THE ROLE OF IMPACTS AND MOMENTUM TRANSFER FOR THE EVOLUTION OF ... - AMOS Conference · 2020. 7....

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2017 AMOS Technical Conference, 19-22 September, 2017, Maui, Hawaii, USA THE ROLE OF IMPACTS AND MOMENTUM TRANSFER FOR THE EVOLUTION OF ENVISAT’S ATTITUDE STATE Thomas Schildknecht, Jiri Silha, Astronomical Institute, University of Bern, Sidlerstr. 5, CH-3012 Bern, Switzerland Holger Krag Space Debris Office, ESA/ESOC, Germany ABSTRACT The currently proposed space debris remediation measures include the active removal of large objects and “just in time” collision avoidance by deviating the objects using, e.g., ground-based lasers. These techniques require precise knowledge of the attitude state and state changes of the target objects. In the former case, e.g. to devise methods to cap- ture the target with a tug spacecraft, in the latter, to precisely propagate the orbits of potential collision partners, as dis- turbing forces like air drag and solar radiation pressure depend on the attitude of the objects. The long-term evolution of the attitude motion is, among many other causes, depending on the effects of possible im- pacts of debris and meteoroid, while momentum transfer from reaction wheels or other moving internal components may contribute to the root cause of the initial attitude motion. Impacts of small particles like meteoroids and space de- bris pieces on compact space objects are unavoidable events, which were already observed several times, e.g., on Inter- national Space Station, or rather recently on the Sentinel-1A on August 23, 2016. This paper will discuss a detailed analysis of the effects of momentum transfer from the reaction wheels and of debris and meteoroid impacts for the particular case of Envisat. Based on the physical model of Envisat and the MASTER environment model, the likelihood to have an impact-related attitude rate increase in ten years larger than selected threshold rates was determined. 1. INTRODUCTION Recently the determination of attitude states, and in particular rotation rates, of space objects became a topic of interest in the space debris community. This is to be seen in the context of the multitude of techniques which are currently pro- posed to remove space debris from orbit or to re-orbit them into disposal orbits. The majority of the techniques to re- move large objects, which are driving the evolution of the space debris population on the long term, require capturing the target with a robotic arm, a net, a harpoon, or another mechanism. The attitude motion is in all these cases a critical parameter and the maximum tolerable target rotation rate is limited. The attitude motion of an inactive Earth orbiting object may change either due to dissipation of stored internal energy or internal momentum transfer, or because of external forces. Internal energy may be released, e.g., in form of leaking atti- tude control systems or pressurizes tanks, any type of breakup events, and momentum can be transferred from reaction wheels. External torques may results from the interaction with the gravity field gradients and the magnetic field of the Earth or from impulse transfer when colliding with other objects. The aim of this study is to assess the maximum angu- lar momentum change to be expected for the defunct Envisat spacecraft, on one hand due to angular momentum transfer from its reaction wheels, and, on the other hand, from impacts with space debris objects or micrometeorites. The latter was analyzed once for a single impact event and for a statistical particle flux over a then year period. The study was in particular triggered by the sudden acceleration of Envisat’s rotation observed about two months after its failure when Envisat’s attitude changed from an almost stable NADIR fixed attitude to a rotation with 0.547 rpm [1], [2], [3] (inertial rotation period ~ 110s; see Figure 1). Copyright © 2017 Advanced Maui Optical and Space Surveillance Technologies Conference (AMOS) – www.amostech.com

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2017 AMOS Technical Conference, 19-22 September, 2017, Maui, Hawaii, USA

THE ROLE OF IMPACTS AND MOMENTUM TRANSFER FOR THE EVOLUTION OF ENVISAT’S ATTITUDE STATE

Thomas Schildknecht, Jiri Silha, Astronomical Institute, University of Bern, Sidlerstr. 5, CH-3012 Bern, Switzerland

Holger Krag Space Debris Office, ESA/ESOC, Germany

ABSTRACT

The currently proposed space debris remediation measures include the active removal of large objects and “just in time” collision avoidance by deviating the objects using, e.g., ground-based lasers. These techniques require precise knowledge of the attitude state and state changes of the target objects. In the former case, e.g. to devise methods to cap-ture the target with a tug spacecraft, in the latter, to precisely propagate the orbits of potential collision partners, as dis-turbing forces like air drag and solar radiation pressure depend on the attitude of the objects.

The long-term evolution of the attitude motion is, among many other causes, depending on the effects of possible im-pacts of debris and meteoroid, while momentum transfer from reaction wheels or other moving internal components may contribute to the root cause of the initial attitude motion. Impacts of small particles like meteoroids and space de-bris pieces on compact space objects are unavoidable events, which were already observed several times, e.g., on Inter-national Space Station, or rather recently on the Sentinel-1A on August 23, 2016.

