Lecture 1 - EE743 - PowerPoint PPT Presentation

About This Presentation
Title:

Lecture 1 - EE743

Description:

SYNCHRONOUS MACHINES Two-pole,3-phase,wye-connected,salient-pole synchronous machine DYNAMIC PERFORMANCE DURING A SUDDEN CHANGE IN INPUT TORQUE Dynamic performance of ... – PowerPoint PPT presentation

Number of Views:94
Avg rating:3.0/5.0
Slides: 44
Provided by: ValuedGa508
Category:
Tags: ee743 | lecture | phase

less

Transcript and Presenter's Notes

Title: Lecture 1 - EE743


1
SYNCHRONOUS MACHINES
Two-pole,3-phase,wye-connected,salient-pole
synchronous machine
2
SYNCHRONOUS MACHINES
  • In abc reference frame, voltage equations can be
    written as

3
SYNCHRONOUS MACHINES
  • flux linkage equations

4
SYNCHRONOUS MACHINES
  • flux linkage equations
  • Referring all rotor variables to the stator
    windings

5
SYNCHRONOUS MACHINES
  • Referring all rotor variables to the stator
    windings

6
SYNCHRONOUS MACHINES
  • Referring all rotor variables to the stator
    windings

7
SYNCHRONOUS MACHINES
  • TORQUE EQUATION IN MACHINE VARIABLES

8
SYNCHRONOUS MACHINES
  • SWING EQUATION

9
SYNCHRONOUS MACHINES
  • Stator Voltage Equations in Arbitrary
    Reference-frame Variables
  • The rotor voltage equations are expressed only in
    the rotor reference frame

10
SYNCHRONOUS MACHINES
  • The flux linkage equations may be expressed as
  • The sinusoidal terms are constant, independent
    of ? and ?r only if ? ?r

11
SYNCHRONOUS MACHINES
  • Therefore, the time-varying inductances are
    eliminated from the voltage equations only if the
    reference frame is fixed in the rotor.
  • Voltage Equations In Rotor Reference-frame
    variables park's Equations

12
SYNCHRONOUS MACHINES
13
SYNCHRONOUS MACHINES
  • Park's voltage equations are often written in
    expanded form
  • Flux linkages in expanded form

14
SYNCHRONOUS MACHINES
  • The Equivalent q-axis Circuits

15
SYNCHRONOUS MACHINES
  • The Equivalent d-axis Circuits

16
SYNCHRONOUS MACHINES
  • The Equivalent 0-axis Circuits

17
SYNCHRONOUS MACHINES
  • It is often convenient to express the voltage
    and flux linkage equations in terms of reactances
    rather than inductances

18
SYNCHRONOUS MACHINES
  • Also, it is convenient to define

19
SYNCHRONOUS MACHINES
  • If we select the currents as independent
    variables

20
SYNCHRONOUS MACHINES
  • If we select the flux linkages per second as
    independent variables

21
SYNCHRONOUS MACHINES
  • Torque Equations in Substitute Variables

22
SYNCHRONOUS MACHINES
  • Rotor Angle

it is convenient to relate the position of the
rotor of a synchronous machine to a voltage or to
the rotor of another machine.
The electrical angular displacement of the rotor
relative to its terminal voltage is defined as
the rotor angle,
The rotor angle is the displacement of the rotor
generally referenced to the maximum positive
value of the fundamental component of the
terminal voltage of phase a
23
SYNCHRONOUS MACHINES
  • Rotor Angle

It is important to note that the rotor angle is
often used as the argument in the transformation
between the rotor and synchronously rotating
reference frames
The rotor angle is often used in relating torque
and rotor speed (if ?e is constant)
24
SYNCHRONOUS MACHINES
PER UNIT SYSTEM
  • Base voltage
  • the rms value ofthe rated phase voltage for
    the abc variables
  • the peak value for the qd0 variables.
  • Base power
  • When considering the machine separately, the
    power base is selected as its volt-ampere rating.
  • When considering power systems, a system
    power base (system base) is selected
  • Once the base quantities are established, the
    corresponding base current and base impedance may
    be calculated.
  • Base torque is the base power divided by the
    synchronous speed of the rotor

25
SYNCHRONOUS MACHINES
  • The torque expressed in per unit

26
SYNCHRONOUS MACHINES
  • ANALYSIS OF STEADY-STATE OPERATION

For balanced conditions the 0s quantities are
zero. ?r is constant and equal to ?e the rotor
windings do not experience a change of flux
linkages the current is not flowing in the
short-circuited damper windings the time rate of
change of all flux linkages neglected
27
SYNCHRONOUS MACHINES
  • ANALYSIS OF STEADY-STATE OPERATION

For balanced conditions
28
SYNCHRONOUS MACHINES
  • ANALYSIS OF STEADY-STATE OPERATION

Hence
and if it is noted that
Then
29
  • ANALYSIS OF STEADY-STATE OPERATION

It is convenient to define the last term on the
right-hand side as (excitation voltage)
if rs is neglected, the expression for the
balanced steady-state electromagnetic torque in
per unit can be written as
30
DYNAMIC PERFORMANCE DURING A SUDDEN CHANGE IN
INPUT TORQUE
31
DYNAMIC PERFORMANCE DURING A SUDDEN CHANGE IN
INPUT TORQUE
Dynamic performance of a hydro turbine generator
during a step increase in input torque from zero
to rated
32
DYNAMIC PERFORMANCE DURING A SUDDEN CHANGE IN
INPUT TORQUE
Torque versus rotor angle characteristics
33
DYNAMIC PERFORMANCE DURING A SUDDEN CHANGE IN
INPUT TORQUE
34
DYNAMIC PERFORMANCE DURING A SUDDEN CHANGE IN
INPUT TORQUE
Dynamic performance of a steam turbine generator
during a step increase in input torque from zero
to 50 rated.
35
DYNAMIC PERFORMANCE DURING A SUDDEN CHANGE IN
INPUT TORQUE
Torque versus rotor angle characteristics
36
DYNAMIC PERFORMANCE DURING A 3 PHASE FAULT AT THE
MACHINE TERMINALS
a hydro turbine generator
37
DYNAMIC PERFORMANCE DURING A 3 PHASE FAULT AT THE
MACHINE TERMINALS
Torque versus rotor angle characteristics
38
DYNAMIC PERFORMANCE DURING A 3 PHASE FAULT AT THE
MACHINE TERMINALS
a steam turbine generator
39
DYNAMIC PERFORMANCE DURING A 3 PHASE FAULT AT THE
MACHINE TERMINALS
Torque versus rotor angle characteristics
40
COMPUTER SIMULATION
Simulation in Rotor Reference Frame
Where
41
COMPUTER SIMULATION
Simulation in Rotor Reference Frame
42
COMPUTER SIMULATION
Simulation of Saturation
43
COMPUTER SIMULATION
Simulation of Saturation
Write a Comment
User Comments (0)
About PowerShow.com