IRENE Cycle Variation (Stu)
[example POES inverted fluxes]
User request for low-altitude protons - controlled by atmosphere as much/more than magnetic field
Inside IRENE need to be able to map to some kind of reference state
How will it be used? Factor 10 differences are possible but those are in regions of low flux
How can we forecast solar cycle to use this analysis? Cycle appears at different times (lag) for different energies...
Requirement to cover: 0.1 - 2000 MeV; 0<K^0.5<3; 0 < hmin < 1000
Correlation of flux related to F10.7 (with phasing lag) - using POES/Selesnick Inner Zone Proton Model (SIZM) to derive parameters (lag, h_min and flux scaling)
SAMPEX data not used at present but there are plans to reprocess that and then make use of it.
DH: Why K^0.5 and not K? SH: Seems better results away from equatorial region.
DH: Why are you using hmin? POB: Basically we found it was a better measure of the low altitude environment.
RH: factor 10 variation in POES data inverted, do you need anything beyond the worst case? SH: Previously we were just using solar min design, user case it not clear.
LARB (Daniel)
[model maps, e.g.slide 17]
Reconstruct PSB97 for quick revision of mission rad. env. (previously XIPE, now THESEUS)
Then establish the new LARB model.
<1000 km & 0.1 - 1000 MeV p+
Fluxes range from 10^6 down to 10^-3
10 deg pitch angle bins on REPT not easily mapped to equatorial pitch angle - N.B. equatorial pitch angle not used for the model
RPS has
L, a_eq breaks down at these low altitudes so h_min used along with density parameter, n, as a proxy of L*
h_min is found tracing the drift shell but claculation is heavy so parabolic fits are using
Plan to use REPT to cover part of K v n map that SAMPEX doesn't
Geographical maps starting to come together - some more cleaning to be done
SH: using rho instead of h_min doesn't seem to improve performance
DH: hoping to capture the density in the same fit
RH: anything else matters apart from density?
DH: Well, there are injections but it's not clear how these should be incorporated
VALIRENE Toolkit
[slide 5 or 8]
Validation toolkit for the Ap9/AE9/SPM models against in-situ data sets and comparisons to other ECSS-recommended models also performed
Outputs also given for effects quantities.
Data used includes SAMPEX, EPT, PROBA-1/SREM, TSX-5/CEASE and AZUR + MERLIN, GPS, etc....
IRENE outputs of perturbed mean account for the uncertainties ain flux maps whilst m-c results are needed to capture space weather impacts
INTEGRAL p+ results shows that medium L ranges at lower energies AP8 appears to do better but all high energies AP9 appears to be better
RPS p+ data is almost always better matched to AP9 than AP8
INTEGRAL e- shows that for the most part one of AE8 max/min are better than AE9
However, for CRRES/MEA e- AE9 appears to be equally out-performing of AE8
AE9 doesn't appear to capture the variabilty even in M-C mode
AE9 appears to fall between MEO upper and MEO mean
Low-altitude high inclination orbits are not well-captured by IRENE
At GEO AE9 and AE8 are higher than IGE-POLE
EPOR for <1 year should use M-C mode of operation
YS: How do you know that the data sets are valid
PT: We also passed the fluxes from the model through the responses to compare counts which seems to show similar results.
YS: 1990-1991 CRRES/MEA should be higher than the model
PT: The comparisons don't bear this out
IJ: Your thinking is that if you use IRENE be cautious?
PT: There are cases fir the electrons where even 95% doesn't appear to span up to some of the data set yearly variables.
POB: This is really due to the nature of IRENE as a consensus model and data sets (especially e-) have likely much higher intrinsic errors than data owners claim
AE9/AP9-IRENE (Paul)
[image?]
V1.55 to US gvt contractors in 04/2019
v2.0 planned to include solar protons and sample solar cycle
Need: long-term (> cycle) assimilation (or just physics) run output (10 eV - 10 MeV e- and 10-eV - 1 GeV p+, 10 eV - 200 keV He+, O+
Like to check also the low altitude electrons (e.g. using DEMETER data)
Inside model all distributions are Weibull or lognormal. In AE9 this creates discontinuities.
Could use TREPEM-style approach but hard to capture the errors when you don't have a distribution fit
Effects kernels in V1.55 will replace SHIELDOSE2 and extend to charging
Need: thin shielding dose tools, plasma effects and ion effects
POB: for development the python version will be shared within collaboration
RH: why is the low altitude stuff so hard? It's well-understood.
POB: We need (physical) models we can use that get the numbers right
YS: What is plasma in this context?
