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Volumn , Issue , 1998, Pages

Application of the terminator tether™ Electrodynamic drag technology to the Deorbit of constellation spacecraft

Author keywords

[No Author keywords available]

Indexed keywords

COMMUNICATION SATELLITES; DRAG; ELECTRODYNAMICS; ORBITS; PROPULSION; ROCKETS; SATELLITES; SPACE FLIGHT; SPACECRAFT;

EID: 34548152975     PISSN: None     EISSN: None     Source Type: Conference Proceeding    
DOI: None     Document Type: Conference Paper
Times cited : (43)

References (19)
  • 1
    • 84963881539 scopus 로고    scopus 로고
    • JLoftus@ems.jsc.nasa.gov, personal communication via email Monday 10 June 199615:50:10
    • Loftus, JP., JLoftus@ems.jsc.nasa.gov, personal communication via email Monday 10 June 199615:50:10.
    • Loftus, J.P.1
  • 3
    • 84963849772 scopus 로고
    • Interagency Report on Orbital Debris 1995, The National Science and Technology Council
    • Office of Science and Technology Policy: 1995, Interagency Report on Orbital Debris 1995, The National Science and Technology Council
    • (1995)
  • 4
    • 84963916177 scopus 로고    scopus 로고
    • NSS 1740.14, August 95
    • NASA Safety Standard: Guidelines and Assessment Procedures for Limiting Orbital Debris. (NSS 1740.14, August 95).
  • 5
    • 84963916165 scopus 로고    scopus 로고
    • March 31-April 6
    • Space News, March 31-April 6, 1997, p 16.
    • (1997)
  • 6
    • 84963906165 scopus 로고    scopus 로고
    • Aug 4-10
    • Space News, Aug 4-10, 1997, p 30.
    • (1997)
  • 7
    • 84963814979 scopus 로고    scopus 로고
    • restes@mars.harvard.edu, personal communication via email Friday 31 May, 10:39:16
    • Estes, R., restes@mars.harvard.edu, personal communication via email Friday 31 May 1996 10:39:16.
    • (1996)
    • Estes, R.1
  • 8
    • 84963870027 scopus 로고    scopus 로고
    • JLoftus@ems.jsc.nasa.gov, personal communication via email Wednesday 19 June, 08:20:39
    • Loftus, JP. JLoftus@ems.jsc.nasa.gov, personal communication via email Wednesday 19 June 1996 08:20:39.
    • (1996)
    • Loftus, J.P.1
  • 13
    • 84963924620 scopus 로고    scopus 로고
    • Appendix E of High Strength-To-Weight Tapered Hoytether for LEO to GEO Payload Transport, Final Report on NASA Contract NAS8-40690,10 July
    • Hoyt, RP., Forward, R.L., “Electrodynamic Hoytethers for ISS and LEO Spacecraft”, Appendix E of High Strength-To-Weight Tapered Hoytether for LEO to GEO Payload Transport, Final Report on NASA Contract NAS8-40690,10 July 1996.
    • (1996) Electrodynamic Hoytethers for ISS and LEO Spacecraft
    • Hoyt, R.P.1    Forward, R.L.2
  • 14
    • 84963870059 scopus 로고    scopus 로고
    • Note that in Eq. 9, vM=vo~®E'r cosA, between the orbiting spacecraft and the geomagnetic field, since the geomagnetic field rotates with the Earth at the rate of ooE=27t rad/day. For an equatorial orbit at an altitude of 1000 km, the velocity of the geomagnetic field is 0.536 km/s or only 7% of the orbital velocity of 7350 m/s. For nonequatorial orbits the difference is even smaller. We will ignore this small difference to keep the equations manageable
    • Note that in Eq. 9, the correct velocity vector to use is the relative velocity vM=vo~®E'r cosA, between the orbiting spacecraft and the geomagnetic field, since the geomagnetic field rotates with the Earth at the rate of ooE=27t rad/day. For an equatorial orbit at an altitude of 1000 km, the velocity of the geomagnetic field is 0.536 km/s or only 7% of the orbital velocity of 7350 m/s. For nonequatorial orbits the difference is even smaller. We will ignore this small difference to keep the equations manageable.
  • 15
    • 84963924626 scopus 로고    scopus 로고
    • the transverse magnetic field Bj and therefore voltage V given by Eq. 11 are both essentially constant over the entire orbit, despite the fact that the horizontal magnetic field varies from a maximum at the magnetic equator Bff(A=0) to a smaller value of Bff(A=A,) at the northernmost portion of an orbit with geomagnetic inclination A,. The variation in horizontal magnetic field strength Bfj(A) with latitude A on the Earth and the variation in the angle at which the velocity vector crosses BN, combine to produce a constant transverse magnetic field BT=Bff(A=X) over the entire orbit
    • By a geometric coincidence, the transverse magnetic field Bj and therefore voltage V given by Eq. 11 are both essentially constant over the entire orbit, despite the fact that the horizontal magnetic field varies from a maximum at the magnetic equator Bff(A=0) to a smaller value of Bff(A=A,) at the northernmost portion of an orbit with geomagnetic inclination A,. The variation in horizontal magnetic field strength Bfj(A) with latitude A on the Earth and the variation in the angle at which the velocity vector crosses BN, combine to produce a constant transverse magnetic field BT=Bff(A=X) over the entire orbit.
  • 17
    • 84963859571 scopus 로고    scopus 로고
    • The results for orbits with i>78.5, the deorbit times will be roughly twice as long, due to portions of the day when the orbit is retrograde to the magnetic dipole
    • The results for orbits with i>78.5 assume that the tether system can carry current in both directions; if the tether system is designed to carry current in one direction only, the deorbit times will be roughly twice as long, due to portions of the day when the orbit is retrograde to the magnetic dipole.
  • 18
    • 84963832511 scopus 로고
    • Tethers In Space Handbook, 2nd Edition, NASA/OSF
    • Penzo, P.A., and Ammann, P.W., eds., Tethers In Space Handbook, 2nd Edition, NASA/OSF, 1989, p. 168-9.
    • (1989) , pp. 168-169
    • Penzo, P.A.1    Ammann, P.W.2
  • 19
    • 0003039607 scopus 로고    scopus 로고
    • The Hoytether: A Failsafe Multiline Space Tether Structure
    • Huntsville, AL, Sept 9-10
    • Hoyt, RP., Forward, R.L., “The Hoytether: A Failsafe Multiline Space Tether Structure,” Tether Technical interchange Meeting, Huntsville, AL, Sept 9-10, 1997.
    • (1997) Tether Technical Interchange Meeting
    • Hoyt, R.P.1    Forward, R.L.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.