3. mathematical analysis of air-gap fields · 3. mathematical analysis of air-gap fields . ... =...
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![Page 1: 3. Mathematical Analysis of Air-Gap Fields · 3. Mathematical Analysis of Air-Gap Fields . ... = 1.2 /2 = 1.88 m = 188 cm -v syn ... Inserting form-wound two-layer winding in stator](https://reader031.vdocuments.us/reader031/viewer/2022013006/5b14175e7f8b9af1638b465d/html5/thumbnails/1.jpg)
Institut für Elektrische
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Prof. A. Binder : Electrical Machines and Drives
3/1
3. Mathematical Analysis of Air-Gap
Fields
![Page 2: 3. Mathematical Analysis of Air-Gap Fields · 3. Mathematical Analysis of Air-Gap Fields . ... = 1.2 /2 = 1.88 m = 188 cm -v syn ... Inserting form-wound two-layer winding in stator](https://reader031.vdocuments.us/reader031/viewer/2022013006/5b14175e7f8b9af1638b465d/html5/thumbnails/2.jpg)
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Rotating waves - Travelling waves Rotating wave: x is stator circumference co-ordinate (rotating machine)
Travelling wave: x is stator linear co-ordinate (linear machine)
tf
xBtxB
p
2cosˆ),( 11
Wave velocity: Observer, who is moving with the
wave, sees constant argument of cos() = const.
pp
syn fftconstdt
d
dt
dxv
2)2.(
Wave in opposite direction: )2cos(ˆ),( 11 tfx
BtxBp
psyn fv 2
Example:
At frequency f = 50 Hz: vsyn in m/s is SAME number as pole pitch in cm:
e.g. 2-pole turbine generator (2p = 2) in thermal power plant: nsyn = 3000/min:
- stator bore diameter dsi = 1.2 m, pole pitch p = 1.2/2 = 1.88 m = 188 cm
- vsyn = 188 m/s = 676 km/h = rotor surface velocity, as rotor is spinning
synchronously with rotating stator magnetic field wave (synchronous machine !)
cmp
smsynv /
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Pulsating fields – standing waves
Standing wave is pulsating field: The location of wave nodes and wave amplitudes
is fixed, but the amplitudes are pulsating.
At time t = 0: Maximum of wave at x = 0 has amplitude
at t = T/8: ,
at t = T/4: amplitude is zero !
at t = T/2: and so on. )2cos(cosˆ),( 11 tf
xBtxB
p
2/ˆ1B
1ˆB
1ˆB
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FOURIER-series: A periodical function V() with period 2 may be described
by an infinite sum of sine & co-sine functions with decreasing wave length.
Ordinal numbers:
Amplitudes: ,
Average value:
Magnetomotive force (MMF) of air gap field:
a) NO UNIPOLAR flux: V0 = 0
b) MMF V symmetrical to abscissa: NO even ordinal numbers
c) By choosing origin so, that MMF V is even function V() = V(-):
NO sine-wave functions occur in FOURIER sum.
FOURIER-Analysis: Determining fundamental & harmonic waves
,...3,2,1
,,0 )sin(ˆ)cos(ˆ)(
ba VVVV
....,3,2,1
2
0
, )cos()(1ˆ dVV a
2
0
, )sin()(1ˆ dVV b
2
0
0 )(2
1dVV
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Magnetomotive force Vc(x) is block-shaped function, slot-Ampere-turns Q = 2Ncic
Circumference angle : :
Example: Four pole machine: Half circumference = in "mechanical degrees",
equals two pole pitches x = 2p , thus =2, in "electrical degrees"
FOURIER-Analysis of field of one full-pitched coil (q = 1)
px /
,...5,3,1
, )cos(ˆ)(
cc VV
, 2
sin4
2)cos()(
2ˆ
0
,
Q
cc
ΘdVV ....,5,3,1
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Compare MMF function´s FOURIER series with that of full-pitched coils: Amplitudes are
smaller by the ”pitch coefficient" kp, :
Example: W/p = 5/6 (q = 2): = 1: kp1 = 0.966, = 5: kp5 = 0.259
FOURIER-Analysis of field of one pitched coil (q = 1)
... ,5 ,3 ,1 ,2
sin4
2)cos()(
2ˆ
0
,
p
Q
cc
WΘdVV
2sin,
pp
Wk
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Magnetomotive force of field of full-pitched coil group: = 1, 3, 5, ...
