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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.2 ]5 j6 S! Q% m# b
Wye, Delta with all phase shifts. Auto, and Zigzag with most common configurations.
* d, S2 m2 e/ v F% N* b! _, G% kCard : BRANCH0 y* x6 x1 o. X; p S
Data : Io= Current [A] through magnetizing branch (MB) at steady state.5 t" l5 _3 i( G( C0 L
Fo= Flux [Wb-turn] in MB at steady state.# m9 e0 z N4 K/ \& v4 j
The pair Io, Fo defines the inductance in MB at steady state.
1 Z. @8 o* U, W& S Rm= Resistance in magnetizing branch in [ohm]. 5-leg core or 3-leg shell.. b; ^% y! S8 Y
The magnetizing branch is always connected to the PRIMARY winding and Rm is referred to this voltage.- n) {9 h& Q0 j8 e' v
R0= Reluctance of zero-sequence air-return path for flux. 3-leg core-type
# {6 N1 S8 E/ Z- o7 r) f Vrp= Rated voltage in [V] primary winding (only the voltage ratios matter).
) Y1 r& g8 b; J. ` Rp= Resistance in primary winding in [ohm].
! X/ H6 W' R5 M: T! K; z Lp= Inductance in primary winding in [mH] if Xopt.=0+ a) X! S4 O; v, U
Inductance in primary winding in [ohm] if Xopt.=power freq.. S7 n5 t( t$ _+ d! I
Vrs= Rated voltage in [V] secodary winding.
5 B2 ]; e9 x! [! @8 d' } Rs= Resistance in secondary winding in [ohm].
) l! B8 T; H6 G' _: u4 S Ls= Inductance in secondary winding in [mH] if Xopt.=0
% }/ y4 I; O( f& a! j1 z8 y | Inductance in secondary winding in [ohm] if Xopt.=power freq.9 ?4 V/ U5 r. G2 w+ t- H
Vrt= Rated voltage in [V] tertiary winding. K+ R3 r! H* L* v! T
Rt= Resistance in tertiary winding in [ohm].
& L8 j0 }, X; b- E Lt= Inductance in tertiary winding in [mH] if Xopt.=06 h |9 X t5 Y# p4 [
Inductance in tertiary winding in [ohm] if Xopt.=power freq. 6 w4 }0 y' D/ e: i3 f
RMS= unchecked: Current/Flux characteristic must be entered.; i N" F4 j9 N" V
checked: Irms/Urms characteristic must be entered.
; P& t7 S3 o' a' ?8 r6 W ATPDRAW performs a SATURATION calculation. a" O' l: J9 y
3-leg core = checked: 3-leg core type transformer assumed. TRANSFORMER THREE PHASE, n; B9 w: ]7 p( i! t/ C2 S+ F# _
unchecked: 5-leg or 3-leg shell type assumed. TRANSFORMER.
3 n! Z9 `# o& n: V" c* q& z6 q 3-wind.= turn on tertiary winding. $ q h$ m& m: E4 G
Output specified the magnetization branch output (power&energy not supported). * E( }8 Q* T4 K% z( V! j/ x* t3 O9 q# b
Node : P= Primary side. 3-phase node.
4 w8 j& h: m7 C1 b. v' [* ] S= Secondary side. 3-phase node.
: O5 O: e9 H: S- Y- ]) c% E PN= Neutral point primary side.
k' \8 q9 O. q y# t# F1 M6 N4 f1 ? SN= Neutral point secondary side.
" L% k x8 H+ M \/ D T= Tertiary side. 3-phase node.
1 V- z3 [* p* r9 n7 M; [$ y TN= Neutral point tertiary side.: S) s: ~/ |/ k' {
Sat= Internal node, connection of the magnetization circuit with saturation.
0 H `, h# ]+ W9 \The coupling is specified for each winding, with four coupling options: Y, D, A, Z
! H6 O6 J( D- [+ \3 X+ |% q, f All phase shifts are supported.
# @8 ^( ~6 t8 y" ~, i; i- FSpecial note on Auto-transformers: 0 V$ K, B7 @1 o' A0 l7 b& b
The primary and secondary windings must be of coupling A(uto).
$ @0 t9 R0 {4 M0 cSpecial note on ZigZag-transformers: , i* F/ W' j) P2 W: p
For this type the user can specify a phase shift in the range <-60,0>&<0,60>.
! B% `' ]# \% J; l* N Note that the values -60, 0 and +60 degrees are illegal (as one of the winding parts degenerates).
% P* f: i( F* a# W+ s9 E- P0 G: L The phase shift is given relative to a Y-coupled winding.
' w$ c$ \/ V+ K' o) n6 F( l If the primary winding is Zigzag-coupled, all other windings will be shifted with it.* h3 s: u; z* t. E/ b
If the primary winding is D-coupled, 30 deg. must be added/subtracted to the phase shifts.8 _% G+ i) ]1 j+ B
For negative phase shifts the phase A winding starts on leg 1 (called z with voltage Uz)
$ l( h. [( H# r0 N* n and continues in the opposite direction on leg 3 (called y with voltage Uy).
4 u8 ]; ^+ L& F( D For negative phase shifts the phase A starts on leg 1
. R8 \! k; S& l) R9 g) e& r and continues in the opposite direction on leg 2.
+ c% m3 M6 A4 @* l8 w The normal situation is to specify a phase shift of +/- 30 deg.
# Z4 d. ~4 r- ^; S9 q in which case the two parts of the winding have the same voltage level and leakage impedance.; i; `8 ] i" p9 |! l( h! F8 y
In general the ratio between the second part of the winding Uy and the first part Uz is . @- _# h, W/ X+ F% {7 o
n=Uy/Uz=sin(a)/sin(60-a) where a is absolute value of the phase shift.; p, G% D! d/ ~" ~8 @& k2 S
This gives:& e+ |! E9 }, a9 p* K) O0 |
Uz=U/(cos(a)+n*cos(60-a)) and Uy=Uz*n$ d# ~% p& w- T7 \" n7 G
Lz=L/(1+n*n) and Ly=Lz*n*n, Rz=R/(1+n) and Ry=Rz*n
6 h; d, [5 W! s: E8 X4 Y where Lz and Ly are the leakage inductance of each part of the winding (L is the total leakage inductance)
6 a( _4 r# F" r3 j and Rz and Ry are the winding resistance of each winding part (R is the total).
8 j0 R3 c- Z2 J- z* P7 D% p l The parameters Uz, Uy, Zz, and Zy are automatically calculated by ATPDraw based on the 4 {; m( W5 |! p5 f7 Q) d5 I L; k
equivalent parameters U and Z and the phase shift, a./ s$ y' n+ g5 d) P
- r) w4 U; Z; m' K3 Y9 ]6 ~
3 D. @/ q) j: `" P: \- J9 }
Points: It's possible to enter 9 points on the current/flux characteristic.& z3 i: s0 ?$ s
The required menu is performed immedeately after the input menu.! f( b3 {5 g! R1 D- y' `( l+ W
The points should be entered as increasingly larger values. - I5 v9 F2 c8 w7 U: n- N" [3 a
The point (0,0) is not permitted (added internally in ATP).& Z6 ], U! g! Z, g. z1 F. f
RuleBook: IV.E.1-2 or 3. |
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