Lower-Cost Gps Met Station Design for Use in Dense Network Slant Path Gps-Met Estimates of Tropospheric Wet Delay and Precipitable Water Vapor

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Lower-Cost Gps Met Station Design for Use in Dense Network Slant Path Gps-Met Estimates of Tropospheric Wet Delay and Precipitable Water Vapor 11.5 LOWER-COST GPS MET STATION DESIGN FOR USE IN DENSE NETWORK SLANT PATH GPS-MET ESTIMATES OF TROPOSPHERIC WET DELAY AND PRECIPITABLE WATER VAPOR A.Nagarajan1*, M.C Jacques2, A. Lagace1, D. L. Pepyne2, M. Zink2, and D. J. McLaughlin2 1 Dept. of Mechanical and Industrial Engineering, University of Massachusetts 2 Dept. of Electrical and Computer Engineering, University of Massachusetts 1. Introduction and antenna alone). To reduce this cost, this paper describes a GPS- met station design based GPS meteorology (GPS-met) is a on a low-cost (~$3K), but high performance (dual- technique that uses GPS signals to estimate the frequency), GPS receiver/antenna. The amount of precipitable water in the atmosphere challenge was that, unlike the more expensive (Bevis et al., 1992). In a typical application, this equipment, which comes configured for the GPS- involves combining the slant path signals from the met application right out of the box, we had to 8-12 GPS satellites in view of a ground-based develop the software and hardware infrastructure GPS receiver into an estimate of the zenith to obtain GPS-met capability from the low-cost precipitable water directly over the GPS station. GPS equipment. In combining the multiple slant paths each from a different azimuth and elevation angle into a single After a background review of the GPS- zenith value one loses spatial information about met technique, we describe the software and how the precipitable water is distributed around hardware design of our low-cost GPS-met station the station. Recently there has been growing and give results validating its performance. We interest in combining the slant paths from a then describe our plans to develop a 3D network of closely spaced GPS stations using atmospheric precipitable water network for the tomographic techniques to obtain 3D maps of Dallas-Fort-Worth (DFW) metroplex and how we precipitable water in the atmosphere over a propose to use the network in conjunction with a region. This can be done using existing GPS network of closely spaced polarimetric X-band stations, since many of these do provide (in weather radars that is being deployed in the DFW addition to the zenith estimate), the slant path region to understand relationships between information from which the zenith estimate was precipitable water observations and subsequent obtained. On the other hand, it has been weather radar observations. One ultimate goal is suggested that the ideal spacing for good 3D to improve an ability to forecast severe weather, maps requires a spacing between ground-based such as the urban flooding events that regularly GPS stations of no more than 20km (Braun et al. occur in regions like DFW. 1999, Bender et al. 2010). Deploying such networks, or adding additional GPS-met stations 2.GPS-Met Systems to “densify” existing networks to achieve such GPS-met is a technique for determining spacing can be prohibitively expensive using the amount of precipitable water in the existing GPS-met equipment (which can cost atmosphere from the signal propagation delays upwards of $20K per station for the GPS receiver occurring between a set of signals transmitted by a constellation of GPS satellites and the corresponding set of signals received on the ground by a GPS receiver antenna. For geodists, *Corresponding author address: Aditya these propagation delays are a source of error Nagarajan, Research Assistant, Center for that need to be modeled and compensated for in Collaborative Adaptive Sensing of the order to obtain high precision position estimates. Atmosphere (CASA), College of Engineering, For meteorologists, on the other hand, it was University of Massachusetts, Amherst, MA found that these propagation delays could be 01003, [email protected] used to determine the water vapor content in the atmosphere (Bevis et al., 1992). As a means of STDθ (and hence the resulting ZTD) are estimated measuring water vapor, GPS-met provides an from GPS data using a linear spline method with alternative to radiosondes, which though they 30-min knot intervals, and treating the knots as a provide information about water vapor with Gauss-Markov processes (Duan et al., 1996, altitude are only launched once or twice a day Tralli et al., 1990). from widely spaced locations, and WVR (Water Vapor Radiometry) which provide real-time water The ZTD is then decomposed onto its 2 vapor information at a location is limited in that it fundamental quantities Zenith Hydrostatic Delay does not work in rain. (ZHD) or the delay due to the dry air and Zenith Wet delay (ZWD), or delay due to precipitable GPS signals propagate in two distinctive water vapor, media, the ionosphere and the troposphere. The ionosphere