GNSS Absolute Antenna Calibration at the National Geodetic Survey Gerald L Mader 2, Andria L Bilich 1 1 National Geodetic Survey, NOAA/NOS, Boulder CO;

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Presentation transcript:

GNSS Absolute Antenna Calibration at the National Geodetic Survey Gerald L Mader 2, Andria L Bilich 1 1 National Geodetic Survey, NOAA/NOS, Boulder CO; corresponding author: 2 National Geodetic Survey, NOAA/NOS, Silver Spring, MD GOAL: Serve high precision needs of surveying and geodesy communities Calibration of any geodetic-grade receiving antennas (from chokerings to rovers) Multi-frequency, multi-GNSS calibrations 2-D (elevation, azimuth) phase center patterns Free calibration service with quick turn-around Calibration values publicly distributed via Internet Compatible with IGS ANTEX values from other calibration facilities NGS Absolute Calibration Motivation and Goals o 5 meter baseline (N-S orientation)  precise baseline length and orientation from survey  baseline orientation used to fix robot reference frame N S E W The NGS calibration facility is located in Corbin, VA. Calibration Baseline o Flat field & concrete pad = well-behaved multipath environment o Variable PCO height  highest ARP ~ 50 cm above concrete pad  PCO height controlled by robot tilt  other robot heights tested, but robot height had no effect on calibration results Calibration Setup Robot  2-axis pan and tilt unit produced by Directed Perception  rotation arm = cm mounting bracket cm Sokkia extension  coincident origins for pan and tilt systems  arm length and pan/tilt axis origin precisely measured with Total Station observations over range of robot pan/tilt angles Data Collection North onlyFour Directions Four-orientation Antenna Mount: Mounting the antenna in one orientation (North) on robot cannot sample all directions*. Data are collected with antenna mounted in four different positions (N,S,E,W). * Limitation of 2-axis robot and motor housing Time 1 Time 2 Between two closely spaced times: Robot moves test antenna through large angular change Reference antenna remains fixed Satellite moves negligible amount When the two times are differenced: PCO/PCV of test antenna at two angles is combined PCO/PCV at reference antenna is removed Multipath at reference also removed References & Acknowledgements Bilich A and GL Mader, GNSS Antenna Calibration at the National Geodetic Survey, Proceedings of ION GNSS 2010, Portland, OR, September 2010, pp The authors thank many people at NGS (S.Breidenbach, H.Chen, K.Fancher, C.Geoghegan, H.Han, D.Lokken, F.Marion, J.Neti, G.Sella, B.Tran, J.Saleh, and M.Schenewerk) and the IGS Antenna Working Group (W.Aerts, Q.Baire, F.Blume, B.Goerres, R.Schmidt, M.Schmitz, P.Zeimetz), for contributions to this project. The authors would also like to thank the National Geospatial Intelligence Agency (NGA) for their infinite patience. Please see our website at for more information. Data Reduction Solution Methodology Solution Residuals show a clear correlation with mean satellite elevation angle in antenna frame. Data weights are inverse of  2 PCA identifies which harmonics capture the design matrix. Here, the first 3 principal components = 94% of variance, eliminating 41 harmonic components. Eliminating harmonics prevents over-fitting. Solution depends strongly on selection of noisy data points. Iteration with subsets of data points enables pinpointing best average estimate – here, horizontal PCO components after 200 iterations with ¼ of total data. iterate Next Steps  Determine optimal tracking loop settings and antenna dynamics to maintain time- difference single-difference assumptions  Work with the IGS Antenna Working Group to finalize approval of NGS methods  Set permanent piers for calibration baseline  Add capabilities to software:  Integrated antenna + receiver units  GLONASS  Port production code to Java  Reliable antenna testing facility and capabilities are place at NGS  Detailed methodology paper in progress, for distribution and discussion in IGS AWG  Aspects of methodology (dwell time between motions, data weights, PTU speed) will be tweaked following conclusion of receiver and tracking loop tests. Trimble GNSS chokering (TRM ) New Developments L2P carrier phase is highly dependent upon Antenna dynamics (speed and acceleration) Tracking loop bandwidth Dwell time after antenna stops moving A calibration system must be tuned to optimize tracking loops, antenna motion, and time spacing between motions. Phase difference (L2-L1, in cm) after removing Motion start/stop times are indicated by vertical gridlines. Purple box denotes section in zoomed plot at left. Receiver and Tracking Loop Testing Multi-Method Antenna Comparison In 2012, several models of geodetic antennas were individually calibrated at NGS (field), Geo++ (rooftop) and Bonn (anechoic chamber). Equipment used at each facility varies (see table below). GPS L1 results were within 1-2 mm tolerances of “good agreement”. For antennas such as the TRM , L2 results disagreed by several mm. [This level of disagreement can create mm-cm positioning differences, see talk G13C-04 this afternoon] Conclusions Poor L2 results are attributable to L2W/L2P tracking loop behavior, specifically L1 aiding of L2P loops, which creates apparent (erroneous) motion in L2P TDSD. Note how the L1 and L2C TDSD (left) do not drift. Septentrio AsteRx2eH Javad Delta L1 PLL Bandwidth 0.1 Hz25.0 Hz L2 PLL Bandwidth 0.1 Hz3.0 Hz Used byNGSGeo++ Zoomed section to show detail of phase lag by Septentrio receiver relative to Javad, caused by low tracking lower bandwidth. The tighter bandwidth also results in phase smoothing and phase lag relative to start/stop of motion.