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$ ?2 T! s- \* @. z% Y传输线 巴伦5 A. H8 y7 G/ ~
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& f) T8 N9 n4 S0 B3 |1.基本原型:, H% ? ~, z" h: q
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3 E1 a, m) T# t0 Y' t. s2.最佳传输条件:6 J$ a4 g8 d/ J: G
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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 , I8 w: O) B# V# Z, B
* z0 U+ W' r% y3.相关公式7 B; R& J/ Y6 k
3.1传输损耗公式:) x2 X# T. i; h' v/ t X
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( H8 g/ s5 u5 n! {; m3.2反射损耗公式为:
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' L! ?, a' C! {% _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。 ( A- F+ b+ B; B3 Q0 u3 z2 b0 b
( M3 b8 O6 D0 D# u3.3磁导率
) G# P2 |0 k7 G3 p ]! X9 i铁氧体磁芯磁导率随频率变化的影响:
2 O; e8 v! d2 l/ k7 m磁导率随频率 变化的公式为
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0 K! h3 r8 F3 _6 Q式中,S为斯诺克常数,,fr为截止频率。 4 `: i3 a! ~6 }0 c& F) m$ z1 S
6 L/ D+ v' g, D1 _. u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。
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- C9 g& P; y4 Y: T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。 i# {6 S+ }- c B3 @
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! D/ T5 v) W% r0 c' T2 X) Z7 l4.ADS 中低端巴伦模型
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BALUN1 (Balanced-to-Unbalanced Transformer (Ferrite Core))
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Range of Usage 2 {) n3 L& ~/ n
Z > 0, Len > 0, AL > 0/ T* V( y5 j/ } ]4 N4 I
K ≥ 1. C A' M8 g+ g- x8 C
A ≥ 00 _- E8 V+ C& N; a, K
F ≥ 05 T& |8 x& K6 s: ]
N ≥ 1 . Y: I( i9 k, u) ]% b% n: \/ L
Parameters 2 [, y& Q! ~1 q& C
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 |
0 ^% [( D# X- A2 U. j" u· This component is a length of transmission line(specified by Z, Len, K, A and F) coiled around a ferrite core. : s1 \* z# X0 P- N* G6 O9 l
Choking inductance Lc accountsfor low-frequency roll-off and is given by
" N* c8 s: d: N$ I2 ^Lc = N2 × AL, h5 w: K( V* D9 K
A(f) = A (for F = 0)8 F3 Z2 z/ ~+ @1 }, D
A(f) = A(F) × file:///C:/Users/wanghai/AppData/Local/Temp/msohtmlclip1/01/clip_image013.png
+ y& |" T) R. b(for F ≠ 0)
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f = simulation frequency3 V* \# o/ ?- e/ L0 Z( ~" m2 N, r
F = reference frequency for attenuation 4 c5 b8 g% p: j
For time-domain analysis, an impulseresponse obtained from the frequency-domain analytical model is used. Thiscomponent has no default artwork associated with it.
* Y% d9 |/ A5 M# @. l/ T+ j5 H; ?· The "Temp" parameter is only used in noisecalculations. ' k; |/ r9 J+ Y1 n9 D7 w0 t3 a
· For noise to be generated, the transmission line must belossy (loss generates thermal noise). 3 F9 p! Q8 a4 n# y$ N/ W
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5.小节:' V% w0 U; K w& J9 t: W
调节ADS 中的参数可以仿真出巴伦对应的传输损耗;
/ a, \! I. i# \$ J, j3 P: J介电常数环节需要进一步讨论;. ! {0 L! ~0 o+ D2 W
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