Electric power transmission - what is different at a particle level?

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Discussion Overview

The discussion revolves around the differences in electric power transmission at a particle level, particularly focusing on the implications of voltage and current on energy loss. Participants explore theoretical and conceptual aspects of power transmission, including the use of AC versus DC, and the role of conductors and insulators.

Discussion Character

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

Main Points Raised

  • One participant presents two methods of transmitting 1 MW of power, questioning the particle-level differences in energy loss associated with each method.
  • Another participant uses a water analogy to explain voltage and current, suggesting that high voltage and low current reduce losses due to better insulator performance compared to conductors.
  • A participant asserts that AC transmission results in lower losses compared to DC transmission, referencing historical context involving Edison and Faraday.
  • Contrarily, another participant challenges this claim, stating that losses for a given voltage and current are the same, emphasizing that high AC voltages are easier to achieve due to transformer technology.
  • At the atomic level, it is suggested that higher voltage results in lower current, leading to fewer collisions between electrons and the atomic lattice, thus reducing energy loss to heat.
  • Further discussion includes the implications of constant current versus constant voltage sources in power distribution, with a focus on losses incurred in each scenario.
  • One participant expresses uncertainty about the energetic equivalence of collisions at different voltages and questions which scenario leads to less power loss to phonons.

Areas of Agreement / Disagreement

Participants express differing views on the efficiency of AC versus DC transmission and the implications of voltage and current on energy loss. There is no consensus on the particle-level mechanisms or the best approach to minimize losses.

Contextual Notes

The discussion includes various assumptions about the properties of conductors and insulators, the historical context of power transmission technologies, and the limitations of current materials in achieving optimal efficiency.

SciencePF
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Hello!
1 MW can be transmitted , for example, in 2 ways:

1MW=100V*10000A;

or

1MW=10000V*100A.

In the second case less energy is lost because P=RI^2. But my question is: what is different at a particle level to deeply understand what is going on?

Thanks
 
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Take the water analogy: voltage can be compared to difference in height, and current can be compared to water flow. You can obtain the same power transmission by a small tube mounted 2 km above the surface, which will transport a small water flow a long way, until it arrives at the point of where you want to use the power. There you let it flow downward, and, say, drive a water mill. The high pressure of the water (2 km water column!) makes that a small amount of water can deliver a lot of power.
Or you can have a big tube, at 10 meters above ground, with a big flow of water. This time the pressure isn't very high, but the big flow compensates, and the water mill will deliver the same amount of power.

Why is it interesting to use high voltages and small currents ? For two reasons: our insulators are better than our conductors, and they are cheaper too.

A high voltage over an insulator causes almost no losses. A big current through a conductor does. If we would have had more leaky insulators (say, in the sea), and superconductors, then the decision might have been different.

The power is transported both by the conductors and the insulators.
 
Ok, thanks. I understood, but not at a particle level.
 
The loss is only lower using AC transmission.

It was the primary cause of the falling out between Edison (a DC proponent) and Faraday (an AC proponent) who showed that AC transmission had much lower losses than DC transmission for the same Power delivered to the customer. It's a big part of the reason Westinghouse gave him 20 million for the patent around the 1920's. Imagine, a brand new Ford is $80 and you just got a cheque for 20 million. Good idea that AC.
 
wysard said:
The loss is only lower using AC transmission.

Not true. For a given voltage and current, the losses are the same. The difference is that high AC voltages are much easier to make, since all you need are transformers for the step-up at the generating station, and the step-down at the distribution stations and at the neighborhood distribution transformers. Especially back in Edison's time, DC-DC voltage conversion was not very well developed.

To the OP -- at the atomic level, higher voltage means less current, which means fewer collisions between the electrons and the lattice of atoms in the conducting wires. Fewer collisions means less power lost to phonons in the lattice (vibrations making heat).
 
vanesch said:
Take the water analogy: voltage can be compared to difference in height, and current can be compared to water flow. You can obtain the same power transmission by a small tube mounted 2 km above the surface, which will transport a small water flow a long way, until it arrives at the point of where you want to use the power. There you let it flow downward, and, say, drive a water mill. The high pressure of the water (2 km water column!) makes that a small amount of water can deliver a lot of power.
Or you can have a big tube, at 10 meters above ground, with a big flow of water. This time the pressure isn't very high, but the big flow compensates, and the water mill will deliver the same amount of power.

Why is it interesting to use high voltages and small currents ? For two reasons: our insulators are better than our conductors, and they are cheaper too.

A high voltage over an insulator causes almost no losses. A big current through a conductor does. If we would have had more leaky insulators (say, in the sea), and superconductors, then the decision might have been different.

The power is transported both by the conductors and the insulators.

Very good post. Let me just add a few comments along those lines. Insulators are so good that we just take them for granted. To get a perfect conductor, we must super-cool certain types of materials, which is expensive and unwieldy. Until high-temperature superconductors become available and affordable, conductors will be much much very much lossier than insulators.

We don't use the term "super insulator" because insulators are very good over a vast range of temperature. No super-cooling or heating is needed at all to get super-insulativity.

With power transmission, there are two losses, namely I^2*R (conductor), and V^2*G (insulator). For affordable common materials used as conductors and insulators I^2*R greatly exceeds V^2*G. Hence there is a great advantage to using high V with low I as it minimizes losses.

Also, I used to wonder why power generators are always operated at constant speed to output constant voltage. Why not turn the generator at a constant torque to get a constant current source? The answer is along the same line as above.

With constant current source (CCS) operation, the load receives a constant current, and the voltage varies with resistance of the load. To shut off power, let's say we're turning off a lamp, a switch is placed across the lamp, in parallel, and CLOSED. The constant current is shunted and the lamp turns OFF. Opening the switch turns the lamp on.

So, with CCS power distribution, when we shut off power, a constant current is transported from the power generator all the way to our homes only to be shunted by switches in parallel with the loads. This results in huge power losses. With CVS (constant voltage source) generators, we turn off power by opening a series switch. With CCS we incur I^2*R loss under no load. With CVS we only incur V^2*G. CVS incurs MUCH LOWER power losses than CCS.

The same holds with batteries. All battery producers for many decades have focused their effort on CVS operation, NOT CCS. If we had CCS batteries in our flashlight, and we turn them off by shunting the current through a switch, we get I^2*R losses continuously. A week later, when you attempt to turn on the flashlight, your batteries are gone.

Something to think about. BR.

Claude
 
Thank you berkeman. I was trying to figure out how to explain the collisions part and couldn't come up with a good analogy. I too like the water analogy and will happily watch the thread develop.

Thanks again.
 
berkeman said:
To the OP -- at the atomic level, higher voltage means less current, which means fewer collisions between the electrons and the lattice of atoms in the conducting wires. Fewer collisions means less power lost to phonons in the lattice (vibrations making heat).

Ok, but with lower voltage means more current, which means more collisions between the electrons and the lattice of atoms in the conducting wires.

I think that in both cases the collision are not energetically equal, and the question is: which one contribute with less power lost to phonons in the lattice?

Thanks!
 

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