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#1
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It is said that a transmitted UWB pulse should not have any DC because
of the transmitting antenna: "Without getting into the details of the physical generation of UWB waveforms, it is sufficient to note in this regard that the transmitting antenna has the general effect of differentiating the time waveform presented to it. As a consequence the transmitted pulse does not have a DC (direct current) value-the integral of the waveform over its duration must equal zero." (page 4, http://www.antd.nist.gov/wctg/manet/...rt_April03.pdf) Would someone please explain that for me? Thanks! -- Harry |
#2
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Harry wrote:
Would someone please explain that for me? DC steady-state does not cause electrons to emit photons. For RF photons to be emitted from a copper wire dipole, the free electrons must be accelerated and decelerated. The DC component cannot accomplish that feat. -- 73, Cecil http://www.qsl.net/w5dxp |
#3
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![]() Cecil Moore wrote: Harry wrote: Would someone please explain that for me? DC steady-state does not cause electrons to emit photons. Except in flashlights, apparently. For RF photons to be emitted from a copper wire dipole, the free electrons must be accelerated and decelerated. The DC component cannot accomplish that feat. Quantum mechanics is completely unnecessary here, Cecil. I think Faraday still provides the best explanation. ac6xg |
#4
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![]() Jim Kelley wrote: Cecil Moore wrote: Harry wrote: Would someone please explain that for me? DC steady-state does not cause electrons to emit photons. Except in flashlights, apparently. For RF photons to be emitted from a copper wire dipole, the free electrons must be accelerated and decelerated. The DC component cannot accomplish that feat. Quantum mechanics is completely unnecessary here, Cecil. I think Faraday still provides the best explanation. ac6xg With a ns pulse into a zero resistance conductor in free space all energy should be radiated, so no DC component if you look at the input power. However if you introduce the same pulse to a circuit that has magnetic properties, i.e. a ferrite inductor as an example, there is energy used to align the molecules in the material, not radiated, which results in a DC component. In a flashlight, most of the energy is heat, which will result in a big DC component with no radiation rf wise. That's really advanced stuff for a Ham Radio Newsgroup. Gary N4AST |
#5
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Iok so i am confused on a few things
the photo part so regardless of weither or not there is or isn't ac or dc , when i xmit (ham or other freq's) are photons being generated?? where would they be?? nearfield? around the antenna? how would i measure the presence/qty of such?? the other thing i got fuzzy on static polar field as Mr. clark mentions so why does the battery produce it /how?? are you referring to the fact that is has 'mass' and therefore.... or did i miss the obvious thanks fuzzylogic fuzzynavels fuzzypeaches |
#6
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ml wrote:
Iok so i am confused on a few things the photo part so regardless of weither or not there is or isn't ac or dc , when i xmit (ham or other freq's) are photons being generated?? where would they be?? nearfield? around the antenna? how would i measure the presence/qty of such?? the other thing i got fuzzy on static polar field as Mr. clark mentions so why does the battery produce it /how?? are you referring to the fact that is has 'mass' and therefore.... or did i miss the obvious thanks fuzzylogic fuzzynavels fuzzypeaches Don't listen to these guys. They're changing the subject by changing the scale of the argument in order to digladiate with one another. The truth is, that if an antenna really differentiates a signal so that what it radiates is based on the rate of change of the original signal, then the DC part of the original signal won't contribute to the radiation because the rate of change of a constant(the DC part)is zero. It isn't any more complicated than that. 73, Tom Donaly, KA6RUH |
#7
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Jim Kelley wrote:
Quantum mechanics is completely unnecessary here, Cecil. I think Faraday still provides the best explanation. In this particular case, quantum mechanics offers the easiest-to-understand explanation. As Feynman put it: "So now, I present to you the three basic actions, from which all the phenomena of light (including RF) and electrons arise. -Action #1: A photon goes from place to place. -Action #2: An electron goes from place to place. -Action #3: An electron emits or absorbs a photon." QED^2 :-) -- 73, Cecil http://www.qsl.net/w5dxp |
#8
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Jim Kelley, AC6XG wrote:
"I think Farqaday stilll provides the best explanation." Yes. Faraday showed d-c had nothing to do with wireless. It was the a-c motivating wireless electrical coupling. An Englishman, Faraday, constructed a transformer in 1831. He used two isolateed coils of wire wound on the same spool. He connected a galvanometer across one coil. He noticed a brief deflection of the galvanometer each time he connected or disconnected a battery to the second coil. Joseph Henry, a professor at Albany Academy in New York was independently making the same observations at the same time as Faraday. When Henry got news of Faraday`s discoveries, he made no effort to claim credit for his own work but often referred to Faraday`s discovery. It was the change in the magnetic field which induced electricity without a direct connection, not the value of the steady magnetic field itself. Same with antennas. A battery connected to an antenna sends no signal. A varying field is required to produce a signal in an antenna. Best regards, Richard Harrison, KB5WZI |
#9
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#10
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Joseph Henry, a professor at Albany Academy in New York was
independently making the same observations at the same time as Faraday. When Henry got news of Faraday`s discoveries, he made no effort to claim credit for his own work but often referred to Faraday`s discovery. It was the change in the magnetic field which induced electricity without a direct connection, not the value of the steady magnetic field itself. Slight correction: it is the change in the magnetic flux that gives induced EMF. You can get an induced current from a constant magnetic field if the circuit loop moves in or out of the field, changing the flux throught the loop. Tor N4OGW |
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