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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.
6 w- n3 z6 ^: q4 N/ R- O Wye, Delta with all phase shifts. Auto, and Zigzag with most common configurations.
0 F: M3 p% V6 q' A4 qCard : BRANCH! D- ?1 s7 s5 I8 B
Data : Io= Current [A] through magnetizing branch (MB) at steady state.5 w( R' r' c- g0 S" t
Fo= Flux [Wb-turn] in MB at steady state.1 [$ w; y( ]& e) h" y
The pair Io, Fo defines the inductance in MB at steady state.
9 Y1 X! t: @& j2 E Rm= Resistance in magnetizing branch in [ohm]. 5-leg core or 3-leg shell.( I! N* R( m% f; A
The magnetizing branch is always connected to the PRIMARY winding and Rm is referred to this voltage.* t) ^7 E7 f+ x
R0= Reluctance of zero-sequence air-return path for flux. 3-leg core-type; ?+ v8 n3 y T5 H
Vrp= Rated voltage in [V] primary winding (only the voltage ratios matter).+ q% s4 j; k$ u, d
Rp= Resistance in primary winding in [ohm].
. [2 A3 }3 y3 x" p9 R Lp= Inductance in primary winding in [mH] if Xopt.=0
' ^, Q2 m+ {4 G; a. o% N Inductance in primary winding in [ohm] if Xopt.=power freq.
% ^' h6 r7 J( Q: L# p Vrs= Rated voltage in [V] secodary winding.
( V) B+ _) A d, r0 h, w) N Rs= Resistance in secondary winding in [ohm].4 X; \8 J/ p& |5 u* b& u b
Ls= Inductance in secondary winding in [mH] if Xopt.=0
/ m3 V5 }5 q8 I9 E Inductance in secondary winding in [ohm] if Xopt.=power freq.; t$ z* m3 g; c0 @
Vrt= Rated voltage in [V] tertiary winding.) n. y. [4 u, p& H8 \& E [
Rt= Resistance in tertiary winding in [ohm].
( M" y5 j& i* Y0 G Lt= Inductance in tertiary winding in [mH] if Xopt.=08 v# k: a8 W9 U2 I9 l/ s6 r% G
Inductance in tertiary winding in [ohm] if Xopt.=power freq.
% W9 l; T! {* G- s+ g' ]% x RMS= unchecked: Current/Flux characteristic must be entered.9 e( h* ^9 E+ ^3 M- K C& |; q
checked: Irms/Urms characteristic must be entered.( ^4 ~- i* l( y8 i
ATPDRAW performs a SATURATION calculation.9 g3 ?8 S2 C H% B; t4 Q, j
3-leg core = checked: 3-leg core type transformer assumed. TRANSFORMER THREE PHASE% {! E3 r0 A6 [5 t K
unchecked: 5-leg or 3-leg shell type assumed. TRANSFORMER.
5 x- E0 s9 L3 s. ~ 3-wind.= turn on tertiary winding.
; H, t2 p3 O) L' B _Output specified the magnetization branch output (power&energy not supported). j* Y3 X6 m3 l- }# F
Node : P= Primary side. 3-phase node.
3 I+ `) D2 z( X3 B+ w8 [9 _ S= Secondary side. 3-phase node.
& c# [) g5 U! U& L7 K" X" x4 l. Z PN= Neutral point primary side.$ V" p- I; K1 J Y1 c* s& c
SN= Neutral point secondary side.9 g$ X/ U: \: _
T= Tertiary side. 3-phase node.
3 J; S/ \6 |2 n) T$ m! T+ V4 K$ I4 d TN= Neutral point tertiary side.
+ H. x- E/ l) Z# [# J3 Y) ]# v Sat= Internal node, connection of the magnetization circuit with saturation.
9 L+ l1 M7 ]' u2 S3 WThe coupling is specified for each winding, with four coupling options: Y, D, A, Z3 n. E j0 Y! C+ m, y0 i- B. Z
All phase shifts are supported.* u% g5 _& {' A
Special note on Auto-transformers: % n w1 ^1 M# g1 K6 ?$ M" T
The primary and secondary windings must be of coupling A(uto).) m; X+ I/ i6 @+ C5 A4 t% `9 e
Special note on ZigZag-transformers: " ]* g! M' Y5 N: e7 G
For this type the user can specify a phase shift in the range <-60,0>&<0,60>.
0 G7 y1 n. p7 b8 l% A Note that the values -60, 0 and +60 degrees are illegal (as one of the winding parts degenerates).% A) ^4 n. |3 t/ b O3 l
The phase shift is given relative to a Y-coupled winding. - G- z* A3 _: K
If the primary winding is Zigzag-coupled, all other windings will be shifted with it.# n, \- G) W# k; ]
If the primary winding is D-coupled, 30 deg. must be added/subtracted to the phase shifts.
" L1 C. s; X1 Q j# Z For negative phase shifts the phase A winding starts on leg 1 (called z with voltage Uz)
0 e4 Q% h; Z1 Q5 Q# R and continues in the opposite direction on leg 3 (called y with voltage Uy).6 Q+ p) c$ t! l3 I- v; K g: B
For negative phase shifts the phase A starts on leg 1
2 T! V- w! P7 [6 r$ a5 Q/ l5 i and continues in the opposite direction on leg 2. 2 c/ b7 u; N" t* d; s2 X
The normal situation is to specify a phase shift of +/- 30 deg.
7 P1 t4 t o( E+ c% i( a in which case the two parts of the winding have the same voltage level and leakage impedance.9 N7 M+ K4 C; P' p3 e
In general the ratio between the second part of the winding Uy and the first part Uz is : r0 \, w: @/ q
n=Uy/Uz=sin(a)/sin(60-a) where a is absolute value of the phase shift.1 Q: ]7 i# l" r I z; q0 S
This gives:6 \& }/ Q! m) J; K; e) M! h( P* d: [$ ^
Uz=U/(cos(a)+n*cos(60-a)) and Uy=Uz*n
~) c- o7 g& b2 I5 [ Lz=L/(1+n*n) and Ly=Lz*n*n, Rz=R/(1+n) and Ry=Rz*n 5 ^" Z$ y: V) n( `+ Q
where Lz and Ly are the leakage inductance of each part of the winding (L is the total leakage inductance)
* b5 s3 O! ~! n( {2 e. E _; p, ^ and Rz and Ry are the winding resistance of each winding part (R is the total).7 v5 ~9 ?* r5 _7 t4 O7 @
The parameters Uz, Uy, Zz, and Zy are automatically calculated by ATPDraw based on the
) }; a" X4 P* M! @ equivalent parameters U and Z and the phase shift, a.# e! {" |! e& F m4 D
! O0 U! l% ^5 D/ Y. @4 R
6 e' \$ h3 U) i1 WPoints: It's possible to enter 9 points on the current/flux characteristic.
% F* W: F% v% s- E4 E7 B n3 M+ l The required menu is performed immedeately after the input menu.
* M5 n$ F/ J+ G; }: p. N& R8 r The points should be entered as increasingly larger values. / J7 T" y' _. P' P: ?% x9 M
The point (0,0) is not permitted (added internally in ATP)., u) R) G" ~( ^) h1 I
RuleBook: IV.E.1-2 or 3. |
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