Variable Structure Control ~ Motor Control

Similar documents
Overview Electrical Machines and Drives

Lecture 23: Newton-Euler Formulation. Vaibhav Srivastava

Parks Equations Generalised Machines. Represent ac machines in the simplest possible way.

Electric Machinery and Apparatus 1 AE1B14SP1. Miroslav Chomát room B3-248

ENGI9496 Lecture Notes Multiport Models in Mechanics

NMT EE 589 & UNM ME 482/582 ROBOT ENGINEERING. Dr. Stephen Bruder NMT EE 589 & UNM ME 482/582

ECE 422 Power System Operations & Planning 2 Synchronous Machine Modeling

10/23/2003 PHY Lecture 14R 1

Spin-rotation coupling of the angularly accelerated rigid body

From now, we ignore the superbar - with variables in per unit. ψ ψ. l ad ad ad ψ. ψ ψ ψ

Dynamics of the synchronous machine

ECE 522 Power Systems Analysis II 2 Power System Modeling

Synchronous Machine Modeling

PHYS 705: Classical Mechanics. Newtonian Mechanics

Chapter 11 Angular Momentum

Modeling of Dynamic Systems

Step Motor Modeling. Step Motor Modeling K. Craig 1

Study Guide For Exam Two

The classical spin-rotation coupling

Mechanics Physics 151

JRE SCHOOL OF Engineering

ECE 692 Advanced Topics on Power System Stability 2 Power System Modeling

Rotational Dynamics. Physics 1425 Lecture 19. Michael Fowler, UVa

INDUCTION MOTOR MODEL AND PARAMETERS

EE 742 Chapter 3: Power System in the Steady State. Y. Baghzouz

coordinates. Then, the position vectors are described by

Physics 5153 Classical Mechanics. D Alembert s Principle and The Lagrangian-1

Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science Electric Machines

Chapter 4. Synchronous Generators. Basic Topology

( ) = : a torque vector composed of shoulder torque and elbow torque, corresponding to

11. Dynamics in Rotating Frames of Reference

The synchronous machine (detailed model)

A particle in a state of uniform motion remain in that state of motion unless acted upon by external force.

CHAPTER 10 ROTATIONAL MOTION

Integrals and Invariants of Euler-Lagrange Equations

ECE 422/522 Power System Operations & Planning/ Power Systems Analysis II 2 Synchronous Machine Modeling

Lecture 9: Space-Vector Models

Angular Momentum and Fixed Axis Rotation. 8.01t Nov 10, 2004

Lecture 1: Induction Motor

The POG Modeling Technique Applied to Electrical Systems

Physics 181. Particle Systems

Dynamics of the synchronous machine

Modelling of Closed Loop Speed Control for Pmsm Drive

Iterative General Dynamic Model for Serial-Link Manipulators

Simulations and Control of Direct Driven Permanent Magnet Synchronous Generator

Modelling of Permanent Magnet Synchronous Motor Incorporating Core-loss

A NUMERICAL COMPARISON OF LANGRANGE AND KANE S METHODS OF AN ARM SEGMENT

Notes on Analytical Dynamics

Calculation of Coherent Synchrotron Radiation in General Particle Tracer

2014 Texas Instruments Motor Control Training Series. -V th. Dave Wilson

Analytical classical dynamics

Motor Info on the WWW Motorola Motors DC motor» /MOTORDCTUT.

10/9/2003 PHY Lecture 11 1

Mechanics Physics 151

REAL TIME CONTROL OF DOUBLY FED INDUCTION GENERATOR. Benmeziane Meriem, Zebirate Soraya, Chaker Abelkader Laboratory SCAMRE, ENPO, Oran, Algeria

Chapter 5 Three phase induction machine (1) Shengnan Li

PARAMETER SENSITIVITY ANALYSIS OF AN INDUCTION MOTOR

Modeling And Simulation Of All-electric Aircraft Power Generation And Actuation

Key component in Operational Amplifiers

Solutions to Practice Problems

Modeling Free Acceleration of a Salient Synchronous Machine Using Two-Axis Theory

INVESTIGATION OF A COMPUTER MODEL OF THREE-PHASE MOTOR REGULATED BY FREQUENCY MODE

I 2 V V. = 0 write 1 loop equation for each loop with a voltage not in the current set of equations. or I using Ohm s Law V 1 5.

