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#521 |
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diyAudio Member
Join Date: Jul 2004
Location: Fort St John, BC Canada
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Quote:
Thanks for this jackinnj, I can't operate my calculator after working all night installing a fiber node hanging on the strand on a pole. I can barely type. Is there a formula that includes the time constants? That would be needed for modelling. CdS can be turned on rapidly but are rather passive and slower on the turn off which make them difficult to use in a full range oscillator at higher frequency. David.
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David. |
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#522 | |
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diyAudio Member
Join Date: Feb 2011
Location: Fly over country
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Cordell's schematic is on his site here. http://www.cordellaudio.com/papers/thd_analyzer.pdf |
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#523 | |
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diyAudio Member
Join Date: May 2011
Location: Virginia
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Quote:
The LT Wein bridge circuit claims the same number. So, are people seeing much better numbers out of the Cordell oscillator than the article presents? |
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#524 | |
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diyAudio Member
Join Date: Jul 2004
Location: Fort St John, BC Canada
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Quote:
I'll see if I can find likes to this. http://www.moorepage.net/IG-18-2.html If you look at the bottom of the page the last spectrum display is 0.00063% THD+N and 0.00058% THD @ 10Vrms out to 10KHz. This is very good. Of course the disto will go down at lower level but with the cost of lower SNR. David.
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David. Last edited by davada; 28th September 2012 at 12:58 AM. |
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#525 |
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diyAudio Member
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#526 |
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diyAudio Member
Join Date: Jul 2004
Location: Fort St John, BC Canada
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This is a very simple track and hold circuit I developed.
There are to variations shown here. The first is a single phase reset and the second is a quadrature reset. The quadrature reset version having a longer hold time. A1 generates the signals for the simulation and is replaced by an oscillator in a real world circuit. The circuit offers some improvement over conventional track and hold systems. There is an absents of glitch and ringing associated with fast switching circuits. All of the signals are supplied from the input signal for the rectification and reset. No pulse shaping circuits are required. This TH could be used to replace the conventional peak detector circuit found in oscillator AGC's The output power is far greater than that of a conventional peak detector and will decrease settling time of an oscillator. The circuit illustrated uses a transistor as a very low leakage diode. The output buffer op amp should be a Jfet input type because of their low input bias and leakage currents. The input buffer op amp is not critical provided it cover the desired bandwidth. The arrangement with out feed back around the rectifier offers better performance at higher frequencies and doesn't suffer as much overshoot in the absence of resistive loading. R1 or R3 set the reset current. Higher values of resistance reduce the reset pull down. Like any conventional diode rectifier there is some peaking in the output from the peak of the sine. The circuit tracks and holds on the positive of the sine and resets on the negative swing. For a negative version simply replace the transistors with PNP type. This could be used as a drop in replacement for the peak detector in Bob Cordell's oscillator circuit and others. Cheers, David.
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David. Last edited by davada; 28th September 2012 at 02:52 AM. |
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#527 | |
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diyAudio Member
Join Date: May 2011
Location: Virginia
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Quote:
Also, LT has another circuit with an RMS -> DC converter in the AGC: http://cds.linear.com/docs/LT%20Jour...TC1968-Pei.pdf What I find interesting is that he measured it at 0.0025% THD @ 100kHz. He doesn't mention anything about a lower frequency. Maybe if I combine the features of this oscillator with the other bridge oscillator, I might have something good? |
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#528 | |
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diyAudio Member
Join Date: May 2011
Location: Virginia
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If and when I do build something, I will take your suggestions into consideration. Thanks for your comments! |
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#529 | |
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diyAudio Member
Join Date: May 2011
Location: Virginia
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#530 | |
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diyAudio Member
Join Date: Mar 2009
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L. |
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