Dataset Paper  Open Access
R. Biondi, T. Neubert, "Bending Angle and Temperature Climatologies from Global Positioning System Radio Occultations", Dataset Papers in Science, vol. 2013, Article ID 795749, 5 pages, 2013. https://doi.org/10.7167/2013/795749
Bending Angle and Temperature Climatologies from Global Positioning System Radio Occultations
Abstract
The Global Positioning System (GPS) Radio Occultation (OR) technique provides estimates of atmospheric density, temperature, and water vapour content with high vertical resolution, global coverage, and high accuracy. We have used data acquired using this technique in the period 1995–2009 to create a reference climatology of radio occultation bending angle and atmospheric temperature which are used for meteorological studies. The bending angle is interesting because it is a direct measurement and independent of models. It is given with onedegree spatial resolution and 50meter vertical sampling. In addition, we give the temperature climatology with onedegree spatial resolution and 100meter vertical sampling. This dataset can be used for several applications including weather forecast, physics of atmosphere, and climate changes. Since the GPS signal is not affected by clouds and the acquisitions are evenly distributed in the globe, the dataset is well suited for studying extreme events (such as convective systems and tropical cyclones) and remote areas.
1. Introduction
The Global Positioning System (GPS) Radio Occultation (RO) technique [1] enables measurements of the global atmospheric density structure under any meteorological condition [2]. As illustrated in Figure 1, the RO technique involves a GPS satellite transmitting the signal and a Low Earth Orbit (LEO) satellite carrying a receiver. The signal transmitted by the GPS satellite is refracted in the atmosphere, and the associated propagation delay, refractive index, and bending angle are measured on the LEO satellite. From the measurements, it is possible to estimate profiles of atmospheric parameters such as temperature, water vapour, and pressure [3]. These parameters are secondary products, derived from the refractivity together with the European Centre for MediumRange Weather Forecasts (ECMWF) model, and are given with high vertical resolution. The highest accuracy on the refractivity is achieved between 5 and 25 km altitude with average errors estimated in the range 0.3%–0.5% [4]. The RO technique has improved the weather forecast in regions of the globe that is poorly covered by standard measurements, such as the southern hemisphere which is dominated by oceans [5]. For instance, forecasting the track of tropical cyclones (energized over the oceans) has greatly improved [6]. Also the upper atmosphere is better forecasted as in the case of the ECMWF Upper Troposphere Lower Stratosphere (UTLS) model [7].
However, the use of a model to derive atmospheric parameters involves implicit assumptions on the state of the atmosphere. Therefore, during special atmospheric conditions, the assumptions break down and the atmospheric parameters are poorly estimated. Such conditions arise during extreme storms such as tropical cyclones [8]. Consequently, the direct measurement of the primary parameters of the GPS signal can be more sensitive to atmospheric variations and better reflect the physics of the region, if studied directly.
For example, using the bending angle directly, accurate and detailed information can be estimated for the atmosphere above severe storms [9].
Several GPS RO missions are working at present. They include the Constellation Observing System for Meteorology, Ionosphere, and Climate (COSMIC) sixsatellite constellation [10], the Gravity Recovery And Climate Experiment (GRACE) twin satellites [11], the Meteorological Operational satellite A (MetOpA) [12], the Radio Occultation Sounder for the Atmosphere (ROSA) [13] on board of OceanSat2 [13], MeghaTropique [14], and the Satellite de Aplicaciones CientificasD (SACD) [15]. Several new missions are planned for the near future (e.g., COSMIC2, ACES on the International Space Station, and MetOpB/C).
The number of transmitters will also increase in the near future with the European GALILEO system, with the availability of the Russian GLObal NAvigation Satellite System (GLONASS), and with the new projects from China (COMPASS), India (Indian Regional Navigational Satellite System, IRNSS), and Japan (QuasiZenith Satellite System, QZSS).
The new missions will increase the spatial measurement resolution of the Earth, which is especially needed in the tropical region [16], and the temporal resolution.
2. Methodology
We downloaded the GPS ROs from the COSMIC Data Analysis and Archive Center (CDAAC) website [17]. We collected all the level 2 product profiles in Network Common Data Form (NetCDF) format covering the period 1995–2009 coming from the following missions: the Global Positioning System/Meteorology (GPS/MET, 1995–1997) satellite [18], the CHAllenging Minisatellite Payload (CHAMP, 2001–2008) [18], the Satellite de Aplicaciones CientificasC (SACC, 20002001) [19], the COSMIC (2006–2009) sixsatellite constellation, and the GRACE (2007–2009) satellite.
In total more than 2 700 000 ROs were used (Table 1), mostly coming from COSMIC.

