EC010504(EE) Electric Drives & Control

Slides:



Advertisements
Similar presentations
Request Dispatching for Cheap Energy Prices in Cloud Data Centers
Advertisements

SpringerLink Training Kit
Luminosity measurements at Hadron Colliders
From Word Embeddings To Document Distances
Choosing a Dental Plan Student Name
Virtual Environments and Computer Graphics
Chương 1: CÁC PHƯƠNG THỨC GIAO DỊCH TRÊN THỊ TRƯỜNG THẾ GIỚI
THỰC TIỄN KINH DOANH TRONG CỘNG ĐỒNG KINH TẾ ASEAN –
D. Phát triển thương hiệu
NHỮNG VẤN ĐỀ NỔI BẬT CỦA NỀN KINH TẾ VIỆT NAM GIAI ĐOẠN
Điều trị chống huyết khối trong tai biến mạch máu não
BÖnh Parkinson PGS.TS.BS NGUYỄN TRỌNG HƯNG BỆNH VIỆN LÃO KHOA TRUNG ƯƠNG TRƯỜNG ĐẠI HỌC Y HÀ NỘI Bác Ninh 2013.
Nasal Cannula X particulate mask
Evolving Architecture for Beyond the Standard Model
HF NOISE FILTERS PERFORMANCE
Electronics for Pedestrians – Passive Components –
Parameterization of Tabulated BRDFs Ian Mallett (me), Cem Yuksel
L-Systems and Affine Transformations
CMSC423: Bioinformatic Algorithms, Databases and Tools
Some aspect concerning the LMDZ dynamical core and its use
Bayesian Confidence Limits and Intervals
实习总结 (Internship Summary)
Current State of Japanese Economy under Negative Interest Rate and Proposed Remedies Naoyuki Yoshino Dean Asian Development Bank Institute Professor Emeritus,
Front End Electronics for SOI Monolithic Pixel Sensor
Face Recognition Monday, February 1, 2016.
Solving Rubik's Cube By: Etai Nativ.
CS284 Paper Presentation Arpad Kovacs
انتقال حرارت 2 خانم خسرویار.
Summer Student Program First results
Theoretical Results on Neutrinos
HERMESでのHard Exclusive生成過程による 核子内クォーク全角運動量についての研究
Wavelet Coherence & Cross-Wavelet Transform
yaSpMV: Yet Another SpMV Framework on GPUs
Creating Synthetic Microdata for Higher Educational Use in Japan: Reproduction of Distribution Type based on the Descriptive Statistics Kiyomi Shirakawa.
MOCLA02 Design of a Compact L-­band Transverse Deflecting Cavity with Arbitrary Polarizations for the SACLA Injector Sep. 14th, 2015 H. Maesaka, T. Asaka,
Hui Wang†*, Canturk Isci‡, Lavanya Subramanian*,
Fuel cell development program for electric vehicle
Overview of TST-2 Experiment
Optomechanics with atoms
داده کاوی سئوالات نمونه
Inter-system biases estimation in multi-GNSS relative positioning with GPS and Galileo Cecile Deprez and Rene Warnant University of Liege, Belgium  
ლექცია 4 - ფული და ინფლაცია
10. predavanje Novac i financijski sustav
Wissenschaftliche Aussprache zur Dissertation
FLUORECENCE MICROSCOPY SUPERRESOLUTION BLINK MICROSCOPY ON THE BASIS OF ENGINEERED DARK STATES* *Christian Steinhauer, Carsten Forthmann, Jan Vogelsang,
Particle acceleration during the gamma-ray flares of the Crab Nebular
Interpretations of the Derivative Gottfried Wilhelm Leibniz
Advisor: Chiuyuan Chen Student: Shao-Chun Lin
Widow Rockfish Assessment
SiW-ECAL Beam Test 2015 Kick-Off meeting
On Robust Neighbor Discovery in Mobile Wireless Networks
Chapter 6 并发:死锁和饥饿 Operating Systems: Internals and Design Principles
You NEED your book!!! Frequency Distribution
Y V =0 a V =V0 x b b V =0 z
Fairness-oriented Scheduling Support for Multicore Systems
Climate-Energy-Policy Interaction
Hui Wang†*, Canturk Isci‡, Lavanya Subramanian*,
Ch48 Statistics by Chtan FYHSKulai
The ABCD matrix for parabolic reflectors and its application to astigmatism free four-mirror cavities.
Measure Twice and Cut Once: Robust Dynamic Voltage Scaling for FPGAs
Online Learning: An Introduction
Factor Based Index of Systemic Stress (FISS)
What is Chemistry? Chemistry is: the study of matter & the changes it undergoes Composition Structure Properties Energy changes.
THE BERRY PHASE OF A BOGOLIUBOV QUASIPARTICLE IN AN ABRIKOSOV VORTEX*
Quantum-classical transition in optical twin beams and experimental applications to quantum metrology Ivano Ruo-Berchera Frascati.
The Toroidal Sporadic Source: Understanding Temporal Variations
FW 3.4: More Circle Practice
ارائه یک روش حل مبتنی بر استراتژی های تکاملی گروه بندی برای حل مسئله بسته بندی اقلام در ظروف
Decision Procedures Christoph M. Wintersteiger 9/11/2017 3:14 PM
Limits on Anomalous WWγ and WWZ Couplings from DØ
Presentation transcript:

