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#1
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Sorry for the dumb question, but I see the phrase "RF current" used in
so many contexts that I am not sure what it is. What I "think" it is, is: 1. The sinusoidal, voltage / current that is impressed on the, e.g., coax feedline's center conductor by the transmitter (a.k.a., generator) 2. The voltage / current on the conductive portion of the radiator 3. The sinusoidal, voltage / current that is picked up by the "other" conductive portion of the radiator (e.g., other pole of a dipole or the ground, radials or counterpoise system of a vertical antenna) 4. The sinusoidal, voltage / current that is returned to the transmitter via the shield of the coax. 5. The induced voltage / current in the counterpart of the receiving system. 6. The current that "flows" in a dielectric, otherwise known as displacement current, the original notion that allowed Maxwell to posit the existence of the ether. That is, RF current is no difference than "current" except for its frequency. What RF current is NOT is the transverse electromagnetic wave. That is, once the effect is in the ether there is no RF current. Looking for confirmation or refutation of the specific points above. Thanks. Thomas |
#2
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Short response...
This pretty much describes what I think of when I hear the term. Current at a "high" frequency. An object for discussion will certainly turn out to be just when does the frequency get high enough to be considered RF and I will say that I think that depends on a lot of things, the first probably being wavelength, others being a matter of much discussion. Verbose response... Some pretty minor things... RF Current, of course is the current, though you say "...voltage / current ...." "sinusoidal"... If there are harmonics present, then there can be multiple sine waves and the resultant (superposition of them) won't look sinusoidal, but a sum of sines. RE your #3: I'd say that the current in a dipole (or ground plane, for that matter) is "pushed into" one side and "pulled out of" the other side (the sides alternating each half cycle) rather than being "picked up" by something considered to be an "other side". If the coax center conductor happens to be pushing at any given instant, then the shield is doing the accompanying pulling. If we view the dipole with a balanced feed line, then the push & pull may be easier to swallow. A dipole is balanced and there is a tendency to consider the coax shield to be at ground potential at all times. This is not correct and is at the root of a VERY large amount of discussion on these news groups... An RF "circuit", if you will, requires two connections to the source, just like a bulb and battery. The rest of the "complete circuit" isn't as obvious with RF -- as you appear to understand. I also suspect you MAY get some discussion on displacement current since it isn't being carried by the classical electrons-in-a-wire, but if the current is present on both sides of the displacement current medium (say, a capacitor dielectric), then there certainly must be RF current getting through it somehow, so to speak. RE the EM wave. I also think this is correct. You have the fields present as though the voltages and currents were doing their thing, but there ain't no electrons in space. This is a fascinating symbiotic (sp) relationship, indeed... 73, -- Steve N, K,9;d, c. i My email has no u's. "Thomas" wrote in message m... Sorry for the dumb question, but I see the phrase "RF current" used in so many contexts that I am not sure what it is. What I "think" it is, is: 1. The sinusoidal, voltage / current that is impressed on the, e.g., coax feedline's center conductor by the transmitter (a.k.a., generator) 2. The voltage / current on the conductive portion of the radiator 3. The sinusoidal, voltage / current that is picked up by the "other" conductive portion of the radiator (e.g., other pole of a dipole or the ground, radials or counterpoise system of a vertical antenna) 4. The sinusoidal, voltage / current that is returned to the transmitter via the shield of the coax. 5. The induced voltage / current in the counterpart of the receiving system. 6. The current that "flows" in a dielectric, otherwise known as displacement current, the original notion that allowed Maxwell to posit the existence of the ether. That is, RF current is no difference than "current" except for its frequency. What RF current is NOT is the transverse electromagnetic wave. That is, once the effect is in the ether there is no RF current. Looking for confirmation or refutation of the specific points above. Thanks. Thomas |
#3
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#4
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Thomas wrote:
Sorry for the dumb question, but I see the phrase "RF current" used in so many contexts that I am not sure what it is. What I "think" it is, is: 1. The sinusoidal, voltage / current that is impressed on the, e.g., coax feedline's center conductor by the transmitter (a.k.a., generator) No, current is not "voltage/current". It's current. Voltage is something else. This comment applies to 2-5 also. It also doesn't have to be sinusoidal. 2. The voltage / current on the conductive portion of the radiator 3. The sinusoidal, voltage / current that is picked up by the "other" conductive portion of the radiator (e.g., other pole of a dipole or the ground, radials or counterpoise system of a vertical antenna) Now, the question is, how is that current "picked up"? 4. The sinusoidal, voltage / current that is returned to the transmitter via the shield of the coax. 5. The induced voltage / current in the counterpart of the receiving system. 6. The current that "flows" in a dielectric, otherwise known as displacement current, the original notion that allowed Maxwell to posit the existence of the ether. That is, RF current is no difference than "current" except for its frequency. And the fact that it can "flow" through non-conductors as a "displacement current". This can make its behavior a lot different than zero-frequency current (DC). What RF current is NOT is the transverse electromagnetic wave. That is, once the effect is in the ether there is no RF current. "Displacement current" IS an electromagnetic field. It's the mechanism which induces conductive current in one conductor as a result of conductive current in another. (This the answer to the question I asked after point 3.) Looking for confirmation or refutation of the specific points above. Thanks. Thomas Roy Lewallen, W7EL |
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