All the products are provided from CDAAC in a common standard format.(i)Atmospheric Profile (atmPrf). It is a product containing the bending angle, refractivity, impact parameter, and the socalled dry pressure and dry temperature (derived assuming no water vapor). All the parameters are reported versus the geometric height above the mean sea level from the surface to 60 km of altitude and the coordinates of the perigee point with vertical resolution from 60 meters in the low troposphere to 1.5 km in the stratosphere [4].(ii)Wet Profile (wetPrf). It is an interpolated product sampled every 100 meters and obtained using a nonstandard 1DVar (onedimensional variational) technique [16] together with ECMWF lowresolution analysis data. This profile contains latitude and longitude of the perigee point, pressure, temperature, water vapor pressure, refractivity, and mean sea level altitude of the perigee point from the surface to 40 km of altitude.
Using all the GPS ROs collected from the CDAAC website from 1995 to 2009, we have created a grid with onedegree resolution containing the average bending angle profiles (from the atmPrf product) and the average temperature profiles (from the wetPrf product). This grid becomes our reference and is defined in the text as “climatology” [20].
Figure 2 shows the map with the number of occultations used for any box. The density of measured vertical profiles of atmospheric parameters is higher at the midlatitudes, between ±27 and ±60 degrees, and it decreases between the tropics, which is a key region for atmospheric circulation [8].
The full process to compute the climatology fundamentally consists in 3 steps.(i)Interpolation. The vertical distribution of atmPrf acquisitions is not fixed, providing anytime a different number of measurements in the altitude range 0–60 km. To create a standard reference to be comparable with other products, we decided to interpolate the atmPrf data with a common vertical sampling of 50 meters. The wetPrf products are already provided by CDAAC with a sampling of 100 meters. (ii)Geolocation. The interpolated profiles were indexed with respect to the tangent point latitude and longitude at 16 km of altitude (average altitude of the tropical tropopause) with onedegree resolution. We have created this dataset specifically for studying the upper troposphere lower stratosphere; for this reason, the GPS RO profiles are categorized into the onedegree box corresponding to the RO coordinates at 16 km of altitude.(iii)Average. In each geolocated box, we averaged all the values at the same altitude obtaining one reference profile for every latitude/longitude degree: this becomes the climatological reference (climatology) for the corresponding coordinates.
3. Dataset Description
The dataset associated with this Dataset Paper consists of 3 items which are described as follows.
Dataset Item 1 (Binary Data). The bending angle climatology structure in matlab format (.mat) formed by cells corresponding to the onedegree latitude/longitude grid boxes in the following order: row 1 is latitude −90°; row 180 is latitude 90°; column 1 is longitude −180°; column 360 is longitude 180°. Whenever a value is missing, it is replaced by Not a Number (NaN). When the number of profiles for a certain grid box is and the NaN at each altitude is , the climatological value for the box and related altitude is computed averaging values. If , the climatological value is NaN. Each cell contains an array of 1200 single values representing the climatological bending angle profile from the surface to 60 km of altitude with a vertical resolution of 50 meters.
Dataset Item 2 (Binary Data). The bending angle climatology structure in matlab format (.mat) formed by cells corresponding to the onedegree latitude/longitude grid boxes in the following order: row 1 is latitude −90°; row 180 is latitude 90°; column 1 is longitude −180°; column 360 is longitude 180°. Whenever a value is missing, it is replaced by Not a Number (NaN). When the number of profiles for a certain grid box is and the NaN at each altitude is , the climatological value for the box and related altitude is computed averaging values. If , the climatological value is NaN. Each cell contains an array of 400 single values representing the climatological temperature profile (in Celsius) from the surface to 40 km of altitude with a vertical sampling of 100 meters.
Dataset Item 3 (Binary Data). The number of profiles used to get the final climatologies in matlab format (.mat) formed by cells corresponding to the onedegree latitude/longitude grid boxes in the following order: row 1 is latitude −90°; row 180 is latitude 90°; column 1 is longitude −180°; column 360 is longitude 180°. Whenever a value is missing, it is replaced by Not a Number (NaN). When the number of profiles for a certain grid box is and the NaN at each altitude is , the climatological value for the box and related altitude is computed averaging values. If , the climatological value is NaN. Each cell contains an integer representing the number of profiles used to compute the climatological temperature and bending angle for the corresponding onedegree box.
4. Concluding Remarks
We have already used this dataset for studying the atmospheric physics during convective systems [9] and tropical cyclones and for detecting the tropical cyclones cloud top [21]. The results were very satisfactory revealing the capabilities of GPS ROs detecting a detailed atmospheric structure in the upper troposphere. In Figure 3, we report a schematic thermal structure of convective systems (red line) obtained using 53 cases [9] in comparison with the average standard temperature profile (from wetPrf data) colocated with the systems (blue line). During convective systems, the temperatures decrease from the surface with a moist adiabatic lapse rate until a few kilometers from the cloud top. At this altitude, the lapse rate increases revealing a relative temperature minimum (cold point) near the top of the system. Above the cloud top, a strong inversion occurs, reestablishing a climatological temperature profile at higher altitudes.
