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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.; Z. [4 a) b! N" ]3 B9 b
Wye, Delta with all phase shifts. Auto, and Zigzag with most common configurations.
5 y2 ~4 m6 I' V. CCard : BRANCH
+ _" K+ L- K) ?) H% A# z: wData : Io= Current [A] through magnetizing branch (MB) at steady state.: Y& F; D+ ?; s+ ?: @( [
Fo= Flux [Wb-turn] in MB at steady state.
1 a; d' V2 Q0 ?2 _" X& r$ r The pair Io, Fo defines the inductance in MB at steady state.! F; f2 @0 `8 d+ K& a" y2 j
Rm= Resistance in magnetizing branch in [ohm]. 5-leg core or 3-leg shell.* j$ x. U, z$ R0 F3 Y) V- |
The magnetizing branch is always connected to the PRIMARY winding and Rm is referred to this voltage.
8 _) n$ b; K) Z7 @' [: G) K R0= Reluctance of zero-sequence air-return path for flux. 3-leg core-type8 I, o2 T- w" O7 M5 x
Vrp= Rated voltage in [V] primary winding (only the voltage ratios matter).
2 J/ X! H( C' ~ Rp= Resistance in primary winding in [ohm].
" q5 F l" ]- ^$ r9 t7 N( c Lp= Inductance in primary winding in [mH] if Xopt.=0+ _" U; A& F/ g2 ]9 N
Inductance in primary winding in [ohm] if Xopt.=power freq.
/ v7 r! H0 Y- t! X/ S; }- Y! Q" ~ Vrs= Rated voltage in [V] secodary winding. 2 w6 c3 n3 I# N- F5 E6 G
Rs= Resistance in secondary winding in [ohm].
! t4 u$ l1 G0 M Ls= Inductance in secondary winding in [mH] if Xopt.=0
3 Q, a* ~# K5 ~- n; ]& W5 E8 z Inductance in secondary winding in [ohm] if Xopt.=power freq.3 j+ p9 z) c( B, N: r8 A* A
Vrt= Rated voltage in [V] tertiary winding.
7 R! J. Z2 `4 m' z+ Z/ ^3 I1 N$ C) O+ u Rt= Resistance in tertiary winding in [ohm].2 I: T" t# R. W$ t& z
Lt= Inductance in tertiary winding in [mH] if Xopt.=0
0 K- R! F6 a7 V' e4 I0 D Inductance in tertiary winding in [ohm] if Xopt.=power freq. ) p' s5 o) H. l0 M5 s9 T% e
RMS= unchecked: Current/Flux characteristic must be entered.2 n+ L. S& [7 R# K- F2 \- q
checked: Irms/Urms characteristic must be entered.4 d5 a( r8 {' A( Z" e
ATPDRAW performs a SATURATION calculation.
* @% F# @7 T" H. D' B. U+ B 3-leg core = checked: 3-leg core type transformer assumed. TRANSFORMER THREE PHASE2 N" D- q L# u
unchecked: 5-leg or 3-leg shell type assumed. TRANSFORMER.
% e& V$ I; \9 ]- X 3-wind.= turn on tertiary winding.
. {3 _6 k# o3 Y! ]! V" }3 tOutput specified the magnetization branch output (power&energy not supported).
{2 v9 _+ I" Q( U4 |, X' TNode : P= Primary side. 3-phase node.
8 R- q- H- ]: R. W1 X S= Secondary side. 3-phase node.7 }, G5 @# C# T( S ?- ^( I
PN= Neutral point primary side." v1 |2 c& t/ m) w1 {. Q
SN= Neutral point secondary side.* E. h. R& x+ I4 C$ G+ ?
T= Tertiary side. 3-phase node.
0 f' ]9 s6 {2 g" K' G Q% M TN= Neutral point tertiary side.. u8 O7 m2 q5 y+ P7 e2 l7 M
Sat= Internal node, connection of the magnetization circuit with saturation.; K, g D& \$ ^
The coupling is specified for each winding, with four coupling options: Y, D, A, Z
, d7 `# m* i! |2 m' w All phase shifts are supported.. g: o4 B3 e& q! L, ^ w
Special note on Auto-transformers:
/ i' E% {% ]8 P5 l' A; N The primary and secondary windings must be of coupling A(uto).
" `0 W& S" g: [( N0 t `Special note on ZigZag-transformers: : x; q! Q/ i/ P1 E+ j" i( _
For this type the user can specify a phase shift in the range <-60,0>&<0,60>.
4 N% Q* b( p0 `) F3 r- d Note that the values -60, 0 and +60 degrees are illegal (as one of the winding parts degenerates).
! u( j# j2 L4 t The phase shift is given relative to a Y-coupled winding. ' y- n5 l( c; C+ Z, f+ \
If the primary winding is Zigzag-coupled, all other windings will be shifted with it.2 k% v) C, q! l. F3 U: g
If the primary winding is D-coupled, 30 deg. must be added/subtracted to the phase shifts.
1 v7 a) y5 j/ J2 X For negative phase shifts the phase A winding starts on leg 1 (called z with voltage Uz) ) ~- a( f; [- K+ {
and continues in the opposite direction on leg 3 (called y with voltage Uy).# I$ Z( n0 H4 P/ }; W- c i5 J
For negative phase shifts the phase A starts on leg 1
( k) q% G: X& J3 u! Z: [7 Q" b and continues in the opposite direction on leg 2.
2 J% }; I J& F1 l' X$ p" k9 G The normal situation is to specify a phase shift of +/- 30 deg.
# I- M W: j! i$ B& ~ in which case the two parts of the winding have the same voltage level and leakage impedance.% o' E9 K; c: g% T+ p# y* X
In general the ratio between the second part of the winding Uy and the first part Uz is
J3 ], y6 {( h5 m! Y n=Uy/Uz=sin(a)/sin(60-a) where a is absolute value of the phase shift.0 ?* x! l& m4 r% \8 l
This gives:3 Q5 ^! s! G0 y% d) X
Uz=U/(cos(a)+n*cos(60-a)) and Uy=Uz*n0 ]7 u+ S9 ~( C- W
Lz=L/(1+n*n) and Ly=Lz*n*n, Rz=R/(1+n) and Ry=Rz*n , Z' h5 S6 W2 }
where Lz and Ly are the leakage inductance of each part of the winding (L is the total leakage inductance)
3 H9 U Q8 u" I- I$ B7 d and Rz and Ry are the winding resistance of each winding part (R is the total).
% n; G0 y' }; r% | The parameters Uz, Uy, Zz, and Zy are automatically calculated by ATPDraw based on the
9 _8 y- z" t8 X2 r: E0 } equivalent parameters U and Z and the phase shift, a.2 T q0 _9 g5 M0 n5 k4 w: j2 N
7 Y) k$ l8 Y6 V! z: c& S
) T! l" h7 e/ u. j6 NPoints: It's possible to enter 9 points on the current/flux characteristic.
' s6 H5 H) g1 y6 Z8 D( Q/ ^ The required menu is performed immedeately after the input menu.
3 V; S8 l# g0 h The points should be entered as increasingly larger values. 8 ] |4 _; A# P/ c: T
The point (0,0) is not permitted (added internally in ATP).
- P0 ]2 x; V0 ^6 [RuleBook: IV.E.1-2 or 3. |
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