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% J5 l. F* z: V) }2 n9 ~传输线 巴伦
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1.基本原型:, ^% {3 n: u! e% a/ W0 b" y2 k% v, p
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2.最佳传输条件:2 P0 M0 F- {% t. ]( t: n
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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 ! k3 ?& U/ R' }& y6 j. n
- o- W0 k8 ?2 ` Q3.相关公式
. c7 L" [# D& ]; {- t( P8 n3.1传输损耗公式:
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3.2反射损耗公式为:
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$ L. }4 f" ]0 U0 U2 Y- [5 N+ L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
" [3 a0 y/ R- S ~# @铁氧体磁芯磁导率随频率变化的影响:
6 [- }0 L. D7 u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。 $ \1 v$ O) k3 z! s, D) D
4 F$ O8 e, [( p* f2 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。 $ R/ O, w. n- e. s/ }5 R
# _/ W8 m' A0 T! D- k. e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。 1 A# e# Q% i' C8 W1 x
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4.ADS 中低端巴伦模型9 ]! i8 H# W! q" [7 x# A' f
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BALUN1 (Balanced-to-Unbalanced Transformer (Ferrite Core)) $ P# g; V' a9 H2 a
Symbol 1 t2 h% L: b9 U( v# V9 P
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Range of Usage
$ Z( Y) _+ B; V' h* ^4 CZ > 0, Len > 0, AL > 0
s" E# j6 _5 XK ≥ 1
/ E6 |% X8 t2 Y3 p) QA ≥ 0$ E" T8 y" v+ [$ {* Q6 ~2 f
F ≥ 0
/ G8 ] |! D/ p8 t8 M8 i! S: iN ≥ 1 1 w% t2 j3 }' b$ y6 m; R" J
Parameters 9 G2 ?+ }/ B* Y0 d: o% W* u
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 |
- O7 K5 D5 ~ c% C· This component is a length of transmission line(specified by Z, Len, K, A and F) coiled around a ferrite core. ) L4 s# {% U- q- \" Z
Choking inductance Lc accountsfor low-frequency roll-off and is given by
1 Z8 P: i5 A, l+ Z& C6 I. S2 xLc = N2 × AL
1 B" r" q3 [; EA(f) = A (for F = 0)
% _7 W$ @% o5 ?6 eA(f) = A(F) × file:///C:/Users/wanghai/AppData/Local/Temp/msohtmlclip1/01/clip_image013.png
' f0 }. [1 j$ c4 r* ^(for F ≠ 0)6 D0 h5 X9 v7 w! p2 [( c9 B
where. {- ]1 D/ p' I* W6 z
f = simulation frequency- ^ q% l! P% y1 X7 e1 c m- p) ?
F = reference frequency for attenuation - E% A. c& ~) n8 Z
For time-domain analysis, an impulseresponse obtained from the frequency-domain analytical model is used. Thiscomponent has no default artwork associated with it.
2 {, \5 T8 l7 f3 `' ~· The "Temp" parameter is only used in noisecalculations. : Q7 h9 U5 \# ~6 V- Z
· For noise to be generated, the transmission line must belossy (loss generates thermal noise). . x E: V+ g- Q3 \+ m \7 P
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5.小节:
) @% x4 \0 f" D- C2 ^3 \, N调节ADS 中的参数可以仿真出巴伦对应的传输损耗; . o/ S% ?! G) ?. r7 x# T6 e, A
介电常数环节需要进一步讨论;.
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