermionic electron gun M.Hoseinzade 1;1), A.Sadighzadeh 1) Plasma Physics and Nuclear Fusion Research School, Nuclear Science and Technology Research Institute, AEOI,
More informationChapter 18. Temperature, Heat, and the First Law of Thermodynamics Temperature
Chapter 18 Temperature, Heat, and the First Law of Thermodynamics 18.2 Temperature 18.3: The Zeroth aw of Thermodynamics If bodies A and B are each in thermal equilibrium with a third body T, then A and
More informationMCQs E M WAVES. Physics Without Fear.
MCQs E M WAVES Physics Without Fear Electromagnetic Waves At A Glance Ampere s law B. dl = μ 0 I relates magnetic fields due to current sources. Maxwell argued that this law is incomplete as it does not
More informationSerway_ISM_V1 1 Chapter 10. Thermal Physics. it would if filled with the material making up the rest of the object.
Serway_ISM_V1 1 Chapter 10 10 Thermal Physics ANSWERS TO MULTIPLE CHOICE QUESTIONS 1., and the correct response is choice (e). 2. The correct choice is (b). When an object, containing a cavity, is heated,
More informationAnnouncements Self-inductance. Self-inductance. RL Circuit. RL Circuit, cont 3/11/2011. Chapter (not.9-.10) τ = R. Electromagnetic Waves
Chapter 21.8-13(not.9-.10) Electromagnetic Announcements Clicker quizzes NO LONGER GRADED! WebAssign HW Set 8 due this Friday Problems cover material from Chapters 21-22 Office hours: My office hours today
More informationChapter4: Quantum Optical Control
Chapter4: Quantum Optical Control Laser cooling v A P3/ B P / C S / Figure : Figure A shows how an atom is hit with light with momentum k and slows down. Figure B shows atom will absorb light if frequency
More informationAtomic Spectra & Electron Energy Levels
CHM151LL: ATOMIC SPECTRA & ELECTRON ENERGY LEVELS 1 Atomic Spectra & Electron Energy Levels OBJECTIVES: To measure the wavelength of visible light emitted by excited atoms to calculate the energy of that
More informationReview for Final. elementary mechanics. Lagrangian and Hamiltonian Dynamics. oscillations
Review for Final elementary mechanics Newtonian mechanics gravitation dynamics of systems of particles Lagrangian and Hamiltonian Dynamics Lagrangian mechanics Variational dynamics Hamiltonian dynamics
More informationTransformer Modelling Looking Inside to Access the Key Data. Stefan Tenbohlen, University of Stuttgart, Germany
Transformer Modelling Looking Inside to Access the Key Data Stefan Tenbohlen, University of Stuttgart, Germany 1www.ieh.uni www.ieh.uni-stuttgart.de 1. Introduction 2. Winding Modelling by Lumped Elements
More information18.13 Review & Summary
5/2/10 10:04 PM Print this page 18.13 Review & Summary Temperature; Thermometers Temperature is an SI base quantity related to our sense of hot and cold. It is measured with a thermometer, which contains
More informationChapter 14 Temperature and Heat
Chapter 14 Temperature and Heat To understand temperature and temperature scales. To describe thermal expansion and its applications. To explore and solve problems involving heat, phase changes and calorimetry.
More informationMINIMIZING REFLECTION AND FOCUSSING OF INCIDENT WAVE TO ENHANCE ENERGY DEPOSITION IN PHOTODETECTOR S ACTIVE REGION
Progress In Electromagnetics Research, PIER 65, 71 80, 2006 MINIMIZING REFLECTION AND FOCUSSING OF INCIDENT WAVE TO ENHANCE ENERGY DEPOSITION IN PHOTODETECTOR S ACTIVE REGION A. A. Pavel, P. Kirawanich,
More informationLecture 9 Thermal Analysis
Lecture 9 Thermal Analysis 16.0 Release Introduction to ANSYS Mechanical 1 2015 ANSYS, Inc. February 27, 2015 Chapter Overview In this chapter, performing steady-state thermal analyses in Mechanical will
More informationEngineering Electromagnetics
Nathan Ida Engineering Electromagnetics With 821 Illustrations Springer Contents Preface vu Vector Algebra 1 1.1 Introduction 1 1.2 Scalars and Vectors 2 1.3 Products of Vectors 13 1.4 Definition of Fields
More informationELEC Introduction to power and energy systems. The per unit system. Thierry Van Cutsem
ELEC0014 - Introduction to power and energy systems The per unit system Thierry Van Cutsem t.vancutsem@ulg.ac.be www.montefiore.ulg.ac.be/~vct October 2018 1 / 12 Principle The per unit system Principle
More informationASTR-1010: Astronomy I Course Notes Section IV
ASTR-1010: Astronomy I Course Notes Section IV Dr. Donald G. Luttermoser Department of Physics and Astronomy East Tennessee State University Edition 2.0 Abstract These class notes are designed for use
More informationDESY/TEMF Meeting Status 2012