MEEM 3700 Mechanical Vibrations

Mathematical Modeling and Dynamic Simulation of a Class of Drive Systems with Permanent Magnet Synchronous Motors

Dynamic Modeling of a Synchronous Generator Using T-S Fuzzy Approach

Mechanics Physics 151

TORQUE-SPEED ADAPTIVE OBSERVER AND INERTIA IDENTIFICATION WITHOUT CURRENT TRANSDUCERS FOR CONTROL OF ELECTRIC DRIVES

High-Order Hamilton s Principle and the Hamilton s Principle of High-Order Lagrangian Function

An adaptive sliding mode control scheme for induction motor drives

τ rf = Iα I point = mr 2 L35 F 11/14/14 a*er lecture 1

1.050 Content overview Engineering Mechanics I Content overview. Outline and goals. Lecture 28

The Feynman path integral

Tensor Analysis. For orthogonal curvilinear coordinates, ˆ ˆ (98) Expanding the derivative, we have, ˆ. h q. . h q h q

The Analysis of Coriolis Effect on a Robot Manipulator

Behaviour of synchronous machine during a short-circuit (a simple example of electromagnetic transients)

Physics 443, Solutions to PS 7

Lagrange Multipliers. A Somewhat Silly Example. Monday, 25 September 2013

A Status Review OF IPM MOTOR DRIVES FOR ELECTRIC SUBMERSIBLE PUMP IN HARSH COLD OCEANS

Field and Wave Electromagnetic. Chapter.4

A new FOC technique based on predictive current control for PMSM drive

C/CS/Phy191 Problem Set 3 Solutions Out: Oct 1, 2008., where ( 00. ), so the overall state of the system is ) ( ( ( ( 00 ± 11 ), Φ ± = 1

SUPPLEMENTARY INFORMATION

> To construct a potential representation of E and B, you need a vector potential A r, t scalar potential ϕ ( F,t).

Week 11: Chapter 11. The Vector Product. The Vector Product Defined. The Vector Product and Torque. More About the Vector Product

2016 Kappa Electronics Motor Control Training Series Kappa Electronics LLC. -V th. Dave Wilson Co-Owner Kappa Electronics.

PHYSICS - CLUTCH CH 28: INDUCTION AND INDUCTANCE.

Generation, transmission and distribution, as well as power supplied to industrial and commercial customers uses a 3 phase system.

Experimental Determination of Mechanical Parameters in Sensorless Vector-Controlled Induction Motor Drive

Parameter Estimation of Three Phase Squirrel Cage Induction Motor

Modeling and simulation aspects of AC machines

EML 5223 Structural Dynamics HW 10. Gun Lee(UFID )

Zero speed sensorless drive capability of fractional slot inset PM machine

MEM 255 Introduction to Control Systems Review: Basics of Linear Algebra

Modeling and analysis of parallel connected permanent magnet synchronous generators in a small hydropower plant

-magnetic dipoles are largely analogous to electric dipole moments -both types of dipoles

A single-plane rotating imbalance experiment

2014 Texas Instruments Motor Control Training Series. -V th. Dave Wilson

Lecture 6: Control of Three-Phase Inverters

ROBUSTNESS OF THE DIRECT TORQUE CONTROL OF DOUBLE STAR INDUCTION MOTOR IN FAULT CONDITION

Transcription:

Varable Structure Control ~ Motor Control Harry G. Kwatny Department of Mechancal Engneerng & Mechancs Drexel Unversty

Outlne Moels of ac Motors Synchronous motors Inucton motors Brushless c motors VS Control formulaton Ajustable spee synchronous motor Poston control of brushless c motor

