Analog ORricothetroll said:I just don't know how to select the higher of two signals
Analog ORricothetroll said:I just don't know how to select the higher of two signals
Analog OR
It would, provided the vactrol has the necessary low "on" resistance (or using several in parallels). The results would be source-dependant, and there would probably be some frequency response issues under GR. In fact, if the input used a xfmr, a "standard" vactrol could be used.ricothetroll said:Hi !
After a few very busy weeks, I finally have some time again to work on this project.
An idea came to my mind : what about putting a vactrol across the hot and cold input, and use it as an input limiter ? using it as the reduction cell of a feedback design, it could make the preamp virtually un-clippable ! I guess that it will interact with the mic's output impedance, it's not-necessarly-log response wil be compensated by the feedback topology as for fet compressors like 1176, and its noise will be balanced out.
I realise it's quite utopic, but I'd be glad to know at least why it wouldn't work
Best regards.
Eric
That would not be right, because the attack time would be the time the vactrol takes to recover from full light, which is loooong. You want the vactrol to be a shunt element, either on the source or the NFB path.ricothetroll said:Well you're right for the unpredictable effet with different mics. Maybe I should try to put a low Ron vactrol (VTL5C3) in series with the THAT1512's gain resistor.
That would not be right, because the attack time would be the time the vactrol takes to recover from full light, which is loooong. You want the vactrol to be a shunt element, either on the source or the NFB path.
A limiter pre or as part of the gain stage is rather appealing...the Shure SM82 (US 4000370) Line Mic was a fantastic piece of kit and provided excellent results even with the most exuberant sports reporters.
I did try a vactrol/optofet in series with the gain resistor with a 2017 some years ago but never managed to get the required Ron for the normal state.
Any one seen the Aphex 207 mic pre schematic? the data notes that it's transformerless. Does it use their 6266423 patent?
Most of the mic front end limiters i've encountered in broadcast equipment are based on shunting the feedback resistance of the gain stage with a Vactrol....
tc
It would certainly work, but would not prevent the first stage to distort when overloaded. Putting the vactrol in parallels with C2 would not have this limitation but the limiter's behaviour would much depend on the actual setting of the gain pot, in particular at the lowest gain settings.ricothetroll said:What would be easy would be to implement an LDR as a shunt across R6 in Samuel's "shared gain topology" :
If you wanted to include this in a Cohen topology, you would need two perfectly matched potentiometers. Any mismatch would ruin the CMRR. That's what THAT have done to a certain extent with the 5171, taking advantage of laser trimming for controlling the resistors..Could this circuit, though more expensive, implemented with high end opamps, compete with Graeme Cohen's topology's specifications ?
ricothetroll said:What would be easy would be to implement an LDR as a shunt across R6 in Samuel's "shared gain topology" :
http://home.datacomm.ch/gronerfamily/DIY/Shared_Gain_PreAmp/Shared_Gain_PreAmp_r1.gif
And use it with a LL1528 (that would give me a "free" 14dB gain when configured in 1:5).
Could this circuit, though more expensive, implemented with high end opamps, compete with Graeme Cohen's topology's specifications ?
Samuel ?
Thanx a lot for your help !
Best regards.
Eric
The 1512 is optimized for low impedance sources '200-800 ohms). With a 1/5 xfmr, the impedance is about 5kohms, so the noise factor is too high. Increasing the impedance in order to make the vactrol's job easier is detrimental to the noise figure. If you want to use a higher Z, you must use an input stage that is optimized for 5kohms; fortunately, any good old 5534 or one of the new über opamp will be perfectly happy with that.ricothetroll said:I did a comparison of the THAT1512 circuit with and without the trafo, to see if the DCR adds any significant noise. Here are the results, normalised for compensating the gain difference :
The input is terminated with a 220R 0,6W metal film resistor. LL1528 is configured 1:5 and has a 900R DCR on the secondary (in series for 1:5)
We can hear that the hiss (white noise) is pretty equivalent, but there is an added "vinyl crackling" with the trafo in the circuit. Though I'm not used to recognising to those noises, the "crackling" doesn't look like thermal noise to me. Could that be burst noise ? Or is it more likely some parasitics, magnified by the 14dB extra gain of the LL1528 ? The circuit lies unshielded on a breadboard. By the way there is a slight hum on the test without the trafo, most certainly due to the lack of shielding and the long test wires.
