Regional forecast of ionospheric scintillation dedicated to offshore operators Ph. Yaya, L. Hecker CLS (Collecte Localisation Satellites) Toulouse, FRANCE ESWW13, Session 6, 15 Nov 2016 Summary Page 2 1. Introduction 2. Ionospheric scintillation phenomenon 3. Scintillation characteristics in West Africa o An ionospheric dedicated network o Time distribution of scintillations 4. An improved model based on measurements o Main principles o Performances of local forecast 5. Pilote sites of the service 6. Future steps ESWW13, Session 6, 15 Nov 2016 Summary Page 3 1. Introduction 2. Ionospheric scintillation phenomenon 3. Scintillation characteristics in West Africa o An ionospheric dedicated network o Time distribution of scintillations 4. An improved model based on measurements o Main principles o Performances of local forecast 5. Pilote sites of the service 6. Future steps ESWW13, Session 6, 15 Nov 2016 Introduction Page 4 Observation: some positioning processing based on GNSS may be degraded, sometimes very severely, on recurrent moment of the day Consequences: very important financial issues for off-shore applications. A consortium (CLS, Fugro, Telecom B.) worked under a CITEPH funding from 2011 to 2013 : More than 10 m of error Observation of the scintillations in West Africa Correlation with positioning anomalies Investigate means to forecast the scintillation Work in 2014-2015: development of a model based on the long-term observations (few years) and the very last observations (few hours) an operational service is proposed. Fugro-Topnav ESWW13, Session 6, 15 Nov 2016 Introduction S4 modelization near Libreville (Gabon) PPP processing with CNES/GINS software on NKLG IGS station (Libreville), from 13 to 21 March 2014: • • • • • Page 5 10 m Interval: 30s Constellation: GPS only Mode: undifferenced ambiguity resolution Cutoff : 15 deg Corrections: none (ocean or atmospheric tides,…) 10 m 10 m ESWW13, Session 6, 15 Nov 2016 Schematic impact Page 6 OK OK OK NOK OK NOK GPS receiver ESWW13, Session 6, 15 Nov 2016 Summary Page 7 1. Introduction 2. Ionospheric scintillation phenomenon 3. Scintillation characteristics in West Africa o An ionospheric dedicated network o Time distribution of scintillations 4. An improved model based on measurements o Main principles o Performances of local forecast 5. Pilote sites of the service 6. Future steps ESWW13, Session 6, 15 Nov 2016 Vizualisation of scintillation bubbles Page 8 The origin of the scintillation phenomenon is an instability of Rayleigh-Taylor in the E layer (100 km) at the sunset. These instabilities are sub-ionized structures which can elevate up to 1400 km. Numerical simulation of bubbles The color code corresponds to an increasing ionization density with the altitude (Huton, 2008) Observations of bubbles : Structures measured at Jicamarca (9°N) : the altitudes are between 400 and 1400 km before 21:00 LT. On GPS signal there are decreases of TEC and scintillations (Valladares,2005) ESWW13, Session 6, 15 Nov 2016 Ionospheric scintillations Page 9 Yellowknife, 29 Oct. 2003 (Lassudrie, Fleury) When the environment crossed by a radioelectric signal is homogeneous, its phase and amplitude are regular and predictable. But when the signal crosses a medium where the electronic density is not constant, both amplitude and phase are affected by rapid fluctuations that may last up to a few hours ESWW13, Session 6, 15 Nov 2016 Quantification of degradation Ascension, 27 March 2000 (Groves,2004) Define standardized indices Page 10 Amplitude Phase Normalized standarddeviation of the signal intensity (amplitude) S4 index gives the level of perturbation on the signal amplitude Standard deviation of the signal phase sf index gives the level of perturbation on the signal phase ESWW13, Session 6, 15 Nov 2016 Climatological models Climatological models (WBMOD and GISM) give global occurrence probabilities. They are not adapted to local phenomenon (in time and space) The accumulation of scintillation observations points out zones of high electronic density, the equatorial « crests » at +/- 15-20° on each side of the equator. Page 11 Map of scintillation intensity (WBMOD climatological model). IPS. Map of scintillation intensity (GISM climatological model). IEEA North equatorial crest South equatorial crest ESWW13, Session 6, 15 Nov 2016 Summary Page 12 1. Introduction 2. Ionospheric scintillation phenomenon 3. Scintillation characteristics in West Africa o An ionospheric dedicated network o Time distribution of scintillations 4. An improved model based on measurements o Main principles o Performances of local forecast 5. Pilote sites of the service 6. Future steps ESWW13, Session 6, 15 Nov 2016 Ionospheric Monitor Network Page 13 ISM = Iono. Scintillation Monitor = GNSS receiver robust to scintillations, and rated at 50 Hz (= frequency adapted to observe the scintillations, which have characteristic times of a few ms) These monitors directly give S4 and sf. Monitor installed in 2011 on Fugro bases on the Guinean Gulf. Position of the ISMs w.r.t. the South equatorial crest : • • • Port-Gentil station (POG1) on the maximum Pointe-Noire station (PNR1) is a bit lower Lagos station (LOS1) is almost on the magnetic equator ESWW13, Session 6, 15 Nov 2016 Time distribution of scintillations Page 14 Data span : about 2 years and ½ Scintillation occurrence: - Depends on local time: o o beginning at