Nomenclature (3 phase synchronous motor) θ rotor angle n nertal frame ω rotor angular velocty v,, q fel wnng voltage, current, charge q = t f f f f f v,, q, j = 1,2,3 stator wnng voltage, current, charge τ M M J R j j j, j ff ( q), mechancal torque (loa) nerta matrx n neral frame nerta matrx n rotatng (Blonel) frame mechancal rotatng nerta sspaton matrx,, j = 1,2,3 stator nuctances - self ( = j) an mutual ( j) fel wnng self nuctance f, = 1,2,3 fel/stator wnng mutual nuctance

Lagrange Equatons L L = Q, L q, q = q, q U q t q q = θ 1 2 3 f q q q q q q = ω 1 2 3 f q generalze coornates L Lagrangan ( ) ( ) ( ) 1 ( ) = 2 M ( ) U( q) = knetc energy, q, q q q q U potental energy, 0 Q generalze force Q= D qwhere ( ) 1 D potental functon Dqq, = 2 qrq + τ v1 v2 v3 vf q

Synchronous Motor J 0 0 0 0 0 L1 L3 L3 L5cosθ 2π 0 L3 L1 L3 L5cos θ 3 M ( q) = 2π 0 L3 L3 L1 L5cos θ + 3 2π 2π 0 L5cosθ L5cos θ L5cos θ + ff 3 3 2π 2π = L1, j = L3, f 1 = L5cos θ, f 2 = L5cos θ, f 3 = L5cos θ + 3 3 R= ag rrrr ( 0,,,, )

ransform to Rotatng Frame,,,, v, v, v v, v, v 1 2 3 q 0 1 2 3 q 0 2π 2π cosθ cos θ cos θ + 3 3 1 2 2 2 π π q = B 2, B= snθ sn θ sn θ + 3 3 3 0 3 1 1 1 2 2 2 J 0 0 0 0 ω 0 0 Lff 0 0 ω τ 0 Ls 0 0 L f 0 r ωl 0 0 s v 0 0 Ls 0 0 q= L f f ω L s r 0 0 q+ v q t 0 0 0 L0 0 0 0 0 0 r 0 0 v0 0 Lf 0 0 L f f 0 0 0 0 r f f vf 3 Ls : = L1+ L3, L0 = L1 2 L3, Lf = Lff 2

Synchronous ~ spee control We want to esgn a spee controller that mantans a esre spee, ω 1 1) ω ω exponentally: y1 = ω+ λ( ω ω) = { Lff q τ} + λ( ω ω), λ > 0 J 2) zero -axs current: y = 2 3 0 0 () 3) balance operaton: y χ, χ v t t 4) constant fel current: y4 = f Proceure: - reuce to regular form, - check zero ynamcs - esgn slng surfaces, - esgn reachng controller, - smulate = = f t

Synchronous ~ spee control Now, we have the system n the form: ( ) ( ) x = f x + G x v [ ω θ χ] ( ) [ ] Reuce to normal form 1 2 3 4 1 2 3 4 ( ) ( ) r = 1, r = 1, r = 1, r = 1 z x = h x an m zeroynamcs = 3 In fact zero ynamcs are: r ω = λω, 0 = L B x = vb = v vq v0 vf y = h x y = y y y y 0 0, θ = ω Note that slng ynamcs are the zero ynamcs! ( ) he stanar choce for K k = 1, = 1,2,3,4 s z = z

Synchronous ~ spee control Now, set up V = sqs= zqz V = 2zQz ( ) ( ) Furthermore, snce z = h x h x z = x = H( x) f ( x) + H( x) G( x) v x z = H x f x + H x G x B x v ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) { } V = 2zQz= 2h xqh x f x + H x G x B x v ( *) * ( ) ( ) v = Vmax, sgn s, s x = HGB Qh x, B

