Speed Control of Brushless DC Motor Using Proportional Integral Controller

Similar documents
Determination of the Sampling Period Required for a Fast Dynamic Response of DC-Motors

Lecture -14: Chopper fed DC Drives

Introduction to AC Power, RMS RMS. ECE 2210 AC Power p1. Use RMS in power calculations. AC Power P =? DC Power P =. V I = R =. I 2 R. V p.

copper ring magnetic field

Principle and Analysis of a Novel Linear Synchronous Motor with Half-Wave Rectified Self Excitation

Silicon Controlled Rectifiers UNIT-1

Basic Circuit Elements Professor J R Lucas November 2001

Hall effect. Formulae :- 1) Hall coefficient RH = cm / Coulumb. 2) Magnetic induction BY 2

3. Alternating Current

R.#W.#Erickson# Department#of#Electrical,#Computer,#and#Energy#Engineering# University#of#Colorado,#Boulder#

Comparative study between two models of a linear oscillating tubular motor

4. Electric field lines with respect to equipotential surfaces are

Advanced Power Electronics For Automotive and Utility Applications

Dynamic Effects of Feedback Control!

Computation of the Effect of Space Harmonics on Starting Process of Induction Motors Using TSFEM

The problem with linear regulators

Reading from Young & Freedman: For this topic, read sections 25.4 & 25.5, the introduction to chapter 26 and sections 26.1 to 26.2 & 26.4.

Detection of Tire Lateral Force Based on a Resolver Mechanism

Chapter 2: Principles of steady-state converter analysis

L1, L2, N1 N2. + Vout. C out. Figure 2.1.1: Flyback converter

dv 7. Voltage-current relationship can be obtained by integrating both sides of i = C :

INDEX. Transient analysis 1 Initial Conditions 1

- If one knows that a magnetic field has a symmetry, one may calculate the magnitude of B by use of Ampere s law: The integral of scalar product

Speed Control of BLDC Motor by Using Tuned Linear Quadratic Regulator

2.4 Cuk converter example

Physics for Scientists & Engineers 2

Some Basic Information about M-S-D Systems

A FAMILY OF THREE-LEVEL DC-DC CONVERTERS

Chapter 4 AC Network Analysis

Name: Total Points: Multiple choice questions [120 points]

Section 3.8, Mechanical and Electrical Vibrations

EECS 141: FALL 00 MIDTERM 2

Chapter 7 Response of First-order RL and RC Circuits

Fundamentals of Power Electronics Second edition. Robert W. Erickson Dragan Maksimovic University of Colorado, Boulder

RC, RL and RLC circuits

V AK (t) I T (t) I TRM. V AK( full area) (t) t t 1 Axial turn-on. Switching losses for Phase Control and Bi- Directionally Controlled Thyristors

Module 2 F c i k c s la l w a s o s f dif di fusi s o i n

On the Analysis and Optimal Control Design of BLDC Drives

Chapter 10 INDUCTANCE Recommended Problems:

Lab 10: RC, RL, and RLC Circuits

Experimental Buck Converter

Chapter 5 Digital PID control algorithm. Hesheng Wang Department of Automation,SJTU 2016,03

Physical Limitations of Logic Gates Week 10a

Final Spring 2007

Optimal Control of Dc Motor Using Performance Index of Energy

Loss Analysis of a 100kW PV Inverter

CHAPTER 12 DIRECT CURRENT CIRCUITS

Topic Astable Circuits. Recall that an astable circuit has two unstable states;

Dead-time Induced Oscillations in Inverter-fed Induction Motor Drives

Electrical Circuits. 1. Circuit Laws. Tools Used in Lab 13 Series Circuits Damped Vibrations: Energy Van der Pol Circuit

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is

Electrical and current self-induction

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Spring Experiment 9: Faraday s Law of Induction

I. Define the Situation

Embedded Systems and Software. A Simple Introduction to Embedded Control Systems (PID Control)

LAPLACE TRANSFORM AND TRANSFER FUNCTION

Suggested Practice Problems (set #2) for the Physics Placement Test

PHYSICS 149: Lecture 9

Mechanical Fatigue and Load-Induced Aging of Loudspeaker Suspension. Wolfgang Klippel,

Chapter 8 The Complete Response of RL and RC Circuits

Q.1 Define work and its unit?