”Distribution coefficient„
Example: q = 2
MMF amplitude: qQ/2 = Q
With relationship we get
FOURIER-Analysis of field of a full-pitched coil group q > 1
)2
sin(
)2
sin(
2sin
4
2)cos()(
2ˆ
0
,
mqq
mqdVV
Qgrgr
)2
sin(
)2
sin(
,
mqq
mkd
,,
2sin
4
2ˆ
22
2
2dgr
cccc
Qk
p
iNV
p
iN
p
ai
a
pqNiqN
qΘ
![Page 8: 3. Mathematical Analysis of Air-Gap Fields · 3. Mathematical Analysis of Air-Gap Fields . ... = 1.2 /2 = 1.88 m = 188 cm -v syn ... Inserting form-wound two-layer winding in stator](https://reader031.vdocuments.us/reader031/viewer/2022013006/5b14175e7f8b9af1638b465d/html5/thumbnails/8.jpg)
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FOURIER-analysis of MMF of one phase Vphase() :
Phase current
The MMF distribution (and hence the air gap field) is a sum of
pulsating, standing waves („Pulsating field“).
"Winding coefficient"
FOURIER-series of field of one phase with pitched coil groups
q > 1, W/p < 1
... ,5 ,3 ,1 , 4
2ˆ
,,,
dpphase kkp
iNV
)cos(2 tIi
... ,5 ,3 ,1 , 122ˆ
,,,
Ikkp
NV dpphase
,...5,3,1
, )cos()cos(ˆ),(
tVtV phasephase
,d,p,w kkk
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Pitch coefficient, distribution coefficient and winding coefficient for pitched
winding with 6, 12 and 18 slots per pole pair Q/p
Pitch and distribution coefficient REDUCE certain field harmonic amplitudes.
Winding coefficient is a PERIODICAL function of ordinal number .
Example of typical three phase windings A, B, C
kw,
kd, kp, kw, kd, kp, kw, kd, kp,
0.866 1
-0.866 1
0.866 1
-0.866 1
0.866 1
-0.902 0.960 -0.067 0.259
0.067 -0.259
0.933 -0.966
-0.933 -0.966
-0.067 -0.259
0.902 0.960
-0.038 0.218
-0.136 -0.177
-0.136 -0.177
-0.038 0.218
0.902 0.960 0.933 0.966
0.067 0.259 -0.866 1
0.866 1
-0.940 -0.259 0.866 19
0.940 -0.259 -0.866 17
-0.174 -0.966 0.866 13
0.766 0.966 -0.866 11
0.766 0.259 0.866 7
-0.174 0.259 -0.866 5
0.940 0.966 0.866 1
Q/p = 18 Q/p = 12 Q/p = 6
q = 3, W/p = 7/9 q = 2, W/p = 5/6 q = 1, W/p = 2/3
C B A
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Inserting form-wound two-layer winding in
induction generator stator
72436
2
qmpQ
Source:
Winergy
Germany
Stator iron
stack
coil ends
Winding
overhang
Q = 72 slots
72 coils
m = 3 phases
2p = 4 poles
q = 6 slots per
pole and phase
72634
2
qmpQ
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Inserting form-wound two-layer winding in stator
slots
Source:
ABB, Switzerland
Stator iron
stack
60 slots for a
4-pole
induction
machine
q = 5:
Winding
overhang
60534
2
qmpQ
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Stator three phase two-layer winding of induction
generator
Source:
Winergy
Germany
Q = 72 slots
72 coils
m = 3 phases
2p = 4 poles
q = 6 slots per
pole and phase
72634
2
qmpQ
- Completed two-
layer winding after
the impregnation with
resin
- Some resin “noses”
are removed after the
impregnation to get a
smooth air gap
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FOURIER-analysis of field of a 3-phase winding
Pulsating fields per phase are shifted spatially by 2p/3 as phases U, V, W. These
3 phases are fed by sinusoidal AC current with phase shift of T/3.
