Home |
Search |
Today's Posts |
#11
![]() |
|||
|
|||
![]()
I read in sci.electronics.design that Paul Burridge
wrote (in 8afvf05guvnvmjgqtafgau2d2li3ckn ) about 'The bi-polar transistor at RF', on Thu, 22 Jul 2004: IOW, as the signal frequency increases, the BSR becomes the dominant component of the device's input impedance... Phew! Unless of course, someone knows otherwise... Emitter lead inductance? -- Regards, John Woodgate, OOO - Own Opinions Only. The good news is that nothing is compulsory. The bad news is that everything is prohibited. http://www.jmwa.demon.co.uk Also see http://www.isce.org.uk |
#12
![]() |
|||
|
|||
![]()
On Thu, 22 Jul 2004 14:41:45 +0100, John Woodgate
wrote: I read in sci.electronics.design that Paul Burridge wrote (in 8afvf05guvnvmjgqtafgau2d2li3ckn ) about 'The bi-polar transistor at RF', on Thu, 22 Jul 2004: IOW, as the signal frequency increases, the BSR becomes the dominant component of the device's input impedance... Phew! Unless of course, someone knows otherwise... Emitter lead inductance? Er, yes, but I'm only interested in the *internal* characteristics of the device here, so even the bonding wires' inductance isn't an issue. Thanks for giving me the chance to clarify, though. -- "What is now proved was once only imagin'd." - William Blake, 1793. |
#14
![]() |
|||
|
|||
![]() |
#15
![]() |
|||
|
|||
![]()
On Thu, 22 Jul 2004 15:46:25 +0100, John Woodgate
wrote: I read in sci.electronics.design that Paul Burridge wrote (in 61kvf05660gk62pnm7o3bthepkujnep ) about 'The bi-polar transistor at RF', on Thu, 22 Jul 2004: Er, yes, but I'm only interested in the *internal* characteristics of the device here, so even the bonding wires' inductance isn't an issue. Thanks for giving me the chance to clarify, though. A bit of the emitter lead is inside the encapsulation, and a bit is on the die. Thank you, John, that gives me another chance to re-state the question more succinctly. I'm not concerned with inductances here at all, though. Does the Ebers-Moll equation hold good at UHF+, provided the value one inserts for Vbe is adjusted to account for the loss of signal voltage the B/E junction will suffer as much of it (the applied signal voltage) is shunted around it via the device's internal capacitances? There! I think I've nailed it this time! -- "What is now proved was once only imagin'd." - William Blake, 1793. |
#16
![]() |
|||
|
|||
![]()
In article ,
Paul Keinanen writes: On Thu, 22 Jul 2004 03:09:10 +0000 (UTC), (John S. Dyson) wrote: One big disadvantage of the typical SiGe transistors is that their breakdown voltage is low. Unless the transistor is too fast for a given layout, SiGe can be used at low frequencies (e.g. VHF) while still avoiding the low frequency noise problems that are common from GaAs FETS and even other fast BJTs. While the IP3 and compression figures may good to comparable devices working in the GHz bands, the huge gain with the low Vce (typically less than 2.3 V) will damage the input IP3 values quite quickly at VHF. This can be a problem in the VHF and lower UHF bands, in which signal levels can be quite high and multiple strong signals may pass the front end selectivity. "Noiseless feedback' is very helpful to mitigate the excess amounts of gain, while pushing the return loss match (the impedance match) closer to the noise match (the input impedance where the noise is lowest.) A simple emitter (source) inductor and a little bit of parallel, noisy feedback can be used to tame some of the interesting UHF+ components. (The emitter (source) inductor is a case where a small amount of inductance is much better than too much, because instability can ensue with too much series feedback (too large an emitter (source) inductor).) I do agree with your implication that a high current device can be helpful at low frequencies, but some SiGe components do seem to maintain reasonable noise performance at high currents. In any case, the SiGe components do give the GaAs type components a run for their money. In some cases, the SiGe components are actually better. The PHEMTs (HP 54143) are also an interesting variation on the 'fet' theme, which helps to mitigate some of the problems WRT GaAs. For example, a PHEMT can provide a good noise match at 50ohms, a transconductance of almost 1MHO at 60ma, and reasonable IP3 (38dBm isn't impossible.) Feedback can be especially helpful with the high transconductance FETs. John |
#17
![]() |
|||
|
|||
![]() |