Measured physical and optical properties of a stable polydisperse carbon black particle cloud at 532 nm and 1064 nm are reported. The particle cloud consisted of 99.7% spheroid primary particles (45–570 nm diameter) and 0.3% large irregularly shaped agglomerates (1.2–7.25 μm equivalent diameter). Although the numerical fraction of the agglomerates was only 0.2%, they contributed 60% to the cloud’s scattering cross section. The extinction coefficient, scattering coefficient and the scattering phase function were measured for both parallel and perpendicular polarized radiation at linear extinction coefficients ranging from 0.6 to 4.1 m−1. The cloud exhibited strong forward scattering, with 62% of all scattered energy in a forward lobe of 15° at 532 nm and 48% at 1064 nm. The scattering albedo was measured to 35% at 532 nm and 47% at 1064 nm. The dimensionless extinction coefficient was measured to 8.25 at 532 nm. The experimental data was compared to standard Mie theory by integrating the weighed contribution based on particle size, including agglomerates, according to the detailed measured population distribution. Neglecting the contribution of the agglomerates to the cloud’s optical properties was shown to introduce discrepancies between Mie theory and measured results. The results indicate that the-Mie theory can be used for estimating the optical properties of a partially agglomerated carbon black particle cloud for simulation of a solar particle receiver.

1.
Abdelrahman
,
P.
,
Fumeaux
,
Initial
, and
Suter
,
P.
,
1979
, “
Study of Solid-Gas Suspension used for Direct Absorption of Concentrated Solar Radiation
,”
Sol. Energy
,
22
, pp.
45
48
.
2.
Hunt, A. J., 1979, “A New Solar Receiver Utilizing a Small Particle Heat Exchanger,” 4 Int. Soc. Energy Conversion Engrg. Conf., 1, pp. 159–163.
3.
Hunt, A. J., and Brown, C. T., 1983, “Solar Test Results of an Advanced Direct Absorption High Temperature Gas Receiver (SPHER),” 8 Solar World Congress, Szokolay, S. V., Ed., Pergamon, 2, pp. 959–963.
4.
Bertocchi, R., Karni, J., and Kribus, A., In Press, “
Experimental Evaluation of a Non-Isothermal High Temperature Solar Particle Receiver,” Energy—The International Journal.
5.
Steinfeld, A., 1998, “Research and Development of the Process Technology for Converting Concentrated Solar Energy into Chemical Fuels,” PSI Report PSI-EF-REN(92)033.
6.
Haueter
,
P.
,
Moeller
,
S.
,
Palumbo
,
R.
, and
Steinfeld
,
A.
,
1999
, “
The Production of Zinc by Thermal Dissociation of Zinc Oxide-Solar Chemical Reactor Design
,”
Sol. Energy
,
67
, pp.
161
167
.
7.
Faeth
,
G. M.
, and
Ko¨ylu¨
,
U¨. O¨.
,
1995
, “
Soot Morphology and Optical Properties in Nopremixed Turbulent Flame Environments
,”
Combust. Sci. Technol.
,
108
, pp.
207
229
.
8.
Erlick
,
C.
,
Russel
,
L. M.
, and
Ramaswamy
,
V.
,
2000
, “
A Microphysics-based Investigation of the Radiative Effects of Aerosol-cloud Interactions for Two MAST Experiment Case Studies
,” J. Geophys. Res.
9.
Kaneyasu
,
N.
, and
Murayama
,
S.
,
2000
, “
High Concentrations of Black Carbon Over Middle Latitudes in the North Pacific Ocean
,”
J. Geophys. Res.
,
105
, pp.
19881
19890
.
10.
Bertocchi
,
R.
,
2002
, “
Carbon Particle Cloud Generation for a Solar Particle Receiver
,”
J. Sol. Energy Eng.
,
124
, pp.
230
236
.
11.
van de Hulst, H. C., 1957, Light Scattering by Small Particles, Wiley, New York.
12.
Kocifaj
,
M.
, and
Lukac
,
J.
,
1998
, “
Using the Multiple Scattering Theory for Calculation of the Radiation Fluxes from Experimental Aerosol Data
,”
J. Quant. Spectrosc. Radiat. Transf.
,
60
, pp.
933
942
.
13.
Erickson
,
W. D.
,
Williams
,
G. C.
, and
Hottel
,
H. C.
,
1964
, “
Light Scattering Measurements on Soot in a Benzene-Air Flame
,”
Combust. Flame
,
8
, pp.
127
132
.
14.
Dalzell
,
W. H.
,
Williams
,
G. C.
, and
Hottel
,
H. C.
,
1970
, “
A Light Scattering Method for Soot Concentration Measurements
,”
Combust. Flame
,
14
, pp.
161
170
.
15.
Bohren, C. F., and Huffman, D. K., 1983, Absorption and Scattering of Light by Small Particles, Wiley, New York.
16.
Dalzell
,
W. H.
, and
Sarofim
,
A. F.
,
1969
, “
Optical Constant of Soot and their Application to Heat Flux Calculations
,”
J. Heat Transfer
,
91
, pp.
100
104
.
17.
Dobbins
,
R. A.
,
Mulholland
,
G. W.
, and
Bryner
,
N. P.
,
1994
, “
Comparison of a Fractal Smoke Optics Model with Light Extinction Measurements
,”
Atmos. Environ.
,
28
, pp.
889
897
.
18.
Ko¨ylu¨
,
U¨. O¨.
, and
Faeth
,
G. M.
,
1994
, “
Optical Properties of Overfires Soot in Buoyant Turbulent Diffusion Flames at Long Residence Times
,”
J. Heat Transfer
,
116
, pp.
152
159
.
19.
Wu
,
J. S.
,
Krishnan
,
S. S.
, and
Faeth
,
G. M.
,
1997
, “
Refractive Indices at Visible Wavelengths of Soot Emitted from Buoyant Turbulent Flames
,”
J. Heat Transfer
,
119
, pp.
230
237
.
20.
Taylor, J. R., 1982, An Introduction to Error Analysis, University Science Books.
21.
Zhu
,
J.
,
Choi
,
M. Y.
,
Mulholland
,
G. W.
, and
Gritzo
,
L. A.
,
2000
, “
Measurements of Soot Optical Properties in the Near Infrared Spectrum
,”
Int. J. Heat Mass Transfer
,
43
, pp.
3299
3303
.
22.
Krishnan, S. S., Lin, K. C., and Faeth, G. M., 2000, “Extinction and Scattering of Soot Emitted from Turbulent Diffusion Flames for Wavelengths of 250-5200 nm,” 34th National Heat Transfer Conference, S. C. Yao, Ed., Pittsburgh, ASME.
You do not currently have access to this content.