Pulsating field per phase is decomposed in negative and positive sequence
rotating field waves (clockwise and counter-clockwise rotation) by use of
trigonometric summation law:
)cos()cos(ˆ),( , tVtV phaseU
)3/2cos())3/2(cos(ˆ),( , tVtV phaseV
)3/4cos())3/4(cos(ˆ),( , tVtV phaseW
)cos()cos(2
1coscos
)cos(2
ˆ)cos(
2
ˆ),(
,,t
Vt
VtV
phasephaseU
)3
2
3
2cos(
2
ˆ)
3
2
3
2cos(
2
ˆ),(
,,
t
Vt
VtV
phasephaseV
)3
4
3
4cos(
2
ˆ)
3
4
3
4cos(
2
ˆ),(
,,
t
Vt
VtV
phasephaseW
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Fundamental of air gap MMF (and field)
Resulting effect (summation) of all 3 pulsating phase fields U, V, W:
Summation for ordinal number = 1 (“Fundamental”):
Result: rotating wave:
,...5,3,1 ,...5,3,1
),()),(),(),((),(
tVtVtVtVtV WVU
)cos(2
ˆ)cos(
2
ˆ),(
1,1,1 t
Vt
VtV
phasephaseU
)cos(2
ˆ)
3
4cos(
2
ˆ),(
1,1,1 t
Vt
VtV
phasephaseV
:get we0)3
8cos()
3
4cos()cos(With
)cos(ˆ2
3),( 1,1 tVtxV phase
)cos(2
ˆ)
3
8cos(
2
ˆ),(
1,1,1 t
Vt
VtV
phasephaseW
/ 0VB
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Harmonic waves of air gap MMF and field
Summation of pulsating phase fields for > 1:
For ordinal numbers , which are divisible by 3, the summation of harmonic phase fields
U, V, W is zero: The 3 positive and negative sequence phase waves cancel.
For = 7, 13, 19, ... cancel the 3 negative sequence phase waves. The 3 positive
sequence phase waves add with the SAME phase angle and rotate WITH the fundamental
wave.
For = 5, 11, 17, .... cancel the 3 positive sequence phase waves. The 3 negative
sequence phase waves add with the SAME phase angle, rotating inverse to fundamental.
Facit: A 3-phase winding, fed by symmetrical 3-phase sinusoidal current system, excites a
step-like MMF distribution in air gap V(x,t), which may be decomposed into fundamental
and harmonic rotating waves. Wave lengths are determined by ordinal numbers. Only odd
ordinal numbers exist = 1, 5, 7, 11, 13, 17, 19, ..., which are indivisible by 3.
000),(3 tV )5cos(ˆ2
3),( 5,5 tVtV phase
)7cos(ˆ2
3),( 7,7 tVtV phase 000),(9 tV
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Fundamental and harmonic air gap field waves
= 1, -5, 7, -11, 13, -17,... Phase number m: is usually 3
Positive and negative ordinal numbers:
Velocity of harmonic waves decreases with 1/ :
Wave amplitudes (% of fundamental): (%) Underlined: “slot harmonics” !
)cos(
2),(),(
,t
xI
kN
p
mtxVtxV
p
w
-5.3 0.38 5.3 19
5.9 -0.4 -5.6 -17
-0.3 7.7 7.7 13
-1.4 -9.1 -9.1 -11
-2.2 -1.0 14.3 7
-0.8 1.4 -20 -5
100 100 100 1
q = 3, W/p = 7/9, Q/p = 18 q = 2, W/p = 5/6, Q/p = 12 q = 1, W/p = 2/3, Q/p = 6
...,3,2,1,021 gmg
/fv p,syn 2
1 B̂/B̂
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Magnetomotive force and air gap field of squirrel cage winding
a) Rotor: Squirrel cage: Qr conductive bars (copper, aluminium) in Qr slots. Bars are
short-circuited by 2 conductive rings an the front ends.
b) Symmetrical rotor current system: In each bar flows a sinusoidal bar current
with a constant phase shift to the current of the adjacent bar. Thus each bar is a
phase of a Qr-phase system.