Zhihan Xu, Matt Proctor, Ilia Voloh

ECE 2100 Circuit Analysis

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still.

Section 2.2 Charge and Current 2.6 b) The current direction is designated as the direction of the movement of positive charges.

Università degli Studi di Roma Tor Vergata Dipartimento di Ingegneria Elettronica. Analogue Electronics. Paolo Colantonio A.A.

Circuit Variables. AP 1.1 Use a product of ratios to convert two-thirds the speed of light from meters per second to miles per second: 1 ft 12 in

2.9 Modeling: Electric Circuits

NDP4050L / NDB4050L N-Channel Logic Level Enhancement Mode Field Effect Transistor

Module 4: Time Response of discrete time systems Lecture Note 2

Electromagnetic Induction: The creation of an electric current by a changing magnetic field.

Silicon Diffused Power Transistor

University of Cyprus Biomedical Imaging and Applied Optics. Appendix. DC Circuits Capacitors and Inductors AC Circuits Operational Amplifiers

θ with respect to time is

Structural Dynamics and Earthquake Engineering

Involute Gear Tooth Bending Stress Analysis

LabQuest 24. Capacitors

Sub Module 2.6. Measurement of transient temperature

A Predictive Torque Control for Inverter-fed Induction Machines

IE1206 Embedded Electronics

Is Vs. Electrical Machinery Part 4 Some Ideal Machines. Transformers. fig 4.1. Vp t. fig 4.2

where the coordinate X (t) describes the system motion. X has its origin at the system static equilibrium position (SEP).

Direct Current Circuits. February 19, 2014 Physics for Scientists & Engineers 2, Chapter 26 1

CHANGE IN THE RESISTANCE OF THE SEMICONDUCTOR IN THE VARIABLE DEFORMATION FIELD

Voltage/current relationship Stored Energy. RL / RC circuits Steady State / Transient response Natural / Step response

( ) = Q 0. ( ) R = R dq. ( t) = I t

Lecture 4 Kinetics of a particle Part 3: Impulse and Momentum

Physics 218 Exam 1. with Solutions Fall 2010, Sections Part 1 (15) Part 2 (20) Part 3 (20) Part 4 (20) Bonus (5)

Combined Bending with Induced or Applied Torsion of FRP I-Section Beams

Linear Response Theory: The connection between QFT and experiments

Chapter 2: Logical levels, timing and delay

Sliding Mode Controller for Unstable Systems

Problemas das Aulas Práticas

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3

DOUBLE STAR INDUCTION MOTOR DIRECT TORQUE CONTROL WITH FUZZY SLIDING MODE SPEED CONTROLLER

Phys1112: DC and RC circuits

IXGH48N60C3D1. GenX3 TM 600V IGBT with Diode V CES = 600V I C110. = 48A V CE(sat) 2.5V t fi(typ) = 38ns. High speed PT IGBT for kHz Switching

V L. DT s D T s t. Figure 1: Buck-boost converter: inductor current i(t) in the continuous conduction mode.

Learning Objectives: Practice designing and simulating digital circuits including flip flops Experience state machine design procedure

