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#1
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When people talk about tuning caps for transmitting loop antennas, they
always talk about air or vacuum capacitors. I was wondering why dielectrics are never used. Someone in a Yahoo group mentioned that the variation of dielectric constant (εr) with temperature will cause the tuning to drift out of the bandwidth when keyed. I guess this also requires a poor dissipation factor (DF), or at least a poor DF relative to the application. I took a look at some potential materials and indeed, many have a rather steep slope of εr with temperature varying many percent over a 50°C range. But they make fixed capacitors that have low temperature coefficients. I looked up some materials for fixed capacitors and found dielectrics with εr change with temperature as low as 10 ppm/°C. These materials also have a loss tangent less than 0.001, some much less. I'm wondering if they would be practical to use for the dielectric in a variable capacitor. -- Rick |
#2
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On Fri, 30 Oct 2015 03:29:26 -0400, rickman wrote:
When people talk about tuning caps for transmitting loop antennas, they always talk about air or vacuum capacitors. I was wondering why dielectrics are never used. Someone in a Yahoo group mentioned that the variation of dielectric constant (?r) with temperature will cause the tuning to drift out of the bandwidth when keyed. I guess this also requires a poor dissipation factor (DF), or at least a poor DF relative to the application. I took a look at some potential materials and indeed, many have a rather steep slope of ?r with temperature varying many percent over a 50°C range. But they make fixed capacitors that have low temperature coefficients. I looked up some materials for fixed capacitors and found dielectrics with ?r change with temperature as low as 10 ppm/°C. These materials also have a loss tangent less than 0.001, some much less. I'm wondering if they would be practical to use for the dielectric in a variable capacitor. Me thinks you are overlooking the very high voltages involved. |
#3
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On 10/30/2015 9:07 AM, Jeff wrote:
I looked up some materials for fixed capacitors and found dielectrics with ?r change with temperature as low as 10 ppm/°C. These materials also have a loss tangent less than 0.001, some much less. I'm wondering if they would be practical to use for the dielectric in a variable capacitor. Me thinks you are overlooking the very high voltages involved. I would have thought that glass was a good candidate and in plentiful supply in various thicknesses, and would withstand very high voltages. The Er is in the range 5 to 10 depending on the actual type. It is the high voltages that makes the dielectric useful. The plates in these capacitors have to be widely separated and the use of dielectric allows this spacing to be reduced, that's one dimension. The Er increases the capacitance which allows the capacitor to be reduced in the other two dimensions. The problem is the change in Er with temperature which will cause the resonance of the antenna to change, potentially outside the bandwidth if the Q is high enough. I'm not sure how low the loss tangent would need to be to minimize self heating to a point that higher Er changes with temperature won't matter. Even if self heating is not a problem, larger Er changes will temperature would mean you could not retune the capacitor to the same value with environmental temperature changes and so the tuning would not be repeatable. Possibly this could be compensated for by measuring the temperature and calibrating for temperature. -- Rick |
#4
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On 10/30/2015 10:46 AM, rickman wrote:
On 10/30/2015 9:07 AM, Jeff wrote: I looked up some materials for fixed capacitors and found dielectrics with ?r change with temperature as low as 10 ppm/°C. These materials also have a loss tangent less than 0.001, some much less. I'm wondering if they would be practical to use for the dielectric in a variable capacitor. Me thinks you are overlooking the very high voltages involved. I would have thought that glass was a good candidate and in plentiful supply in various thicknesses, and would withstand very high voltages. The Er is in the range 5 to 10 depending on the actual type. It is the high voltages that makes the dielectric useful. No, it is the increase in capacitance that makes the dielectric useful. The plates in these capacitors have to be widely separated and the use of dielectric allows this spacing to be reduced, that's one dimension. The Er increases the capacitance which allows the capacitor to be reduced in the other two dimensions. Yes. The problem is the change in Er with temperature which will cause the resonance of the antenna to change, potentially outside the bandwidth if the Q is high enough. Are you planning to operate this antenna over a wide range of temperatures? I'm not sure how low the loss tangent would need to be to minimize self heating to a point that higher Er changes with temperature won't matter. Even if self heating is not a problem, larger Er changes will temperature would mean you could not retune the capacitor to the same value with environmental temperature changes and so the tuning would not be repeatable. Possibly this could be compensated for by measuring the temperature and calibrating for temperature. Sure. Have you mathematically analyzed any of your proposed scenarios? That might help. |
#5
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On 10/30/2015 12:01 PM, John S wrote:
