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what a 1:1 choke balum used for
In article . com,
wrote: I mainly wanted to know if it would work on 160 & 80m, I dont care if it acts like a choke/balun only at higher frequencys as long as as it doesnt interfere with 160 & 80s swr. It should not interfere. If the ferrites don't have enough reactance to make it act as an effective choke on 160/80, then it'll just "look like" a foot or two of coax to the signals. -- Dave Platt AE6EO Hosting the Jade Warrior home page: http://www.radagast.org/jade-warrior I do _not_ wish to receive unsolicited commercial email, and I will boycott any company which has the gall to send me such ads! |
what a 1:1 choke balum used for
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what a 1:1 choke balum used for
On Tue, 28 Mar 2006 12:59:52 -0500, John Popelish
wrote: With this in mind, do we add a characteristic of loss to the definition? A lossy air core transformer with series driven, bucking sections. Air core? It is a ferrite core transformer with two one turn Hi John, If there's a transformer in the sense of windings; then it is an air core, the ferrite is wholly transparent to the transverse currents. You could remove the ferrite and it wouldn't make a bit of difference in that sense of transforming. this current mismatch would cause the transformer to produce more or less voltage across the windings In fact, nothing of that sort happens - at least not by your description. The ferrite is simply bulk resistance inserted into the common mode path. That is why common mode current is suppressed. The same thing occurs in the coiled transmission line choke, but the resistance is replaced by reactance. Again, common mode current is snubbed by encountering this too. The transformer property is in the isolation of the balanced circuit from the unbalanced circuit through this resistive characteristic. You are missing one path. The two from the source in the form of the inner shield of the coax, and the center conductor, and the one from the load in the form of the outer shield of the coax (same shield, but isolated circuits). Further, there is no flux linkage of the two conductors coming from the source. Their magnetic lines never break the cores, whereas the common mode current does break the core which thus inserts the resistance of the ferrite. 73's Richard Clark, KB7QHC |
what a 1:1 choke balum used for
|
what a 1:1 choke balum used for
On Tue, 28 Mar 2006 17:39:52 -0800, Richard Clark
wrote: Further, there is no flux linkage of the two conductors coming from the source. That was not correctly expressed, the flux between the two are tightly bound and: Their magnetic lines never break the cores, whereas the common mode current does break the core which thus inserts the resistance of the ferrite. |
what a 1:1 choke balum used for
John I will have to take it down and measure it, im going to do it
anyway because the balun will not load up like it should even with wire on each leg cut to the proper length. I dosent dip with the dip meter at the proper freq either, after i take it down ill post the ohmeter results. |
what a 1:1 choke balum used for
Richard Clark wrote:
On Tue, 28 Mar 2006 12:59:52 -0500, John Popelish wrote: Air core? It is a ferrite core transformer with two one turn Hi John, If there's a transformer in the sense of windings; then it is an air core, the ferrite is wholly transparent to the transverse currents. I said that. It is a common mode transformer. You could remove the ferrite and it wouldn't make a bit of difference in that sense of transforming. The short length of the two conductors passing through the ferrite is certainly a poorer transformer (less mutual inductance between them) if you remove the cores. this current mismatch would cause the transformer to produce more or less voltage across the windings In fact, nothing of that sort happens - at least not by your description. The ferrite is simply bulk resistance inserted into the common mode path. Make that, "impedance (mostly inductive, if the ferrite is well suited to the frequency)" and I agree. That is why common mode current is suppressed. The same thing occurs in the coiled transmission line choke, but the resistance is replaced by reactance. Again, common mode current is snubbed by encountering this too. I agree with this, except that the purpose of the ferrite is to increase the common mode inductance of the section of coax passing through it, not add resistance. Some resistance is inevitable, because no ferrite is lossless, but the intention is for inductance. The transformer property is in the isolation of the balanced circuit from the unbalanced circuit through this resistive characteristic. Try transmitting through such a resistance and you are going to lose a lot of your power. You are missing one path. The two from the source in the form of the inner shield of the coax, and the center conductor, and the one from the load in the form of the outer shield of the coax (same shield, but isolated circuits). I can't parse this. There are two metal conductors entering the choke, and two exiting it. All currents pass through those 4 conductors. Further, there is no flux linkage of the two conductors coming from the source. Their magnetic lines never break the cores, I think you mean by this that a normal unbalanced signal in a coax has no magnetic field external to the shield. It is all between the center conductor and the shield. And I agree that this is what you are trying to accomplish by adding this two conductor choke between the coax and the balanced antenna. Without it, there would be some magnetic field from a net (uncanceled) current and voltage on the outside of the shield that would cause the coax to radiate. And the voltages and currents fed to the balanced antenna would not be equal and opposite (balanced) but somewhat unbalanced. There would also be non equal currents in the center conductor and shield. I think we agree on all that, but have a different picture