EC010504(EE) Electric Drives & Control Dr. Unnikrishnan P.C. Professor, EEE

Module II Transformer √ Three Phase Induction Motor Single Phase Induction Motor Alternator Synchronous Motor

Induction Motor Advantages Robust; No brushes. No contacts on rotor shaft High Power/Weight ratio compared to DC motor Lower Cost/Power Easy to manufacture Almost maintenance-free, except for bearing and other mechanical parts wide range of power ratings: fractional HP to 10 MW

Induction Motor Disadvantages Essentially a “fixed-speed” machine Speed is determined by the supply frequency To vary its speed need a variable frequency supply

Parts of an Induction Motor

Construction An induction motor has two main parts a stationary stator consisting of a steel frame that supports a hollow, cylindrical core core, constructed from stacked laminations (why?), having a number of evenly spaced slots, providing the space for the stator winding

Construction- Stator

Construction-Rotor Two basic designs Squirrel-Cage: conducting copper or aluminium bars laid into slots and shorted at both ends by shorting rings. (Squirrel Cage Induction Motor) Wound-Rotor: complete set of three-phase windings exactly as the stator. Usually Y-connected, the ends of the three rotor wires are connected to 3 slip rings on the rotor shaft. In this way, the rotor circuit is accessible. (Slip-Ring Induction Motor)

Construction Squirrel cage rotor Wound rotor Notice the slip rings

Construction- Rotor

Construction-Wound Rotor Slip Ring Induction Motor Slip rings Cutaway in a typical wound-rotor IM. Notice the brushes and the slip rings Brushes

Rotating Magnetic Field Balanced three phase windings, i.e. mechanically displaced 120 degrees form each other, fed by balanced three phase source A rotating magnetic field with constant magnitude is produced, rotating with a speed Where fe is the supply frequency and P is the no. of poles and nsync is called the synchronous speed in rpm

Synchronous speed P 50 Hz 60 Hz 2 3000 3600 4 1500 1800 6 1000 1200 8 750 900 10 600 720 12 500

Rotating Magnetic Field

Rotating Magnetic Field

Principle of operation This rotating magnetic field cuts the rotor windings and produces an induced voltage in the rotor windings Due to the fact that the rotor windings are short circuited, for both squirrel cage and wound-rotor, a current flows in the rotor windings The rotor current produces another magnetic field A torque is produced as a result of the interaction of those two magnetic fields 𝑇 𝑖𝑛𝑑 =𝑘 𝐵 𝑟 𝐵 𝑠 Where 𝑇 𝑖𝑛𝑑 is the induced torque and BR and BS are the magnetic flux densities of the rotor and the stator respectively.

