Laserfiche WebLink
<br />concentrated on observing winter storm behavior and making measurements of <br />supercooled liquid water. A team of scientists and technicians have established <br />a year-round facility in the project area that consists of a project office and <br />a ground based observi ng faci 1 i ty known as the Grand Mesa Observatory. The <br />observatory has the capabil ity to measure state parameters at the surface and a <br />height of about 20 meters. Other equipment at the observatory includes a 5-cm <br />radar, a dual wavelength microwave radiometer to measure liquid water, precipi- <br />tation gages, and Particle Measuring System's 2-dimensional cloud particle <br />probe. Measurements above the surface of the Mesa are made using an instru- <br />mented cloud physics aircraft. Initial investigations (Holroyd and Super, 1984) <br />have confirmed the presence of supercooled liquid water in sufficient quantities <br />to i ndi cate that cloud seedi ng coul d potentially be successful. Terrai n, rather <br />than ice particle presence, appears to be the dominant influence in determining <br />the distribution of liquid water over the slopes and top of Grand Mesa (see <br />Figure 5). The water appears to be concentrated in the lowest levels and is <br />present in sufficient significant amounts only for limited periods of time (mean <br />= 3 h, upper standard deviation = 6.5 h). The presence of the highest liquid <br />water in the lowest levels may make ground seeding most practical. <br /> <br />6. Related research <br /> <br />a. Microwave radiometer <br /> <br />In the description of the CRADP and SCPP programs, an instrument was described <br />which appears to have a high potential for detecting clouds which are seedable. <br />The instrument is called a dual wavelength radiometer and remotely senses the <br />amount of water vapor and supercooled liquid water that is present in nearby <br />clouds. It does this by passively measuring incoming microwave radiation at <br />wavelengths appropriate to water vapor (20.6 GHz) and to liquid water (31.6 <br />GHz). The brightness of the radiation is a measure of the integrated water in <br />that phase along the line of sight. The computer-controlled antenna which <br />receives the signal can be operated in a stationary or a scanning mode, and the <br />data are recorded on disk and/or on tape. <br /> <br />A cross-section of the physical layout of the system is shown in Figure 6. The · <br />electronics for both the 20.6 and 31.6 GHz radiometers are located in a single <br />package. The minicomputer is also located inside the trailer. Equal beamwidths <br />(2.50) are produced at both frequencies. Mobility of the instrument is achieved <br />by using an enclosed trailer as both a small laboratory and an antenna platform. <br />A more detailed description of the radiometer unit is found in Hogg et al. <br />(1983). <br /> <br />Several analyses have been performed to determine the veracity of the radiometer <br />data. Westwater (1978) found the accuracy of vapor values to be better than 15 <br />percent for a wide range of cloudy conditions. Guiraud et al.(1979) showed that <br />the accuracy in measurement of precipitable water vapor is about the same or <br />somewhat better than that of operational radiosondes. He also found that a con- <br />siderable amount of vapor often passes overhead unobserved by sondes. The <br />liquid measurements have been compared against cloud physics aircraft data <br />(Holroyd, 1984) and with a more accurate combination receiver-radiometer that <br />utilizes absorption of a signal from the COMSTAR satellite as well as the <br />absorption of microwave energy by liquid water (Snider et al., 1980),. <br /> <br />8 <br />