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发表于 2013-2-24 23:43:40
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Name : LINEZT_3 - Distributed parameters (Clarke) 3 phase. Transposed/ g) G) q6 D- f" J `% u
Card : BRANCH6 G5 C) l$ D I( S. a: P
Data: Values are entered in the two independent modes of the system, here called + and 0. P4 a0 Y1 d; e( U7 D
R/l= Resistance pr. length in [Ohm/m]1 [" V3 m- m3 R# o# j
The lossless part can be described in three ways9 K, @# O; C) V" `# P
0. Inductance L' in [mH/m] if Xopt=0 or in [ohm/m] if Xopt=power frequency
- y/ _# E: T6 X! e' ? Capacitance C' in [uF/m] if Copt=0 or in [uMho/m] if Copt=power frequency4 M x4 ], Z( b$ S" d! |
1. Modal surge impedance in [ohms]; Z=sqrt(L'/C')
8 ^+ c- M, |1 a- C9 R Modal propagation velocity in [m/s]; v=1/sqrt(L'*C')" u+ P$ f% ?2 V& R; s
2. Modal surge impedance in [ohms]
+ {) y9 s" `/ c% F5 {: n Modal propagation time in ; T=sqrt(L'*C')*length
1 |$ E) R% ?8 v1 b/ j, ^ Xopt. and Copt. are set in menu: ATP|Settings/Simulation.9 H1 }9 G* _) |: q* C: a
The user can choose conductance modeling G=0 (the usual case) and G=R*C/L (distortionless); e8 I8 `/ e, e: G4 i; A* m
length= length of line in [m]" \7 ` \% l: ? ]; S6 g9 @
Node : IN1= Start node. Letter 'A', 'B' or 'C'
# Z- v K/ @1 g5 ~ j' r is added to nodename for node 1, 2 and 3.
: M: w5 h1 T( i OUT1= End node. Letter 'A', 'B' or 'C'
* E! Y6 e( Q/ F8 s) q" }+ b2 R is added to nodename for node 1, 2 and 3.) y0 X1 U7 J3 B2 V" w4 B
Only branch voltage output is reliable.
* v3 V" v, b3 L3 V) K$ P" `0 P/ jRuleBook: IV.D.1 |
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