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Figure 5.3 Radiant energy
per unit wavelength emitted
by a blackbody with a surface
temperature of 5777 K.
0
0.0
0.5
1.0
1.5
2.0
2.5
3.0
Wavelength (
μ
m)
directions and absorbs all incident radiation. The area across a small hole in
a  container whose internal surface temperature is uniform approximates the
behavior of a black body.
The spectral irradiance, i.e., radiant energy emitted per unit wavelength by a
blackbody, R l , expressed as function of the surface temperature T s (in K) is shown
in Fig. 5.3 and is given by Planck's Law , which has the form:
C
1
R
=
λ
(5.1)
C
5
l
exp
1
2
l
T
s
where C 1
λ max , at
which most blackbody radiation is emitted is given by We i n's L aw , which has the
form:
=
3.74
×
10 −16 W m −2 and C 2
=
1.44
×
10 −2 K. The wavelength,
2897
l
=
[with
l in
μ
m and T S in K]
(5.2)
max
T
s
The total flux of radiation, R , emitted by a blackbody per unit area of surface per
unit time is given by the Stefan - Boltzmann Law , which has the form:
4
RRd T
=
l
=
σ
(5.3)
l
s
0
in which
Boltzmann constant, R is in W m −2
and T s is in K. Together Equations (5.2) and (5.3) require that as the surface tem-
perature rises, the maximum wavelength at which most radiation is emitted
σ
=
5.67
×
10 −8 W m −2 K −4 is the Stefan
 
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