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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.
. J* z3 `" R: D" B0 P2 V Wye, Delta with all phase shifts. Auto, and Zigzag with most common configurations.
2 c6 G3 {) k c; A! pCard : BRANCH/ c, _- C1 r0 A* F; }8 N# ]
Data : Io= Current [A] through magnetizing branch (MB) at steady state.8 \+ C& X6 }% J) c
Fo= Flux [Wb-turn] in MB at steady state.2 e' l* D% ?/ |' |6 }1 ]
The pair Io, Fo defines the inductance in MB at steady state.
: Z6 ]3 F9 Q% \+ S! R0 A$ I0 g Rm= Resistance in magnetizing branch in [ohm]. 5-leg core or 3-leg shell.
9 G# ~/ W, F1 d2 e- J2 m The magnetizing branch is always connected to the PRIMARY winding and Rm is referred to this voltage.
0 t* I. V' Q! u: E6 c/ ^ R0= Reluctance of zero-sequence air-return path for flux. 3-leg core-type
/ X+ n# N* ?6 E3 J Vrp= Rated voltage in [V] primary winding (only the voltage ratios matter).
4 K0 x( m, O$ w [; }2 U+ H F! ? Rp= Resistance in primary winding in [ohm].& H |4 x& P9 Z: k/ K5 Q
Lp= Inductance in primary winding in [mH] if Xopt.=0- |2 t3 H- M8 y" G% `. L# W: F2 w2 p
Inductance in primary winding in [ohm] if Xopt.=power freq.5 [; N3 H* G' y
Vrs= Rated voltage in [V] secodary winding.
" z" B, s+ ^- |1 L Rs= Resistance in secondary winding in [ohm].
3 w% ]7 v8 b; R Ls= Inductance in secondary winding in [mH] if Xopt.=0, @2 ]8 f. D; k( q2 X: t
Inductance in secondary winding in [ohm] if Xopt.=power freq.
# |; c) ]! ^4 z2 _; A0 o Vrt= Rated voltage in [V] tertiary winding.
, I" r P! [$ X0 Y. g% a# Q Rt= Resistance in tertiary winding in [ohm].
( j" k/ O2 z9 e4 @. {; G Lt= Inductance in tertiary winding in [mH] if Xopt.=0
) d u. ?5 V& _ V. R Inductance in tertiary winding in [ohm] if Xopt.=power freq. ' ?( C$ Z: U' x V
RMS= unchecked: Current/Flux characteristic must be entered.
! Y1 r& A! C. k' M5 Y& Y checked: Irms/Urms characteristic must be entered.
0 ?% K7 M, _4 o3 p [) }. j9 S ATPDRAW performs a SATURATION calculation.
: |/ e2 e# g+ q4 O+ |" G- V4 k 3-leg core = checked: 3-leg core type transformer assumed. TRANSFORMER THREE PHASE- C, w9 S( H. {
unchecked: 5-leg or 3-leg shell type assumed. TRANSFORMER., O( K# e7 O% v' z8 u# _
3-wind.= turn on tertiary winding. " ]+ y# N- E. r- V* ~
Output specified the magnetization branch output (power&energy not supported). " d) B5 z. K" { t! b
Node : P= Primary side. 3-phase node.3 L- {; W6 L0 ~+ f/ i( l; u8 i+ K
S= Secondary side. 3-phase node. Y% c4 [ |1 N6 E4 o
PN= Neutral point primary side.
+ ?/ x0 E3 }2 L* X SN= Neutral point secondary side.
. d( J5 g2 }+ r) E. E# ` T= Tertiary side. 3-phase node.- H2 M- N1 ?) @% d7 r; k
TN= Neutral point tertiary side.
0 _1 ~; P8 D: B- `( | Sat= Internal node, connection of the magnetization circuit with saturation.
: n5 D0 w% a3 W9 HThe coupling is specified for each winding, with four coupling options: Y, D, A, Z
. Q1 Z. a4 p9 L8 b All phase shifts are supported.
- ^& E# \3 Q5 u( [/ k' D2 |6 A9 FSpecial note on Auto-transformers: / B9 M# G) o" @
The primary and secondary windings must be of coupling A(uto).
! r7 L# [/ d' P& ^; q) N/ kSpecial note on ZigZag-transformers:
* D. r6 @) N8 x5 K D ] For this type the user can specify a phase shift in the range <-60,0>&<0,60>.
% V& }" d8 |0 A' T( X7 N Note that the values -60, 0 and +60 degrees are illegal (as one of the winding parts degenerates).
+ a3 A2 s# v) V: J# { The phase shift is given relative to a Y-coupled winding. " u) J7 W2 G6 S' N5 e) ~; G
If the primary winding is Zigzag-coupled, all other windings will be shifted with it.' z, a, y( ~& F9 X6 N
If the primary winding is D-coupled, 30 deg. must be added/subtracted to the phase shifts.* {% m* f8 u9 Q. L+ u5 F
For negative phase shifts the phase A winding starts on leg 1 (called z with voltage Uz)
+ [- u) S! z8 N, q+ y' {% U c and continues in the opposite direction on leg 3 (called y with voltage Uy).% y# w4 q) P% X1 Q8 S
For negative phase shifts the phase A starts on leg 1 2 Z$ \8 B, ]9 b
and continues in the opposite direction on leg 2. 0 Q/ O# @ |1 y1 J. R/ D
The normal situation is to specify a phase shift of +/- 30 deg.
1 T; R9 P2 i. h2 g8 j in which case the two parts of the winding have the same voltage level and leakage impedance.
F* O) I- c, `6 V9 m In general the ratio between the second part of the winding Uy and the first part Uz is % D8 r( _+ i& S
n=Uy/Uz=sin(a)/sin(60-a) where a is absolute value of the phase shift.
5 y0 W# ?4 s: c# L* h7 Y+ [ This gives:
& g, I0 S5 ?. @6 ~ Uz=U/(cos(a)+n*cos(60-a)) and Uy=Uz*n
" g# X" j. C4 [1 R [0 ?; S* v5 k8 H Lz=L/(1+n*n) and Ly=Lz*n*n, Rz=R/(1+n) and Ry=Rz*n ; R. H4 z6 b) X, q" e/ j+ {
where Lz and Ly are the leakage inductance of each part of the winding (L is the total leakage inductance)
3 Y* B% ~0 S" N* S: U! c: f and Rz and Ry are the winding resistance of each winding part (R is the total).
8 ~" e3 G1 l# T7 ~4 k The parameters Uz, Uy, Zz, and Zy are automatically calculated by ATPDraw based on the 7 r& e: ]4 G- p1 ?: }
equivalent parameters U and Z and the phase shift, a.3 u: u0 r. k( g+ Y
9 b/ K8 I; m$ `# ]0 c7 G- o9 g
. r! m( q2 a2 j' n! H6 VPoints: It's possible to enter 9 points on the current/flux characteristic.% K1 W7 d& L% P5 m6 \5 i
The required menu is performed immedeately after the input menu.
6 w( f; d2 x* z+ O6 p" }8 a( Z, ` B The points should be entered as increasingly larger values. `0 q! a: U9 l8 N
The point (0,0) is not permitted (added internally in ATP).8 H7 L* F$ A( Y$ d
RuleBook: IV.E.1-2 or 3. |
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