| Home | 
| Search | 
| Today's Posts | 
| 
	 | 
| 
		 
			 
			#1  
			
			
			 
		
	   
			
			
		 | 
|||
		
		
  | 
|||
| 
		
	
		
		
			
			 "Mark" wrote in message oups.com... Must be my lucky week!. I needed to make some similar readings. Thanks!. I still puzzle over the oft quoted "up to about 30mVrms the output from the diode offers a square law response and will approximate a true RMS measurement. As the OP found, there's very little happening down there. Who makes these sweeping statements?. regards john No it's true. Look at the curves and notice that the current scale on the x axis is a log scale. When the RF input is very small, the DC out is proportional to the log of the RF level i.e. the RF in dB. This is how the normal power meter works. It also provides a true RMS value for modulated RF signal. Once the signal gets too big and the diode begins to work as a converntoin rectifier, this relationship no longer holds true. Notice the curves break upeards. When the RF volatge to log I curves are straight line, this is rhe square law region where the diode current gives you true RMS readings of the RF voltage. Think of it as a voltage in dB to current converter. Mark I know where you're coming in from, but whichever way I look at Win's graphs I'm seeing a straight line for that 1N4148 at 0-30mv levels. Yes, the scales are log-log but the constant of proportionality is dead straight linear. I.e 1mv RF in gives 1e-10 amps and 10mV in gives 1e-9 amps and pro-rata for all points in between (you did see the double decade increments?). This agrees with the 10Mohm value that's marked on the graph. It shouldn't matter if the RF signal is swept over a 1 to 30mV range or just a 5 to 5.01mV range, the DC out will be directly proportional to the 'DC' in and no distortion of the waveform can occur, hence no dc offsets or harmonics. The graph next door though , the 1n5819, looks like it could offer up a tad of rf dB-I rectification. Though to my eyes it still looks way more like a resistor than anything with a square or log law response. There'll be better devices out there that offer (say) quadratic like classical responses at these low levels but it's moving out of the 'common or garden' playground. regards john  | 
| 
		 
			 
			#2  
			
			
			 
		
	   
			
			
		 | 
|||
		
		
  | 
|||
| 
		
	
		
		
			
			 
			
			john jardine wrote... 
		
		
		
		
		
		
		
		
	
	I know where you're coming in from, but whichever way I look at Win's graphs I'm seeing a straight line for that 1N4148 at 0-30mv levels. Yes, the scales are log-log but the constant of proportionality is dead straight linear. I.e 1mv RF in gives 1e-10 amps and 10mV in gives 1e-9 amps and pro-rata for all points in between (you did see the double decade increments?). This agrees with the 10Mohm value that's marked on the graph. Right, but that part of my measurements cries out for further bench exploration. It represents only one part, and is unconfirmed. Also, what happens if the voltage is reversed? Are we to believe the diode is a 10M resistor, shunted by a diode? I'm not comfortable with that. -- Thanks, - Win  | 
| 
		 
			 
			#3  
			
			
			 
		
	   
			
			
		 | 
|||
		
		
  | 
|||
| 
		
	
		
		
			
			 "Winfield Hill" -edu wrote in message ... john jardine wrote... I know where you're coming in from, but whichever way I look at Win's graphs I'm seeing a straight line for that 1N4148 at 0-30mv levels. Yes, the scales are log-log but the constant of proportionality is dead straight linear. I.e 1mv RF in gives 1e-10 amps and 10mV in gives 1e-9 amps and pro-rata for all points in between (you did see the double decade increments?). This agrees with the 10Mohm value that's marked on the graph. Right, but that part of my measurements cries out for further bench exploration. It represents only one part, and is unconfirmed. Also, what happens if the voltage is reversed? Are we to believe the diode is a 10M resistor, shunted by a diode? I'm not comfortable with that. -- Thanks, - Win Yes. Ive been mulling that over. If there is no static bias current flowing through the diode and it magically switches to 'open circuit' when the incoming voltage reverses sign, then it would still make a perfect 'average respsonding' rectifier even at these mV or even uV levels. Just how does the reverse current start to act in the reverse direction?. On the face of it, a IN4148 seems easy enough to check out. regards john  | 
| 
		 
			 
			#4  
			
			
			 
		
	   
			
			
		 | 
|||
		
		
  | 
|||
| 
		
	
		
		
			
			 
			
			In article , hill_a@t_rowland-dotties- 
		
		
		
		
		
		
		
