occultation tomography of internal gravity waves analyzing

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Analyzing Constellation Performance for the Radio Occultation Tomography of Internal Gravity Waves Riley Fitzgerald 1 , Lucy Halperin 1 , Stephen Leroy 2 , Amelia Gagnon 1 , Kerri Cahoy 1 , Jim Clark 1 1 Massachusetts Institute of Technology, 2 Atmospheric and Environmental Research

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Page 1: Occultation Tomography of Internal Gravity Waves Analyzing

Analyzing Constellation Performance for the Radio Occultation Tomography of Internal Gravity Waves

Riley Fitzgerald1, Lucy Halperin1, Stephen Leroy2, Amelia Gagnon1, Kerri Cahoy1, Jim Clark1

1Massachusetts Institute of Technology, 2Atmospheric and Environmental Research

Page 2: Occultation Tomography of Internal Gravity Waves Analyzing

• Formation Flying for Clustered Occultations

• Occultation Cluster Quality and Distribution

• Examining Trends in Cluster Quality

• Conclusions

Outline

2April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

Page 3: Occultation Tomography of Internal Gravity Waves Analyzing

Formation Flight & Constellations

3IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and ClarkApril 8, 2021

Page 4: Occultation Tomography of Internal Gravity Waves Analyzing

• Technique demonstrated with COSMIC-1 data, before satellites dispersed: Wang and Alexander, JGR (2010); Schmidt, Alexander, de la Torre (2016). Sensitive only to long wavelengths (~1000 km) and low frequencies ( ~1/day) in order to find any clusters.

• A dedicated mission can find short wavelength (~50 km), high frequency waves (~1/30 min). Otherwise ~10,000 randomly distributed LEO satellites would be needed to develop an RO momentum flux climatology of these waves.

4

Alexander et al., QJRMS (2010)

Previous Work: RO Tomography of Gravity Waves

IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and ClarkApril 8, 2021

Page 5: Occultation Tomography of Internal Gravity Waves Analyzing

Formation Flight for Tomography

5IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

Flying small satellites in close formation yields RO sounding that are closely spaced on the ground. These can be used to infer internal gravity wave vectors.

April 8, 2021

Page 6: Occultation Tomography of Internal Gravity Waves Analyzing

Formation Flight for Tomography

6April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

Flying small satellites in close formation yields RO sounding that are closely spaced on the ground. These can be used to infer internal gravity wave vectors.

Page 7: Occultation Tomography of Internal Gravity Waves Analyzing
Page 8: Occultation Tomography of Internal Gravity Waves Analyzing
Page 9: Occultation Tomography of Internal Gravity Waves Analyzing

Mutual Orbit Group v. RAAN-Spread

9April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

Mutual Orbit Groups RAAN-Spread Constellation

Page 10: Occultation Tomography of Internal Gravity Waves Analyzing

10April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

Mutual Orbit Groups RAAN-Spread Constellation

See previous paper (in IEEE JSTARS) on MOG maintenance at DOI: 0.1109/JSTARS.2019.2961084

Page 11: Occultation Tomography of Internal Gravity Waves Analyzing

MOG Alternative: RAAN-Spread

11April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

↖ Colinearity

• RAAN-Spread constellations space satellites only in right ascension of the ascending node (RAAN)—no inclination difference is required.

• However, groups approach collinearity at min./max. elevation out of equatorial plane; the clusters produced tend to approach lines.

Page 12: Occultation Tomography of Internal Gravity Waves Analyzing

Quantifying the MOG/RS Tradeoff

12April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

• Main question: Can we quantify the tomographic performance tradeoff of the MOG v. RAAN-Spread architectures?

• What constellation designs are best for tomography, without requiring prohibitive constellation maintenance propulsion?

Page 13: Occultation Tomography of Internal Gravity Waves Analyzing

Occultation Cluster Quality

13April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

Page 14: Occultation Tomography of Internal Gravity Waves Analyzing

Occultation Cluster Quality Metrics

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• Occultation Cluster Wave Vector Uncertaintyy

x kx

kyPhase Fronts

April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

Page 15: Occultation Tomography of Internal Gravity Waves Analyzing

Example Clusters and Qualities

15April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

Page 16: Occultation Tomography of Internal Gravity Waves Analyzing

Latitude Dependence of Quality

16April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

Even distribution of good clusters for both; RAAN-Spread constellation has more fair/poor clusters at high latitudes.