This paper will discuss a detailed analysis of the effects of momentum transfer from the reaction wheels and of debris and meteoroid impacts for the particular case of Envisat. Based on the physical model of Envisat and the MASTER environment model, the likelihood to have an impact-related attitude rate increase in ten years larger than selected threshold rates was determined.

1. INTRODUCTION

Recently the determination of attitude states, and in particular rotation rates, of space objects became a topic of interest in the space debris community. This is to be seen in the context of the multitude of techniques which are currently pro-posed to remove space debris from orbit or to re-orbit them into disposal orbits. The majority of the techniques to re-move large objects, which are driving the evolution of the space debris population on the long term, require capturing the target with a robotic arm, a net, a harpoon, or another mechanism. The attitude motion is in all these cases a critical parameter and the maximum tolerable target rotation rate is limited.

The attitude motion of an inactive Earth orbiting object may change either due to dissipation of stored internal energy or internal momentum transfer, or because of external forces. Internal energy may be released, e.g., in form of leaking atti-tude control systems or pressurizes tanks, any type of breakup events, and momentum can be transferred from reaction wheels. External torques may results from the interaction with the gravity field gradients and the magnetic field of the Earth or from impulse transfer when colliding with other objects. The aim of this study is to assess the maximum angu-lar momentum change to be expected for the defunct Envisat spacecraft, on one hand due to angular momentum transfer from its reaction wheels, and, on the other hand, from impacts with space debris objects or micrometeorites. The latter was analyzed once for a single impact event and for a statistical particle flux over a then year period. The study was in particular triggered by the sudden acceleration of Envisat’s rotation observed about two months after its failure when Envisat’s attitude changed from an almost stable NADIR fixed attitude to a rotation with 0.547 rpm [1], [2], [3] (inertial rotation period ~ 110s; see Figure 1).

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Fi

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[kg.m

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Table 1: Mo

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igure 1: Inertia

ion between ce meteoroids any times. In completely dihe impacted b

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2]

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omenta of iner

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2. MOME

compact spaceand space debcase that the srupted, the imbody and parttude state of nd on the imph respect to thg of a bus (a s 14m x 5m xr this model.

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ed the probabion we derivedssuming givennd the orbital act velocity, ancase also the ading to a rotate impacting pue arrow) to b) or ̂ (Figurem that these p

22 September

f Envisat meas

ENTUM AND

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[kg.m2]

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lity for a collid the resultingn scenario. Aelements of End impact angangular velociion around th

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ch as spacecrahereafter collecle will not cae impacting panear momentubody. The si

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ision betweeng angular momA representativEnvisat from Ogle we calculaity change

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aft and upper ectively calledause a catastrarticle will beum. Such an eize and directact velocity, anss. In our inveensions 4m x 2). By using t, , and ̂ fo

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n Envisat and amenta that partve synthetic pOctober 2014.ated the result

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stages on a gd MMOD) is rophic collisioe partially tranevent will caution of the resnd on the impstigation we u4m x 10m, 7

he parallel axor the given p

[kg.m2]

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gular cube (sat

a particle withticle would trapopulation has For every ge

ting received ae resulting spirespectively, wcations (greenating either ararticles per macomputed. Th

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geocentric orbunavoidable

on, meaning tnsferred to theuse, among otsulting angulapact geometryused a simple 7512 kg) and xis theorem, wprincipal axis

tellite bus) and

h a mass withiansfer to the s

as been generaenerated particangular momein period P. Twere analyzedn points defineround the priass interval whe resulting p

3]).

bit, and smalland has been

that the targete angular mo-ther effects, aar momentum, i.e. the loca-model for thesolar panel (a

we determinedof inertia are

d a thin plate

in the intervalatellite modelated by usingcle which wasentum , and

Three differentd. These casesed by positionincipal axis

were generatedprobability for

l n t -a

m -e a d e

l l g s d t s n

d r

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different angThe correspo

Figure 2: Visulting angul

These resultschange of thee.g., only a 0would changa mass of ~1the angular man event is pperiod of twspin rate charemote sensin

Figure 3: Proing a perfec(blue) and

and impact v

Technical Co

gular momentuonding angula

isualization oflar velocity ch

s clearly showe angular mom

0.9% probabilige the angular 100 g is requirmomentum chpredicted witho months. As

ange of Envisang observation

obability of coct inelastic col̂ (green). The

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onference, 19-2

um changes ar velocities ar

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in the positio

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red to spin uphange observedh a probabilitys a conclusionat as a collision show no evi

ollision duringllision for three figures showbutions) gener

22 September

around the thrre provided in

nt collision scearget after a coon marked by

is an very smthus in a substus would be hi0.15 deg/s, corp Envisat fromd two months

y of 0.24% ovn we may cleaon with an obidence of any

g ten years of eee different caw the result of rated by the M

r, 2017, Maui,

ree principal aFigure 4.

