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Weather Modification
Title
Corrections of Surface Particle Probe Measurements for the Effects of Aspiration
Date
8/4/1988
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<br />Reprinted from JOURNAL OF ATMOSPHERIC AND OcEANIC TECHNOLOGY, Vol. 5, No.4, August 1988 <br />American Meteorological Society <br /> <br />Corrections of Surface Particle Probe Measurements for the Effects of Aspiration <br /> <br />TERRY DESHLER <br />Bureau of Reclamation. Auburn. California <br />(Manuscript received I June 1987, in final form II January 1988) <br /> <br />ABSTRACT <br /> <br />Particle probes from Particle Measuring Systems are routinely designed to be mounted on an aircraft or other <br />mo.vable. plat~orm. There are attempts, however, to apply this technology to stationary surface measurements <br />by indUCing 81rflow through th: sample area. U~ o~ th~ measurements quantitatively requires an understanding <br />of how the meas~rements are distort~ by the art1fiClal81rflOW. In an application to surface snowfall measurements <br />a 2D-C probe With a horn-shaped aspIrator has been used for six winter seasons in the Sierra Nevada of California' <br />~o co?,e~ m~asurements from this instrument, three other methods to measure ice particle concentrations and <br />sIze dlstnbutlo?s at the ground are presented. and compared to simultaneous measurements by the aspirated <br />2D-C. The ~?Irated 2D-C was found to routinely overestimate ice particle concentration by factors of 2.4 to <br />3.~. In addltton, the amount of overestimation was found to be a function of particle size and surface <br />Wind speed. <br /> <br />1. Introduction <br /> <br />In-cloud measurements of hydrometeors have ben- <br />~fite~, in. the past decade, from an array of particle <br />Im~gIng mstruments manufactured by Particle Mea- <br />sunng Systems (PMS) (Knollenberg 1981). Unfortu- <br />nately, similar upgrades in surface measurements have <br />not followed, although there are attempts to use particle <br />prob.es (~axena et al. 1986; Humphries 1985). A direct <br />apphcatIOn of PMS-2D instruments to surface mea- <br />sure~ents is limited by the need to know the speed of <br />partIcles as they pass through the sampling area so <br />that they can be imaged properly. In a PMS-2D pr~be, <br />a focused laser beam illuminates a linear array of pho- <br />todiodes which are scanned, or clocked, at a set fre- <br />quency to determine their state. The size and number <br />of photodiodes determine the size resolution and range <br />of the instrument. As a particle falls through the laser <br />beam it shadows, the photodiodes. The Y dimension <br />of the particle is determined by the number of diodes <br />s~adowed while the X dimension is determined by the <br />tIme, or number of scans, a diode remains shadowed. <br />To correctly size a particle in the X dimension the <br />scan rate of the photodiodes must be set such th~t for <br />e~ch scan, the ~article moves a distance equal to the <br />SIZe of a photodiode. If a particle moves slower or faster <br />t~an th~s it will be stretched or compressed in the X <br />dImenSIOn. For an instrument in motion, airspeed <br />controls the residence time of a particle in the imaging <br />beam and can thus be used to control the clock rate <br />of the photodiodes. However, with a stationary instru- <br /> <br />Co"esponding aut~or ~ddress: Dr. ~erry Deshler, Dept. of Physics <br />and Astronomy, Umverslty of Wyoming, Laramie, WY 82071. <br /> <br />men~, particle .speed is controlled by wind speed and <br />termmal velOCIty of the particle. The resultant images <br />ll!e stretched along the direction of particle motion, <br />smce the clock rate of the photodiodes is constant and <br />usually faster than the slow and variable fall speed of <br />the particles. To remedy this problem, probes have been <br />fitted with parabolic horns and suction fans to draw <br />p~cles through the sampling area at a constant speed, <br />while the clock rate of the photodiodes is held constant. <br />A 2D-C optical array probe, with parabolic horn- <br />shaped aspirator held vertically, has been used to mea- <br />sure ~nowfall at the ground for six winter seasons during <br />the S.lerra Cooperativ~ Pilot Project (Humphries 1985). <br />The mstrument prOVIdes a continuous record of snow- <br />f~l and requires ~inimum attention while in opera- <br />tion. After collectIOn, the data are in a form that can <br />be easily managed with computer processing. These <br />advantages are in stark contrast to other techniques of <br />recording ice particle concentrations (IPC) and size <br />distributions during snowfalL at the ground. Other <br />techniques for recording similar data require photo- <br />graphic or replication methods to preserve sedimen- <br />tation slides (Reinking 1975; Hobbs and Radke 1975). <br />After collection, particles preserved in the samples must <br />be counted and sized. Both the data collection and <br />data reduction methods are highly labor intensive. Un- <br />fortunately, the errors introduced by aspiration into <br />the computer recorded measurements of IPC and size <br />distribu~ions by the 2D-C are not easily obtained, yet <br />are reqUIred before the data can be used quantitatively. <br />Preliminary evidence collected by the first users of <br />an aspirated 2D-C suggests that it overestimates IPC <br />(Holroyd 1986). This evidence stimulated several at- <br />tempts at quantifying the overestimation. Norment <br /> <br />::JJIi:if';;- <br />
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