Page 17: Occultation Tomography of Internal Gravity Waves Analyzing

Latitude-Dependent Distributions

17April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

Page 18: Occultation Tomography of Internal Gravity Waves Analyzing

Examining Trends in Quality

18April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

Page 19: Occultation Tomography of Internal Gravity Waves Analyzing

Latitude-Azimuth Distribution

19April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

• Shown: Distribution of all clusters in latitude and ray path azimuth angle.

• Equatorial soundings tend to be closer to east-west, high-latitude clusters tend to be aligned north-south.

• Distribution dependent on reference orbit, not constellation type.

Page 20: Occultation Tomography of Internal Gravity Waves Analyzing

Latitude-Azimuth Distribution

20April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

Mutual Orbit Groups: Best clusters occur at a specific latitude, but consistent good clusters matching total distribution.

RAAN-Spread: Fewer best clusters, and higher-latitude good clusters get cut down to poor (though fewer poor).

Page 21: Occultation Tomography of Internal Gravity Waves Analyzing

Latitude-Azimuth Distribution

21April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

Mutual Orbit Groups: Best clusters occur at a specific latitude, but consistent good clusters matching total distribution.

RAAN-Spread: Fewer best clusters, and higher-latitude good clusters get cut down to poor (though fewer poor).

Page 22: Occultation Tomography of Internal Gravity Waves Analyzing

Causes of Cluster Quality

22April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

RAAN-Spread• Good clusters tend to taper

off into the high latitudes.

• Geometric effects still present, but bad clusters continue above inclination.

• Best clusters concentrated into equatorial regions.

Mutual Orbit Groups• Even distribution of

good-quality clusters over all surveyed latitudes.

• Worst clusters due to geometric effects that stop at latitudes > inclination.

• Good clusters extend all the way up to high latitudes.

Page 23: Occultation Tomography of Internal Gravity Waves Analyzing

Cluster Quality (MOGs)

23April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

Page 24: Occultation Tomography of Internal Gravity Waves Analyzing

Cluster Quality (RAAN-Spread)

24April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

Page 25: Occultation Tomography of Internal Gravity Waves Analyzing

25April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

MOGsA. RS improves east-west

equatorial clusters.C. North-south eq. clusters

are worse for MOG.

B. Best high-latitude clusters are worse for RS.

D. MOG has no bad clusters above orbit inclination.

A B D

C

Page 26: Occultation Tomography of Internal Gravity Waves Analyzing

RAAN-Spread

26April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

A. RS improves east-west equatorial clusters.

C. North-south eq. clusters are worse for MOG.

B. Best high-latitude clusters are worse for RS.

D. MOG has no bad clusters above orbit inclination.

A B D

C

Page 27: Occultation Tomography of Internal Gravity Waves Analyzing

Conclusions• Though Mutual Orbit Group architecture yields

slightly-improved cluster geometry in higher latitudes, it requires significant propulsion to maintain constellation; this limits mission lifetime.

• RAAN-Spread constellations, which do not require RAAN maintenance, are a valid alternative to MOGs; they have slightly improved performance in equatorial regions, but more low-performance clusters in higher latitudes.

• This work is in second review with IEEE JSTARS. 27April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

Page 28: Occultation Tomography of Internal Gravity Waves Analyzing

Questions?Thank you to the National Science Foundation for funding this study via NSF Award 8150276.

28April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

Page 29: Occultation Tomography of Internal Gravity Waves Analyzing

Backup Slides

29April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

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Out-of-Plane Thrusts• Symmetric arcs of thrust at

the maximum and minimum latitudes can counter J

2

torques.• Angle γ gives required thrust

arc length:– Impulsive propulsion lets γ

approach zero.– Electric propulsion requires

that γ be a substantial fraction of the orbit arc.

31April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

Page 32: Occultation Tomography of Internal Gravity Waves Analyzing

Burn Arc Length and Efficiency• Rate of ΔV use is determined by ideal rate (α*, from

orbit geometry) and efficiency (η, from burn arc):

• For correction every Nth orbit with thrust/mass αmax

:

32April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

Page 33: Occultation Tomography of Internal Gravity Waves Analyzing

Rate of ΔV Expenditure

• Example (ISS):– i = 51.4⁰– δ = 0.172⁰– h = 400 km

• Frequent burns or higher thrust per mass raises efficiency.

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April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark

Page 34: Occultation Tomography of Internal Gravity Waves Analyzing

Latitude-Dependent Distributions

34April 8, 2021 IROWG-8 – Fitzgerald, Halperin, Leroy, Gagnon, Cahoy, and Clark