On 10/30/2015 10:46 AM, rickman wrote: On 10/30/2015 9:07 AM, Jeff wrote: I looked up some materials for fixed capacitors and found dielectrics with ?r change with temperature as low as 10 ppm/°C. These materials also have a loss tangent less than 0.001, some much less. I'm wondering if they would be practical to use for the dielectric in a variable capacitor. Me thinks you are overlooking the very high voltages involved. I would have thought that glass was a good candidate and in plentiful supply in various thicknesses, and would withstand very high voltages. The Er is in the range 5 to 10 depending on the actual type. It is the high voltages that makes the dielectric useful. No, it is the increase in capacitance that makes the dielectric useful. That sounds rather argumentative. I explain this in the next paragraph which you seem to be agreeing with. So which is it? The plates in these capacitors have to be widely separated and the use of dielectric allows this spacing to be reduced, that's one dimension. The Er increases the capacitance which allows the capacitor to be reduced in the other two dimensions. Yes. The problem is the change in Er with temperature which will cause the resonance of the antenna to change, potentially outside the bandwidth if the Q is high enough. Are you planning to operate this antenna over a wide range of temperatures? I'm not sure how low the loss tangent would need to be to minimize self heating to a point that higher Er changes with temperature won't matter. Even if self heating is not a problem, larger Er changes will temperature would mean you could not retune the capacitor to the same value with environmental temperature changes and so the tuning would not be repeatable. Possibly this could be compensated for by measuring the temperature and calibrating for temperature. Sure. Have you mathematically analyzed any of your proposed scenarios? That might help. -- Rick |
#6
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rickman wrote:
On 10/30/2015 12:01 PM, John S wrote: On 10/30/2015 10:46 AM, rickman wrote: On 10/30/2015 9:07 AM, Jeff wrote: I looked up some materials for fixed capacitors and found dielectrics with ?r change with temperature as low as 10 ppm/°C. These materials also have a loss tangent less than 0.001, some much less. I'm wondering if they would be practical to use for the dielectric in a variable capacitor. Me thinks you are overlooking the very high voltages involved. I would have thought that glass was a good candidate and in plentiful supply in various thicknesses, and would withstand very high voltages. The Er is in the range 5 to 10 depending on the actual type. It is the high voltages that makes the dielectric useful. No, it is the increase in capacitance that makes the dielectric useful. That sounds rather argumentative. I explain this in the next paragraph which you seem to be agreeing with. So which is it? It's clearly both, as an insulator with a higher breakdown voltage than air would enable the plates to be closer and thus smaller for a given capacitance, as well as more fitting into a given length, even if the dielectric constant was the same as air. The plates in these capacitors have to be widely separated and the use of dielectric allows this spacing to be reduced, that's one dimension. The Er increases the capacitance which allows the capacitor to be reduced in the other two dimensions. Yes. The problem is the change in Er with temperature which will cause the resonance of the antenna to change, potentially outside the bandwidth if the Q is high enough. Are you planning to operate this antenna over a wide range of temperatures? I'm not sure how low the loss tangent would need to be to minimize self heating to a point that higher Er changes with temperature won't matter. Even if self heating is not a problem, larger Er changes will temperature would mean you could not retune the capacitor to the same value with environmental temperature changes and so the tuning would not be repeatable. Possibly this could be compensated for by measuring the temperature and calibrating for temperature. Sure. Have you mathematically analyzed any of your proposed scenarios? That might help. -- Roger Hayter |
#7
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On 10/30/2015 11:40 AM, rickman wrote:
On 10/30/2015 12:01 PM, John S wrote: On 10/30/2015 10:46 AM, rickman wrote: On 10/30/2015 9:07 AM, Jeff wrote: I looked up some materials for fixed capacitors and found dielectrics with ?r change with temperature as low as 10 ppm/°C. These materials also have a loss tangent less than 0.001, some much less. I'm wondering if they would be practical to use for the dielectric in a variable capacitor. Me thinks you are overlooking the very high voltages involved. I would have thought that glass was a good candidate and in plentiful supply in various thicknesses, and would withstand very high voltages. The Er is in the range 5 to 10 depending on the actual type. It is the high voltages that makes the dielectric useful. No, it is the increase in capacitance that makes the dielectric useful. That sounds rather argumentative. I explain this in the next paragraph which you seem to be agreeing with. So which is it? Your posts are beginning to make me think you are a troll. Every person who responds gets a provocative answer from you. If you already have in mind the answer you want, why ask? |
#8
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On 10/30/2015 12:18 PM, Jeff wrote:
I would have thought that glass was a good candidate and in plentiful supply in various thicknesses, and would withstand very high voltages. The Er is in the range 5 to 10 depending on the actual type. It is the high voltages that makes the dielectric useful. The plates in these capacitors have to be widely separated and the use of dielectric allows this spacing to be reduced, that's one dimension. The Er increases the capacitance which allows the capacitor to be reduced in the other two dimensions. The problem is the change in Er with temperature which will cause the resonance of the antenna to change, potentially outside the bandwidth if the Q is high enough. I'm not sure how low the loss tangent would need to be to minimize self heating to a point that higher Er changes with temperature won't matter. Even if self heating is not a problem, larger Er changes will temperature would mean you could not retune the capacitor to the same value with environmental temperature changes and so the tuning would not be repeatable. Possibly this could be compensated for by measuring the temperature and calibrating for temperature. Glass is used as a dielectric in high quality low loss RF capacitors so I suspect that it would be usable in a home-made one. Doesn't necessarily follow. The loss tangent of glass is low to very low so it won't heat up much in use. But the important part is the change in Er with temperature as I explain. In fixed value caps changes in capacitance of a few percent are usually not a problem. But in this application tuning of the circuit may be very critical and require a much higher degree of stability. I am also looking at alumina ceramics. The properties vary with composition, but there are composites with very high stability numbers. They usually are in a materials data sheet rather than in a product offered for sale. Seems a lot of ceramics are custom items. -- Rick |
#9
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On 10/31/2015 6:01 AM, Jeff wrote:
Glass is used as a dielectric in high quality low loss RF capacitors so I suspect that it would be usable in a home-made one. Doesn't necessarily follow. The loss tangent of glass is low to very low so it won't heat up much in use. But the important part is the change in Er with temperature as I explain. In fixed value caps changes in capacitance of a few percent are usually not a problem. But in this application tuning of the circuit may be very critical and require a much higher degree of stability. I am also looking at alumina ceramics. The properties vary with composition, but there are composites with very high stability numbers. They usually are in a materials data sheet rather than in a product offered for sale. Seems a lot of ceramics are custom items. I think the change of Er with temperature is the least of your worries when talking about a tuning capacitor for a magnetic loop. The change of capacitance due to mechanical changes in the plates is likely to be at least an order of magnitude greater than the dielectric changes. I wonder about that. I know metals have a high tempco of expansion and this will make changes in the capacitance. I haven't analyzed it to see how significant that would be. So let me give it a try. Expansion of the air gapped metal capacitor will have two opposing effects. Enlargement of the plate surface area will increase the area and so increase capacitance by the square of the tempco of the metal. Enlargement of the spacing will decrease capacitance directly by the tempco of the metal assuming the spacers are the same material. The net effect will be to increase the capacitance in direct proportion to the tempco of the metal. Using a dielectric would reduce the effect of the plate spacing on capacitance to a very small value since most of the capacitance will be due to the material and much less to any air gap remaining. So it would return the overall effect on the capacitance to the square of the expansion tempco. Does that sound right? In other words, it would be good if the dielectric had an effect that was opposite to the effect of the metal tempco. I'll meed to consider that as I search for materials. -- Rick |
#10
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rickman wrote:
On 10/31/2015 6:01 AM, Jeff wrote: Glass is used as a dielectric in high quality low loss RF capacitors so I suspect that it would be usable in a home-made one. Doesn't necessarily follow. The loss tangent of glass is low to very low so it won't heat up much in use. But the important part is the change in Er with temperature as I explain. In fixed value caps changes in capacitance of a few percent are usually not a problem. But in this application tuning of the circuit may be very critical and require a much higher degree of stability. I am also looking at alumina ceramics. The properties vary with composition, but there are composites with very high stability numbers. They usually are in a materials data sheet rather than in a product offered for sale. Seems a lot of ceramics are custom items. I think the change of Er with temperature is the least of your worries when talking about a tuning capacitor for a magnetic loop. The change of capacitance due to mechanical changes in the plates is likely to be at least an order of magnitude greater than the dielectric changes. I wonder about that. I know metals have a high tempco of expansion and this will make changes in the capacitance. I haven't analyzed it to see how significant that would be. So let me give it a try. Expansion of the air gapped metal capacitor will have two opposing effects. Enlargement of the plate surface area will increase the area and so increase capacitance by the square of the tempco of the metal. Enlargement of the spacing will decrease capacitance directly by the tempco of the metal assuming the spacers are the same material. The net effect will be to increase the capacitance in direct proportion to the tempco of the metal. Using a dielectric would reduce the effect of the plate spacing on capacitance to a very small value since most of the capacitance will be due to the material and much less to any air gap remaining. So it would return the overall effect on the capacitance to the square of the expansion tempco. Does that sound right? In other words, it would be good if the dielectric had an effect that was opposite to the effect of the metal tempco. I'll meed to consider that as I search for materials. An aluminum plate 6 inches square at 75 F heated to 200 F changes dimensions by 0.0092 inches. For plate glass the change is 0.0031 inches. I will leave it to you to calculate how much that will change capacitance. http://www.engineeringtoolbox.com/li...on-d_1379.html -- Jim Pennino |
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