View the thread, titled "Circuit Wire For Long Run" which is posted in UK Electrical Forum on Electricians Forums.

Ok, say you've got a lighting run with the last fixture being 1,280 meters away. 1,800 watts per phase 3 phase, 277/480Y volts though in this example we can use 230/400Y for the ease of discussion.

My question is- what size wire do I run for each phase and earth? What disconnection time do I use? Do I use a Type B, C or D breaker? What should my max R1+R2 come out to be?





1617360309073.png
 
If it is 75-30 = 45C colder then it would be 17.7% lower for the resistive part.

For big cables with X dominating Z the overall difference is going to be less, as that won't change much with temperature.


So my ignorance will show, but if I type in 17.7% of 2.0 in Google I will have the 30*C Ac resistance of 12 gauge wire?
 
Will this work with all wires sizes from 2.08mm2 to 1013mm2?
Yes, but only the the R term, the X term won't vary much with temperature and for large conductors that inductance starts to dominate the overall Z.

E.g. looking at post #40 you see X becomes comparable to R at cables around the 150mm or so size.
 
Yes, but only the the R term, the X term won't vary much with temperature and for large conductors that inductance starts to dominate the overall Z.

E.g. looking at post #40 you see X becomes comparable to R at cables around the 150mm or so size.


Last question- I promise ?

Any idea what the AC R would be at 150*C and 250*C? I'd like to use that as a basis to calc final short circuit conditions.
 
Last question- I promise ?

Any idea what the AC R would be at 150*C and 250*C? I'd like to use that as a basis to calc final short circuit conditions.
The basic assumption is copper is fairly linear w.r.t. temperature up to around 1000C (so anything that might be usable for a cable) so you have:

R = R20 * (1 + alpha20 * (t - 20))

Where R20 is the temperature at 20C (e.g. from tables) and alhpa20 is the coefficient at 20C which is around 0.00393 (depending on copper purity and annealing, etc, but not far off this).

So if looking at 250C and the 20C tabulated values for UK cables, then the adjustment factor is:

1 + 0.00393 * (250 -20) = 1.9039

So basically almost double the cold resistance.
 
What about 150*C?
Ummm......

R = R20 * (1 + alpha20 * (t - 20))

Where R20 is the temperature at 20C (e.g. from tables) and alhpa20 is the coefficient at 20C which is around 0.00393 (depending on copper purity and annealing, etc, but not far off this).

So if looking at 250C and the 20C tabulated values for UK cables, then the adjustment factor is:

1 + 0.00393 * (250 -20) = 1.9039

1618003633770.png
 
The basic assumption is copper is fairly linear w.r.t. temperature up to around 1000C (so anything that might be usable for a cable) so you have:

R = R20 * (1 + alpha20 * (t - 20))

Where R20 is the temperature at 20C (e.g. from tables) and alhpa20 is the coefficient at 20C which is around 0.00393 (depending on copper purity and annealing, etc, but not far off this).

So if looking at 250C and the 20C tabulated values for UK cables, then the adjustment factor is:

1 + 0.00393 * (250 -20) = 1.9039

So basically almost double the cold resistance.


If curious here is why I ask:



UL and the NFPA are using 25*C for their loop impedance calcs and a Ze of 0.25 ohms.

It is the belief of many electricians that the fault current is universally much higher than 500 amps.

If this is the case, that arc fault coverage reaches much further into the circuit. If we can prove that to be the case, much of 210.12 is nullified.




1618030597208.png



1618030660594.png



There is more, but thats the general part of it.
 
Last edited:

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