is a dispersive media. As such the 푍푇퐷 = 푍퐻퐷 + 푍푊퐷 (2) delay in this media are a function of frequency that can be determined from phase differences in The ZHD can be estimated using surface the L1, L2 frequencies of a dual-frequency GPS meteorological readings of barometric pressure receiver (Spilker, 1980). The delay in the (Saastamoinen, 1972; Davis et al., 1985), troposphere, termed the neutral delay, consists of two quantities, the hydrostatic delay and the wet (2.2779 ± 0.0024) ∗ Ps (3) 푍퐻퐷 = delay (Saastamoinen, 1972). Typically the 푓 (휆, 퐻) neutral delay is resolved onto a zenith component (the vertical component above the GPS-Met station), referred to as the Zenith Tropospheric where Ps is the surface pressure in millibars and, delay (ZTD). As shown in Figure 1, this is done 푓(휆, 퐻) = (1 − 0.00266 cos(2휆) − 0.00028퐻) (4) by combining the so-called Slant Total Delays (STD) (the Si in the figure) between the GPS receiver and each of the satellites in its view such λ is the latitude of the GPS antenna and H is that, elliptical height of the antenna in km. Subtracting the ZHD from the ZTD, one obtains the quantity of 푆푇퐷 = 푍푇퐷 ∙ 푚(휃) 휃 (1) meteorological interest, the ZWD. This quantity can be mapped onto the amount of precipitable here STDθ is the slant total delay seen at an water given by (Bevis et al., 1994), elevation angle θ and m(θ) is a mapping function 푃푊 = 훱 ∗ 푍푊퐷 (5) which is approximately equal to 1/sin(θ). The where PW or precipitable water is the column of water vapor above the GPS antenna measured in millimeters, and Π is a constant which depends on temperature and partial pressure of water vapor (Davis et al., 1985). This approach of measuring precipitable water vapor has shown an accuracy better than rms 2mm (Duan et al. 1996). GPS-met has matured in many significant ways since it was first introduced. With the availability of near real time predicted orbits (Springer et al., 2001) and better modeling of antenna phase center variations (PCV) to reduce errors in station position and height estimates, Figure 1. Representation of the signals from more timely and accurate measurements of various satellites Si (i=1...32) onto the Zenith precipitable water are produced. Currently there component ZTD. are 600+ GPS-Met stations operating in the United States by agencies such as Scripps 3.Low cost GPS-Met Station Design Institute of Oceanography, NOAA and JPL, with near real-time estimates of precipitable water The four main components of a GPS-met published online every hour from a large number station are the GPS receiver, antenna, barometric of stations (www.gpsmet.noaa.gov). pressure sensor, and ambient temperature sensor. In selecting and deploying equipment for 2.1Slant path tomography the GPS-met application, the IGS (International GNSS services) provides a set of guidelines that By not including azimuth angle, mapping a continuously operating GPS-station should function m(θ) in Equation (1) makes the meet (Moore, 2014). In particular, the GPS assumption that the atmosphere is azimuthally receiver should be capable of receiving at least 2 isotropic (Bevis et al., 1992). In doing so, the frequencies L1 (1.57542 GHz) and L2 (1.2275 mapping function ignores the spatial distribution GHz) and should be set to track satellites down of water vapor around the GPS-met station. To to 5o elevation angle. In addition, the GPS overcome this limitation of the zenith GPS-met antenna should be mounted such that errors due method, the so called slant path GPS methods to blockage, multi path and antenna movement have been proposed as a potential way to are minimized. This means that the antenna estimate both the azimuthal and vertical needs to be mounted onto a rigid bracket and distribution of water vapor over a region. deployed in a location and at a height such that The slant path methods are based on the the antenna field-of-view is clear of foliage, idea that, since a typical GPS site sees 8 to 12 buildings, metal poles, towers, and other objects satellites, a dense network of GPS-Met stations that might block the GPS signals or produce would thus form a web of intersecting slant paths. multi-path reflections. Using tomographic or other approaches In general, the cost of a GPS-met station combined with precise ultra-rapid orbit prediction, is dominated by the cost of the GPS it could therefore be possible to obtain a 4D receiver/antenna equipment. A low-cost GPS- picture of the temporal and spatial evolution of met station, therefore, starts with low-cost GPS atmospheric water vapor (Flores et al., 2000, equipment. The lowest cost GPS equipment we Troller et al., 2006, Bender et al., 2010, could find that could potentially meet the IGS Shangguan et al., 2012). requirements were the Hemisphere P320/P306 In deploying a network of GPS-Met receiver and the A42/A52 antenna (Hemisphere stations for slant path tomography, slant path GNSS), the cost of which was just over $2800 density over a given domain is a key factor.
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