
[
9.3.1 — Planck’s law
]
© FLIR Systems AB –
Publ. No.
557 369 –
Ed. A
53
where:
W
λ
b
= the blackbody spectral radiant emittance at wavelength
λ.
c
= the velocity of light = 3 x 10
8
m/sec.
h
= Planck’s constant = 6.6 x 10
-34
Joule sec.
k
= Boltzmann’s constant = 1.4 x 10
-23
Joule/K.
T
= the absolute temperature (K) of a blackbody.
λ
= wavelength (m).
N.B. –
The factor 10
-6
is used since spectral emittance in the curves is expressed
in Watt/m
2
µm. If the factor is excluded, the dimension will be Watt/m
2
m.
Planck’s formula, when plotted graphically for various temperatures, produces a
family of curves. Following any particular Planck curve, the spectral emittance is
zero at
λ
= 0, then increases rapidly to a maximum at a wavelength
λ
max
and after
passing it approaches zero again at very long wavelengths. The higher the temper-
ature, the shorter the wavelength at which maximum occurs.
Figure 9.2
Blackbody spectral radiant emittance according to Planck’s law,
plotted for various absolute temperatures.
W
λ
b
2
π
hc
2
λ
5
e
hc
λ
k T
⁄
1
–
(
)
---------------------------------------
10
6
–
×
Watt m
2
µ
m
⁄
[
]
=
Summary of Contents for ThermaCAM PM575
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