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发表于 2019-11-29 15:38
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汪洋大海 发表于 2019-9-6 09:31
1 w( b" c) {2 Lhttps://www.eda365.com/thread-188514-1-1.html
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奇怪,两者对比,偏差有点大。
$ ?) D B2 w9 O# T$ v4 b b1 tThe Bridged-T Attenuator is another resistive attenuator design which is a variation on the standard symmetrical T-pad Attenuator. b6 B# N( k9 n$ U8 Y& c' Y7 Y) E
As its name implies, the bridged-T attenuator has an additional resistive element forming a bridged network across the two series resistors of the standard T-pad.* @" x, W" ~- V/ B
This additional resistive element enables the circuit to reduce the level of a signal by the required attenuation without changing the characteristic impedance of the circuit
$ Z" m6 I+ ]% r/ b8 ias the signal appears to “bridge” across the T-pad network. Also the two series resistances of the original T-pad are always equal to the input source and output load
4 P6 \ E, w0 F, T4 _impedances.
' j0 c2 ]8 v& X2 w- AThe circuit for a “bridged-T attenuator”, ( T ) is given below.0 j4 ^7 Z) }# P# D: k
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O; w0 E( _- d7 a! L" H& U( yResistor, R3 forms the bridge network across a standard T-pad attenuator. The two series resistors, R1 are chosen to equal the source/load line impedance. One major
1 |* l) _" b7 zadvantage of the bridged-T attenuator over its T-pad cousin, is that the bridged-T pad has a tendency to match itself to the transmissions lines characteristic impedance.
( ^/ Z( d/ x# |However, one disadvantage of the bridged-T attenuator circuit is that the attenuator requires that its input or source impedance, ( Z ) equals its output or load impedance,
4 G9 M" o5 B3 f* N0 A; L( Z ) and therefore cannot be used for impedance matching.7 J" `( Y+ |: s
The design of a bridged-T attenuator is as simple as for the standard T-pad attenuator. The two series resistors are equal in value to the lines characteristic
9 Q, O; G3 k, G2 f' X$ Eimpedance and therefore require no calculation. Then the equations given to calculated the parallel shunt resistor and the additional bridging resistor of a bridged-T attenuator circuit used for impedance matching at any desired attenuation are given as:" F U& K7 h9 }1 _
Bridged-T Attenuator Equations:: `7 c( Q# K! i0 b/ c; [( h6 `6 e7 u
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+ r5 ]# u! z/ t* x- ewhere: K is the impedance factor, and Z is the source/load impedance.
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