Lumped Elements for RF and Microwave Circuits phần 1 pdf

... xix 1 Introduction 1 1 .1 History of Lumped Elements 1 1.2 Why Use Lumped Elements for RF and Microwave Circuits? 2 1. 3 L, C, R Circuit Elements 4 1. 4 Basic Design of Lumped Elements 6 1. 4 .1 Capacitor ... 14 Lumped Elements for RF and Microwave Circuits [13 ] Pengelly, R. S., and J. S. Turner, ‘‘Monolithic Broadband GaAs FET Amplifiers,’’...

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... in RFICs. At low frequencies, the total dc resistance of the coil is given by R dc = ᐉ Wt ␴ (3 .1) 32 Lumped Elements for RF and Microwave Circuits Y ′ 11 = Y 11 − (Y 12 + Y 14 )(Y 21 + Y 41 ) Y 22 + ... ′ 13 Y ′ 31 Y ′ 33 ͬͫ V 1 V 3 ͬ (2.22) where 78 Lumped Elements for RF and Microwave Circuits f res = 1 2 ␲ √ LC p (3.6) For L = 8nHandC p =...

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... 10 1. 0 0.4 14 0.7 0 .1 1,579 31 1. 61 8 4 10 1. 0 0.4 23 1. 7 0.3 3 ,18 1 26 0. 81 9 2 10 2.0 0.4 10 1. 2 0 .1 1 ,16 3 30 1. 44 10 4 10 2.0 0.4 19 2.9 0.3 2,8 91 21 0.68 11 2 10 0.4 0.6 17 0.6 0.2 1, 142 19 ... 0.2 1, 537 21 1.34 24 4 10 0.4 0.8 34 1. 4 0.8 5,455 23 0.74 25 2 4 1. 0 1. 0 8 0.9 0 .1 9 51 33 1. 84 26 2 6 1. 0 1. 0 12 1. 1 0 .1 1,479 32 1...

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... 0.0343 11 .0 18 1. 024, 40.3 1. 062, 41. 8 0.0220 16 .0 16 1. 290, 50.8 1. 3 31, 52.4 0. 015 2 22.0 14 1. 628, 64 .1 1.674, 65.9 0.0086 32.0 12 2.052, 80.8 2 .10 1, 82.7 0.0055 41. 0 10 2.588, 10 1.9 2.639, 10 3.9 ... 10 .0 0.274, 10 .8 0.3385 0.86 28 0.320, 12 .6 0.343, 13 .5 0. 212 9 1. 40 26 0.404, 15 .9 0.429, 16 .9 0 .13 39 2.20 24 0. 511 , 20 .1 0.5 41, 21. 3 0.08...

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... (− ␾ 1 /2) + B 11 cos (− ␾ 1 /2) B 12 sin (− ␾ 2 /2) (7 .10 ) ␾ 1 = M 1 ␲ + tan − 1 ͭ 2 ΀ B 11 + B 22 | B | ΁ 1 + B 2 22 − B 2 11 − | B 2 | ͮ (7 .11 a) ␾ 2 = M 2 ␲ + tan − 1 ͭ 2 ΀ B 22 + B 11 | B | ΁ 1 ... tan − 1 ͭ 2 ΀ B 22 + B 11 | B | ΁ 1 + B 2 11 − B 2 22 − | B | 2 ͮ (7 .11 b) where B 11 = B 11 /Y 1 , B 22 = B 22 /Y 2 , B 12 = B 12 / √ Y 1 Y 2...

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... (m 2 ) W = ᐉ (mm) 10 0.29 × 10 − 6 0.539 20 0.58 × 10 − 6 0.762 50 1. 45 × 10 − 6 1. 204 10 0 2.90 × 10 − 6 1. 703 200 5.80 × 10 − 6 2.408 250 Lumped Elements for RF and Microwave Circuits material, ... = 15 mil; and (d) double via, h = 25 mil. (From: [20].  19 92 IEEE. Reprinted with permission.) 252 Lumped Elements for RF and Microwave Circuits...

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... [16 ] and shown in Figure 10 .11 . Here 302 Lumped Elements for RF and Microwave Circuits ␾ ˜ ( ␤ ,0)= 0 (10 .1a) ␾ ˜ ( ␤ , h ′ 4 ) = 0 (10 .1b) ␾ ˜ ( ␤ , h 1 + 0) = ␾ ˜ ( ␤ , h 1 − 0) (10 .1c) ⑀ r1 d dy ␾ ˜ ( ␤ , ... (11 .31a) 2 ␲ f H = ␻ H = R ′ G /[L 1 (1 − k )] (11 .31b) Equation (11 .31a) is the same as (11 .29) when R 1 = 0 and k = 1. The relative bandwidth...

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... 0.900 −0.46 10 .00 1. 11: 1 4 16 0.940 −0.26 12 .30 1. 06 :1 5 25 0.960 −0 .17 14 .10 1. 04 :1 6 36 0.973 −0 .12 15 .70 1. 03 :1 8 64 0.984 −0.07 18 .30 1. 02 :1 10 10 0 0.990 −0.04 −20.00 1. 01: 1 12 14 4 0.993 ... R 2 (⍀) R 1 (⍀) R 2 (⍀) R 1 (⍀) R 2 (⍀) 0.5 1. 4 868 2.9 1, 737 3 843 1 2.9 433 5.8 869 6 409 3 8.5 14 2 17 .6 292 20 12 0 5 14 82 31 179 39 64 10 26 3...

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... 1. 444 ͪͮ − 1 for (W /h ≥ 1) (14 .1a) (14 .1b) where ␩ = 12 0 ␲ ohm and ⑀ re = ⑀ r + 1 2 + ⑀ r − 1 2 F(W /h) (14 .2) F(W /h) = ͭ (1 + 12 h/W ) − 1/ 2 + 0.0 41( 1 − W /h ) 2 for (W /h ≤ 1) (1 + 12 h/W ) − 1/ 2 for ... /hZ 0 ⑀ re (dB/cm) (pF /10 0 ␮ m) (nH /10 0 ␮ m) 25 0.07 16 4.6 2.75 0. 214 0.003 0.0 91 50 0 .13 14 2.2 2.82 0 .15 9 0.004 0.080 75 0.20 12 8.5...

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... 2,049 1, 445 1, 020 720 1 260 18 1 12 9 91 3 10 7 76 53 38 7 715 13625 10 63 44 31 22 *Gold conductors are 4.5 ␮ m thick except in 3- ␮ m polyimide case, where t = 9 ␮ m and ⑀ rd = 3.2. Figures 14 .10 , 14 .11 , ... 3 41 49 See also Transformers substrates, 57 Ferroelectric capacitors, 214 16 GaAs-based inductors, 86 11 8 BST, 215 , 216 2.5-turn, 93 materials, 214 compactor,...

Ngày tải lên: 08/08/2014, 01:21