How to calculate magnetic/electric field near an overhead power line?

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SUMMARY

This discussion focuses on calculating the magnetic and electric fields produced by overhead power lines, specifically those operating at 230V. Participants highlight the complexity of these calculations due to the dynamic nature of the fields and the importance of current over voltage for accurate assessments. Key equations provided include the vector magnetic potential and the relationship between magnetic and electric fields, emphasizing the near-field approximation for distances like 5 meters. The conversation also touches on the configuration of power lines in the US, where two insulated wires operate at 115V each, 180 degrees out of phase, effectively canceling their fields beyond a few wire diameters.

PREREQUISITES
  • Understanding of electromagnetic theory, particularly Maxwell's equations.
  • Familiarity with vector calculus, specifically curl and divergence operations.
  • Knowledge of power line configurations and their electrical characteristics.
  • Basic principles of alternating current (AC) and phase relationships.
NEXT STEPS
  • Study the calculation of vector magnetic potential using the formula: \vec A=\frac {\mu_0\;I}{4\pi}\oint_c \frac {e^{-j\beta R}}{R}d\vec l'.
  • Learn about the near and far field approximations in electromagnetic field theory.
  • Explore Yungman's formula for calculating fields around multiple conductors.
  • Investigate the impact of phase differences in AC circuits on electromagnetic emissions.
USEFUL FOR

Electrical engineers, physicists, and anyone involved in power distribution or electromagnetic field analysis will benefit from this discussion.

arroy_0205
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The usual overhead power distribution wires are said to have potential of 230V in a certain locality. (These are voltage levels in wires seen along streets electricity pillars and these enter house of consumers.) How does one calculate magnetic field and electric field produced by the wire at a certain distance, say 5m from the wire? I am confused because when we say 230V, we do not mention, with respect to what this is stated. It becomes easier if current instead of voltage is stated for the wires which however is never the case. Can anybody please help?
 
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arroy_0205 said:
The usual overhead power distribution wires are said to have potential of 230V in a certain locality. (These are voltage levels in wires seen along streets electricity pillars and these enter house of consumers.) How does one calculate magnetic field and electric field produced by the wire at a certain distance, say 5m from the wire? I am confused because when we say 230V, we do not mention, with respect to what this is stated. It becomes easier if current instead of voltage is stated for the wires which however is never the case. Can anybody please help?

I think this is a hard problem since it is not static. I can only make a guess from material of antennas. And I don't think you can calculate from the voltage.

We start by finding the vector magnetic potential:

\vec A=\frac {\mu_0\;I}{4\pi}\oint_c \frac {e^{-j\beta R}}{R}d\vec l' \;\hbox { where } R \;\hbox { is distance from dl' to the observation point and }\; \beta =\frac {2\pi}{\lambda}

The line integral integrate along the transmission line. First pass assume it to be a straight line and make it easy. But it is really like a hanging chain problem and the equation of the line is more complicate.Then find magnetic field B using \vec B = \nabla \times \vec A

Since it is a time varying field, there is always an electric field accompany with the magnetic field. We find the electric field by:

\vec E =\frac 1 {j\omega \epsilon_0}\nabla \times \vec H

Since this is power line, the wave length is very long, so \beta \approx 0. This will simplify the calculation. But still when you work the whole problem out, it is going to be in three space. Further approximation on how far the observation point from the line and simplify the \nabla \times\; result. This is basically the near and far field approximation. In your case of 5m distance only, a near field approx should be good enough.

I don't claim this is the answer, I just want to joint in and put in my piece.
 
Last edited:
hmmmm

here in US the wires entering a house are run as a pair, two at nominal 115V , 180 degrees out of phase. They are insulated.
Both of them are twisted around a bare metal supporting cable,
forming a twisted pair, if unshielded.

Yungman's formulae should be applied to all three conductors and the results added.

i think, since at any instant one wire has opposite polarity from the other,
that beyond a few wire diameters the two fields will so nearly cancel out that the net electric field is for all practical purposes,,, zero.
The magnetic field would be also very nearly zero because any unbalance in current between the two insulated wires returns through the bare one.
So, since the currents add to zero, [h dot dl ] around the wire bundle is zero. No magnetic field ??

........

"I am confused because when we say 230V, we do not mention, with respect to what this is stated."

walk out in your back yard and study the transformer.
here in US, the low voltage winding is the one with shorter insulators and your two insulated wires going to the house come from the ends of that winding. It is 230 volts between those two insulators.
The center-tap of that winding is connected to the bare support wire and to earth.
Each of the insulated wires is 115V respect to centertap (and therefore to earth), but they're of exactly opposite phase
so the difference between them ( + 115 to - 115) is 230.
i think of the centertap as my reference. Many folks use Earth instead, note the centertap and Earth are are connected so we'll get same answer.

go back about a month in this forum and look for threads on "ground" - some of the folks who are more capable than me put up excellent drawings. Good reading!

old jim
 
I only think of it is a single wire! If it is two wires twisted together, theoretically it has no emission as the return is 180 deg out of phase.
 

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