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SATELLITE THREAT DUE TO HIGH ALTITUDE NUCLEAR DETONATIONS DENNIS PAPADOPOULOS PHYSICS DEPARTMENT UNIVERSITY OF MARYLAND Acknowledge Input From DTRA HAND/HALEOS STUDY TETHER PANEL HAARP STUDY

“Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

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Page 1: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

SATELLITE THREAT DUE TOHIGH ALTITUDE NUCLEAR

DETONATIONS

DENNIS PAPADOPOULOSPHYSICS DEPARTMENT

UNIVERSITY OF MARYLAND

Acknowledge Input From

• DTRA HAND/HALEOS STUDY• TETHER PANEL HAARP STUDY

Page 2: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

OUTLINE

• The Threat : Nuclear Detonations in Space• EMP Effects – Prompt (<1sec)HEMP, MHD-EMP, SGEMP

• Relativistic Particle Injection into the RadiationBelts (Van Allen Belts) – Delayed EffectsMonths to Years

• Damage to Space Assets and Mitigation Options

Page 3: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

How Could It Happen?How Could It Happen?

• Collateral damage from regional nuclear war or TMD/NMD intercept:– Nuclear warning shot in a regional conflict;– Effort to damage adversary forces/infrastructure with

electromagnetic pulse;– Detonation of salvage-fused warhead upon exoatmospheric

intercept attempt.

• Deliberate effort to cause economic damage with lower likelihood of nuclear retaliation:– By rogue state facing economic strangulation or imminent

military defeat;– Pose economic threat to the industrial world without causing

human casualties or visible damage to economic infrastructure.

From HALEOS Study

Page 4: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

H and MHD EMP• Line of Sight•Not a Threat to

space assets• Major Threat toGround Systemsand groundinfrastructure

Early (nanosecs) and late (secs)GHz to Hz

• MitigationHardeningexcept forMHD

Page 5: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

50 KT Burst over North Korea at 120 km altitude50 KT Burst over North Korea at 120 km altitude

Upset >>>>>> Burnout

Prompt XPrompt X-radiation impacts 5-10% of each LEO constellation.

0

0.02

0.04

0.06

0.08

0.1

0.12

0.14

1.00E

-06

3.00E

-06

1.00E

-05

3.00E

-05

1.00E

-04

3.00E

-04

Minimum X-ray fluence level (cal/cm2)

Globalstar(1414 km 52deg)Iridium (780km 86.4 deg.)

Fraction of satellite constellation exposed to X-ray level

(Simplified, single-plane,polar orbit illustration.)

SYSTEM GENERATED EMP - SGEMP

From HALEOS Study

•Prompt – line of sight – burst dependent

Page 6: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

10-6 10-5 10-4 10-3 10-2 10-1 1

Pro

gram

Cos

t (%

) 6

5

4

3

2

1

0

Thermo-Mechanical

and neutron effects

Latchup(screen)

TREE & SGEMP Upset Analysis & Design

SGEMP Protection

& Test

TREEBurnout

Protection & Test

Cost to harden to natural environments

X-ray Fluence [cal/cm2]

Cost increases for higher threat levels

Hardening goal

COST OF HARDENING AGAINST SGEMP

From HALEOS Study

Page 7: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

• Effect of a single high altitude nuclear weapon detonation on LEO satellites

– Nuclear burst “pumps” Earth’s Van Allen radiation belts with energetic electrons generated from beta decay of fission fragments

– Satellites that fly through these enhanced belt regions will be rapidly degraded/destroyed due to a rapid accumulation of total ionizing dose on critical satellite electronic parts.

RADIATION BELT PUMPING

Page 8: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

BASICS- THEEARTH’s MAGNETICFIELD

• Magnetic Configuration• L - Shells• Inner RB (1.5<L<2.2)• Slot (2.2<L<3)• Outer (L>3)• Invariant Latitude

Page 9: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

TRAPPING AND MIRRORING OFTRAPPING AND MIRRORING OFENERGETIC PARTICLES IN THEENERGETIC PARTICLES IN THE

RADIATION BELTSRADIATION BELTS

Page 10: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

THE VAN ALLEN BELTS

Page 11: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university
Page 12: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

Low earth orbit (LEO)

Elliptical orbit

Geosynchronous Orbit (GEO, GSO)

Inner RadiationBelt

Outer RadiationBelt

Medium earth orbit (MEO)

Highly idealized depiction of natural radiation belts.Inclination of each satellite orbit set to zero for display purposes.

Semi-synchronous orbit

Earth

SATELLITE MOTION THROUGH THE BELTS

Page 13: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

THE ROLE OF MeV ELECTRONS

– MeV electrons cause internal charging of dielectric surfaces

-Cumulative radiation dose

-Loss of attitude control•Degradation of performance

•Swelling of mirror surfaces

•Darkening of glassy surfaces

•Solar cell degradation

•Thermal control degradation

•Damage electronic components

•Limits lifetime

ESA Study 2001Most of satellite designers identified internal chargingcaused by MeV electronsas their most important problem(Horne 2001)

Page 14: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

• Internal charging and ESD is related to MeVelectron flux (variations)– more than 20 spacecraft damaged [Wrenn and Smith,

1996]

• Several examples of spacecraft damaged during storms when flux was enhanced, e.g., Baker et al. [1998]– 1994: Intelsat K, Anik E1, & E2– 1997: Telstar 401– 1998: Galaxy IV

