15 years of LANL data compared to ECSS guidelines for surface charging

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Presentation transcript:

15 years of LANL data compared to ECSS guidelines for surface charging 23rd SPINE meeting April 4th, 2017, ESA HQ, Paris J.C. Mateo-Velez (1), A. Sicard(1), D. Payan(2) (1) (2)

Context From Choi 2011, electron < 100 keV seem to have similar behaviors with spacecraft anomalies 1997-2009 95 anomalies from Satellite News Digest 32 anomalies with known times: 72 % (23/32) in night sector, with high kp index, correlation with 50-75 keV e- Seasonal effects: increased kp and eclipse situations during equinox seasons Probable cause for anomalies = surface charging by electron injection in the geomagnetic tail causing electrostatic discharges (ESD) Choi et al. 2011

Context At spacecraft design phase, the risk assessment combines two approaches Surface charging risk is generally assessed at spacecraft scale by using computational tools (SPIS, NASCAP, MUSCAT, etc.) Threshold and effects of ESDs assessed by testing in order to limit/avoid power losses on solar cells for instance Knowing the ‘severe’ and ‘extreme’ environments at GEO/MEO is of prime importance Worst-case environments from guidelines (ECSS, NASA) defined in the 80’s More recent data can be used to check that guidelines remain conservative and/or to propose new environment specifications Objectives Analyse 15 years of data on LANL spacecraft at GEO Investigate possible correlation with anomalies from Choi 2011 Compare with guidelines

LANL data Analysis of 7 GEO LANL satellites data 1989-049, 1990-095, 1991-080, 1994-084, LANL-97A, LANL-01A, LANL-02A: > 60 satellites-years Electron and proton detectors from 1 keV up to some MeV Thomsen-2013 analyzed 13 years of data from 1995 to 2007 Large negative potential (< -100 V) seen during geomagnetically active times, in the region surrounding midnight local time Increased probability in the declining phase of the solar cycle 2003-2004 Increased probability in equinox seasons (march-april; sept-oct) Best correlation with 8 keV electron flux if threshold of 1.4×103 cm-2.s-1.sr-1.eV-1 is exceeded Same statistical dependence as anomalies from Choi-2011 Thomsen et al. 2013

LANL data 15 years of data from 1989 to 2005 : additional statistical information Electron and proton spectra corrected by the spacecraft potential : eg. 8 keV electron measured by -2 kV spacecraft mean that initial electron energy was 10 keV Electron spectra binned in 10-50 keV, 50-100 keV, 100-200 keV ranges Best correlation of potentials with 10-50 keV (consistent with Thomsen-2013). Probability to get a voltage below -1000 V is 20 % if 10-50 keV electron flux exceeds 2 ×108 cm-2.s-1.sr-1 (0.01 % of the time) 10 % if 10-50 keV electron flux is 1-2 ×108 cm-2.s-1.sr-1 (1 % of the time) 1 % if 10-50 keV electron flux is 0.4-1 ×108 cm-2.s-1.sr-1 (10 % of the time) Used in Spacestorm Satellite Risk Indicators webpage http://www.risk.spacestorm.eu/

‘Severe’ LANL environments Maximum electron fluxes above 10 keV [FE10k] Averaged over 15 minutes; declustering by selection of maximum flux each month on each spacecraft (>600 events); selection of top 100 events over all spacecraft-month 8 keV electron flux > 4×103 cm-2.s-1.sr-1.eV-1 (exceed Thomsen-2013 threshold) Top events April 5th 2004 July 15th, 2000 Oct 29th, 2003 Solar-cycle dependence : least probability during solar minimum (1996), more probable during declining phase (1992-1993; 2003-2004) Spacecraft potential < -100 V down to -1500 V Geomagnetic activity dependence: kp index greater than 4 and up to 9 MLT dependence: 9 PM - 6 AM night sector Unclear seasonal effect Related anomalies ? July 30th, 1999 (ANIK E2, tmp outage) Sept 12th, 1999 (PAS-8, tmp outage) Oct 28th, 2003 (Kodama, tmp safe mode) Jan 17th, 2005 (JCSat1B, tmp outage) Sept 14th, 2005 (Koreasat 2, tmp outage)