The GPS RO climatology is useful for climatological [22] atmospheric physics [9] and meteorological [6] studies. The bending angle and temperature climatology can be used as reference for detecting anomalies from the standard atmosphere. The horizontal and vertical sampling of the temperature and bending angle is high enough to study mesoscale processes.
The future development of this dataset, including new missions acquisitions and the extension of the reference period, will provide a solid background for seasonal or monthly climatologies (not possible at the moment due to the small number of profiles at certain latitudes). Several new deliverables have already been planned for the next 2 years within the project CONvective SYstems DEtection and analysis using Radio occultations (CONSYDER) within the EU Program FP7PEOPLE2012IEF, including specific datasets for different type of clouds.
Dataset Availability
The dataset associated with this Dataset Paper is dedicated to the public domain using the CC0 waiver and is available at http://dx.doi.org/10.7167/2013/795749/dataset. In addition, the dataset is available in the DTU server at http://outer.space.dtu.dk/~ribi/.
Acknowledgments
The authors thank CDAAC for the availability of the GPS RO datasets and DTU for the availability of the infrastructure to create this dataset.
Dataset Files
 795749.item.1.mat
Dataset Item 1 (Binary Data). The bending angle climatology structure in matlab format (.mat) formed by cells corresponding to the onedegree latitude/longitude grid boxes in the following order: row 1 is latitude −90°; row 180 is latitude 90°; column 1 is longitude −180°; column 360 is longitude 180°. Whenever a value is missing, it is replaced by Not a Number (NaN). When the number of profiles for a certain grid box is and the NaN at each altitude is , the climatological value for the box and related altitude is computed averaging values. If , the climatological value is NaN. Each cell contains an array of 1200 single values representing the climatological bending angle profile from the surface to 60 km of altitude with a vertical resolution of 50 meters.
 795749.item.2.mat
Dataset Item 2 (Binary Data). The bending angle climatology structure in matlab format (.mat) formed by cells corresponding to the onedegree latitude/longitude grid boxes in the following order: row 1 is latitude −90°; row 180 is latitude 90°; column 1 is longitude −180°; column 360 is longitude 180°. Whenever a value is missing, it is replaced by Not a Number (NaN). When the number of profiles for a certain grid box is and the NaN at each altitude is , the climatological value for the box and related altitude is computed averaging values. If , the climatological value is NaN. Each cell contains an array of 400 single values representing the climatological temperature profile (in Celsius) from the surface to 40 km of altitude with a vertical sampling of 100 meters.
 795749.item.3.mat
Dataset Item 3 (Binary Data). The number of profiles used to get the final climatologies in matlab format (.mat) formed by cells corresponding to the onedegree latitude/longitude grid boxes in the following order: row 1 is latitude −90°; row 180 is latitude 90°; column 1 is longitude −180°; column 360 is longitude 180°. Whenever a value is missing, it is replaced by Not a Number (NaN). When the number of profiles for a certain grid box is and the NaN at each altitude is , the climatological value for the box and related altitude is computed averaging values. If , the climatological value is NaN. Each cell contains an integer representing the number of profiles used to compute the climatological temperature and bending angle for the corresponding onedegree box.
References
 E. R. Kursinski, G. A. Hajj, J. T. Schofield, R. P. Linfield, and K. R. Hardy, “Observing Earth's atmosphere with radio occultation measurements using the global positioning system,” Journal of Geophysical Research D, vol. 102, no. 19, pp. 23429–23465, 1997. View at: Google Scholar
 Y. H. Kuo, W. Schreiner, J. Wang, D. L. Rossiter, and Y. Zhang, “Comparison og GPS radio occultation soundings with radiosondes,” Geophysical Research Letters, vol. 32, no. 5, Article ID L05817, 2005. View at: Publisher Site  Google Scholar
 F. Pelliccia, P. Bonafoni, P. Basili, P. Ciotti, and N. Pierdicca, “Atmospheric profiling in the intertropical ocean area based on neural network approach using GPS radio occultations,” The Open Atmospheric Science Journal, vol. 4, pp. 202–209, 2010. View at: Publisher Site  Google Scholar