of how a choke balun corrects these problems. whereas the common mode current does break the core which thus inserts the resistance of the ferrite. The common mode current causes flux in the core, and the conductors passing through that flux produce a voltage proportional to the rate of change of that flux, just as the conductor passing through any inductor would. The transformer aspect is that since both conductors pass through the exact same rate of change of flux, there is the same voltage produced at the ends sticking out of the core, and this voltage gets algebraically added to what is already there. If the inductance of each winding is high enough (5 to 10 times the coax impedance) a very small common mode current is enough to produce a large enough voltage across the ends to the two conductors to correct most of the unbalanced to balanced coupling. Admittedly, there is no need to get this inductance (including mutual inductance) with the aid of ferrite around the coax. You could just wind the coax into an air core transformer. But it would be considerable larger than one made with a high permeability core, though, probably lower loss. |
what a 1:1 choke balum used for
John Popelish wrote:
Richard Clark wrote: . . . In fact, nothing of that sort happens - at least not by your description. The ferrite is simply bulk resistance inserted into the common mode path. Make that, "impedance (mostly inductive, if the ferrite is well suited to the frequency)" and I agree. "Low frequency" ferrites are well suited to applications as HF chokes and broadband transformers. What you don't want to do is use them for a high Q inductor in a filter, tuned circuit, or similar application. That is why common mode current is suppressed. The same thing occurs in the coiled transmission line choke, but the resistance is replaced by reactance. Again, common mode current is snubbed by encountering this too. I agree with this, except that the purpose of the ferrite is to increase the common mode inductance of the section of coax passing through it, not add resistance. Some resistance is inevitable, because no ferrite is lossless, but the intention is for inductance. Baluns work fine with a resistive impedance, with the exception of applications involving large power. In fact, resistive impedance is desirable because the impedance changes little with frequency, and is relatively free of resonance effects. (More below.) The transformer property is in the isolation of the balanced circuit from the unbalanced circuit through this resistive characteristic. Try transmitting through such a resistance and you are going to lose a lot of your power. You're not "transmitting through" a balun's impedance. Only the common mode current effectively flows through it, and the power dissipated by the balun is Icm^2 * R, where Icm is the common mode current and R is the resistive part of the balun's common mode impedance. If R is small, dissipation is low. But if R is large, that makes Icm small, so dissipation is also low. It's really an impedance matching problem when the balun is resistive -- a very low or very high balun R results in low dissipation. Dissipation is maximum at some intermediate value of R and decreases on each side. A typical balun made with "low frequency" ferrite (e.g. Fair-Rite 70 series) and operating at HF or above (and therefore primarily resistive) having a common mode impedance of 500 ohms or greater generally won't dissipate any significant fraction of the transmitted power. However, if you're running high power, even a fraction of a dB dissipated in the balun will cause it to overheat. Consequently, people running high power often resort to type 43 ferrite (a Fair-Rite designation; or its equivalent from other manufacturers), which is less resistive than lower frequency ferrites. In extreme cases, high frequency (60 series) ferrite is necessary. The problem is that it's increasingly difficult to get adequate impedance with the higher frequency ferrites. Type 43 is often a good compromise, and it's widely available in many core sizes. . . . I think you mean by this that a normal unbalanced signal in a coax has no magnetic field external to the shield. It is all between the center conductor and the shield. And I agree that this is what you are trying to accomplish by adding this two conductor choke between the coax and the balanced antenna. Without it, there would be some magnetic field from a net (uncanceled) current and voltage on the outside of the shield that would cause the coax to radiate. And the voltages and currents fed to the balanced antenna would not be equal and opposite (balanced) but somewhat unbalanced. There would also be non equal currents in the center conductor and shield. I think we agree on all that, but have a different picture of how a choke balun corrects these problems. . . . Common and differential mode currents are physically separated in a coax cable, and so are the fields from the two components, providing that the shield is at least several skin depths thick. The differential mode current and its fields are entirely inside the coax, decaying rapidly as you go outward from the inner boundary of the shield. By the time you reach the outer boundary of the shield the fields from the differential current is negligibly small. So any core you put over the coax doesn't see or interact with the common mode current or its fields at all, and you can completely ignore it when analyzing balun action. Similarly, you can ignore the core when analyzing the differential mode properties of the system. The common mode current resides in a thin layer on the outside of the shield, it and its fields never reaching the inside. The balun provides an impedance to this current just as it would to any current on the outside of a conductor. When bifilar wound, the fields from the differential mode current are primarily between the turns, although some relatively small amount extends beyond to interact with the core. The net result is nearly the same. . . . Roy Lewallen, W7EL |