‘Severe’ LANL environments Top event March 13th, 1997 Long durations with potential < -5000 V [PG5k] 8 keV electron flux > 3×103 cm-2.s-1.sr-1.eV-1 (exceeds Thomsen-2013 threshold) Solar-cycle dependence : more probable during declining phase (1992-1993; 2003-2004) Geomagnetic activity dependence: kp index between 2 and 6 MLT dependence: midnight Seasonal effect: equinoxes (march-april; sept-oct)  high probability in eclipse High negative charging exceeds the eclipse duration from times to times Related Anomalies ? March 17th, 2004 (PAS-6, pow er anomaly) Sept 19th, 2003 (Telstar 4, total loss)

‘Severe’ LANL environments High flux above 200 keV and medium flux below 50 keV [HFAE] Solar-cycle dependence : less probable during solar minimum (1996), more probable during declining phase (1992-1993; 2003-2004) 8 keV electron flux > 2×103 cm-2.s-1.sr-1.eV-1 (exceeds Thomsen-2013 threshold) Geomagnetic activity dependence: kp index between 3 and 8 Top events May 29th, 2003 July 15th, 2000 Oct 29th, 2003 MLT dependence: 09 PM – 09 AM night sector No seasonal effect High negative charging down to -5000 V in eclipse from times to times Related Anomalies ? Jan 11th, 1997 (Telstar 401, ESD, total loss) Aug. 27th, 2000 (Solidaridad 1, total loss) Sept 19th, 2003 (Telstar 4, total loss) April 5th, 2005 (Garuda 1, pow loss)

‘Severe’ LANL environments Low flux above 200 keV and high flux below 50 keV [LFHE] Solar-cycle dependence : no clear dependence 8 keV electron flux > 6×103 cm-2.s-1.sr-1.eV-1 (exceeds Thomsen-2013 threshold) Geomagnetic activity dependence: kp index between 3 and 8 Top event Sept 9th, 1997 MLT dependence: 09 PM – 09 AM night sector Least probability in solstice (june, dec) High negative charging down to -5000 V in eclipse from times to times Related Anomalies ? Sept 1st, 1998 (Sirius 2, loss of some solar cells) Oct 23rd, 2001 (Echostar VI, loss of 2 strings)

‘Severe’ LANL environments LANL top events have been fitted by tri-maxwellian distributions Date loc. Ref Electron 1   Electron 2 Electron 3 Proton 1 Proton 2 Proton 3 N (106/m3) T (keV) April 05, 2004 GEO LANL FE10k N°1 0.6 1 0.7 7 0.1 15 0.01 40 May 29, 2003 LANL HFAE N°1 0.05 0.2 5 0.25 20 2 0.35 0.15 Sept 03, 1997 LANL LFHE N°1 10 1.1 0.007 March 13, 1997 LANL PG5k N°1 0.4 0.004 30 0.03 0.5 12 0.005 July 15, 2000 LANL FE10k_05min N°3 3 25 50 October 29, 2003 LANL FE10k_05min N°5 0.28 0.3

‘Severe’ LANL environments and guidelines ECSS Guidelines from event on SCATHA April 24th, 1979 Two-maxwellian distribution that exceeded the actual data above 20 keV Tri-maxwellian distribution is suggested to mimick the actual data protons electrons NASA guideline Simple maxwellian for the 90th percentile GEO flux Alternative worst-case to be discussed with US people because of some uncertainties on so-called SCATHA-Mullen-1 and 2 (to be discussed with HB Garrett and D Ferguson) ATS-6

‘Severe’ LANL environments and guidelines LANL envelope Guidelines envelope LANL Vs. Guidelines LANL Vs. Suggested updated worst-cases (incl. from HB Garrett) Guidelines electron fluxes are significantly higher above 20 keV, and a bit weaker below 5 keV Suggested cases better fit with LANL data LANL fluxes are exceeded in [10-100 keV]

