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发表于 2009-11-18 11:36:55
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Name : SatTrafo - General saturable transformer. 3 phase. 2 or 3 windings.
) K/ |2 S1 }( {1 e. |* z Wye, Delta with all phase shifts. Auto, and Zigzag with most common configurations.
5 @$ G2 j3 }0 W! `Card : BRANCH
) d8 e- j: t" Y& w; }- CData : Io= Current [A] through magnetizing branch (MB) at steady state.
/ m T4 @( ?- g8 T" v" M9 c Fo= Flux [Wb-turn] in MB at steady state.
; M% l* U- t- {4 J8 i% ~: [ The pair Io, Fo defines the inductance in MB at steady state.
) K% E$ E. S: G- j Rm= Resistance in magnetizing branch in [ohm]. 5-leg core or 3-leg shell.$ b6 g* r( s" V5 C
The magnetizing branch is always connected to the PRIMARY winding and Rm is referred to this voltage.
5 s! k+ w8 T: ?$ N4 x' B! D R0= Reluctance of zero-sequence air-return path for flux. 3-leg core-type
3 i/ Z, f# _* m& |1 S Vrp= Rated voltage in [V] primary winding (only the voltage ratios matter).; U- g. Z& v W, V. s
Rp= Resistance in primary winding in [ohm].! m4 d9 Y) ~4 z, S
Lp= Inductance in primary winding in [mH] if Xopt.=0
. p; }. z9 I: a8 Q# C( S5 v Inductance in primary winding in [ohm] if Xopt.=power freq.
# {0 E( P0 e% J7 k" n8 ~+ K; v/ x Vrs= Rated voltage in [V] secodary winding.
) X$ B5 g1 \* j5 F! [$ W' W$ J Rs= Resistance in secondary winding in [ohm].+ J* Z' M; T; x3 E* M* `: H
Ls= Inductance in secondary winding in [mH] if Xopt.=0
( q- @: L( X- k. E# h4 J P Inductance in secondary winding in [ohm] if Xopt.=power freq.' e7 _& u# R) @2 {( y% C+ z
Vrt= Rated voltage in [V] tertiary winding.
3 p# \! r. j) i" M* ] Rt= Resistance in tertiary winding in [ohm].
) O: K6 X( }1 k" F' ? Lt= Inductance in tertiary winding in [mH] if Xopt.=0
" A* K8 H" U7 O) m6 P0 X Inductance in tertiary winding in [ohm] if Xopt.=power freq. ' f% m) `& Y$ K5 \6 z7 l# T
RMS= unchecked: Current/Flux characteristic must be entered.
* W" }. @' H7 A9 A8 J" i' j5 v" I checked: Irms/Urms characteristic must be entered.4 y% ?: t4 i o9 l) X6 p7 Q! K* Z# Q
ATPDRAW performs a SATURATION calculation.7 o+ H1 y+ @/ J3 R' _4 F" ~. Y) g
3-leg core = checked: 3-leg core type transformer assumed. TRANSFORMER THREE PHASE0 X' |: o* w( Q' T
unchecked: 5-leg or 3-leg shell type assumed. TRANSFORMER.
6 o! ~5 l7 A5 H. S 3-wind.= turn on tertiary winding.
1 f/ X% k4 K" @Output specified the magnetization branch output (power&energy not supported). : k( [( g2 Y7 ?1 e+ A6 n
Node : P= Primary side. 3-phase node.8 q& o* L+ r4 S" @) F
S= Secondary side. 3-phase node.( K1 G. Z* |% l4 X. O8 ~7 a
PN= Neutral point primary side.$ f# J- H- D4 m; ~
SN= Neutral point secondary side.
e; { V; F9 c6 m7 G* a" V7 p( } T= Tertiary side. 3-phase node.- [: Y* f. l' c- r. k) p
TN= Neutral point tertiary side.
$ d% n; f( Z( L# c Sat= Internal node, connection of the magnetization circuit with saturation.
8 \2 K$ f [# LThe coupling is specified for each winding, with four coupling options: Y, D, A, Z; J3 j! L9 m f0 k) Y
All phase shifts are supported.! w/ j) O9 ~# I
Special note on Auto-transformers: . u$ k. L; ~0 s: w4 q I( O5 U
The primary and secondary windings must be of coupling A(uto).
/ h* k2 F6 f" N0 P5 B/ rSpecial note on ZigZag-transformers:
( F: m5 J2 ^1 z( T. x For this type the user can specify a phase shift in the range <-60,0>&<0,60>.5 e2 X8 o0 {8 ~$ {& u) U
Note that the values -60, 0 and +60 degrees are illegal (as one of the winding parts degenerates).* P y: F I4 y* q
The phase shift is given relative to a Y-coupled winding. * C8 X4 l2 i3 c: R3 o
If the primary winding is Zigzag-coupled, all other windings will be shifted with it.
, U7 s/ I. n, M: r If the primary winding is D-coupled, 30 deg. must be added/subtracted to the phase shifts.* @2 u' S( r* }) @% I \; T# A% G T6 n& R
For negative phase shifts the phase A winding starts on leg 1 (called z with voltage Uz)
/ I' m4 b# E1 s$ T) n4 E% G and continues in the opposite direction on leg 3 (called y with voltage Uy).
8 m( B# ^* H1 u9 U1 W+ K( M7 F) B For negative phase shifts the phase A starts on leg 1 5 w; x7 B! e9 L# a; ~
and continues in the opposite direction on leg 2. % u) z- i* S% ]- J) C" j
The normal situation is to specify a phase shift of +/- 30 deg.
- X( ?4 Y" f! V! ^ in which case the two parts of the winding have the same voltage level and leakage impedance.
+ ?- s$ r2 T6 Q" ?. ?. N In general the ratio between the second part of the winding Uy and the first part Uz is
" p1 r% l1 X- k( M" v) } n=Uy/Uz=sin(a)/sin(60-a) where a is absolute value of the phase shift.3 H. s( e$ B3 t5 H6 L
This gives:4 N/ k- L/ e2 }; W
Uz=U/(cos(a)+n*cos(60-a)) and Uy=Uz*n# N1 {( Y; O& X
Lz=L/(1+n*n) and Ly=Lz*n*n, Rz=R/(1+n) and Ry=Rz*n
. ~- H' O5 _5 F% u5 E+ F where Lz and Ly are the leakage inductance of each part of the winding (L is the total leakage inductance), ?# l% d# G2 P. ]2 u0 a
and Rz and Ry are the winding resistance of each winding part (R is the total).
+ v& i, S$ d& R1 O The parameters Uz, Uy, Zz, and Zy are automatically calculated by ATPDraw based on the , x/ i0 w! L5 A! q9 {$ c2 X8 h* [
equivalent parameters U and Z and the phase shift, a.
9 h8 }- H+ _% J) X0 p3 j6 M3 B; y1 H; T4 j2 F# M( _+ ]
2 q" d; W# r$ v1 lPoints: It's possible to enter 9 points on the current/flux characteristic.
- n# l M* ]' \! ~! ~" h The required menu is performed immedeately after the input menu.; ]& {- w' g. O/ Q+ ]' |
The points should be entered as increasingly larger values. # y6 s7 j/ e8 m2 T" R
The point (0,0) is not permitted (added internally in ATP).; C# `/ v7 T% G* _! n9 T
RuleBook: IV.E.1-2 or 3. |
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