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传输线 巴伦
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1.基本原型:2 `/ d! ^6 n7 _5 T
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2.最佳传输条件:
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2.2 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, |/ k7 E G1 s; i$ Q$ I: {1 D
3.1传输损耗公式:1 p3 Y6 B, E) m2 e% j* |! d
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3.2反射损耗公式为:
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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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3.3磁导率
) [$ q% d8 I6 W% x铁氧体磁芯磁导率随频率变化的影响:
$ t- `! }/ N$ k; O磁导率随频率 变化的公式为
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式中,S为斯诺克常数,,fr为截止频率。
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; @8 l, }' j; h* d) J; c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。 6 ?8 v8 i. Z* H
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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。 3 r F3 P8 N# T: A( ]
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1 j7 r: W7 Z9 i+ E+ i0 ?, K u4.ADS 中低端巴伦模型8 G5 U5 w) ?- i# t
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BALUN1 (Balanced-to-Unbalanced Transformer (Ferrite Core)) 1 t% l3 x5 X; N( J
Symbol " y, J. w- I9 N' q8 c
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Range of Usage " F5 _% ~) s" o) X. z
Z > 0, Len > 0, AL > 0
5 w d4 u( b; c! X1 x' `- {9 ZK ≥ 1
( h9 p. ^7 w/ ]' x. i# [1 nA ≥ 0
9 k K! E8 z8 Q; JF ≥ 0. b% F' ]! }9 j5 L
N ≥ 1
) S- } O3 I M" n! t6 m5 ^Parameters
2 n4 T9 q1 m6 @- D: ^% U) x! I 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 | ( u+ J$ y& i: p' |3 @4 S. q
· This component is a length of transmission line(specified by Z, Len, K, A and F) coiled around a ferrite core.
U" s' J* e+ b" vChoking inductance Lc accountsfor low-frequency roll-off and is given by, M% K' f8 @: x" x! }
Lc = N2 × AL
1 B( ?7 y! z, ?( @) S( g( W& LA(f) = A (for F = 0)
5 |* Z' k' L" F) W: d4 [: K, uA(f) = A(F) × file:///C:/Users/wanghai/AppData/Local/Temp/msohtmlclip1/01/clip_image013.png! u$ K& W2 r/ F& h
(for F ≠ 0)
* J. [0 Y$ b% H8 Wwhere
9 d2 v3 Y6 i% e; x' z. o" X l1 S% F" Uf = simulation frequency2 D; t1 q; u5 O5 J) i3 [8 G
F = reference frequency for attenuation - R# U+ z2 x. b# t. F) r$ t
For time-domain analysis, an impulseresponse obtained from the frequency-domain analytical model is used. Thiscomponent has no default artwork associated with it. 7 A3 H- q$ ^3 d( Y e! P$ y' h
· The "Temp" parameter is only used in noisecalculations.
- j- ^$ ~' G- ^3 G· For noise to be generated, the transmission line must belossy (loss generates thermal noise). 9 g: S+ @" ~3 E. |8 _' F
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5.小节:
S/ M# x( E% C调节ADS 中的参数可以仿真出巴伦对应的传输损耗;
1 I; h# w% x# M介电常数环节需要进一步讨论;.
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