Home |
Search |
Today's Posts |
|
#1
![]() |
|||
|
|||
![]()
Hi all,
Firstly, does anyone bother designing with Y-parameters *at all* these days? Then... (talking of the common-emitter configuration in this case) The only variable according to the Ebers-Moll transistor model apart from the device-specific "Is" which has any effect on Ic is the potental difference applied across the B/E junction. The signal voltage thus applied is loaded by the resistance of this diode. At DC., the loading is at a maximum and the entire PD appears across it. Right so far? As the applied signal voltage increases in frequency, the feedback capacitance (B-C) and the B-E junction capacitance form an AC bypass path across the B/E resistance above-mentioned. The two capacitances acting in concert shunt more and more of the applied signal voltage to ground, bypassing the emitter diode resistance, lowering the device input impedance and resulting in less and less applied Vbe across this diode and consequently less and less Ic output swing? What I'm getting at is that Ebers-Moll is still good at RF, *provided* one allows for the bypassing of the emitter diode's resistance by the combination of Cb and Ce. Correct? And CJC and CJE are the relevant Spice model parameters? Thanks, p. -- "What is now proved was once only imagin'd." - William Blake, 1793. |
#2
![]() |
|||
|
|||
![]()
You didn't even mention base spreading resistance, a major
figure of merit for RF transistors. Newer designers have considerably lower r-sub-bb-prime than legacy transistors. Look up the hybrid-pi transistor model. SiGe technology's claim to fame is low base spreading resistance. Rick N6RK "Paul Burridge" wrote in message ... Hi all, Firstly, does anyone bother designing with Y-parameters *at all* these days? Then... (talking of the common-emitter configuration in this case) The only variable according to the Ebers-Moll transistor model apart from the device-specific "Is" which has any effect on Ic is the potental difference applied across the B/E junction. The signal voltage thus applied is loaded by the resistance of this diode. At DC., the loading is at a maximum and the entire PD appears across it. Right so far? As the applied signal voltage increases in frequency, the feedback capacitance (B-C) and the B-E junction capacitance form an AC bypass path across the B/E resistance above-mentioned. The two capacitances acting in concert shunt more and more of the applied signal voltage to ground, bypassing the emitter diode resistance, lowering the device input impedance and resulting in less and less applied Vbe across this diode and consequently less and less Ic output swing? What I'm getting at is that Ebers-Moll is still good at RF, *provided* one allows for the bypassing of the emitter diode's resistance by the combination of Cb and Ce. Correct? And CJC and CJE are the relevant Spice model parameters? Thanks, p. -- "What is now proved was once only imagin'd." - William Blake, 1793. |
#3
![]() |
|||
|
|||
![]()
In article 4hFLc.141721$JR4.5322@attbi_s54,
"Rick Karlquist N6RK" writes: You didn't even mention base spreading resistance, a major figure of merit for RF transistors. Newer designers have considerably lower r-sub-bb-prime than legacy transistors. Look up the hybrid-pi transistor model. SiGe technology's claim to fame is low base spreading resistance. What you say about rbb is true, but SiGe has other 'cool' characteristics, some derived from low rbb, and some due to other effects of the 'strained' silicon?... Ignoring the rbb itself, SiGe tends also to have very low 1/f noise and good LF noise in general. Also, it tends to have high Beta (at LF.) So, where an RF transistor might tend to have a Beta of 20-50, an SiGE part might be 100-300 or higher. With the combo of the low rbb (and low 1/f noise), along with the high Beta, the total amount of input current noise and input voltage noise is damned low. SiGe would make good oscillators (for less PM noise) and of course, good preamps. This is one case where GaAs FETS that are very fast, might be undesirable because of their worse 1/F noise characteristics. One big disadvantage of the typical SiGe transistors is that their breakdown voltage is low. However, the tradeoff of breakdown voltage is BETTER for a given frequency response and Beta than a normal Si transistor. The SiGe transistors are also not very expensive. A part that works well with reasonably low distortion and reasonably low noise figure at 600MHz would be significantly less than $1.00. 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. John |
#4
![]() |
|||
|
|||
![]()
Hi John,
Interesting. As a tubehead myself, I have not heard of these. Who mfrs them? What's a typical part #? Thanks :-) -- Gregg t3h g33k "Ratings are for transistors....tubes have guidelines" http://geek.scorpiorising.ca |
#5
![]() |
|||
|
|||
![]()
Gregg schrieb:
Hi John, Interesting. As a tubehead myself, I have not heard of these. Who mfrs them? What's a typical part #? SiGe Transistors? One example: http://www.infineon.com/cmc_upload/d...669/bfp620.pdf -- Cheers Stefan |
#6
![]() |
|||
|
|||
![]()
John S. Dyson wrote...
The SiGe transistors are also not very expensive. A part that works well with reasonably low distortion and reasonably low noise figure at 600MHz would be significantly less than $1.00. Examples of low-cost high-performance (30GHz at 10mA) SiGe transistors would be Infineon's BFP620 (82 cents at DigiKey) http://www.infineon.com/cgi/ecrm.dll....jsp?oid=26182 and Philips' BFU510 and BFU540 http://www.semiconductors.philips.com/pip/BFU510.html http://www.semiconductors.philips.com/pip/BFU540.html The Philips transistors look good, but I don't know where to get them. Mouser stocks a set of CEL's nice SiGe transistors, http://www.mouser.com/?handler=produ...riteria =SiGe Thanks, - Win (email: use hill_at_rowland-dot-org for now) |
#7
![]() |
|||
|
|||
![]() |
#8
![]() |
|||
|
|||
![]()
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 |
#9
![]() |
|||
|
|||
![]() |
#10
![]() |
|||
|
|||
![]()
Rick Karlquist N6RK wrote:
You didn't even mention base spreading resistance, a major figure of merit for RF transistors. Newer designers have considerably lower r-sub-bb-prime than legacy transistors. Look up the hybrid-pi transistor model. SiGe technology's claim to fame is low base spreading resistance. Rick N6RK "Paul Burridge" wrote in message ... Hi all, Firstly, does anyone bother designing with Y-parameters *at all* these days? Then... (talking of the common-emitter configuration in this case) The only variable according to the Ebers-Moll transistor model apart from the device-specific "Is" which has any effect on Ic is the potental difference applied across the B/E junction. The signal voltage thus applied is loaded by the resistance of this diode. At DC., the loading is at a maximum and the entire PD appears across it. Right so far? As the applied signal voltage increases in frequency, the feedback capacitance (B-C) and the B-E junction capacitance form an AC bypass path across the B/E resistance above-mentioned. The two capacitances acting in concert shunt more and more of the applied signal voltage to ground, bypassing the emitter diode resistance, lowering the device input impedance and resulting in less and less applied Vbe across this diode and consequently less and less Ic output swing? What I'm getting at is that Ebers-Moll is still good at RF, *provided* one allows for the bypassing of the emitter diode's resistance by the combination of Cb and Ce. Correct? And CJC and CJE are the relevant Spice model parameters? Thanks, p. -- "What is now proved was once only imagin'd." - William Blake, 1793. Beat me to it; see my comment. |