A two-color pyrometer is a device that is used to measure the temperature of a diffuse surface, T s . The device measures the spectral, directional intensity emitted by the surface at two distinct wavelengths separated by Δ λ . Calculate and plot the ratio of the intensities I λ + Δ λ , e ( λ + Δ λ , θ , ϕ , T s ) and I λ , e ( λ , θ , ϕ , T s ) as a funtion of the surface temperature over the range 500 K ≤ T s ≤ 1000 K for λ =5 μ m and Δ λ = 0.1 , 0.5 , a n d 1 μ m . Comment on the sensitivity to temperature and on whether the ratio depends on the emissivity of the surface. Discuss the tradeoffs associated with specification of the various values of Δ λ . Hint: The change in the emissivity over small wavelength intervals is modest for most solids, as evident in Figure 12.17.
A two-color pyrometer is a device that is used to measure the temperature of a diffuse surface, T s . The device measures the spectral, directional intensity emitted by the surface at two distinct wavelengths separated by Δ λ . Calculate and plot the ratio of the intensities I λ + Δ λ , e ( λ + Δ λ , θ , ϕ , T s ) and I λ , e ( λ , θ , ϕ , T s ) as a funtion of the surface temperature over the range 500 K ≤ T s ≤ 1000 K for λ =5 μ m and Δ λ = 0.1 , 0.5 , a n d 1 μ m . Comment on the sensitivity to temperature and on whether the ratio depends on the emissivity of the surface. Discuss the tradeoffs associated with specification of the various values of Δ λ . Hint: The change in the emissivity over small wavelength intervals is modest for most solids, as evident in Figure 12.17.
Solution Summary: The author explains the R value (ratio of intensities) emitted from surface at nominal wavelength oflambda.
A two-color pyrometer is a device that is used to measure the temperature of a diffuse surface,
T
s
. The device measures the spectral, directional intensity emitted by the surface at two distinct wavelengths separated by
Δ
λ
. Calculate and plot the ratio of the intensities
I
λ
+
Δ
λ
,
e
(
λ
+
Δ
λ
,
θ
,
ϕ
,
T
s
)
and
I
λ
,
e
(
λ
,
θ
,
ϕ
,
T
s
)
as a funtion of the surface temperature over the range
500
K
≤
T
s
≤
1000
K
for
λ
=5
μ
m
and
Δ
λ
=
0.1
,
0.5
,
a
n
d
1
μ
m
. Comment on the sensitivity to temperature and on whether the ratio depends on the emissivity of the surface. Discuss the tradeoffs associated with specification of the various values of
Δ
λ
. Hint: The change in the emissivity over small wavelength intervals is modest for most solids, as evident in Figure 12.17.
Consider an ideal gas enclosed in a spectral tube. When a high voltage is placed across the tube, many atoms are excited, and all excited atoms emit electromagnetic radiation at characteristic frequencies. According to the Doppler effect, the frequencies observed in the laboratory depend on the velocity of the emitting atom. The nonrelativistic Doppler shift of radiation emitted in the x direction is f = f0(1 + vx / c). The resulting wavelengths observed in the spectroscope are spread to higher and lower values because of the (respectively) lower and higher frequencies, corresponding to negative and positive values of vx. We say that the spectral line has been Doppler broadened. This is what allows us to see the lines easily in the spectroscope, because the Heisenberg uncertainty principle does not cause signifi cant line broadening in atomic transitions. (a) What is the mean frequency of the radiation observed in the spectroscope? (b) To get an idea of how much the spectral line is…
as fast as.
Determine the following:
a. Average emissivity of both surfaces
b. Absorptivity of both surfaces
c. reflectivity of both surfaces
d. which surface is more suitable to serve as a solar absorber?
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