Induction Motor Speed At what speed will the IM run? Can the IM run at the synchronous speed, why? If rotor runs at the synchronous speed, which is the same speed of the rotating magnetic field, then the rotor will appear stationary to the rotating magnetic field and the rotating magnetic field will not cut the rotor. So, no induced current will flow in the rotor and no rotor magnetic flux will be produced so no torque is generated and the rotor speed will fall below the synchronous speed When the speed falls, the rotating magnetic field will cut the rotor windings and a torque is produced

Induction Motor Speed So, the IM will always run at a speed lower than the synchronous speed The difference between the motor speed and the synchronous speed is called the Slip Where 𝑁 𝑠 = speed of the magnetic field 𝑁 𝑚 = mechanical shaft speed of the motor S = The slip S = 𝑁 𝑠 − 𝑁 𝑚 𝑁 𝑠

The Slip Notice that : if the rotor runs at synchronous speed s = 0 if the rotor is stationary s = 1 Slip may be expressed as a percentage by multiplying the above eq. by 100, notice that the slip is a ratio and doesn’t have units

Frequency The frequency of the voltage induced in the rotor is given by Where fr = the rotor frequency (Hz) P = number of stator poles n = slip speed (rpm)

Torque While the input to the induction motor is electrical power, its output is mechanical power and for that we should know some terms and quantities related to mechanical power Any mechanical load applied to the motor shaft will introduce a Torque on the motor shaft. This torque is related to the motor output power and the rotor speed 𝑇 𝑙𝑜𝑎𝑑 = 𝑃 𝑜𝑢𝑡 𝜔 𝑚 and 𝜔 𝑚 = 2𝜋 𝑛 𝑚 60 rad/s

Horse Power Another unit used to measure mechanical power is the horse power It is used to refer to the mechanical output power of the motor Since we, as an electrical engineers, deal with watts as a unit to measure electrical power, there is a relation between horse power and watts. hp =746 𝑊𝑎𝑡𝑡𝑠

Torque-Slip Equation 𝑇 𝛼 𝐸 2 𝐼 2 𝑐𝑜𝑠 ∅ 2 𝑇 𝛼 𝐸 2 𝐼 2 𝑐𝑜𝑠 ∅ 2 𝑇=𝑘 𝐸 2 𝑆 𝐸 2 𝑅 2 2 + (𝑆 𝑋 2 ) 2 𝑅 2 𝑅 2 2 + (𝑆 𝑋 2 ) 2 𝑇= 𝐾𝑆 𝐸 2 2 𝑅 2 𝑅 2 2 + (𝑆 𝑋 2 ) 2

Torque-Slip Characteristics 𝑻= 𝑲𝑺 𝑬 𝟐 𝟐 𝑹 𝟐 𝑹 𝟐 𝟐 + (𝑺 𝑿 𝟐 ) 𝟐 Low Slip Region: 𝑇𝛼 𝑆 High Slip Region: 𝑇𝛼 1 𝑆

Starters- Squirrel Cage IM Direct-On-line Starting Stator Rheostat Starting Autotransformer Starting Star-Delta Starter

Direct On-Line(DOL) Starter Used for motors upto 2 kW Starting torque about twice the full load torque

Stator Rheostat Starter Advantages: High PF during start, Less Expensive, Smooth acceleration Disadvantages: Losses in Resistors, Expensive, Low torque efficiency

Auto-Transformer Starter Advantages: High torque/Ampere, Long starting period, Can be used for star and delta connected motors, Disadvantages: Low PF (Lagging), Higher cost

Star-Delta Starter Reduced starting current but the starting torque is also reduced by the same amount Limited to applications where high starting torque is not necessary

Starters- Slip Ring IM Rotor Rheostat Autotransformer Starting Star-Delta Starter

Rotor Rheostat Starter for Slip Ring IM By increasing rotor resistance, the rotor current is reduced at starting. The torque is increased due to improvement in PF Such motors can be started under load

Power losses in Induction Machines Copper losses Copper loss in the stator (PSCL) = I12R1 Copper loss in the rotor (PRCL) = I22R2 Core loss (Pcore) Mechanical power loss due to friction and windage How this power flow in the motor?