The 1512 is optimized for low impedance sources '200-800 ohms). With a 1/5 xfmr, the impedance is about 5kohms, so the noise factor is too high. Increasing the impedance in order to make the vactrol's job easier is detrimental to the noise figure. If you want to use a higher Z, you must use an input stage that is optimized for 5kohms; fortunately, any good old 5534 or one of the new über opamp will be perfectly happy with that.
There must be something wrong with the calc.ricothetroll said:I did some calculations that confirm that the trafo in front of the 1512 isn't a good idea, based on TI's noise calculator sheet :
- THAT1512 without trafo : EIN = 1.162 nV/Hz^0.5
- THAT1512 with trafo : EIN = 3.514 nV/Hz^0.5 => + 4,22 dB compared to 1512 without trafo :s
- Shared gain with NE5532 : EIN = 2.65 nV/Hz^0.5 => + 1.77 dB / 1512
- Shared gain with OPA2277 : EIN = 2.40 nV/Hz^0.5 => + 0.91 dB / 1512
There must be something wrong with the calc.
The 5532's noise voltage is specified at 5nV/sqrtHz. Provided with a source impedance of 7 kohms, the EIN should be around 7nV/sqrtHz.
Reflected to the input of a 1:5 xfmr, that computes at 1.4. The 5534 has a better (guranteed noise performance at 3.5, which would put its noise factor very close to that of the 1512 (provided the right xfmr).
I don't understand the 2.65 figure
Well, I couldn't use the calc (I'm using a Noptebook) but using the 5532's noise specs, I get 5nV/sqrtHz for noise voltage and 0.7pA/sqrtHz multiplied by 7k that gives another 5nV/sqrtHz; combined quadratically, that computes to 7nV/sqrtHz. THe other resistances are negligible.ricothetroll said:There must be something wrong with the calc.
The 5532's noise voltage is specified at 5nV/sqrtHz. Provided with a source impedance of 7 kohms, the EIN should be around 7nV/sqrtHz.
Reflected to the input of a 1:5 xfmr, that computes at 1.4. The 5534 has a better (guranteed noise performance at 3.5, which would put its noise factor very close to that of the 1512 (provided the right xfmr).
I don't understand the 2.65 figure
Well, from TI's noise calculator, I obtain :
- 624,6 nV/sqrtHz output noise of the first stage (non inverting, Rs = 6k95, R2/R1 = 22k/470, G=47,81)
I'm not sure; are you using arithmetic summing or quadratic? (not that is changes much since the 2nd stage noise is swamped by the first).- Total noise = 624,6n x 9,16 + 77,3n = 5,80 uV/sqrtHz
I couldn't find how to do it on a notebook perched on my knees...https://dl.dropboxusercontent.com/u/28610725/Noise%20Calculator%203_05.xls
...I just replaced "Opamp V noise" and "Opamp I noise" by the 5532's values, an the values of the resistors and bandwidth.
Well, I couldn't use the calc (I'm using a Noptebook) but using the 5532's noise specs, I get 5nV/sqrtHz for noise voltage and 0.7pA/sqrtHz multiplied by 7k that gives another 5nV/sqrtHz; combined quadratically, that computes to 7nV/sqrtHz. THe other resistances are negligible.
Taking into account the 1:5 gain provided by the xfmr, I get 1.4nV/sqrtHz.
Put differently, I get about 350nV/sqrtHz at the output of the 1st stage. I don't know how the calc finds nearly twice...
Quote
I'm not sure; are you using arithmetic summing or quadratic? (not that is changes much since the 2nd stage noise is swamped by the first).
Enter your email address to join: