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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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