		
	
	harvard-dot.s-edu says... of my measurements cries out for further bench exploration. It represents only one part, and is unconfirmed. Also, what happens if the voltage is reversed? Are we to believe the diode is a 10M resistor, shunted by a diode? I'm not comfortable with that. I'm confused. Is there some reason to expect the semiconductor material to be a perfect insulator with no resistivity at all? Nothing's perfect, and those diodes probably aren't made in the most exacting processes. I would be blown away if you *couldn't* measure some ohmic current flow in a diode at any particular voltage level. -- jm ------------------------------------------------------ http://www.qsl.net/ke5fx Note: My E-mail address has been altered to avoid spam ------------------------------------------------------  | 
| 
		 
			 
			#5  
			
			
			 
		
	   
			
			
		 | 
|||
		
		
  | 
|||
| 
		
	
		
		
			
			 
			
			John Miles wrote... 
		
		
		
		
		
		
		
		
	
	Winfield Hill wrote... http://www.picovolt.com/win/elec/com...de-curves.html ... that part of my measurements cries out for further bench exploration. It represents only one part, and is unconfirmed. Also, what happens if the voltage is reversed? Are we to believe the diode is a 10M resistor, shunted by a diode? I'm not comfortable with that. I'm confused. Is there some reason to expect the semiconductor material to be a perfect insulator with no resistivity at all? Nothing's perfect, and those diodes probably aren't made in the most exacting processes. I would be blown away if you *couldn't* measure some ohmic current flow in a diode at any particular voltage level. Agreed. It's the rather low 10M value that raises my eyebrows. Hence my suggestion that the measurements be revisited. Picked up by John Jardine, who obtained similar values, copied below: Test on a 1N4148. ForwardV DiodeR +50mV 8megs. +30mV 9megs. +20mV 10megs. +10mv 12megs. +5mV 21megs. ReverseV -5mV 21megs. -10mV 30megs. -30mV 270megs. John also suggests the measurements may need further refinement. Oops! I can think of several circuits I've designed over the years using diodes for discharge protection that might not work exactly as I intended, given this observation. And I recall several circuits where I intentionally back biased the diode a few hundred millivolts to insure an open circuit. -- Thanks, - Win  | 
| 
		 
			 
			#6  
			
			
			 
		
	   
			
			
		 | 
|||
		
		
  | 
|||
| 
		
	
		
		
			
			 
			
			Winfield Hill wrote... 
		
		
		
		
		
		
		
		
	
	John Miles wrote... Winfield Hill wrote... http://www.picovolt.com/win/elec/com...de-curves.html ... that part of my measurements cries out for further bench exploration. It represents only one part, and is unconfirmed. Also, what happens if the voltage is reversed? Are we to believe the diode is a 10M resistor, shunted by a diode? I'm not comfortable with that. I'm confused. Is there some reason to expect the semiconductor material to be a perfect insulator with no resistivity at all? Nothing's perfect, and those diodes probably aren't made in the most exacting processes. I would be blown away if you *couldn't* measure some ohmic current flow in a diode at any particular voltage level. Agreed. It's the rather low 10M value that raises my eyebrows. Hence my suggestion that the measurements be revisited. Picked up by John Jardine, who obtained similar values, copied below: Test on a 1N4148. ForwardV DiodeR +50mV 8megs. +30mV 9megs. +20mV 10megs. +10mv 12megs. +5mV 21megs. ReverseV -5mV 21megs. -10mV 30megs. -30mV 270megs. John also suggests the measurements may need further refinement. Oops! I can think of several circuits I've designed over the years using diodes for discharge protection that might not work exactly as I intended, given this observation. And I recall several circuits where I intentionally back biased the diode a few hundred millivolts to insure an open circuit. And others where I used a transistor collector or JFET gate instead. Pease Porridge in the Feb 3rd issue of Electronic Design mentions this problem, and Bob suggests using a transistor. "Using 2n3904s as diodes is very important because most ordinary diodes are much too leaky around +/-60mV to work well. Ordinary gold-doped 1n914s and 1n4148s are quite unsuitable..." -- Thanks, - Win  | 
| 
		 
			 
			#7  
			
			
			 
		
	   
			
			
		 | 
|||
		
		
  | 
|||
| 
		
	
		
		
			
			 
			
			I haven't followed this thread very thoroughly, so this might not be 
		
		
		
		
		
		
		