Example: Qr = 28 bars, 2p = 4: Bar current system repeats after Qr/p = 14 bars. Phase
shift is ”slot angle” Q = 2p/Qr = /7.
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FOURIER-Analysis of MMF (and field) of squirrel cage
Each bar = 1 phase AND each bar = half turn of a coil. Hence:
Pitch and distribution coefficient = 1.
: Ordinal number of harmonic waves of rotor field of cage winding
Relationships:
FOURIER-series:
with ordinal numbers
Example: Qr = 28 bars, 2p = 4: Ordinal numbers = 1, -13, 15, -27, 29, ...
Wave amplitudes decrease with 1/ !
,,1,,2/1 , barwr IIkQmN
,...1
)2cos(1
2
12),(
tf
xI
p
QtxV r
pbar
r
,...2,1,01 rrr gg
p
Q
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Copper cage rotor of an induction machines
Source:
Breuer Motors,
Germany
![Page 20: 3. Mathematical Analysis of Air-Gap Fields · 3. Mathematical Analysis of Air-Gap Fields . ... = 1.2 /2 = 1.88 m = 188 cm -v syn ... Inserting form-wound two-layer winding in stator](https://reader031.vdocuments.us/reader031/viewer/2022013006/5b14175e7f8b9af1638b465d/html5/thumbnails/20.jpg)
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Salient pole air gap field, excited by DC current Air gap field H : e.g. 2-pole rotor of salient pole synchronous machine: Rotor
winding ampere-turns NfPol.If , (NfPol : number of turns per pole)
Air gap enlarged at inter-pole gaps, hence air gap is function of circumference co-
ordinate (x).
Calculation of radial component B of rotor air gap field by AMPERE´s law:
(Iron: Fe )
)(22)(222 xHHxHVINsdH FeFefffPol
C
)()()( 00
x
VxHxB
f
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Completed salient pole before mounting
Source:
Andritz Hydro,
Austria
Pump storage
hydro power plant
Vianden/Belgium
Refurbishment
Three-fold hammer
head fixation
“Cooling fins” by
increased copper
width
Damper ring
segments
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Completed “big hydro” salient pole synchronous rotor for high
centrifugal force at over-speed, 14 poles
Source:
Andritz Hydro,
Austria
Dove tail fixation of
rotor poles
“Cooling fins” by
increased copper
width
Damper ring
Damper retaining
bolts
Rotor back iron
Rotor spider
Generator shaft
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Field curve is symmetrical to abscissa:
only harmonics with odd ordinal numbers
Field curve as FOURIER-Cosine-series:
Shape of field curve is determined by air gap function (x) ( = contour of pole shoe);
hence also ordinal numbers, divisible by 3, are existing !
Poles rotate with constant rotational speed n: m = 2n = 2vm/dsi Hence all rotor waves
(fundamental and harmonics) B move with same speed vm with respect to stator winding.
Stator induced voltage of -th harmonic has -times higher frequency than that of
fundamental = 1.
Facit: In stator winding sinusoidal voltage due to fundamental rotor wave ( = 1) is induced,
but ALSO harmonic voltages with higher frequencies, whose harmonic stator currents,
excite magnetic fields, which may interfere from power line to parallel telephone cables.
FOURIER-Analysis of air gap field of DC-excited salient poles
)()( BB
... ,9 ,7 ,5 ,3 ,1 )cos(ˆ)(,...5,3,1
BB
npp
f m
22tptt mrrs )()(
)cos(ˆ)cos(ˆ)cos(ˆ)( tx
BtpBBBp
msrr