Transcription:

www.ijrase.com Volume 3 Issue XII, December 2015 Inernaional Journal for Research in Applied Science & Engineering Speed Conrol of Brushless DC Moor Using Proporional Inegral Conroller Vikramarajan Jambulingam Elecrical and Elecronics Engineering, VIT Universiy, India. Absrac: Ease conrol and high power densiy are he wo main reasons for using brushless DC moor in wide range of indusrial applicaions. In general he brushless DC moors are conrolled using power Semiconducor bridge. So he roor posiion sensors are used in he inverer bridge for saring and o provide proper commuaion sequence o he power swiches. In building inverer bridge power swiches are used due o high reliabiliy and performance. In his paper he hree phase brushless DC moor model is designed wih proporional inegral conroller and esed in MATLAB sofware. The PI conroller is used o conrol he speed of he brushless DC moor. On he oher hand parameers like Back EMF, curren, speed and orque are evaluaed for he designed models of BLDC moor. Due o he easy implemenaion and simple conrol srucure he convecional PI conroller are used in indusries. Keywords: Brushless DC moor, PI conroller, PMBLDC. I. INTRODUCTION The replacemen for convenional DC moor is BLDC moor in many cases. The characerisic of DC moor is reained by BLDC moor excep brushes and commuaor. To provide large amoun of orque for a wide range of speed BLDC moor suis he mos wih high performance. Acually for applicaions ha require high power, high reliabiliy and high efficiency BLDC moor is he ideal choice. A small BLDC moor is used in hard disk drives and large BLDC moor is used in elecric vehicles. In BLDC moor physical commuaor is no necessary because he elecric curren powers he permanen magne ha causes roaion in moor. So curren commuaion akes place because of solid sae swiches. In his case commuaion happens elecronically. Mos commonly used BLDC moors are hree phases raher han wo phase BLDC moor. Due o he roor roaion volage is induced in he saor winding called back-emf of BLDC moor. So orque is primarily influenced by back-emf of BLDC moor. In case size of he moor and orque delivered raio is higher so he criical facors are space and weighs in cerain applicaion o make i useful. When pracical speaking he orque ripple exi mainly due o imperfecion emf, ripple curren and phase curren commuaion. Due o he magne size and shape of he BLDC moor he imperfecion emf is occurred. On he oher side hyseresis and PWM conrol generaes ripple in curren. The Bimbra [1] has explained he generalized machine heory. II. BLOCKING DIAGRAM OF PROPOSED METHOD Figure 1: Block diagram of BLDC moor s Speed conrol The block diagram of brushless dc moor wih is speed conroller is shown in [Figure.1].I consis of four main pars hey are IJRASET 2015: All Righs are Reserved 471

www.ijrase.com Volume 3 Issue XII, December 2015 Inernaional Journal for Research in Applied Science & Engineering BLDC moor, sensors, conroller and power converers. The power is ransformed from source o BLDC moor hrough converer. So he BLDC moor in urn convers elecrical energy in o mechanical energy. To he power converer gae signal is applied on he basis of roor posiion. III. WORKING PRINCIPLE OF BLDC MOTOR One afer anoher he BLDC moor s elecronic commuaor energizes he saor coils and generaes a roaing elecric field ha drags he roor around wih i. N elecrical roaions equaes o one mechanical roaion, where N is he number of magne pairs. To indicae he relaive posiion of saor and roor o he conroller hree phase effec sensors are embedded in he saor of he hree phase brushless DC moor. The hall sensor helps brushless DC moor o energize he winding in a correc sequence and a he correc ime.consrucionally he all sensor is mouned on he non driving side of he sysem [Figure.2]. Figure 2: Hall sensors are embedded in he saor of a BLDC moor The high or low signal is generaed during he roor magneic poles passes he hall sensors by combining he signals from he hree sensors. Due o he movemen of he winding hrough he associaed magneic field he poenial volage is generaed by he elecrical moors and i can be called as elecromoive force. As per Lenz s law he magneic field which opposes original change in flux will give rise in winding curren. In general his means elecromoive force ends o resis he roaion of he moor and referred as back elecromoive force. The Baldursson [2] has developed brushless DC moor modelling and conrol. Padmaraja [3] has developed he fundamenals of brushless DC moor. A new simulaion model is developed by Jeon [4].For complee MATLAB modelling Simulink user s guide is helpful [5]. IV. DESIGN OF PI SPEED CONTROLLER In indusrial sysem PI is a conrol loop feedback mechanism. Acually beween measured process variable and desired se poin error exis. So o correc ha error Proporional inegral conroller is used in indusries. The proporional mode and inegral mode are wo separae modes involved in proporional inegral mode calculaion. The reacion o he curren error is calculaed by Proporional mode and reacion o he recen error is calculaed by inegral mode. So he sum of hese wo modes oupu is considered as correcive acion o he conrol elemen and PI conroller is implemened as, oupu( ) K pe( ) K e( ) d e( ) =se reference value acual calculaed value. The basic model of permanen magne brushless DC moor is shown in figure.2. In ha model i consis of BLDC moor, posiion sensor, pulse widh modulaion curren conroller, volage source inverer, reference curren generaor and PI conroller. The speed error is processed o PI conroller afer comparing he speed of he BLDC moor wih is reference speed. e( ) ( ) ref m T ( ) T ( 1) K [ e( ) e( 1)] K e( ) K ref ref p p & K -gain of speed conroller I I 0 1 IJRASET 2015: All Righs are Reserved 472

