Ray trace model of the Santa Barbara, California, Land-Sea Seismic Refraction Experiment

1983 ◽  
Vol 10 (10) ◽  
pp. 933-936 ◽  
Author(s):  
B. Keller ◽  
W. A. Prothero ◽  
A. M. Trehu ◽  
D. J. Stierman
1983 ◽  
Vol 6 (1) ◽  
pp. 15-37 ◽  
Author(s):  
Greg J. Crandall ◽  
Bruce P. Luyendyk ◽  
Michael S. Reichle ◽  
William A. Prothero

1997 ◽  
Vol 470 ◽  
Author(s):  
M. Fordham ◽  
M. Pan ◽  
J. Hu ◽  
F. Y. Sorrell

ABSTRACTSpectral and spectral band irradiance sensors are developed to measure the spatial heat flux distribution from a rapid thermal processor (RTP) lamp bank. They are used in conjunction with a Sensarray thermocouple wafer to evaluate the thermal uniformity of one axially symmetric lamp bank from a 3 zone RTP system. Measured performance of the lamp bank differs sharply from predictions obtained using a numerical ray trace model. Discrepancies between experimental measurements and model results are resolved by blackening a beveled (focusing) surface introduced to shield process lamp bases from overheating. Further modeling confirms that the bevel causes undesirable focusing of lamp radiation on the planar wafer surface. The shape of the focused component of the irradiance profile is highly dependent on the lamp radiance spatial distribution assumed in the model.


Author(s):  
Clifford K. Ho ◽  
Timothy Wendelin ◽  
Luke Horstman

This paper presents a study of alternative heliostat standby aiming strategies and their impact on avian flux hazards and operational performance of a concentrating solar power plant. A mathematical model was developed that predicts the bird-feather temperature as a function of solar irradiance, thermal emittance, convection, and thermal properties of the feather. The irradiance distribution in the airspace above the Ivanpah Unit 2 heliostat field was simulated using a ray-trace model for two different times of the day, four days of the year, and nine different standby aiming strategies. The impact of the alternative aiming strategies on operational performance was assessed by comparing the heliostat slew times from standby position to the receiver for the different aiming strategies. Increased slew times increased a proxy start-up time that reduced the simulated annual energy production. Results showed that spreading the radial aim points around the receiver to a distance of ∼150 m or greater reduced the hazardous exposure times that the feather temperature exceeded the hazard metric of 160 °C. The hazardous exposure times were reduced by ∼23% and 90% at a radial spread of aim points extending to 150 m and 250 m, respectively, but the simulated annual energy production decreased as a result of increased slew times. Single point-focus aiming strategies were also evaluated, but these strategies increased the exposure hazard relative to other aiming strategies.


2009 ◽  
Vol 27 (1) ◽  
pp. 231-259 ◽  
Author(s):  
S. L. Vadas ◽  
M. J. Taylor ◽  
P.-D. Pautet ◽  
P. A. Stamus ◽  
D. C. Fritts ◽  
...  

Abstract. Six medium-scale gravity waves (GWs) with horizontal wavelengths of λH=60–160 km were detected on four nights by Taylor et al. (2009) in the OH airglow layer near Brasilia, at 15° S, 47° W, during the Spread F Experiment (SpreadFEx) in Brazil in 2005. We reverse and forward ray trace these GWs to the tropopause and into the thermosphere using a ray trace model which includes thermospheric dissipation. We identify the convective plumes, convective clusters, and convective regions which may have generated these GWs. We find that deep convection is the highly likely source of four of these GWs. We pinpoint the specific deep convective plumes which likely excited two of these GWs on the nights of 30 September and 1 October. On these nights, the source location/time uncertainties were small and deep convection was sporadic near the modeled source locations. We locate the regions containing deep convective plumes and clusters which likely excited the other two GWs. The last 2 GWs were probably also excited from deep convection; however, they must have been ducted ~500–700 km if so. Two of the GWs were likely downwards-propagating initially (after which they reflected upwards from the Earth's surface), while one of the GWs was likely upwards-propagating initially from the convective plume/cluster. We also estimate the amplitudes and vertical scales of these waves at the tropopause, and compare their scales with those from a simple, linear convection model. Finally, we calculate each GW's dissipation altitude, location, and amplitude. We find that the dissipation altitude depends sensitively on the winds at and above the OH layer. We also find that several of these GWs may have penetrated to high enough altitudes to potentially seed equatorial spread F (ESF) if located somewhat farther from the magnetic equator.


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