- www. phy. olemiss. edu
in S O 1997 - 2001) An e—BOOk et difference AV across a piece of metal due to a temperattue AT is calÞd the effect2 To tilde of this effect mtroduce a special ccefficient which is cÞfined as potential #ped unit difference, e AT Voltage AV Seebeck effect A gradient along a conductor gives rise to a potential Figure I By convention, sign of S the of the cold side with resxct to hot side
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