Maxwell 3D Transient.

Slides:



Advertisements
Similar presentations
ENERGY CONVERSION ONE (Course 25741)
Advertisements

Capacitive Micromotor
CHAPTER 5: TRANSFORMER AND MUTUAL INDUCTANCE
© 2007 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 23 Physics, 4 th Edition James S. Walker.
Electromagnetic Analysis of a 2 Gap Solenoid
Magnetic Circuits and Transformers
3. ARMATURE VOLTAGE AND GOVERING EQUATIONS
ELECTRIC DRIVES Ion Boldea S.A.Nasar 1998 Electric Drives.
Walker, Chapter 23 Magnetic Flux and Faraday’s Law of Induction
Chapter 6 Workshop 5 Solid Conductor.
Chapter 1 Introduction. Training Manual Electromagnetic Analysis in Workbench March 4, 2005 Inventory # A. Feature Overview Workbench EMAG features.
ET 332a Dc Motors, Generators and Energy Conversion Devices 1.
AP Physics C Montwood High School R. Casao
Lesson 6: Electromagnetic Induction and Magnetic Forces
Inductors Chap 11.
The Electromagnetic Field. Maxwell Equations Constitutive Equations.
Electromagnetic Induction
DC motor model ETEC6419. Motors of Models There are many different models of DC motors that use differential equations. During this set of slides we will.
Magnetically coupled circuits
Elec467 Power Machines & Transformers
Transient Analysis - First Order Circuits
Chapter 5 Overview. Electric vs Magnetic Comparison.
Lecture 18-1 Ways to Change Magnetic Flux Changing the magnitude of the field within a conducting loop (or coil). Changing the area of the loop (or coil)
Fundamentals of Electromagnetics and Electromechanics
ELECTROMAGNETIC THEORY EKT 241/4: ELECTROMAGNETIC THEORY PREPARED BY: NORDIANA MOHAMAD SAAID CHAPTER 4 – MAGNETOSTATICS.
Chapter 6 DC Machines EET103/4.
Day 3: Eddy Currents Back EMF in Motors Eddy Currents Nature of Eddy Currents.
Chapter 31 Faraday’s Law Electricity generator, or from B to E. 1.Battery  Chemical emf 2.Motional emf 3.Faraday’s Law of Induction 4.Lentz Law about.
Magnetic Flux and Faraday’s Law of Induction
Faraday’s Law and Inductance. Faraday’s Law A moving magnet can exert a force on a stationary charge. Faraday’s Law of Induction Induced emf is directly.
EET 221 Synchronous Machines Rafiqi.
DC Motor Speed Modeling in Simulink
1 MAGNETOSTATIC FIELD (MAGNETIC FORCE, MAGNETIC MATERIAL AND INDUCTANCE) CHAPTER FORCE ON A MOVING POINT CHARGE 8.2 FORCE ON A FILAMENTARY CURRENT.
Chapter 30 Induction and Inductance. 30.2: First Experiment: 1. A current appears only if there is relative motion between the loop and the magnet (one.
Magnetic field due to an electric current
ECE 576 – Power System Dynamics and Stability Prof. Tom Overbye Dept. of Electrical and Computer Engineering University of Illinois at Urbana-Champaign.
5. Magnetostatics Applied EM by Ulaby, Michielssen and Ravaioli.
1 ELECTRICAL TECHNOLOGY EET 103/4 Define and analyze the principle of transformer, its parameters and structure. Describe and analyze Ideal transformer,
BASIC ELECTRICAL TECHNOLOGY DET 211/3
Right-hand Rule 2 gives direction of Force on a moving positive charge Right-Hand Rule Right-hand Rule 1 gives direction of Magnetic Field due to current.
Maxwell 2D Boundaries/Sources, Meshing, and Post Processing.
AC Machines. BOOSTER Basic Function:- -Sometimes when we use electrical power we need different voltage level to main supply. It is provided by Booster.
Chapter 5 Armature Gap Sweep Workshop 4. Training Manual Electromagnetic Analysis in Workbench March 4, 2005 Inventory # Workshop #2: Armature.
Example Problem #2 Maxwell 2D Hall Sensor. T7_3D, pg. 2 7/21/02 Hall Sensor Description: The Hall sensor works similarly to the vr sensor, except that.
2D Transient Overview. 4/20/04, pg. 2 2D Transient  Introduction and Theory  Source Types  Source Waveforms  Time-varying materials  Solution Setup.
Example Problem #3 Maxwell 2D Hall Sensor: Rotational Motion using Parametrics.
A Field Construction Technique to Efficiently Model the Dynamic Vector Forces within Induction Machines Dezheng Wu, Steve Pekarek School of Electrical.
ANSYS Workbench 9.0 Electromagnetics Paul Lethbridge
THERMO-STRUCTURAL ANALYSIS
CAPACITANCE AND INDUCTANCE
Inductance and Capacitance Response of First Order RL and RC
Fundamentals of Applied Electromagnetics
Peter Uzunov Associate professor , PhD Bulgaria, Gabrovo , 5300 , Stramnina str. 2 s:
PExprt Modeling Procedure
Eddy Current A current induced in a solid conducting object, due to motion of the object in an external magnetic field. The presence of eddy current in.
Overview of Electrical Engineering
Maxwell 2D Control Panel, Modeler, and Material Manager
Electromagnetic Theory
ENFORCED MOTION IN TRANSIENT ANALYSIS

