Effect of frequency on power in a wire?

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Discussion Overview

The discussion centers on the effect of frequency on power loss in wires, particularly how ordinary wires transition to behaving like antennas at higher frequencies. Participants explore the implications of wire length relative to wavelength and the mechanisms of power radiation versus containment in different frequency ranges.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants note that power losses in copper wire are relatively low at 60 Hz, but increase significantly at MHz frequencies, suggesting a transition to coaxial cables or heliax as transmission lines.
  • It is proposed that once the length of a wire approaches a quarter wavelength of the signal, it can radiate effectively, necessitating shielding or specific configurations like twisted pairs to minimize radiation.
  • One participant mentions that any length of wire can radiate, but it does so most effectively when at resonance with the frequency in question.
  • Another participant highlights that at low frequencies, such as 60 Hz, coupling can occur through electrostatic or magnetic means rather than through radiative coupling, which is more relevant at RF frequencies.
  • There is a suggestion that the question of when a wire begins to radiate is complex and context-dependent, akin to asking "how long is a piece of string?"

Areas of Agreement / Disagreement

Participants express varying views on the frequency ranges and conditions under which ordinary wires begin to radiate power. There is no consensus on a specific frequency or length at which this transition occurs, indicating ongoing debate and exploration of the topic.

Contextual Notes

The discussion includes references to different coupling mechanisms at low frequencies and the distinction between near-field effects and radiative coupling, which may not be fully resolved in the context of the conversation.

Evil Bunny
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We have relatively low power losses in copper wire at 60 Hz, but when you get up into the MHz range of frequencies, we start radiating and losing power and we switch from wire to something like coaxial cable or heliax and call it transmission line instead. We ground the outer conductor (shield) to "contain" the signal in the center conductor... Do I have the basics of that right?

But anyway, my question is at what frequency range does our ordinary wire start turning into an antenna and start radiating?

Any good sources on this?
 
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Once the length of a wire is approaching a quarter wavelength of the signal then it can radiate very well. To cut out the radiation you need to use a screen around it (as in coax) or use two wires - such as a parallel, balanced, transmission line or twisted pair.
In a coax cable, the 'return' current flows along the inside of the screen but you get leakage through the braid and the small currents that flow on the outside cause a small radiated signal and loss.

There isn't a simple answer to your "how long" question. It depends on the layout.
 
Lambda/4 is a reasonable rule of thumb.
 
Evil Bunny said:
But anyway, my question is at what frequency range does our ordinary wire start turning into an antenna and start radiating?

Any good sources on this?

Any length at all will radiate and at any freq. Simple as that :)
It just radiates the best when the length is at resonance with the freq concerned. Which is what is aimed for specifically with an antenna. As the freq in question rises then the resonant length decreases.

Dave
 
Okay... so I've heard the 60 Hz hum in certain equipment with unsheilded cable so I know that it must be radiating on some level. But apparently what you guys are saying is that once we get to a quarter wavelength, we will be in a scenario where most of the power is "radiating" instead of bein "contained" within the wire? That's probably not the best way of saying it, but it's the only way I can think to explain what I'm thinking.

Thank your for your replies!
 
There are other coupling mechanisms at very low frequencies (60 Hz qualifies). The hum you hear can be coupled electrostatically or magnetically, as opposed to by propagating EM waves. The ballasts in fluorescent lights, for example, generate magnetic fields (primarily at 60 Hz and the 3rd harmonic 180 Hz) that induce emfs in any conductive loops. Those loop can exist between wires, between traces on a PCB, or as a ground loop. This is different than the radiative coupling of a length of wire at RF
 
Evil Bunny said:
Okay... so I've heard the 60 Hz hum in certain equipment with unsheilded cable so I know that it must be radiating on some level. But apparently what you guys are saying is that once we get to a quarter wavelength, we will be in a scenario where most of the power is "radiating" instead of bein "contained" within the wire?
At low frequencies, you are in the 'near field' and nowhere near the distance where you need to consider an EM Radiated wave. You are just talking 'coupling' between elements, which can be magnetic or electric.
This whole question is very "how long is a piece of string?" and doesn't have an answer until you actually address a specific scenario.
 

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