		
	
	directly relevant. But it should be of interest to anyone trying to detect small signals with a diode. There are several reasons why diodes do poorly with small AC signals. The first is, of course, the forward drop. However, this can in theory be reduced to an arbitrarily low value by reducing the current to a low enough value (by, for example, making the load impedance high enough). The second is that the ratio of reverse to forward current increases as the signal gets smaller and smaller, reaching one at the limit. This can be observed by looking at the I-V curve of a diode. At the origin, the curve is a straight line -- the diode behaves just like a resistor. The third reason is the diode capacitance. This shunts the diode, effectively lowering the reverse impedance. It also lowers the forward impedance, but when the forward Z is lower than the reverse Z, the net effect is to further degrade the forward/reverse impedance ratio. You can make all the DC measurements you want, but they only tell half the story. When you apply AC, you charge the load capacitor during half the cycle according to the diode's forward impedance, and charge is removed from it during the other half according to the diode's reverse impedance. As the forward/reverse impedance ratio degrades due to the two effects mentioned above, the net charge you get in the load capacitance decreases, hence the voltage it's charged to decreases. This ends up looking like a larger diode forward drop. I spent a lot of time thinking about this some years ago when designing a QRP wattmeter, and some of the conclusions I came to appear in the resulting article, "A Simple and Accurate QRP Directional Wattmeter", published in QST, February 1990. See the analysis on p. 20, "Ac v Dc: Why the Difference?" Roy Lewallen, W7EL  | 
| 
		 
			 
			#8  
			
			
			 
		
	   
			
			
		 | 
|||
		
		
  | 
|||
| 
		
	
		
		
			
			 "Roy Lewallen" wrote in message ... I haven't followed this thread very thoroughly, so this might not be directly relevant. But it should be of interest to anyone trying to detect small signals with a diode. I spent a lot of time thinking about this some years ago when designing a QRP wattmeter, and some of the conclusions I came to appear in the resulting article, "A Simple and Accurate QRP Directional Wattmeter", published in QST, February 1990. See the analysis on p. 20, "Ac v Dc: Why the Difference?" Roy Lewallen, W7EL Your article sounds interesting. Is there a link available to see it?. The simplest approach I've seen, was is in the 'Levell TM6A broadband voltmeter'(UK). Designer chopped the low level diode output at 20Hz, allowing a 1mVac FSD. regards john  | 
| 
		 
			 
			#9  
			
			
			 
		
	   
			
			
		 | 
|||
		
		
  | 
|||
| 
		
	
		
		
			
			 
			
			Roy Lewallen wrote: 
		
		
		
		
		
		
		
		
	
	[...] The second is that the ratio of reverse to forward current increases as the signal gets smaller and smaller, reaching one at the limit. This can be observed by looking at the I-V curve of a diode. At the origin, the curve is a straight line - the diode behaves just like a resistor. [...] Roy Lewallen, W7EL Excellent description - thanks. Only one small problem - as Win pointed out, Bob Pease feels a diode-connected 2N3904 has lower leakage at low voltage than a 1N4148: "What's All This Comparator Stuff, Anyhow?" http://www.elecdesign.com/Articles/A...9517/9517.html Does this mean a 2N3904 has a shallower slope than a 1N4148 through zero, or perhaps one or the other has an offset, such as the Agilent Zero Bias Schottky Detector Diodes shown in AN969? http://www.spelektroniikka.fi/kuvat/schot8.pdf Regards, Mike Monett  | 
| 
		 
			 
			#10  
			
			
			 
		
	   
			
			
		 | 
|||
		
		
  | 
|||
| 
		
	
		
		
			
			 
			
			Mike Monett wrote... 
		
		
		
		
		
		
		
		
	
	Roy Lewallen wrote: The second is that the ratio of reverse to forward current increases as the signal gets smaller and smaller, reaching one at the limit. This can be observed by looking at the I-V curve of a diode. At the origin, the curve is a straight line - the diode behaves just like a resistor. ... Excellent description - thanks. Only one small problem - as Win pointed out, Bob Pease feels a diode-connected 2N3904 has lower leakage at low voltage than a 1N4148: "What's All This Comparator Stuff, Anyhow?" http://www.elecdesign.com/Articles/A...9517/9517.html Does this mean a 2N3904 has a shallower slope than a 1N4148 through zero, or perhaps one or the other has an offset, such as the Agilent Zero Bias Schottky Detector Diodes shown in AN969? No, it means its a better diode at low currents. See my curves again, http://www.picovolt.com/win/elec/com...de-curves.html Note the 1n458 and the JFET diodes, which follow the theoretical 60mV/decade rule down to very low currents. As for Roy Lewallen's "ratio of reverse to forward current" argument, there is no reverse current for these fine fellows, at least for DC and reasonably low frequencies. It's the very crummy gold-doped 1n4148 that falls over. Awwkk! -- Thanks, - Win  |