SPIS simulations Assess telecom spacecraft charging under severe environments Absolute potential and Inverted Potential Gradient (IPG) of solar panels At daylight and in eclipse frame IPG on solar panels Mateo-Velez, Theillaumas et al. 2015 Spacecraft materials from SPIS default database with additional information from ONERA on properties measurements for CMX, MLI

Worst-case charging at Sun  Origin  Title Absolute potential (V)   Differential potential (V) Frame CMX av. CMX max diel min CMX NASA-HDBK-4002A SCATHA-Mullen-1 -12100 -7100 +5000 SCATHA-Mullen-2 -7800 -4500 +3300 Deutsch ATS-6 -3600 -2400 -2000 -5600 +2200 +2600 ECSS‐E‐ST‐10‐04C SCATHA April 24, 1979 -5000 -3300 -2600 -8600 +1700 +2400 90th percentile -2300 -1200 +1100 ‘ECSS‐E‐ST‐10‐04C’ Suggested modification -2200 -1400 -2500 +800 +1000 -300 ‘NASA-HDBK-4002A’ SCATHA-Mullen-2 cor by HBG -880 -530 -440 +350 +440 -320 LANL-ONERA-CNES FE10k – HFAE – LFHE – PG5k +200 to +300 SCATHA-Mullen-1 cor by HBG -380 -220 -200 -620 +160 +180 -240 ? ? at daylight Photoemission limits negative charging, prevent charging of fully conductive spacecraft Charging is made possible by covering insulators on sunlit surfaces Electron fluxes above 10-20 keV control the absolute spacecraft charging Photoemission results in high IPG level on solar arrays

Worst-case charging in eclipse  Origin  Title Absolute potential (V)   Differential potential (V) Frame CMX av. CMX max diel min CMX ‘ECSS‐E‐ST‐10‐04C’ SCATHA April 24, 1979 Suggested modification -6100 -4100 -3700 -6400 +2000 +2400 -300 NASA-HDBK-4002A SCATHA-Mullen-1 -24000 -22000 -21900 -24700 +2100 -700 ECSS‐E‐ST‐10‐04C -11300 -9500 -9400 -12000 +1800 +1900 SCATHA-Mullen-2 -18400 -16800 -16600 -18900 +1600 -500 ‘NASA-HDBK-4002A’ SCATHA-Mullen-2 cor by HBG -2450 -2200 -3900 +1250 +1500 -200 LANL FE10k N°1 April 5th, 2004 -2350 -1550 -1370 -2550 +800 +980 SCATHA-Mullen-1 cor by HBG -1450 -1300 +750 +900 -150 LANL HFAE N°1 May 29th, 2003 -4500 90th percentile -16500 -15900 -15800 -16700 +600 +700 Deutsch ATS-6 -25700 -25100 -25900 ? ? In eclipse Electron above 10 keV control the absolute spacecraft charging Electron below 10 keV generates secondary emission Electron below 10 keV generates high IPG level on solar arrays  Different worst-cases

Conclusion SCATHA experienced a very severe event on April 24th, 1979 that remains above 15 years of LANL data, in terms of surface charging risks The tri-maxwellian spectra suggested in this work is not conservative wrt to ECSS at daylight, but is more conservative in eclipse, at least on the selected telecom spacecraft design The detailed response of other spacecraft may depend on its geometry and materials It is suggested to assess spacecraft charging risk under different ‘severe’ environments Low energy plasma measured by LANL probably at the root of a number of anomalies on GEO satellites Perspectives MEO charging (Van Allen probes) PEO charging (Ambre detector on Jason-3) ‘Extreme’ events (Spacestorm UE project) Adaptation of testing chambers (ONERA/SIRENE)

Acknowledgments This work was funded by CNES R&D program Part of the research leading to these results funded in part by the European Union Seventh Framework Programme (FP7) under grant agreement No 606716 SPACESTORM The authors thank R. Friedel, G. Reeves, M. Thomsen and M. Henderson from LANL for sharing data