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#1
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Most authors explain how a wave is generated, then resort to reciprocity
to explain the reception process. But a clear and simple direct explanation appears in Bailey, _TV and Other Receiving Antennas_ (pp. 141-2), of what happens when an electromagnetic wave strikes a conductor: "The second, and equally important effect [the first being reflection of much of the incident energy] is that some energy /does/ enter the outer skin of the conductor. That part of the energy, which is not reflected, must enter the conductor. The conditions at the surface of the conductor, as we have already seen, give rise to a small resultant electric vector and a large resultant magnetic vector. The presence of these at the conductor is direct evidence that power is entering the conductor. The small electric vector acts on the internal electrons of the conductor and impresses a direction force, tending to drive the electrons along the skin of the conductor in the direction of the electric vector. But from experience we know that /no/ electrons can ever be caused to move without gradually establishing their own magnetic field, and this usually takes /time/. The motion of electrons (which is electric current by definition) never takes place without the magnetic field. How, then, is the electric vector from the electromagnetic wave going to put these electrons in motion? It can only do so because the electromagnetic wave /also supplies a magnetic vector/ as well as an electric vector. And the value of this magnetic vector is exactly proportioned to supply just the right amount of magnetic field energy which the electrons require for immediate motion. Thus the electrons do not have to establish their own magnetic field, since this field is supplied by the electromagnetic wave. Hence, electromagnetic wave energy entering the conductor establishes immediate motion of electrons /along/ the conductor, the direction of motion at any instant corresponding to the direction of the electric vector. If the electric vector changes direction, the electrons will follow suit." Other posters have correctly pointed out that an antenna doesn't and can't receive a signal solely due to the E field; a time-changing E field can't exist without an accompanying time-changing H field. Roy Lewallen, W7EL Paul Taylor wrote: Hi, I am looking for an explanation of how an antenna receives a signal due to the E-field of an electromagnetic wave. I have looked in some books, and can understand transmission, but the books I have looked in don't explain reception. I have found an explanation of how the H-field induces a signal in a loop antenna: a changing magnetic flux will induce a current. But what about the E-field and a dipole antenna? I guess that the E-field causes electrons to move in the antenna wire, because in a solid conductor, electrons will move until the E-field inside the solid is cancelled out? I have googled but having difficulty finding a good explanation. Any pointers? Thanks & regards, Paul. |
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#2
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Roy Lewallen wrote: Most authors explain how a wave is generated, then resort to reciprocity to explain the reception process. But a clear and simple direct explanation appears in Bailey, _TV and Other Receiving Antennas_ (pp. 141-2), of what happens when an electromagnetic wave strikes a conductor: "The second, and equally important effect [the first being reflection of much of the incident energy] is that some energy /does/ enter the outer skin of the conductor. That part of the energy, which is not reflected, must enter the conductor. The conditions at the surface of the conductor, as we have already seen, give rise to a small resultant electric vector and a large resultant magnetic vector. The presence of these at the conductor is direct evidence that power is entering the conductor. The small electric vector acts on the internal electrons of the conductor and impresses a direction force, tending to drive the electrons along the skin of the conductor in the direction of the electric vector. But from experience we know that /no/ electrons can ever be caused to move without gradually establishing their own magnetic field, and this usually takes /time/. The motion of electrons (which is electric current by definition) never takes place without the magnetic field. How, then, is the electric vector from the electromagnetic wave going to put these electrons in motion? It can only do so because the electromagnetic wave /also supplies a magnetic vector/ as well as an electric vector. And the value of this magnetic vector is exactly proportioned to supply just the right amount of magnetic field energy which the electrons require for immediate motion. Thus the electrons do not have to establish their own magnetic field, since this field is supplied by the electromagnetic wave. Hence, electromagnetic wave energy entering the conductor establishes immediate motion of electrons /along/ the conductor, the