myself said:
ah, but the resistance is always constant, whether there is voltage passing through it or not. If you have the resistor hooked up to a 6 volt battery, the resistance is still 220 ohms. True, there is a 6 volt voltage drop across the resistor, but the resistance is constant. It's harder to picture a "current being forced through it" because it is more difficult to make a constant-current source than a constant-voltage source. I hope this clarified something.
it depends on the physical size of the resistor (it's wattage rating) in comparison to the power you are forcing it to dissapate (which is a function of the current). and it depends on the composition of the resistive element (carbon does different things than metal, when heated up). the resistance, under adverse circumstances, is not
always constant. saying that it is "always" is one of those sweeping statements that is pretty damn hard to prove (one valid counter-example will disprove it and anyone who has done volt-amp characteristics of a physical part and pushed it to the limit knows of such a counter example.) there is also some well known physics of the properties of metal and other materials that shows that the resistivity is a function of temperature. see
http://en.wikipedia.org/wiki/Resistivity
The power line doesn't start heating up by that much, because of two things: first, it is low resistance, and second current is low.
for power mains? that's a silly statement.
Why is current low? You look at POWER consumed by the people using electricy. Since energy is conserved, the power is constant, P = IV. But the line carries high voltage, so I is very small within the line.
yeah, but cities are
big. i don't know if it is still the case, but when that big blackout of NYC happened in the 70s or early 80s, i remember reading that the whole of the city was supported by 5 main trunk lines. it was hot and muggy, lot'sa air conditioning, thunderstorms were around, lightning took out 2 of those lines, and the the current load was transferred to the 3 remaining, and they heated up. when one drooped low enough to contact a tree or some structure, that was it. blackout.
i'm not saying that they heated up to anything like melting or softening of the metal, but i'll bet they got warm to the touch. over ambient temperature.
but, even in normal circumstances, those lines are carrying nearly 1000 amperes (less than
1/
2 MV and hundreds of MW, you do the math) and even though the conductors are pretty large in cross-section, in AC lines (nearly all) the great majority of the current is carried very near to the surface of the conductor (called "skin effect").
Then we use P = IR^2 within the line itself (since we want to see power consumed within the line), and since R is small and I is small, power dissipated in the line is small as well.
"small" is a relative term. i read that transformers are about 99% efficient (1% loss), yet the total distribution loss in the power grid and delivery to the consumer is about 7%. where does that other 4% go (assuming 3 levels of distribution, each coupled with a transformer)?
The idea about power lines drooping is true, but you have to realize that thermal expansion doesn't occur on that large of a scale (the expansion coefficient for steel is 12 * 10^-6 (1/K)) which isn't that large.
large enough to cause drooping of several meters that cause contact and shorting in these adverse situations. you cannot claim that
both the temperature change is "small" (in the adverse circumstances)
and that the coefficient of expansion is "small". there would be nothing left to explain the drooping which hasn't been small in these adverse circumstances.
And you also have to remember that power lines dissipate heat through air.
of course they do, just like the resistive element on my electric stove top.
But what you say is true; things like that do happen when power lines carry too much power.