DESY/TEMF Meeting Status 2012 PIC Simulation for the Electron Source of PITZ DESY, Hamburg, 17.12.2012 Ye Chen, Erion Gjonaj, Wolfgang Müller,Thomas Weiland Technische Universität Darmstadt, Computational
More informationIEEE TRANSACTIONS ON PLASMA SCIENCE, VOL. 28, NO. 3, JUNE
IEEE TRANSACTIONS ON PLASMA SCIENCE, VOL. 28, NO. 3, JUNE 2000 841 CTLSS An Advanced Electromagnetic Simulation Tool for Designing High-Power Microwave Sources Simon J. Cooke, Member, IEEE, Alfred A. Mondelli,
More informationAnsoft HFSS 3D Boundary Manager Sources
Lumped Gap Defining s Voltage and Current When you select Source, you may choose from the following source types: Incident wave Voltage drop Current Magnetic bias These sources are available only for driven
More informationApplication of EM- Simulators for Extraction of Line Parameters
Chapter - 2 Application of EM- Simulators for Extraction of Line Parameters 2. 1 Introduction The EM-simulators-2D, 2.5D and 3D, are powerful tools for the analysis of the planar transmission lines structure.
More informationCharge-to-mass ratio for the electron
Charge-to-mass ratio for the electron Introduction This is a variation of the original experiment carried out by J.J.Thomson in 1895. The deflection of a charge moving in a magnetic field is clearly demonstrated.
More informationAir Force Research Laboratory
Air Force Research Laboratory Materials with Engineered Dispersion for the Enhancement of Light-Matter Interactions 10 January 2013 Ilya Vitebskiy, AFRL/RYDP Integrity Service Excellence SUBTOPIC 1 Nonreciprocal
More informationMathematical Modelling Using SimScape (Electrical Systems)
Experiment Three Mathematical Modelling Using SimScape (Electrical Systems) Control Systems Laboratory Dr. Zaer Abo Hammour Dr. Zaer Abo Hammour Control Systems Laboratory 1. Model and simulate MultiDomain
More informationChapter 18 Temperature, Heat, and the First Law of Thermodynamics. Thermodynamics and Statistical Physics
Chapter 18 Temperature, Heat, and the First Law of Thermodynamics Thermodynamics and Statistical Physics Key contents: Temperature scales Thermal expansion Temperature and heat, specific heat Heat and
More informationProblem Solver Skill 5. Defines multiple or complex problems and brainstorms a variety of solutions
Motion and Forces Broad Concept: Newton s laws of motion and gravitation describe and predict the motion of most objects. LS 1.1 Compare and contrast vector quantities (such as, displacement, velocity,
More informationCambridge International Examinations Cambridge International Advanced Level *6106210292* PHYSICS 9702/42 Paper 4 A2 Structured Questions May/June 2014 2 hours Candidates answer on the Question Paper. No
More informationTutorial Number 18: Heat transfer analysis of a teapot
Tutorial Number 18: Heat transfer analysis of a teapot Stefano Morlacchi September 2014 T. 01608 811777 F. 01608811770 E.info@ssanalysis.co.uk W. www.ssanalysis.co.uk 1. Introduction In this tutorial,
More informationThermal Radiation Heat Transfer Mechanisms
18-6 Heat Transfer Mechanisms Thermal Radiation Radiation is an energy transfer via the emission of electromagnetic energy. The rate P rad at which an object emits energy via thermal radiation is Here
More informationSimulation of Electron Behavior in PIG Ion Source for 9 MeV Cyclotron X. J. Mu 1, M. Ghergherehchi 1a, Y.H. Yeon 1, J.S. Chai 1
Simulation of Electron Behavior in PIG Ion Source for 9 MeV Cyclotron X. J. Mu 1, M. Ghergherehchi 1a, Y.H. Yeon 1, J.S. Chai 1 1 College of the Electric and Electrical Engineering, Sungkyunkwan University,
More informationSub-wavelength electromagnetic structures
Sub-wavelength electromagnetic structures Shanhui Fan, Z. Ruan, L. Verselegers, P. Catrysse, Z. Yu, J. Shin, J. T. Shen, G. Veronis Ginzton Laboratory, Stanford University http://www.stanford.edu/group/fan
More informationSri Lankan School Muscat
Sri Lankan School Muscat Withdrawal Examination 2015/2016 Class : Subject : Paper : Duration: Year 11B/R Physics Name :... 1 2 Hours Q.No. Allocated 1 11 2 12 3 12 4 10 5 06 6 08 7 06 8 12 9 10 10 04 11
More informationChapter 16 Temperature and Heat
Chapter 16 Temperature and Heat Temperature and the Zeroth Law of Thermodynamics Temperature Scales Thermal Expansion Heat and Mechanical Work Specific Heats Conduction, Convection, and Radiation 16-1
More informationINTRODUCTION TO TRANSMISSION LINES DR. FARID FARAHMAND FALL 2012
INTRODUCTION TO TRANSMISSION LINES DR. FARID FARAHMAND FALL 2012 http://www.empowermentresources.com/stop_cointelpro/electromagnetic_warfare.htm RF Design In RF circuits RF energy has to be transported
More information1. How much heat was needed to raise the bullet to its final temperature?
