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to the induced voltage, V, across the material divided by the temperature
difference when there is no current flow, such that
r T ¼ dV
E
dT ¼ dV
dx
S ¼
(6 : 2)
dx
dT
d n 3 r 4 n g | 7
.
Figure 6.1
(a) Some remarkable studies of thermoelectric materials. Reprinted with
permission from Ref. 13. Copyright r 2010 WILEY-VCH Verlag GmbH &
Co. KGaA, Weinheim. (b) Eciency of mechanical heat engines compared
with thermoelectric figures of merit. Reprinted with permission from Ref.
11. Copyright r 2009 Nature Publishing Group. 11,13
 
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