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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
8 M$ \9 \3 O/ xhttps://www.eda365.com/thread-188514-1-1.html
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奇怪,两者对比,偏差有点大。 @5 a6 u1 |; i$ o* |
The Bridged-T Attenuator is another resistive attenuator design which is a variation on the standard symmetrical T-pad Attenuator.
" g! X1 r" \5 K2 T: y4 SAs 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.
9 o; x+ i7 B. \" K3 W5 B9 uThis 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' W' E" F) j/ \% y3 i: P9 D
as 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
$ K: p4 ^3 }& Y+ l2 V. |) @impedances.
9 U: ^& d, m b' d3 PThe circuit for a “bridged-T attenuator”, ( T ) is given below.
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3 i6 J4 N) a% Z4 \) \& |2 I* @Resistor, 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 u1 b/ u' d9 L: c4 Eadvantage 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., H6 `* d! ` H+ D) B
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,/ l+ r( j1 i) u$ X
( Z ) and therefore cannot be used for impedance matching.- Z) v+ B4 ~" y0 |
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) E) h9 t1 y7 u
impedance 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- \* ^; v0 l8 J: XBridged-T Attenuator Equations:- o1 o1 s$ {- m+ O6 l* q
6 s( H# e- i+ D+ _2 Z
+ H$ j' R T: m4 O+ ?where: K is the impedance factor, and Z is the source/load impedance.
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