www.ijrase.com Volume 3 Issue XII, December 2015 Inernaional Journal for Research in Applied Science & Engineering The reference orque is nohing bu oupu of he conroller. The hree phase reference curren,, a b c i i i is generaed by reference curren generaor wih he limis of peak curren magniude decided by he conroller and posiion sensor. The swiching commands are generaed o drive he inverer devices by comparing moor curren and is reference curren. KO [3] has implemened he conrol of BLDC moor using PI conroller. V. MATHEMATICAL MODELLING OF THE BLDC MOTOR dia dib dic Va ia Ra La M ab M ac ea Eq.(1) d d d dib dia dic Vb ib Rb Lb M ba M bc eb Eq.(2) d d d dic dib dia Vc icrc Lc M cb M ca ec Eq.(3) d d d Where, Ra, Rb, Rc - Saor resisance of phase a, b and c. La, Lb, Lc - Saor inducance of phase a, b and c. ia, ib, ic -Saor curren of phase a, b and c. Va, Vb, Vc -Volages of phase a, b and c. Ra Rb Rc R -Muual inducance beween phases La, Lb, Lc -Saor self inducance of phase a, b and c. In his case, La Lb Lc L M M M M M M M ab ac bc ba ca cb Assuming hree phase balanced sysem, all phase resisance are equal. R R R R a b c Le us rearrange he above equaions 1, 2 and 3. We ge, dia dib dic Va ia R L M M ea Eq.(4) d d d dib dia dic Vb ib R L M M eb Eq.(5) d d d dic dib dia Vc ic R L M M ec Eq.(6) d d d Le us neglec muual inducance in equaions 4, 5 and 6. We ge, dia Va iar L ea Eq.(7) d dib Vb ib R L eb Eq.(8) d dic Vc icr L ec Eq.(9) d IJRASET 2015: All Righs are Reserved 473

www.ijrase.com Volume 3 Issue XII, December 2015 Inernaional Journal for Research in Applied Science & Engineering VI. TORQUE GENERATION Theoreical moor consan K is he produc of orque and supply curren I. Ta Tb Tc K K K K ( moor ) ( a) ( b) ( c) imoor ia ib ic -Angle Ta, Tb, Tc -Toal orques d P * d 2 The generaed elecromagneic orque is given by, [ eaia ebib ecic ] Te in N-M T K { f ( ) i f ( ) i f ( ) i e a a b b c c d J B Te T1 d The relaion beween angular velociy and angular posiion is given by, d P * d 2 T1 -load orque -Moor ineria B-Damping Consan P-Number of poles VII. SIMULATION MODEL OF THE BLDC MOTOR TABLE I Volage (V dc ) 160 vols Damping consan (T load ) 0.02 N-M/rad/sec Resisance (R) 0.7 ohms Inducance (L) 2.72 mh Momen of ineria (J) 0.000284Kg-m/sec 2 Number of poles 4 Number of phases 3 Table.1. Specificaion of BLDC moor IJRASET 2015: All Righs are Reserved 474