around19h LT, ending at around 02h LT. - Depends on the season: o o maximum at the equinoxes (Spring & Automn), with an earlier beginning (19h instead of 20h LT) minimum at the solstices (even though the occurrences are a bit higher during Summer than during Winter) Télécom Bretagne ESWW13, Session 6, 15 Nov 2016 Time distribution of S4 Page 15 Important : scintillation intensities are not lower at the solstices: they are less frequent Example for Pointe-Noire : - In October 2011 S4 is > 0.8 almost each day - In August 2012, there are also peaks of S4 > 0.8 This behavior cannot be reproduced with a climatological model Need for a model based on real time observation ESWW13, Session 6, 15 Nov 2016 Summary Page 16 1. Introduction 2. Ionospheric scintillation phenomenon 3. Scintillation characteristics in West Africa o An ionospheric dedicated network o Time distribution of scintillations 4. An improved model based on measurements o Main principles o Performances of local forecast 5. Pilote sites of the service 6. Future steps ESWW13, Session 6, 15 Nov 2016 Construction of the crest model Page 17 Data span: January 2013 to December 2014 Type of data: • S4 from the three ISM • S4 derived from GNSS receivers, computed from a Std Dev of SNR on L1. Construction of the model: • Each grid point is computed as the 95th percentile of all data values • FFT low pass filter on the cumulated data leads to a model, which is then adjusted on the last hours in order to forecast the level of scintillation. ESWW13, Session 6, 15 Nov 2016 Forecast method Page 18 • Every hour, the model is adjusted to the observations of the last 2 hours Computation of an observed scale factor • The observed scale factor of the afternoon is correlated to the scale factor of the evening Scale factor at 17 UT (blue) and 20 UT (red) over 24 months ESWW13, Session 6, 15 Nov 2016 Scale factor statistics Page 19 • Based on 24 months statistics, a forecasted scale factor is computed for the next hours • With observations until 17UT, the scale factor for 20UT is predicted with an RMS of 0.24 ESWW13, Session 6, 15 Nov 2016 Regional Forecast examples Page 20 • • Top : observations at the IPPs (Ionospheric Pierce Points) Bottom : Model at same locations NB: only the South crest is considered ESWW13, Session 6, 15 Nov 2016 Local validation (ex. at Libreville) Page 21 • A forecast can be given for any location covered by the model ESWW13, Session 6, 15 Nov 2016 Local validation: 3-h forecast results Page 22 • The daily maximum is predicted 3 hours in advance with an RMS of 0.1 ESWW13, Session 6, 15 Nov 2016 1-6 hours forecast results Page 23 • For all forecast ranges between 1 and 6 hours, the performances for a +/- 0.15 interval of S4 vary from 79% to 85% for daily maxima predictions. ESWW13, Session 6, 15 Nov 2016 Combined model Page 24 • Sinus fitting on the scale factor to derive a climatological model improvement of performances for few hours forecast ESWW13, Session 6, 15 Nov 2016 Summary Page 25 1. Introduction 2. Ionospheric scintillation phenomenon 3. Scintillation characteristics in West Africa o An ionospheric dedicated network o Time distribution of scintillations 4. An improved model based on measurements o Main principles o Performances of local forecast 5. Pilote sites of the service 6. Future steps ESWW13, Session 6, 15 Nov 2016 Pilote web sites Page 26 Put in place as a demo for some oil&gas companies NB. Many feedbacks from TOTAL that help us improving our model Customer’s sites of interest Hourly value of modelised index (Observed on last 18h / Prediction next 6 hours) History of daily max. ESWW13, Session 6, 15 Nov 2016 Summary Page 27 1. Introduction 2. Ionospheric scintillation phenomenon 3. Scintillation characteristics in West Africa o An ionospheric dedicated network o Time distribution of scintillations 4. An improved model based on measurements o Main principles o Performances of local forecast 5. Pilote sites of the service 6. Future steps ESWW13, Session 6, 15 Nov 2016 Perspectives Page 28 Tuning the model in order to: Improve the detection rate, Decrease the false alarm rate. 15 March, NKLG Color : forecasted S4<0.6 Grey : forecasted S4 >0.6 Time forecast per satellite towards a mitigation solution for positioning during scintillation events Analyse the possibility to construct and apply a model for the South-East Brasilian area, as it is also affected by scintillations. ESWW13, Session 6, 15 Nov 2016 Conclusions Page 29 Ionospheric scintillations can severly affect the precision of GNSS-based position techniques (up to several meters during high scintillation events) Scintillations have a global well known behavior but they are very difficult to forecast at a local level. Thanks to ionosphere-dedicated instruments and classical GNSS receivers we propose a model to predict the level of amplitude scintillation (S4) in the Guinean Gulf. The model is adjusted on a few hours of near real time observations and is able to give the maximum level of S4 3 hours before the beginning of the eventual event with a confidence level of 0.15 on 83% of the cases (4% of false alarms, 13% of missed events) The performance can still be improved, and a prediction per satellite will be considered in the future. The same model will be tested for the South-East Brasilian coast. ESWW13, Session 6, 15 Nov 2016
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