what a 1:1 choke balum used for
Roy Lewallen wrote:
So any core you put over the coax doesn't see or interact with the common mode current or its fields at all, and you can completely ignore it when analyzing balun action. Roy probably meant "differential" above instead of "common". Cores on coax definitely "interact with the common mode current or its fields" and that is their purpose. -- 73, Cecil http://www.qsl.net/w5dxp |
what a 1:1 choke balum used for
On Tue, 28 Mar 2006 22:33:18 -0500, John Popelish
wrote: this current mismatch would cause the transformer to produce more or less voltage across the windings In fact, nothing of that sort happens - at least not by your description. The ferrite is simply bulk resistance inserted into the common mode path. Make that, "impedance (mostly inductive, if the ferrite is well suited to the frequency)" and I agree. Hi John, No, the principle of the impedance is overwhelmingly resistive, not reactive. One core (#75) that snuggly fits over RG58, at about 10MHz, exhibits 25 Ohms resistance to common mode current. My BalUn uses 50 such whose combination presents 1250 Ohms resistance. This value varies over frequency, but easily finds a 1000:50 ratio over the entire MF/HF Ham spectrum. I also have two engineering samples boxes full of various material types and geometries and have measured them all. Some exhibit reactance, but are vastly overwhelmed by their intrinsic resistance. That is why common mode current is suppressed. The same thing occurs in the coiled transmission line choke, but the resistance is replaced by reactance. Again, common mode current is snubbed by encountering this too. I agree with this, except that the purpose of the ferrite is to increase the common mode inductance of the section of coax passing through it, not add resistance. Some resistance is inevitable, because no ferrite is lossless, but the intention is for inductance. Quite the contrary. Inductance, or more properly to the application, reactance, may come as a consequence of these cores, but that is really just a minor component to the vastly greater resistance. The transformer property is in the isolation of the balanced circuit from the unbalanced circuit through this resistive characteristic. Try transmitting through such a resistance and you are going to lose a lot of your power. That power, actually current, was forced into a common mode because of one of several problems: 1. Massive imbalance in the radiator design, 2. Massive catastrophe with the radiator. If you are destined to "lose a lot of power" into such resistance, you have far greater problems you are ignoring. However, let's return to this "loss of a lot of power." You have an antenna with a nominal 50 Ohm load resistance (presumably balanced to the common). You have a common mode choke with 1000 Ohms resistance in parallel (to the common of the common mode). Now, why would the power choose the path of 10 to 40 times more resistance to invest its calories in? I will be generous and pour 1.5KW into a balanced 50 Ohm load to develop 275V that is also across the 1000 Ohms of the BalUn. 76W into 50 beads. Now this verges on serious power for this load I will admit, but it also presumes key-down conditions which would only be found for RTTY or SSTV. By my bench measurements, I figure that the core's can tolerate as much power as the bulk equivalent carbon composition resistor - or least this is my rule of thumb. This means about 1 or 2W per bead to offer enough heat to cause pain, but perhaps not enough to blister. This is another benchmark from my days in the Navy. I once asked an ET Chief how much heat a transistor could tolerate. He said "If you can hold onto it and count to 10, it's not too much." I've been blistered by TO-5 cans with just a casual brush and they still filled their design mission. You are missing one path. The two from the source in the form of the inner shield of the coax, and the center conductor, and the one from the load in the form of the outer shield of the coax (same shield, but isolated circuits). I can't parse this. There are two metal conductors entering the choke, and two exiting it. All currents pass through those 4 conductors. Your count is four terminals (not conductors), there are six. You need to come to terms with this shortfall in your count as it explains the utility and design of BalUns. Further, there is no flux linkage of the two conductors coming from the source. Their magnetic lines never break the cores, I think you mean by this that a normal unbalanced signal in a coax has no magnetic field external to the shield. It is all between the center conductor and the shield. And I agree that this is what you are trying to accomplish by adding this two conductor choke between the coax and the balanced antenna. Without it, there would be some magnetic field from a net (uncanceled) current and voltage on the outside of the shield that would cause the coax to radiate. And the voltages and currents fed to the balanced antenna would not be equal and opposite (balanced) but somewhat unbalanced. There would also be non equal currents in the center conductor and shield. I think we agree on all that, but have a different picture of how a choke balun corrects these problems. That is apparent. whereas the common mode current does break the core which thus inserts the resistance of the ferrite. The common mode current causes flux in the core, and the conductors passing through that flux produce a voltage proportional to the rate of change of that flux, just as the conductor passing through any inductor would. This "rate of change" is spurious, call it frequency dependant, but then frequency dependency is neither here nor there at this moment. More to the matter trying to turn this BalUn into a power transformer is doomed in this analysis as it has absolutely no impact to correct most of the unbalanced to balanced coupling. 73's Richard Clark, KB7QHC |
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