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/ F& m+ Y7 e$ F8 t传输线 巴伦
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! `9 K; K! }$ j7 q7 g; R1 E# [1.基本原型:
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2.最佳传输条件:
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: }2 R6 W9 x; }, U% k2.2 传输线长度l应尽可能地小,工程设计中一般取<λ/8
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3.相关公式
`, H5 H+ ?1 w3.1传输损耗公式:( ?" |0 I8 t; h, J- q" S2 Q( P
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% l% V [( b4 r6 O0 q' p5 V T9 T3.2反射损耗公式为: 1 F w: F* L8 t1 |' s
3 u; Z( z4 k) o+ C- k4 k s
/ s9 Z" z. g: [- V. V% h- s式中。Rg为源阻抗。L0为空芯绕组电感,μ’为磁导率实部, μ”为磁导率虚部。磁损耗角正切tanδm=μ”/μ’。选择μ’高、tanδm大的材料能够 同时满足传输损耗、反射损耗的指标要求。
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5 J, _# P3 H& {3.3磁导率+ b6 `5 H4 Q, G
铁氧体磁芯磁导率随频率变化的影响:
& x7 y+ L* T: ]. U磁导率随频率 变化的公式为
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1 B5 o( r" Q" b2 E3 x式中,S为斯诺克常数,,fr为截止频率。
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将上式代人传输损耗公式进行分析得知应选择截止频率低、斯诺克常数高的磁芯材料。 ! O+ J; y$ K' |" J4 f, \5 O
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综上所述,可以得出磁芯材料的选取原则是要求低频初始磁导率μ’高、截止频率fr低、斯诺克常数S 高、损耗大tanδm的材料。 + R8 d- e" T6 ~7 _
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, H. ~# X/ r; b& z; p# S# `4.ADS 中低端巴伦模型
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BALUN1 (Balanced-to-Unbalanced Transformer (Ferrite Core)) 8 ?" M& G8 s. t3 K) E: N
Symbol 9 a/ A' x; `5 D3 v/ W
4 e; M3 C9 R8 @2 }+ eRange of Usage - S* h6 Z4 M3 }& |% c
Z > 0, Len > 0, AL > 0
' C9 W/ R# B9 H& l$ K5 E- \K ≥ 1: Z* V" P4 w9 j& P; r' x
A ≥ 0) Y& D: S7 J4 w4 o
F ≥ 0
! e+ t, C x3 ]6 R2 v' y( |7 R& nN ≥ 1 ! Q. j, B( T) y/ n, A4 s1 F
Parameters
/ r! Q5 t; i4 T. N/ g Name | Description | Units | Default | Z | Characteristic impedance of transmission line | Ohm | 50.0 | Len | Physical length of transmission line | mil | 12.0 | K | Effective dielectric constant(有效介电常数) | None | 2.0 | A | Attenuation (per unit length) of transmission line | dB/meter | 0.0 | F | Frequency for scaling attenuation | GHz | 1.0 | N | Number of turns | None | 5.0 | AL | Inductance index(电感指数) | nH | 960.0 | TanD | Dielectric loss tangent (介质损耗角正切) | None | 0 | Mur | Relative permeability (相对磁导率) | None | 1 | TanM | Magnetic loss tangent(磁损耗正切) | None | 0 | Sigma | Dielectric conductivity (介电导电率) | None | 0 | Temp | Physical temperature | °C | None | 4 {2 ] m5 }! ]7 X3 g# h8 d
· This component is a length of transmission line(specified by Z, Len, K, A and F) coiled around a ferrite core. , [7 w9 y% ?2 C! w; K2 W: Y7 M8 b
Choking inductance Lc accountsfor low-frequency roll-off and is given by
. j& C8 h% W! M! _1 B. d- WLc = N2 × AL
' G7 e( z4 W5 z% iA(f) = A (for F = 0)9 o& W* v1 f* Z+ ~8 U+ O( P. H5 L
A(f) = A(F) × file:///C:/Users/wanghai/AppData/Local/Temp/msohtmlclip1/01/clip_image013.png! W; {0 l2 c, x$ S. C! i! H
(for F ≠ 0)
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f = simulation frequency/ ~" n* l, C, o; B5 b
F = reference frequency for attenuation . f5 S- \" r) N4 q5 n3 w6 [& ? N3 n
For time-domain analysis, an impulseresponse obtained from the frequency-domain analytical model is used. Thiscomponent has no default artwork associated with it.
0 c4 B* ~: f3 X" `7 a· The "Temp" parameter is only used in noisecalculations.
* z) A- x" j0 O& N* N# N6 q· For noise to be generated, the transmission line must belossy (loss generates thermal noise). ' d% b5 I( F( m2 b
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5.小节:& f) W) h6 z q
调节ADS 中的参数可以仿真出巴伦对应的传输损耗;
1 @* E$ Y- I% f* A" F1 A; m% F介电常数环节需要进一步讨论;. . t: q6 Y1 Z5 f& A
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