Name: Date: Use the following to answer question 1: A 0.0500-kg lead bullet of volume 5.00 10 6 m 3 at 20.0 C hits a block that is made of an ideal thermal insulator and comes to rest at its center. At
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.02 Spring 2003 Experiment 17: RLC Circuit (modified 4/15/2003) OBJECTIVES
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8. Spring 3 Experiment 7: R Circuit (modified 4/5/3) OBJECTIVES. To observe electrical oscillations, measure their frequencies, and verify energy
More informationUNIT I ELECTROSTATIC FIELDS
UNIT I ELECTROSTATIC FIELDS 1) Define electric potential and potential difference. 2) Name few applications of gauss law in electrostatics. 3) State point form of Ohm s Law. 4) State Divergence Theorem.
More informationAutomatic Differential Lift-Off Compensation (AD-LOC) Method In Pulsed Eddy Current Inspection
17th World Conference on Nondestructive Testing, 25-28 Oct 2008, Shanghai, China Automatic Differential Lift-Off Compensation (AD-LOC) Method In Pulsed Eddy Current Inspection Joanna X. QIAO, John P. HANSEN,
More informationFinite Element Method based investigation of IPMSM losses
Finite Element Method based investigation of IPMSM losses Martin Schmidtner 1, Prof. Dr. -Ing. Carsten Markgraf 1, Prof. Dr. -Ing. Alexander Frey 1 1. Augsburg University of Applied Sciences, Augsburg,
More informationChapter 31 Electromagnetic Oscillations and Alternating Current LC Oscillations, Qualitatively
Chapter 3 Electromagnetic Oscillations and Alternating Current LC Oscillations, Qualitatively In the LC circuit the charge, current, and potential difference vary sinusoidally (with period T and angular
More informationTransmission Lines. Plane wave propagating in air Y unguided wave propagation. Transmission lines / waveguides Y. guided wave propagation
Transmission Lines Transmission lines and waveguides may be defined as devices used to guide energy from one point to another (from a source to a load). Transmission lines can consist of a set of conductors,
More informationChapter 14 Heat and Temperature Notes
Chapter 14 Heat and Temperature Notes Section 1: Temperature The degree of or of an object. Related to the of an object s atoms or molecules What makes something hot? o Particles that make up o They have
More informationTRANSFORMERS B O O K P G
TRANSFORMERS B O O K P G. 4 4 4-449 REVIEW The RMS equivalent current is defined as the dc that will provide the same power in the resistor as the ac does on average P average = I 2 RMS R = 1 2 I 0 2 R=
More informationChapter 16 Temperature and Heat
Chapter 16 Temperature and Heat 16-1 Temperature and the Zeroth Law of Thermodynamics Definition of heat: Heat is the energy transferred between objects because of a temperature difference. Objects are
More informationLecture 12. Microwave Networks and Scattering Parameters
Lecture Microwave Networs and cattering Parameters Optional Reading: teer ection 6.3 to 6.6 Pozar ection 4.3 ElecEng4FJ4 LECTURE : MICROWAE NETWORK AND -PARAMETER Microwave Networs: oltages and Currents
More informationName... Class... Date...
Radiation and temperature Specification reference: P6.3 Black body radiation (physics only) Aims This is an activity that has been designed to help you improve your literacy skills. In this activity you
More informationECE 546 Lecture 07 Multiconductors
ECE 546 Lecture 07 Multiconductors Spring 2018 Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jesa@illinois.edu ECE 546 Jose Schutt Aine 1 TELGRAPHER S EQUATION FOR N COUPLED
More informationGeneral Physics (PHY 2140)
General Physics (PHY 2140) Lecture 12 Electricity and Magnetism 1. AC circuits and EM waves The Electromagnetic Spectrum The Doppler Effect 6/20/2007 Modern Physics 1. Relativity Galilean Relativity Speed
More information