Synchronous ~ spee control

Synchronous ~ spee control

Inucton Motor he nucton motor has two fel ω ω τ wnngs. hey are v close crcuts so that q q the fel currents are vq M = C + 0 nuce as the cols t 0 v0 move through the f1 f1 0 stator fel. f 2 f 2 0 J 0 0 0 0 0 0 Lff 2 Lff 1 0 0 0 0 Ls 0 0 Lf 0 Lff 2 r ωl 0 0 0 s 0 0 Ls 0 0 Lf Lff 1 ωls r 0 0 0 M =, C = 0 0 0 L0 0 0 0 0 0 r 0 0 0 Lf 0 0 Lf 0 0 0 0 0 rf 0 0 0 Lf 0 0 Lf 0 0 0 0 0 rf = L ( ) f f q f 1 2

Inucton Motor Nomenclature ω rotor angular velocty v f fel wnng voltage v, =1,2,3 stator wnng voltages v a, a=,q,0 stator Blonel voltages f, =1,2 fel wnng currents,, =1,2,3 stator wnng currents a, a=,q,0 stator Blonel currents τ mechancal torque (loa) electrcal torque J mechancal rotatng nerta r,r f stator an fel wnng resstances L s stator & q axs nuctances L 0 stator zero sequence axs nuctance L f fel wnng self nuctance fel/stator mutual nuctance L f

Inucton Motor Spee Control Agan, we wsh to regulate spee ω to the esre value ω. Defne χψ, : χ = v0 ψ = rotor flux magntue, Choose ψ = ψ + ψ, ψ = L + L, ψ = L + L 2 2 1 2 1 f f f 2 f q f f ( q f1 f2 ) ( ω q f1 f2 χ) ( q f f ) y = h ω,,,,,, χ : = ω ω 1 1 0 y = h,,,,,, : = χ 2 2 0 1 2 r = 2, r = 1, r = 2 1 2 3 z ( 1 ω ω0 ) z L + L τ 2 f f 2 f f 1 q z χ 3 = y3 = h3 ω,,, 0,,, χ : = ψ ψ 1 2 z ( 4 ψ ψ0) z rψ rψ 5 f 1 f1 f 2 f 2

2-m Zero Dynamcs {(Ψ 1,Ψ 2 ) Ψ 1 2 +Ψ2 2 = Ψ0 2 } 0 zero ynamcs manfol R S 1

Brushless c Motor In the brushless c motor, the fel cols are replace by permanent magnets; thereby removng one coornate: [ θ 1 2 3] [ ω ] q= q q q q = 1 2 3 3 J 0 0 0 ω 0 0 2 k 0 e ω τ 0 Ls 0 0 0 r ωls 0 v = + 0 0 Ls 0 t q 3 2ke ωls r 0 q vq 0 0 0 L0 0 0 0 0 r 0 v0 = 3 2 k e q

Brushless c ~2 t ω 1 0 ( ( ) ) q τ 0 θ J ω 1 v ( r Lsqω ) L L 3 s = s +, ( ) = k 2 1 v q e q ( ( 32 ) ω) q q rq + Ls ke Ls L 0 s v 0 1 r L 0 0 L0

Brushless c ~ poston control We want to esgn a poston controller that mantans a esre poston, θ 1 3 0 ( ) 1) θ θ exponentally: y = ω+ λ θ θ, λ > 0 2) constant stator current: y = + I or zero -axs: y = 3) balance operaton: y = 2 2 2 2 q s 2 Proceure: - reuce to regular form, - check zero ynamcs - esgn slng surfaces, - esgn reachng controller, - smulate

Brushless c ~ poston control ( θω,,,, ): ( ) q ω λθ θ y = h = + 1 1 0 ( θω ) y = h,,,, : = + I 2 2 2 2 2 q 0 q s ( θω ) y = h,,,, : = 3 3 q 0 0 he zero ynamcs are: θ = λ θ θ ( ) r = 1, r = 1, r = 1 1 2 3 z 1 2 3 0 ( ) z = + I z = ω + λ θ θ = 2 2 2 q s