W
whit3rd
Guest
On Friday, December 10, 2021 at 6:14:23 PM UTC-8, palli...@gmail.com wrote:
The simple ideal metal doesn\'t expand or contract with temperature changes, hasn\'t
any crystal defects, no bandgap changes, no magnetism, Einstein model phonon
spectrum, and all resistance is the consequence of electron-phonon scattering.
Then, if you know the thermal phonon population, THAT determines the resistivity.
Alloys for low tempco have various deviations from these behaviors, so the thermal phonon
population statistic is not dominant.
PT1000/PT100 is ~0.4%/C
Oh, that\'s just about true for all classical metals; getting a non-PTAT (proportional
to absolute temperature) resistor is a notable materials-science achievement.
At 20 C, proportional to absolute temperature means about 0.0034 per kelvin; for
copper, resistance goes 0.00386, for tungsten 0.0045, for aluminum 0.00429,
for platinum 0.0039 ...
The impure (alloyed) metals used for low tempco have very non-ideal metallic nature.
** \" very non- ideal metallic nature\" ???????
Could you please be bit more ambiguous ??
The simple ideal metal doesn\'t expand or contract with temperature changes, hasn\'t
any crystal defects, no bandgap changes, no magnetism, Einstein model phonon
spectrum, and all resistance is the consequence of electron-phonon scattering.
Then, if you know the thermal phonon population, THAT determines the resistivity.
Alloys for low tempco have various deviations from these behaviors, so the thermal phonon
population statistic is not dominant.