 Y. H. Kuo, T. K. Wee, S. Sokolovskiy et al., “Inversion and error estimation of GPS radio occultation data,” Journal of the Meteorological Society of Japan, vol. 82, no. 1, pp. 507–531, 2004. View at: Google Scholar
 D. H. Bromwich and R. L. Fogt, “Strong trends in the skill of the ERA40 and NCEPNCAR reanalyses in the high and midlatitudes of the southern hemisphere, 1958–2001,” Journal of Climate, vol. 17, no. 23, pp. 4603–4619, 2004. View at: Publisher Site  Google Scholar
 C. Y. Huang, Y. H. Kuo, S. H. Chen, and F. Vandenberghe, “Improvements in typhoon forecasts with assimilated GPS occultation refractivity,” Weather and Forecasting, vol. 20, no. 6, pp. 931–953, 2005. View at: Publisher Site  Google Scholar
 C. Cardinali, “Monitoring the observation impact on the shortrange forecast,” Quarterly Journal of the Royal Meteorological Society, vol. 135, no. 638, pp. 239–250, 2009. View at: Publisher Site  Google Scholar
 R. Biondi, T. Neubert, S. Syndergaard, and J. Nielsen, “Measurements of the upper troposphere and lower stratosphere during tropical cyclones using the GPS radio occultation technique,” Advances in Space Research, vol. 47, no. 2, pp. 348–355, 2011. View at: Publisher Site  Google Scholar
 R. Biondi, J. W. Randel, S. P. Ho, T. Neubert, and S. Syndergaard, “Thermal structure of intense convective clouds derived from GPS radio occultations,” Atmospheric Chemistry and Physics, vol. 12, no. 1, pp. 1–87, 2012. View at: Publisher Site  Google Scholar
 R. A. Anthes, P. A. Bernhardt, Y. Chen et al., “The COSMIC/Formosat3 mission: early results,” Bulletin of the American Meteorological Society, vol. 89, no. 3, pp. 313–333, 2008. View at: Publisher Site  Google Scholar
 G. Beyerle, T. Schmidt, G. Michalak, S. Heise, J. Wickert, and C. Reigber, “GPS radio occultation with GRACE: atmospheric profiling utilizing the zero difference technique,” Geophysical Research Letters, vol. 32, no. 13, Article ID L13806, 2005. View at: Publisher Site  Google Scholar
 M. Bonnedal, J. Christensen, A. Carlström, and A. Berg, “MetopGRAS inorbit instrument performance,” GPS Solutions, vol. 14, no. 1, pp. 109–120, 2010. View at: Publisher Site  Google Scholar
 G. Perona, R. Notarpietro, and M. Gabella, “GPS radio occultation onboard the OCEANSAT2 mission: an Indian (ISRO)—Italian (ASI) collaboration,” Indian Journal of Radio and Space Physics, vol. 36, pp. 386–393, 2007. View at: Google Scholar
 J. P. Aguttes, J. Schrive, C. Goldstein, M. Rouze, and G. Raju, “MEGHATROPIQUES, a satellite for studying the water cycle and energy exchanges in the tropiques,” in Proceedings of the International Geoscience and Remote Sensing Symposium (IGARSS '00), vol. 7, pp. 3042–3044, July 2000. View at: Publisher Site  Google Scholar
 A. Sen, K. Yunjin, D. Caruso et al., “Aquarius/SACD mission overview,” in 10th Sensors, Systems, and NextGeneration Satellites, vol. 6361 of Proceedings of SPIE, Stockholm, Sweden, September 2006. View at: Publisher Site  Google Scholar
 R. Biondi, T. Neubert, S. Syndergaard, and J. Nielsen, “Radio occultation bending angle anomalies during tropical cyclones,” Atmospheric Measurement Techniques Discussions, vol. 4, no. 1, pp. 1371–1395, 2011. View at: Publisher Site  Google Scholar
 University Corporation for Atmospheric Research (UCAR), UCARCOSMIC Data Analysis and Archive Center (CDAAC), 2012, http://cdaacwww.cosmic.ucar.edu/cdaac/.
 C. Rocken, R. Anthes, M. Exner et al., “Analysis and validation of GPS/MET data in the neutral atmosphere,” Journal of Geophysical Research D, vol. 102, no. 25, pp. 29849–29866, 1997. View at: Google Scholar
 G. A. Hajj, C. O. Ao, B. A. Iijima et al., “CHAMP and SACC atmospheric occultation results and intercomparisons,” Journal of Geophysical Research D, vol. 109, no. 6, Article ID D06109, 24 pages, 2004. View at: Publisher Site  Google Scholar
 R. Biondi, Upper troposphere lower stratosphere structure during convective systems using GPS radio occultations [Ph.D. thesis], 2012.
 R. Biondi, S. P. Ho, J. W. Randel, S. Syndergaard, and T. Neubert, “Tropical cyclone cloud top height and vertical temperature structure detection using GPS radio occultation measurements,” Journal of Geophysical Research. In press. View at: Google Scholar
 A. K. Steiner, B. C. Lackner, F. Ladstädter, B. ScherllinPirscher, U. Foelsche, and G. Kirchengast, “GPS radio occultation for climate monitoring and change detection,” Radio Science, vol. 46, no. 6, Article ID RS0D24, 2011. View at: Publisher Site  Google Scholar
Copyright
Copyright © 2013 R. Biondi and T. Neubert. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.