POB: 40 keV cut-off between plasma and radiation
YS: What's the use case?
POB: Material degradation primarily
YS: What about surface charging?
POB: In the design scenario you probably take more of a worst-case scenario
SPM-IRENE (Paul)
Tim Guild is the main author.
Want to include MLT variation in the plasma model - nothing in there presently
Grid parameters are Energy, Lm and equatorial pitch angle
Coverage issues are being addressed including THEMIS from v1.2
Limit of 1 keV due to high scatter in conjunctions preventing any kind of cross-calibration between plasma analysers
Templates taken from data sets supplemented by models
Issues: only 1 data set including composition, no mean local time variation
Plan to include HOPE in some way even though it cannot operate that well in the inner zone due to interference
Would like ring current simulators as well.
YS: Can HOPE not become a gold standard?
POB: Should be able to be
JAS: Why does you use the Cluster CIAS data which has time-of-flight and composition?
POB: Initially it wasn't in an interesting orbit, we might have to re-look at it.
Yoshi: Has up to 200 keV data which could be included inside the model (LEPI and MEPI on Arase).
HOPE Plasma data analysis (Dave)
[slide 8,Plasma interactions drive high-level charging
NASA and ECSS have worst case for GEO but other orbits aren't well specified for this effect
HOPE is a top-hat ESA with time-of-flight allowing energy + mass to be determined
Data has been ingested into ODI (25 eV - 51.8 keV)
Charging events result in acceleration of protons (so we don't see the lower energies) - Can check HOPE output against the E-field and waves instruments (but that is limited to 200 V whereas HOPE measures events up to 1000 V)
As is well known the events all occur in the midnight-dawn region of the orbit
Strangely events were mainly seen in 2012 - 2013 (perhaps resulting from a change in material properties)
Rare temperature enhancements show bit enhancements which are most pronounced at L=6 - 6.5
Mean data appears to show peak at L = 3 (would need to be further investigated)
Need electron and ion Maxweillian temperature and density and to see if the data is well fit by these during charging events (data may need to be corrected)
Temperature alone doesn't seem sufficient (maybe a flux ratio at different energies)
POB: Can we use 10 keV e- flux instead of temperature
DR: There are many people using different proxies which is an issue.
POB: How can we filter events to derive the worst-case for spacecraft specification
DR: Indeed
Arase (Yoshi)
1-d Fokker-Planck solver with assimilation using Particle-filter
Prediction from distributions of state (vectors) are then compared to data to give a weighting for the likelihood and then resampling of the data based on this before next set of state vectors are given.
Radial diffusion coeff, lifetime and internal source parameters are output state.
400 - 800 keV electrons
Inclusion of internal source process improved results based on MAPE proxy for time series performance.
Arase data XEP (similar to REPT) to be extended into 2022/2023
RH: What range of energies does the source need to cover?
YM: 300-400 keV
Discussion
POB: We talked about gap filling for environments but templates in IRENE has resulted in kinks in the data. Can use data assimilation in this but would require running the data assimilation inside the model
YS: Can be done but we should add derived dose which is measured(?) and the number of steps that are run is important for smoothing
POB: Should use the BAS model but we might like something which has more of a data assimilative aspect than just GEO boundary conditions.
YS: Need to work out how to use LEO data
POB: we will need to translate the outputs into the IRENE coordinates system from PSD.
We would need to investigate funding process for comparing and integrating data assimilative model outputs.
PJ: Can we really include modes for cycle phases due to how poor cycle predictions tend to be.
YS: For cubesats where the production time is very short one it could be reasonable. They would like to understand to fix launch dates
POB: Tends to be unlikely that someone builds a line of satellites on the basis of being able to launch at only one phase of the cycle.
PJ: If you want to use a cycle phase then it should be used to build a historic picture to capture variability and confidence
RE: We need to define what we want to use for worst cases for spacecraft designers to make use of models.
PJ: How can we work on kinks introduced with low altitude models as opposed to
SH: Doing the templates is the present effort to line these things up.
POB: Using physics-based models at LEO with protons
AS: LEO included as well as we can right now.
POB: OPAL is broadly based on data rather than physics-based modelling.
Inner zone p+ needs to be developed including CRAND and to go down to lower energies (100 keV) whereas now there is an issue below 20 MeV
DH: Need to get people to clean data and introduce processes so we don't have to keep re-processing it.
DH: We are also duplicating effort in cleaning these things up.
PJ: There are issues of trust but no longer issues to release the factors produced under our contract because it's now approved for o/s
POB: Probable in AFRL that this is as much a process issue than something intractable