ENE/EIE 325 Electromagnetic Fields and Waves
6. Maxwell’s Equations In Time-Varying Fields
Induction and Inductance
6. Maxwell’s Equations In Time-Varying Fields
Circuits, cont. Calculating the current in the circuit is called circuit analysis Two types of circuits: DC stands for direct current The current is of.
6. Maxwell’s Equations In Time-Varying Fields
6. Maxwell’s Equations In Time-Varying Fields
5. Magnetostatics 7e Applied EM by Ulaby and Ravaioli.
Electric Machine Design Course
Presentation transcript:

Maxwell 3D Transient

Overview Transient solver computes magnetic fields in the time-domain (instantaneously at each time step) Formulation is based on a current vector potential in solid conductors, and a scalar potential over the entire field domain Field equations are strongly coupled with circuit equations to allow voltage sources and/or external driving circuits Quantity solved is the magnetic field (H) and the current density (J) while magnetic flux density (B) is automatically calculated from the H-field Derived quantities are forces, torques, energy, and inductance

Overview (cont.) Non-linear behavior of magnetic materials is considered Permanent magnets are considered Excitations can be sinusoidal or non-sinusoidal including: Currents and current densities in conductors Voltages and currents applied to windings Permanent magnets Two types of conductors can be considered: Solid: eddy currents are considered Stranded: eddy currents are neglected

Boundaries Thin, perfectly insulating sheets between touching conductors. Same as Neumann, except that current cannot cross the boundary. Insulating Notes: No Balloon Boundary available Planes of symmetry in periodic structures where H is oblique to the boundary. The H-field on the slave boundary is forced to match the magnitude and direction (or the negative of the direction) of the H-field on the master boundary. Matching (Master and Slave) Planes of geometric and magnetic symmetry. Field behaves as follows: Odd Symmetry (Flux Tangential) — H is tangential to the boundary; its normal components are zero. Even Symmetry (Flux Normal) — H is normal to the boundary; its tangential components are zero. Symmetry Ordinary field behavior. Initially, object interfaces are natural boundaries; outer boundaries and excluded objects are Neumann boundaries. Natural boundaries — H is continuous across the boundary. Neumann boundaries — H is tangential to the boundary and flux cannot cross it. Default Boundary Conditions (Natural and Neumann) Used to model… H-Field Behavior Boundary Type

Sources The current density in a conductor. Current Density and Current Density Terminal The terminal (sheet object) for a conductor. Current The terminal (sheet object) for a winding. Coil Terminal Type of Excitation Source The terminal (sheet object) for a current density source. Note: In addition, permanent magnets serve as sources of magnetic fields

Overview of Sources Schematic Option

Source Details A DC “current” (solid or stranded) can be assigned to a terminal A “current density” can be assigned to a 3D object while “current density terminal” is assigned to the 2D sheet object inside of that object Coil terminals allow for the most sources including: voltages, currents, external circuits, or sources which vary with time Coil terminals will automatically report flux linkage and induced voltage plots vs. time under Post Process/ Transient Data For a coil terminal, “Model/Winding Setup” must be used to complete the source setup

Winding Setup Use “Model/ Winding Setup to group windings and assign sources To group coil or conductor terminals, select a terminal from the Coil/Conductor list on the left, and choose Group. To ungroup terminals, select a winding group from the Winding list on the right, and choose Ungroup.

Winding Setup (cont.) Select the winding from the Winding list. To assign a source to a winding: Select the winding from the Winding list. Select the type of source you want to assign: Current, Voltage, or External. Select either Strand or Solid. Enter in extra parameters, such as total turns. For a current or voltage source, you can assign a function. If you want to assign a function, do the following: 1) Choose Function to open the Function window 2) Select or define a function and then choose Done 3) Choose Assign. The source information appears in the Winding list next to the winding name. Choose Assign and Exit to complete winding setup

External Circuits Step 1: Step 3: Edit / Edit External Circuit and launch Schematic Capture Step 3: When exiting Schematic editor specify sources to be either: time, position, or speed dependent Step 2: In Schematic editor each winding appears as inductor symbol

Finalizing Source Setup Completed sources appear in list box in left side window

Setup Solution Options The mesh must be manually created for all transient projects, unless the project is copied from a previously solved Magnetostatic or Eddy Current project Set the Stop time and Time Step appropriately for the simulation (~20 timesteps per cycle)

Setup Solution Options (cont.) Choose Save fields time step for post processing a particular timestep later to create plots After solving at least one timestep, a post processing macro can be created. Select this macro by checking Use Macro and specifying the macro. Any quantities that are written using the Append button in the calculator will appear under Solutions > Transient Data as a new .dat plot file

Setup Solution – Motion Setup Choose Set Band to specify the band object Switch the moving and stationary objects by clicking on Switch Moving Objects

Setup Solution – Motion Setup Specify Rotational or Translation motion Set Anchor Point and End Point for motion Set Positive and Negative limits for motion

Setup Solution – Mechanical Setup For constant velocity, uncheck Consider Mechanical Transient For varying velocity check Consider Mechanical Transient and input: Initial Velocity Moment of Inertia Damping Load