Power Flow in Induction Motor

Power Relations 𝑇 𝑙𝑜𝑎𝑑 = 𝑃 𝑐𝑜𝑛𝑣 𝜔 𝑚 𝑃 𝑆𝐶𝐿 −𝑆𝑡𝑎𝑡𝑜𝑟 𝐶𝑜𝑝𝑝𝑒𝑟 𝐿𝑜𝑠𝑠 𝑃 𝐴𝐺 −𝐴𝑖𝑟 𝐺𝑎𝑝 𝑃𝑜𝑤𝑒𝑟 𝑃 𝑅𝐶𝐿 −𝑅𝑜𝑡𝑜𝑟 𝐶𝑜𝑝𝑝𝑒𝑟 𝐿𝑜𝑠𝑠 ,𝑃 𝑐𝑜𝑛𝑣 −𝑇ℎ𝑒 𝐸𝑙𝑒𝑐𝑡𝑟𝑖𝑐𝑎𝑙 𝑃𝑜𝑤𝑒𝑟 𝑐𝑜𝑛𝑣𝑒𝑟𝑡𝑒𝑑 𝑡𝑜 𝑚𝑒𝑐ℎ𝑎𝑐𝑖𝑐𝑎𝑙 𝑇 𝑙𝑜𝑎𝑑 = 𝑃 𝑐𝑜𝑛𝑣 𝜔 𝑚

Torque-speed characteristics Typical torque-speed characteristics of induction motor

Maximum torque Effect of rotor resistance on torque-speed characteristic

Speed Control Methods of IM Induction Motor Speed Control From Stator Side By Changing The Applied Voltage 𝑇= 𝐾𝑆 𝐸 2 2 𝑅 2 𝑅 2 2 + (𝑆 𝑋 2 ) 2 , T 𝑆 𝐸 2 2 By Changing The Applied Frequency Constant V/F Control Of Induction Motor- Most Popular Changing The Number Of Stator Poles

Constant V/F Control Of Induction Motor  If the supply frequency is reduced keeping the rated supply voltage, the air gap flux will tend to saturate causing excessive stator current and distortion of the stator flux wave. If the ratio of voltage to frequency is kept constant, the flux remains constant. Also, the developed torque remains approximately constant.

Speed Control Methods Of IM ….. Induction Motor Speed Control From Rotor Side Rotor Rheostat Control Cascade Operation By Injecting EMF In Rotor Circuit: By changing the phase of injected emf, speed can be controlled

Cascade Operation

Example A 208-V, 10hp, four pole, 60 Hz, Y-connected induction motor has a full-load slip of 5 percent What is the synchronous speed of this motor? What is the rotor speed of this motor at rated load? What is the rotor frequency of this motor at rated load? What is the shaft torque of this motor at rated load?

Solution

Example A 480-V, 60 Hz, 50-hp, three phase induction motor is drawing 60A at 0.85 PF lagging. The stator copper losses are 2 kW, and the rotor copper losses are 700 W. The friction and windage losses are 600 W, the core losses are 1800 W, and the stray losses are negligible. Find the following quantities: The air-gap power PAG. The power converted Pconv. The output power Pout. The efficiency of the motor.

Solution

Solution

Example A two-pole, 50-Hz induction motor supplies 15kW to a load at a speed of 2950 rpm. What is the motor’s slip? What is the induced torque in the motor in N.m under these conditions? What will be the operating speed of the motor if its torque is doubled? How much power will be supplied by the motor when the torque is doubled?

Solution

Solution In the low-slip region, the torque-speed curve is linear and the induced torque is direct proportional to slip. So, if the torque is doubled the new slip will be 3.33% and the motor speed will be

Question? Q: How to change the direction of rotation? A: Change the phase sequence of the power supply.

Question? Q: Why rotor core loss in a three phase induction motor negligible? A: Usually we operate motor at slip in the range 0.04 ~ 0.06, thus for a stator frequency of 50 Hz , rotor frequency is around 2~3 Hz. As core losses are proportional to square of frequency (Eddy current losses) or proportional to frequency ( Hysteresis losses) , therefore the value of the Core loss is negligible for rotor.