direction of motion at any instant corresponding to the direction of the electric vector. If the electric vector changes direction, the electrons will follow suit." Hi Roy - It's certainly true that a moving charge generates a magnetic field, so perhaps I'm reading it wrong. But it appears to me that Mr. Bailey is arguing here that an electron cannot be compelled to move simply by the application of an electric field. Do you think that is what he is saying? Do you agree? Other posters have correctly pointed out that an antenna doesn't and can't receive a signal solely due to the E field; Given the statement below, I would be interested to know how anyone could have tested the claim. ;-) a time-changing E field can't exist without an accompanying time-changing H field. Roy Lewallen, W7EL Jim Kelley, AC6XG Paul Taylor wrote: Hi, I am looking for an explanation of how an antenna receives a signal due to the E-field of an electromagnetic wave. I have looked in some books, and can understand transmission, but the books I have looked in don't explain reception. I have found an explanation of how the H-field induces a signal in a loop antenna: a changing magnetic flux will induce a current. But what about the E-field and a dipole antenna? I guess that the E-field causes electrons to move in the antenna wire, because in a solid conductor, electrons will move until the E-field inside the solid is cancelled out? I have googled but having difficulty finding a good explanation. Any pointers? Thanks & regards, Paul. |
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#3
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Jim Kelley wrote:
Hi Roy - It's certainly true that a moving charge generates a magnetic field, so perhaps I'm reading it wrong. But it appears to me that Mr. Bailey is arguing here that an electron cannot be compelled to move simply by the application of an electric field. Do you think that is what he is saying? Do you agree? No, I don't believe he's saying that. He says, The small electric vector acts on the internal electrons of the conductor and impresses a direction force, tending to drive the electrons along the skin of the conductor in the direction of the electric vector. . . Roy Lewallen, W7EL |
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#4
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Roy Lewallen wrote: Jim Kelley wrote: Hi Roy - It's certainly true that a moving charge generates a magnetic field, so perhaps I'm reading it wrong. But it appears to me that Mr. Bailey is arguing here that an electron cannot be compelled to move simply by the application of an electric field. Do you think that is what he is saying? Do you agree? No, I don't believe he's saying that. He says, The small electric vector acts on the internal electrons of the conductor and impresses a direction force, tending to drive the electrons along the skin of the conductor in the direction of the electric vector. . . Yes. But then he goes on to say, How, then, is the electric vector from the electromagnetic wave going to put these electrons in motion? That's what I was referring to. Do you understand why he would pose this question if he believed he had already given the answer in the paragraph you quoted? He shoulda quit while he was ahead maybe? ;-) Thanks, Jim Kelley, AC6XG |
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#5
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On Mon, 28 Nov 2005 12:15:30 -0800, Jim Kelley
wrote: How, then, is the electric vector from the electromagnetic wave going to put these electrons in motion? That's what I was referring to. Do you understand why he would pose this question As already stated: But from experience we know that /no/ electrons can ever be caused to move without gradually establishing their own magnetic field, and this usually takes /time/. The need for time (impedance) is accommodated by the wave: It can only do so because the electromagnetic wave /also supplies a magnetic vector/ as well as an electric vector. The phase of the re-radiated signal is a function of the path length. If the path signal required the electric potential to sustain movement (no other motive force available), that would add an additional phase retardation that is not observed. Observation of what does occur is other wise described by Bailey as from experience we know.... Roy's quote comes from a nascent discussion of the topic of Reception that has a complete, later chapter devoted to it. 73's Richard Clark, KB7QHC |
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#6
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Jim Kelley wrote:
Roy Lewallen wrote: Jim Kelley wrote: Hi Roy - It's certainly true that a moving charge generates a magnetic field, so perhaps I'm reading it wrong. But it appears to me that Mr. Bailey is arguing here that an electron cannot be compelled to move simply by the application of an electric field. Do you think that is what he is saying? Do you agree? No, I don't believe he's saying that. He says, The small electric vector acts on the internal electrons of the conductor and impresses a direction force, tending to drive the electrons along the skin of the conductor in the direction of the electric vector. . . Yes. But then he goes on to say, How, then, is the electric vector from the electromagnetic wave going to put these electrons in motion? That's what I was referring to. Do you understand why he would pose this question if he believed he had already given the answer in the paragraph you quoted? He shoulda quit while he was ahead maybe? ;-) Well, it's obvious that an electric field can move an electron. The Lorentz force law tells us how much force results from a given E field, and we can get the resulting acceleration from Newtonian physics. An everyday example is an oscilloscope deflection system which uses an electric field to deflect electrons. (Actually, modern digital scopes typically use raster displays with magnetic deflection -- but many of still have older analog types with electric field deflection.) But if the antenna conductor were perfect, no E field at all could exist at the wire surface regardless of the amplitude of the E field of the oncoming wave. The wave's E field therefore couldn't directly influence the electrons in the (perfect) conductor. Only the H field of the wave, then, can induce a current in the perfect conductor. The direct influence of the E field on an imperfect conductor would be highly dependent on the conductivity of the wire, and I'd guess it would be very small compared to the influence of the H field from a typical oncoming wave on an electron in a good conductor. Maybe that's what he was saying. Roy Lewallen, W7EL |
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#7
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Roy, W7EL wrote:
"But, if the antenna conductor were perfect, no E field at all could exist at the wire surface regardless of the magnitude of the E field of the oncoming wave." If we have a non-varying E field, a perfect conductor in the field would have the same voltage everywhere due to the short-circuit connecting all points. But, an electromagnetic wave sweeping the wire has an alternating electric field. Its phase is uniform (the same) across the wavefront because all points are equidistant from the source. A wire parallel to the E vector would simultaneously experience the same E field force throughout its length. "No E field at all could exist at the wire surface regardless of the magnitude of the E field of the oncoming wave," Why must the wire be perfect? Best regards, Richard Harrison, KB5WZI |
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#8
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Richard Harrison wrote:
Roy, W7EL wrote: "But, if the antenna conductor were perfect, no E field at all could exist at the wire surface regardless of the magnitude of the E field of the oncoming wave." If we have a non-varying E field, a perfect conductor in the field would have the same voltage everywhere due to the short-circuit connecting all points. But, an electromagnetic wave sweeping the wire has an alternating electric field. Its phase is uniform (the same) across the wavefront because all points are equidistant from the source. A wire parallel to the E vector would simultaneously experience the same E field force throughout its length. "No E field at all could exist at the wire surface regardless of the magnitude of the E field of the oncoming wave," Why must the wire be perfect? A time-varying E field can exist in a non-perfect conductor; it cannot exist in a perfect conductor. You can find the explanation for why this is in any electromagnetics text. Roy Lewallen, W7EL |
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#9
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Roy Lewallen wrote: Well, it's obvious that an electric field can move an electron. The Lorentz force law tells us how much force results from a given E field, and we can get the resulting acceleration from Newtonian physics. An everyday example is an oscilloscope deflection system which uses an electric field to deflect electrons. (Actually, modern digital scopes typically use raster displays with magnetic deflection -- but many of still have older analog types with electric field deflection.) Yes, I thought that much was obvious as well. But if the antenna conductor were perfect, no E field at all could exist at the wire surface regardless of the amplitude of the E field of the oncoming wave. The wave's E field therefore couldn't directly influence the electrons in the (perfect) conductor. Only the H field of the wave, then, can induce a current in the perfect conductor. The direct influence of the E field on an imperfect conductor would be highly dependent on the conductivity of the wire, and I'd guess it would be very small compared to the influence of the H field from a typical oncoming wave on an electron in a good conductor. Maybe that's what he was saying. Roy Lewallen, W7EL It could be what he was saying. But conductors are are called conductors for a reason, and it's not necessarily because they conduct magnetic fields well. 73, ac6xg |
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