Don, I agree with you, I posted the numbers above because they are the general numbers used in most class rooms and exams.Roger,
Those are on the high side for most applications. Those are the constants based on a 90?C operating temperature. At 60?C they would be 10.8 and 17.
Don, I agree with you, I posted the numbers above because they are the general numbers used in most class rooms and exams.
Roger
Roger,
Those are on the high side for most applications. Those are the constants based on a 90?C operating temperature. At 60?C they would be 10.8 and 17.
For general use, Copper is 10.371 ohm-circular mil/ft at 20?C plus/minus 0.0409 ohm-circular mil/ft. per ?C change.Is there a formula to calculate the resistivity constants based on temperature?
For general use, Copper is 10.371 ohm-circular mil/ft at 20?C plus/minus 0.0409 ohm-circular mil/ft. per ?C change.
Well there has been some changes in values over the years. The current base value can range from 10.371 to 10.2. Also, many use 0.039 per ?C but that value does not account for the change in volume that occurs with a change in temperature.I am not sure that is correct. I get 13.234 at 90?C
Hmmm.... and what are given as the values of R1 and t1.R2 = R1?(T0+t2)/(T0+t1)
Where T0 = 228 for aluminum, 234.5 for annealed copper, 241 for hard-drawing copper
t1 and t2 are in ?C
Source: Elements of Power System Analysis, William D. Stevenson, Jr., 2nd Edition, 1962.
Hmmm.... and what are given as the values of R1 and t1.
...and this leads to errors, as noted in the reference I linked. For example, if you backfigure R1@20?C from NEC Tables 8 and 9, then convert to ohm-cmil/ft, you see what I mean...R1 is the resistance at temperature t1. R2 is the resistance at temperature t2. The same would apply to resistivity or voltage drop constants that are proportional to resistivity. Maybe it is slightly different for resistivity because of thermal expansion, but not significantly.
See the notes at the end of Table 3 in your reference. The last equation is the same as Stevenson's, using the values of T in Table 3. T = 241 for 97.5% conductivity (hard-drawn) and 234.5 for 100% conductivity (annealed).
The advantage is if you know the resistance at some temperature other than 20?C, e.g. from NEC Table 9, Stevenson's equation is easier for calculating the resistance at a different temperature.
But the difference between your calculated values and 10.371 are very small, considering that the table values are only given to three significant figures, or can be explained by the fact that Table 9 is ac ohms and #6 AWG and larger are stranded in Table 8 (you have an error in ohm/kft for #8)....and this leads to errors, as noted in the reference I linked. For example, if you backfigure R1@20?C from NEC Tables 8 and 9, then convert to ohm-cmil/ft, you see what I mean...
The only values which correspond to a K of 10.371 are those for solid wire in Table 8. For stranded in Table 8, I wouldn't call a departure of 2% small, considering the implications of the result.But the difference between your calculated values and 10.371 are very small, considering that the table values are only given to three significant figures, or can be explained by the fact that Table 9 is ac ohms and #6 AWG and larger are stranded in Table 8 (you have an error in ohm/kft for #8).