Electric Machine Design Course

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Electric Machine Design Course
Mod 1 Copyright: JR Hendershot 2012
Electric Machine Design Course
Electric Machine Design Course
Electric Machine Design Course
Electric Machine Design Course
Electric Machine Design Course
Electric Machine Design Course
Electric Machine Design Course
Electric Machine Design Course
Electric Machine Design Course
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Presentation transcript:

Electric Machine Design Course Basic Electric Motor & Generator Operational Theory Lecture # 2 Mod 2 Copyright: JR Hendershot 2012

Electric motor Genealogy chart SMMA Mod 2 Copyright: JR Hendershot 2012

Electric Machine Cross Sections b c Type f is an example of a double salient pole machine Types b & h are single salient pole machines Types a, c, d, e, f & g are non-salient pole machines This design class is limited to the study of machines that use similar stators with the same laminations & phase windings. These are type b, c, e, g & h. d e f g h Courtesy TJE MILLER Mod 2 Copyright: JR Hendershot 2012

Mod 2 Copyright: JR Hendershot 2012 Motoring & Generating Operational modes (Known as 4 quadrant operation) - Torque +Torque + Speed + Speed Torque + Torque Speed - Speed Mod 2 Copyright: JR Hendershot 2012

Motoring & Generating Operation (Known as 4 quadrant operation) Mod 2 Copyright: JR Hendershot 2012

Mod 2 Copyright: JR Hendershot 2012 Example of two quadrant motor operation (Ball screw, timing belt or rack and pinion geared) Quad 1 + Torque -Torque + RPM + RPM Quad 2 Lowest power required when times are each 1/3 Area under motion profile = motor shaft angle Mod 2 Copyright: JR Hendershot 2012

Introduction to basic electric motor theory Pre-requisite technical understanding: - First Course: Electric Machines & Drives * - Maxwell equations for E & B field relationships - Biot-Savart’s Law for forces on a current wire loop - Lorentz forces from a magnetic field on a conductor - Ampere’s Law to calculate the magnetic circuit - Faraday’s law describes how a voltage is generated * By Prof. Ned Mohan, Wiley2012, ISBN 978-1-118-07481-7 Mod 2 Copyright: JR Hendershot 2012

Machine control and power source The AC or DC power source to the inverter, converter or controller can be either from the grid or from batteries The motor types for this series of lectures are limited to motors powered by inverters or converters & controllers. Electric machine design techniques and strategies for grid powered machines is not covered in these lectures. Mod 2 Copyright: JR Hendershot 2012

General concepts of electric machines Flux linkages between stator & rotor across air gap create or require tangential forces (resulting in torque on or from shaft) for motoring or generating. All machines require magnetization of rotor-stator motor magnetic circuit creating circuit paths though the poles at the air gap. - Permanent, magnets can provide magnetization - Phase or armature windings can create field flux - Salient pole rotors close magnetic circuit paths Mod 2 Copyright: JR Hendershot 2012

Tangential air-gap forces producing shaft torques PM DC commutated motor example Mod 2 Copyright: JR Hendershot 2012

PM Rotor with Slotted vs. Slotless stator Magnet Air Gap Mod 2 Copyright: JR Hendershot 2012

Mod 2 Copyright: JR Hendershot 2012 Basic operation of AC Induction machines (Most technically elegant of all machines) Consider a simple transformer Square frame of iron Wound with primary Wound with secondary Voltage applied primary, induces a voltage in secondary (either can be primary) Voltage in the secondary winding is proportional to turns ratio Mod 2 Copyright: JR Hendershot 2012

Mod 2 Copyright: JR Hendershot 2012 Basic operation of AC Induction machines (Most technically elegant of all machines) Cut iron core frame into two halves Mount one half in bearings to facilitate rotation Short the secondary winding or connect to external power source via slip rings Apply AC voltage across primary AC voltage is induced into secondary as before as flux crosses small air gaps. With proper mechanical configuration of secondary part as a rotor in bearings and adding three phases of primary windings in a stator forces created in the air gap creates torque on the shaft. Mod 2 Copyright: JR Hendershot 2012

PMDC commutated vs. AC induction & PM brushless AC Induction motor PM DC commutated PM Brushless Used over 100 yrs. Used about 60 yrs Used about 35 yrs. Switched Reluctance motors used about 25-30 yrs. Reluctance Synchronous motors (old motor) used a couple of years Bodine Electric Mod 2 Copyright: JR Hendershot 2012

AC Induction motor (Rotating Transformer) PRIMARY SECONDARY Mod 2 Copyright: JR Hendershot 2012

Space vector diagrams for (2) pole machines Classic DC machine Phase of AC induction motor (1) Phase of PMSM Mod 2 Copyright: JR Hendershot 2012

Classic PMDC to BLDC conversion Perhaps original cross section representations of difference between the PM DC commutated motor and the PM Brushless motor now known as a permanent magnet synchronous machine. Taken from the ELECTRO-CRAFT HANDBOOK (organized by Erland Persson), over 80,000 copies Mod 2 Copyright: JR Hendershot 2012

Voltage Produced in PM Machine Faraday’s law came first so we must first consider the open circuit voltage generated in the phase windings. 1-A moving conductor linking the flux of a constant magnetic field produces an induced voltage. 2-An induced voltage will be induced in a conductive coil of a magnetic flux varies inside that coil loop. In other words an induced voltage is always produced by rate of change of flux linkage between the magnetic poles and the phase conductors Mod 2 Copyright: JR Hendershot 2012

Reluctance machine concept Ld Lq Note: The RSM has only a single magnetic flux source (in stator) Torque is produced by attraction of salient rotor poles to stator poles The level of attraction (torque) is proportional to Lq / Ld Mod 2 Copyright: JR Hendershot 2012

Mod 2 Copyright: JR Hendershot 2012 PMSM IM Mod 2 Copyright: JR Hendershot 2012

Mod 2 Copyright: JR Hendershot 2012 Title Mod 2 Copyright: JR Hendershot 2012