• US National Security Space Architect:– 13 satellites lost in 16 years that can be attributed clearly

to natural enhancement ( flux of 108 #/cm2 sec) of MeV electrons

Page 15: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

STARFISH High Altitude Burst - 1962

• Yield: 1.4 MT• Altitude: 400 km above Johnson Island• Produced a large number of beta electrons

which became trapped in the Earth’s magnetic field causing an intense, artificial radiation belt

• “Pumped Belts” lasted until the early 1970’s

•• Seven satellites destroyed within seven monthsSeven satellites destroyed within seven months–– Examples:Examples:

Satellite Satellite CauseCauseTransit 4BTransit 4B Solar Cell DegradationSolar Cell DegradationTraacTraac Solar Cell DegradationSolar Cell DegradationArielAriel Solar Cell DegradationSolar Cell DegradationTelstarTelstar Command Decoder FailureCommand Decoder Failure

Page 16: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

Natural Electron Population

Flux [e-/cm2/s]

>106

>105

104

Energy > 1MeV electrons

Page 17: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

Natural and Enhanced Electron Population One Day After Burst Over Korea

Flux [e-/cm2/s]

>106

>105

104

Energy > 1MeV electrons

>108

Page 18: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

Natural and Enhanced Electron Population Two Years After Burst Over Korea

>106

>105

104

Flux [e-/cm2/s]

Energy > 1MeV electrons

>108

>107>106

Page 19: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

RUMSFELD II REPORT

Page 20: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

SUMMARY

• LEO constellations present tempting targets to future nuclear-missile-armed rogues, lowering the nuclear threshold.

• LEO constellations may be destroyed as a by-product of nuclear detonations with other objectives (e.g., EMP generation, salvage-fusing at nmd intercept, nuclear interceptor).

• Loss of civilian and military communications, imaging, weather forecasting, scientific infrastructure in space

• Socio-economic and political damage due to dependence on LEO constellations

Is there mitigation besides hardening ?

Page 21: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

0.1 1.0 10

40

30

20

10

Months After Burst

30 Krad (Si)

Source: DNA

Bay of Bengal50 kT burstAt 250 km100 mil Al

Num

ber

of A

sset

s

Rem

aini

ng

1.5 MeV Electrons Flux

LEO SATELLITE DEGRADATION

• Possible mitigation if MeV electron lifetime is reduced to fewdays. TETHER PANEL RECOMMENDATION

Page 22: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

in

out

in=out

in

out

in=out

Inject a bucket of water

• Time to return to the equilibrium level depends on outflow rate. The bigger the outflow hole the faster the system will get back to its natural equilibrium.

CONTROL OF ELECTRON LOSS RATE

• What process controls the electron loss rate

Page 23: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

Interaction with VLF Waves Controls Loss

Rate

• ELF/VLF waves resonantly interact with charged particles

• Interaction pushes the particle velocity vector toward the magnetic field line - long lifetime ⇔ high reflection altitude ⇔ low v||

• Particles become more likely to precipitate into the upper atmosphere

• Lifetime reduction is proportional to the ELF/VLF signal energy stored in the radiation belts

Page 24: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

LIFETIME CONTROL BY VLF WAVES

Page 25: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

>106 >105104

>108

Explosion-excited region

Loss rate proportional to local energy density of VLF waves

Is it feasible to pump up the VLF energy in the selectedregions to the required level ?

Page 26: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

• How many satellites are neededto reduce lifetime to ten days ?

• Too many (100s).

• Is there a way out ?

• Yes - Amplification

• The energy of the relativistic electrons can amplify the waves10 dB amplification reduces the# of satts to tens while 20 dBto few.Is there evidence for amplification ?

Page 27: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

VLF Wave-Injection Experiments

Interaction Region

VLF Wave-injection fromSiple Station, Antarctica

Page 28: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

§ Injected Siple signals often amplified by 10 to 30 dB and new emissions triggered– For input Bw > Bth

• Bth =0.1 to 0.5 pT

• Amplification is more likely to occur during times of enhanced fluxes of energetic radiation belt electrons

Siple Experiments Natural Amplification of Injected

Signal

Page 29: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

Understanding and Using Natural Amplification

• Using natural amplification can dramatically reduce the size and cost of a satellite protection system

• To use natural amplification reliably, experiments are needed which transmit and receive ELF/VLF over a wide range of frequencies

• Experiments could use satellite or ground-based transmitters, but: conventional transmitters (ground or satellite) can only cover a narrow frequency range

Page 30: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

• Observe amplified and triggered waves– At conjugate region (Southern

Pacific) – Near HAARP upon reflection

in the south

• Observe ionospheric effects of precipitated electrons with HAARP diagnostics

TETHER Panel Recommendation: Use HAARP facility in Alaska as a “wind tunnel”to determine the feasibility and engineeringspecifications of a mitigation system.

Page 31: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

What is HAARP?

• Large ionospheric research facility in central Alaska• Joint project of AFRL and ONR• Powerful, flexible source of ELF/VLF signals over a very wide

frequency range (0.1 Hz – 40 kHz)

Page 32: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university
Page 33: “Satellite Threat Due to High Altitude Nuclear Detonations” · PDF filesatellite threat due to high altitude nuclear detonations dennis papadopoulos physics department university

CONCLUDING REMARKS

• A HANE will have deleterious consequences to the LEO constellations– Prompt EMP effects will affect line of sight ground

and space based systems• Affect < 10% of LEO constellations• Only mitigation is hardening• Replacement possible

– Long term effects involve pumping of the radiation belts with MeV electrons due to beta decay

• Affect the entire fleet of satellites at the injection L-shell• Replacement not possible for probably one year• Mitigation includes orbit changing and radiation belt

“pump out”