enarios to deteollision. The ithe green poin

mall probabilittantial changeit by a particlerresponding to

m a stable attits after the conver a time spaarly excludedbject of this mdamage on E

exposure (verases causing mf 1,000 simula

MASTER prog

Hawaii, USA

axes over a pe

ermine the traimpactor is shnt and blue po

ty for an impe of the spin rae of 6.31 g who spin period otude to about

ntact with the san of 10 yearsd an impact evmass would haEnvisat.

rtical axis) vermaximum rotatations using thgram assuming

A

eriod of ten y

nsferred anguhowed as a redosition vector.

act which woate around anyhich in the woof ~40 min. A0.4 rpm, whicspacecraft hass or with a provent for the exave damaged

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he MASTER Mg Envisat orbi

years are given

ular momentumd point collidin.

ould result inny axis of Envorst case (caseAn impact of ach would be cs been lost (Fiobability of 0xplanation ofthe spacecraf

angular momehe principal axMMOD populit and 10 years

n in Figure 3.

m and the re-ng with target

a substantialvisat. There is,e (a) Figure 2)an object withcomparable toigure 1). Such

0.004% over af the observedft severely but

entum assum-xes (red), lation (mass s of exposure.

.

t

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-

.

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For each impangular momlar velocity ((left vertical

Figure 4: Prohorizontal axcases causing

1,000 simu

To investigatESA MASTEare given in Fa 10 year pertion and assuangular mom(a), 12.2 kg given in Figuwith a mass 0.033 deg/s,

Figure 5: Cwas generate

Technical Co

pact geometrymentum we can(lower horizonaxis).

obability of coxis) and resultg maximum roulations using

M

te the effect thER model MMFigure 5. Theriod. In total aume that all immentum receiv

m2s-1 for caseure 6.The resuequal to ~0.4and 0.042 de

Cumulative died by MASTE

2014 to 01-1

onference, 19-2

y (related also n calculate thental axis) and

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MASTER pro

4. S

hat would be MOD populati MASTER toabout 5 106 pampacts occurreved from this e (b), and 97.ults of these c45 g, ~0.45g eg/s for the thr

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22 September

to given mome obtained rotresulting spin

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STATISTICA

caused by a flion of particleol was then uarticles were ied at one of thflux of particl.6 kg m2s-1 focumulative mand ~0.55g, r

ree cases.

r the mass (onvisat orbit (refg the MASTER

r, 2017, Maui,

ment of inertiatation velocityn period (uppe

exposure (leftzontal axis) as

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AL PARTICLE

flux of particlees heavier tha

used to predictimpacting Envhe positions (ales over 10 ye

or case (c), remomentum tran

respectively,

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Hawaii, USA

a, see Error! y of the modeler horizontal a

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E FLUX IMPA

es impacting En 10-15 kg wat impacts of thvisat. We maya), (b), or (c) ears is relativespectively. Sonsfers are equresulting in a

size (on the ri02014). The spulation in the

A

Reference sol. In Figure 4 axis) as a func

) versus receivrfect inelastic ̂ (green). The

velocity distribrs of exposure

ACTS

Envisat durings used. The pr

his MMOD poy now again cdefined in Figely small, namome characteruivalent to an angular veloci

ight) of the Msimulation cove mass range 1

ource not foucan be seen re

ction of probab

ved angular vecollision for te figures showbutions) genere.

g ten years of roperties of thopulation withconsider a wogure 2. The tomely 29.4 kg ristics of thesimpact of a s

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MMOD particlevered 10 year10-15 g - 1 kg.

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exposure, thehis populationh Envisat overrst case situa-

otal amount ofm2s-1 for casee impacts are

single particlef 0.013 deg/s,

es. The flux s from 01-11-

l -t

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-

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Figure 6: Imcles. The f

years fro

There are in Figure 7. Ontem used in tare aligned a

Figure 7: D

Each of the fmum angula

= 8

For this analywere determi

[kg

17023.3

The maximube transferred

Technical Co

mpact velocityflux was generom 01-11-201

total five reane reaction whthis paper). Tw

along the

Distribution an

five reaction war momentum 0 N m s and f

ysis we used sined by ESA (

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onference, 19-2

y distribution rated by MAS14 to 01-11-20

5. MOMEN

action wheels heel is alignedwo reaction w(along the a

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wheels has a c which

for it is

slightly differ(Table 2).

