So I plug in a circuit 299,792,458 meters long into my wall outlet

  • Context: Graduate 
  • Thread starter Thread starter BrianConlee
  • Start date Start date
  • Tags Tags
    Circuit Wall
Click For Summary

Discussion Overview

The discussion revolves around the theoretical implications of connecting a circuit that is 299,792,458 meters long (one light second) to a standard wall outlet providing 60 Hz AC current. Participants explore concepts related to signal propagation, circuit behavior, and the physical characteristics of such a long circuit.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that the signal in the circuit would travel from both terminals simultaneously, meeting in the middle after half a second, while others suggest that the circuit behaves like independent wave-guides with significant capacitance and impedance.
  • There is a discussion about whether the entire loop would change polarity in unison or if it would propagate as waves running down the loop.
  • One participant emphasizes the complexity of turning on a 60 Hz signal, noting that a sinusoidal waveform modulated by a step function would contain high-frequency information and not reach a steady state immediately.
  • Another participant introduces the idea of using parallel wires to create electric and magnetic fields, discussing the time it would take for a TEM wave to propagate along the wires.
  • There is mention of the need to consider the Telegrapher's equation to understand the propagation of signals in such a long circuit, indicating that the initial behavior would not be straightforward.
  • One participant suggests an experimental approach using a long section of wire to observe the effects of signal propagation and the limitations of Fast-Ethernet over long distances.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the behavior of the circuit, particularly concerning signal propagation and the nature of the current flow. The discussion remains unresolved with no consensus on the specific dynamics of the circuit.

Contextual Notes

Limitations include the assumptions made about the circuit's ideal conditions, the simplifications regarding wave propagation, and the complexities introduced by real-world factors such as resistance and radiative losses.

BrianConlee
Messages
65
Reaction score
0
Hope the subject caught your attention, I just wanted to clarify my some things about ac current...

Ok, for our "circuit" we're going to have copper wire for simplicity's sake. Also, we're going to say that our Electric force travels at c on the wire. Just a big loop, no sharp turns, nothing crazy. Ignore the obscene Ohmic losses we would have unless our voltage was in the google range. (wow, can you imagine that?) And the circumfrence is 299,792,458 meters long.

Now, with the 60 Hz current coming out of my wall, and the circuit an entire light second long:

1. Does the signal travel from positive to negative, taking an entire second to circle the circuit or does the signal leave both terminals simultaneously and "meet in the middle" taking 1/2 a second to effectively traverse the entire circuit?

2. At any given instant, if you freeze the circuit in time, is the current changing direction 120 times along the entire circuit? (2 direction changes per hertz on a sinosoidial wave).

3. Since the whole circuit is just one big loop with a current, is it a solenoid? Or, if question 2 is "yes," how does this affect things?

4. Assuming copper is about .75 per meter, does anyone have about 225 million dollars I can borrow to build it? I'm sure the U.S. Government could just write a check, right?Thanks!
 
Physics news on Phys.org
The paradigm for your example as an AC circuit with long length relative to the wavelength of the AC signal. When you switch on the current the two ends of the circuit will behave like independent wave-guides. They will have a large capacitance and impedance at the given ac frequency and so the 60Hz waves will propagate down each end meeting at the far point a half second later. Given it is exactly 1 light-second in length and given the AC signal is exactly 60Hz you'll get constructive interference at the far end and after one second the current should settle down to approximately the long term cyclic behavior.

Now this is a gross simplification. The actual propagation will initially follow the Telegrapher's equation, propagating more like a series of diffusive waves until it settles down to long term "steady" state. Even with no pure resistance you'll get radiative losses.

What you have is basically a loop antenna for ELF (Extremely Low Frequency) radio.
 
jambaugh said:
after one second the current should settle down to approximately the long term cyclic behavior.

Now this is a gross simplification. The actual propagation will initially follow the Telegrapher's equation, propagating more like a series of diffusive waves until it settles down to long term "steady" state.


So, basically, the entire loop will be changing polarity in unison? Not as waves running down the loop?

Oh, and thank you very much for the answer to the 1 second / .5 second question.
 
You need to remember that there is no such thing as "suddenly" turning on a 60Hz signal; try drawing the waveform (in the time-domain) and you will see why.
I guess what you have in mind is a sinusodial waveform modulated by a step function (which obviously won't be a real step-function in a real circuit).
However, a waveform like that will contain a LOT of high-frequency information meaning it is not really a "steady state" 60 Hz sine until everything has settled down which can take quite a while. As jambaugh has already suggested you need to solve a telegraph equation in order to see how thing really evolve in time (not really difficult, but quite messy).

If you are interested in this I would suggest you download e.g. LTSpice (free from www.linear.com) and play with some simple circuits.
 
If you had two parallel wires, one for positive and one for negative, or one for hot AC and one for neutral AC, you would have both electric and magnetic fields between the two conductors. The pair would be about 1.5 x 10^8 meters long, and a TEM (transverse electric magnetic) wave would take about 1/2 second to get to the end, and another 1/2 second to get back. If you had a single turn coil (solenoid) you still need time to charge up the magnetic field in the center of the loop, and the time would be similar. If there are no losses, and the coil did not radiate (like a loop antenna), it would just oscillate, using the permeability and permittivity of free space as the resonant inductance and capacitance.
 
If you have access to a 1Ghz DSO, a signal source, and a hundred meter or longer section of wire not in a tight coil, but looped back gently on itself, you have a very instructive experiment.

Several reasons why Fast-Ethernet doesn't work well beyond about 200m are visible.
 

Similar threads

  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 14 ·
Replies
14
Views
3K
  • · Replies 19 ·
Replies
19
Views
3K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 10 ·
Replies
10
Views
11K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 9 ·
Replies
9
Views
2K
  • · Replies 0 ·
Replies
0
Views
922