www.ijrase.com Volume 3 Issue XII, December 2015 Inernaional Journal for Research in Applied Science & Engineering Figure 3: MATLAB Simulink model of BLDC moor Figure 4: MATLAB Simulink Sub sysem model of BLDC moor IJRASET 2015: All Righs are Reserved 475

www.ijrase.com Volume 3 Issue XII, December 2015 Inernaional Journal for Research in Applied Science & Engineering Figure 5: MATLAB Simulink Sub sysem model of PI conroller A. Curren VIII. SIMULATION RESULTS Figure 6: Curren Phase A in amperes Figure 7: Curren Phase B in amperes IJRASET 2015: All Righs are Reserved 476

www.ijrase.com Volume 3 Issue XII, December 2015 Inernaional Journal for Research in Applied Science & Engineering B. Back EMF Figure 8: Curren Phase C in amperes Figure 9: Back EMF Phase A in Volages Figure 10: Back EMF Phase B in Volages IJRASET 2015: All Righs are Reserved 477

www.ijrase.com Volume 3 Issue XII, December 2015 Inernaional Journal for Research in Applied Science & Engineering C. Speed Figure 11: Back EMF Phase c in Volages D. Torque Figure 12: Speed in radian / second Figure 13: Torque in Newon meer IX. CONCLUSION The speed conrol of Proporional inegral conroller is shown in [Figure.12].The Proporional inegral conroller he moor reaches he reference speed wih a percenage overshoo of 6.23.Iniially he reference speed is se as 700rpm wih 0.005 seconds a res. A he same ime he iniial phase back elecromoive force of he BLDC moor is zero. Therefore he phase curren a he ime of saring is ransien bu once he speed reaches is reference speed. Then he curren also reach is reference speed he conducion period of curren is 120 degree as shown in [Figure.6]. In general o provide mechanical work in indusry and generae elecric power in power plans elecrical machines are used. Due o high efficiency and good dynamic response he permanen magne brushless DC moor gains araciveness in he recen years. Because of low cos and high reliabiliy he brushless DC drives are preferred. In his mission speed conrol of permanen magne brushless DC moor is achieved using Proporional inegral conroller in MATLAB sofware and also esed successfully by evaluaing he parameers like back EMF, curren, orque and speed. IJRASET 2015: All Righs are Reserved 478

www.ijrase.com Volume 3 Issue XII, December 2015 Inernaional Journal for Research in Applied Science & Engineering REFERENCES [1] P. S. Bimbhra, Generalized Theory of Elecrical Machines, Khanna Publishers, Delhi, India, 2001, pp. 93-98. [2] Padmaraja Yedamale, Brushless DC (BLDC) Moor Fundamenals, Microchip Technology Inc. 2003. [3] J.S.Ko, Robus Posiion Conrol of BLDC Moors Using Ineral-Proporional-Plus Fuzzy Logic Conroller, IEEE Trans. On IE, Vol, June 1994, pp.308-315. [4] S. Baldursson, BLDC Moor Modelling and Conrol A MATLAB/Simulink Implemenaion, Maser Thesis, May, 2005. [5] Y.S. Jeon, H.S.Mok, G.H.Choe, D.K.Kim and J.S. Ryu, A New Simulaion Model of BLDC Moor wih Real Back EMF waveforms, IEEE CNF. On compuers in Power Elecronics, 2000. COMPEL 2000.pp. 217-220, July 2000. [6] Sim power Sysems for use wih Simulink, user s guide, Mah Works Inc., Naick, MA, 2002. Mah Works, 2001, Inroducion o MATLAB, he Mah Works, Inc. BIOGRAPHY Mr.J.Vikramarajan received his Maser degree in Power Elecronics and Drives and Bachelor degree in Elecrical and Elecronics Engineering from VIT Universiy, India. He has published several inernaional research books and journals. His research ineress are elecrical machines, power elecronic applicaions, power qualiy, power elecronic converers and power elecronic conrollers for renewable energy sysems. IJRASET 2015: All Righs are Reserved 479