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angular veloc, is given in T

22 September

(left) and impSTER for the E024 using the

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installed on d along the wheels are aligaxis)

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Envisat [1]. T axis (ESA

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0 N m s (40 ksferred from tN m s.

r moment of in

m2]

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ree axes, if the

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and elevation d(reference to 2MOD populat

OM REACTIO

The configurareference sys

e axis (al

ed on Envisatcoordinate sys

kg m-2/s) with the wheels to

nertia of the p

spacecraft de

e momentum

A

distribution (ri21102014). Thtion in the mas

ON WHEELS

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in the satellitstem.

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[kg.m2]

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s is shown inreference sys-action wheels

inate system

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n wheel would

n -s

-=

h

d

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Principal axis No.ofreactionwheelsaligned withaxis

Reactionwheel capaci‐ty

[kgm2s‐1]

ENVISAT

momentof

inertia

[kgm2]

Maximum

angularvelocitychange[degs‐1]

Correspondingrotational

period

[hour]

1 40 17023.3 0.1346 0.743

2 40 + 40 124825.7 0.0367 2.723

2 40 + 40 129112.2 0.0355 2.817

Table 3: The maximum angular velocities and corresponding rotational periods of Envisat which can be obtained from reaction wheel(s) assuming different principal axis of inertia.

These results show that a momentum transfer from the reaction wheels cannot explain the observed spin-up of Envisat as the maximum change in angular velocity from this transfer is almost two orders of magnitudes smaller than the ob-served one (period of ~120s).

6. SUMMARY

Effects of debris and meteoroid impacts and of momentum transfer from the reaction wheels for the particular case of Envisat were analyzed. Based on the physical model of Envisat and the MASTER environment model, the likelihood to have an impact-related spin rate change in ten years was determined.

There is an very small probability for a single impact which would result in a substantial change of the angular momen-tum and thus in a substantial change of the spin rate around any axis of Envisat over a ten year time period. A particle of ~100 g is required to spin up Envisat from a stable attitude to about 0.4 rpm, which would be comparable to the angular velocity change observed two months after the contact with the spacecraft has been lost. The probability for such an event is less than 0.25%. Simulations showed that the accumulated momentum transfer from the entire MASTER MMOD population is also minor and would in with worst case assumption result in angular velocity change of 0.04 deg/s.

The maximum momentum which could be transfer from the Envisat’s reaction wheels to its body, assuming that the wheels were fully loaded, would result in an angular velocity change of 0.14 deg/s, 0.037 deg/s, and 0.036 deg/s, re-spectively, for the three main axes of inertia. Again, this is by far not sufficient to explain the observed spin-up of Envi-sat after its failure.

7. ACKNOWLEDGEMENTS

This work was performed in the context of the ESA study “Debris Attitude Motion Measurements and Modelling”, (ESA/ESOC 4000112447/14/D/SR).

8. REFERENCES

[1] Sommer, S., Rosebrock, J., Cerutti-Maori, D., & Leushacke, L. (2017). Temporal analysis of ENVISAT’s rotation-al motion. In 7th European Conference on Space Debris, ESA/ESOC, Darmstadt/Germany, 2017.

[2] D. Kucharski, G. Kirchner, F. Koidl, C. Fan, R. Carman, C. Moore, A. Dmytrotsa, M. Ploner, G. Bianco, M. Medvedskij, A. Makeyev, G. Appleby, M. Suzuki, J. M. Torre, Z. Zhongping, L. Grunwaldt, and Q. Feng, “Atti-tude and spin period of space debris envisat measured by satellite laser ranging,” IEEE T. Geosci. Remote, vol. 52, no. 12, pp. 7651–7657, 2014.

[3] Kirchner, G., Steindorfer, M., Wang, P., Koidl, F., Kucharski, D., Silha, J., Schildknecht, T., Krag, H. & Flohrer, T. Determination of Attitude and Attitude Motion of Space Debris, Using Laser Ranging and Single-Photon Light Curve Data. In 7th European Conference on Space Debris, ESA/ESOC, Darmstadt/Germany, 2017.

[4] Flegel, S., Gelhaus, J., Möckel, M., Wiedemann, C., Kempf, D., Krag, H. and Vörsmann, P. Maintenance of the

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ESA MASTER Model – Final Report. Technical Report ESA Contract Number: 21705/08/D/HK, Institute of Aero-space Systems (ILR), June 2011.

[5] Bargellini, P.; Garcia Matatoros, M. A.; Ventimiglia, L.; Suen, D., Envisat Attitude and Orbit Control In-Orbit Per-formance: AN Operational View, 6th International ESA Conference on Guidance, Navigation and Control Systems, held 17-20 October 2005 in Loutraki, Greece. Edited by D. Danesy. ESA SP-606. European Space Agency, 2006. Published on CDROM., id.52.1

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