keplerian element
Short Description
gps keplerian element orbit calculation...
Description
GPS SATELLITE ORBIT COMPUTATION INTRODUCTION OF KEPLER’S LAWS The orbit of each planet is an ellipse with the Sn at one focs! The line "oinin# the planet to the sn sweeps ot e$al areas in e$al ti%es an&' the s$are of the perio& of a planet is proportional to the cbe of its %ean &istance to the sn! Orbit of the satellite is (nown as Keplerian, as Keplerian, i!e! orbit is an ellipse with earth at one of the foci' where) Ass%ptions are) * Earth is a point %ass or e$i+alentl, a sphere with nifor% &ensit, so the attraction is towar& center * Mass of the satellite is ne#li#ible * Satellite %o+es in a +ac% E-ceptions) * Gra+it, fiel& +ariation' attraction of sn' %oon an& other planets * At%ospheric &ra# an& solar ra&iation pressre * Relati+istic effects etc!
.i#re / ) Coor&inate s,ste% in the orbital plane!
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KEPLERIAN ELEMENT
There are 0 t,pes of ele%ents in &eter%inin# the orbit! It is calle& the satellite orbital ele%ent (nown as 1eplerian Ele%ent 2na%e& after 3ohann 1epler 2/45/6/0789! In the 1eplerian' satellite orbitin# the ellipse is the shape an& orientation of the e$ip%ent! The Earth is at one focs of the ellipse an& not in the %i&&le 2bt when the elliptical orbit is a co%plete circle9!
A normal orbit is co%pletel, #i+en b, the followin# (eplerian orbital ele%ents' see fi#res /9 :9 79 s orbit an& e$ator! Elliptical orbit is a flat area (nown as the orbital plane! This habit orbital plane thro#h &irectl, into the center of the earth bt will sli#htl, tilt at an, an#le relati+e to the e$ator! Inclination is the an#le between the orbital plane an& the e$atorial plane! Nor%all,' the inclination is a n%ber between 8 an& /?8 &e#rees! .or orbit with inclination close to 8 is calle& the e$atorial orbit 2this is becase the satellite passe& o+er the north an& soth poles9! Crossin# the e$atorial plane an& the orbital plane is a line calle& the line of no&es!
.i#re 7) inclination
7! E""e!$ri"i$% ( e In the 1eplerian orbit %o&el' the satellite orbit is elliptical! Eccentricit, is %ore abot the shape of an ellipse! @hen the +ale of e ; 8' the ellipse is a circle! @hen the +ale of e approaches /' the ellipse will be a +er, lon# an& thin!
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.i#re < ) eccentricit, an& %a"or a-is
Line of no&es> can co%e at an, point alon# the e$ator! If it is fon& at the e$ator where the >line of no&es> co%e off' then the orbital plane can be specifie&! Ar#abl,' it #oin# off at : locations' so we onl, nee& to specif, one onl,! One of the calle& as >ascen&in# no&es> where the satellite will cross the e$ator fro% soth to north! .or the other' it is calle& as >&escen&in# no&e> where the satellite will cross the e$ator fro% north to soth! Nor%all,' the >ascen&in# no&es> will be specifie&! If the earth in a state of spin' this %eans we cannot se the sal %etho& of latit&e or lon#it&e coor&inate s,ste% to specif, the location of the >line of no&es! Con+ersel,' we can also se an astrono%ical coor&inate s,ste%' (nown also as the ri#ht ascension &eclination where it &oes not rotates with the earth! >Ri#ht ascension of ascen&in# no&e> is the an#le' %easre& fro% the %i&point of the earth' fro% the >+ernal e$ino-> to the ascen&in# no&e!
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.i#re 4 ) Lon#it&e of ascen&in# no&e
4! Ar&'me!$ o) Perigee ( ω Also (nown as the Ar#%ent of Periapsis! In a&&ition' it is preferable to specif, a corner! The point where the satellite is closer to the earth is calle& peri#ee' or also calle& periapsis! @hile the farthest point fro% the earth is calle& apo#ee! @hen we &raw a line fro% peri#ee to apo#ee' this line is calle& the line of apsi&es! Line of apsi&es thro#h the center of the earth an& another line thro#h the center of the earth' as it is (nown the line of no&es! The an#le between two lines is (nown as ar#%ent of peri#ee! @hen two lines intersect' the, for% two a&&itional an#les! To %ore clearl,' we can sa, that ar#%ent of peri#ee is the an#le of the ascen&in# no&e to the peri#ee!
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.i#re 0 ) Ar#%ent of Perigee
0! Mea! a!oma#% ( M or ( v Mean ano%al, is an an#le that %o+es nifor%l, in ti%e fro% 8 to 708 &e#rees in the rotation! This &efines that 8 &e#rees is at peri#ee an& apo#ee of /?8 &e#rees! Mean no%al, is a pre %athe%atical $antit, #i+en below b, 1eplers e$ation)
M ; E 6 e sin E
If the satellite is in a circlar orbit 2%o+in# at a constant spee&9 an& +iewe& on the center of the earth an& %easrin# the an#le fro% peri#ee' this will be reflecte& towar&s the satellite! Satellite in orbit is not a circle that %o+es at the spee& of ne+en' then the relationship will not last! This relationship will re%ain for : %ain point in orbit' howe+er' re#ar&less of eccentricit,! Usall, the peri#ee will appear on the Mean Ano%al, ; 8' an& apo#ee also appeare& in Mean Ano%al, ; /?8 &e#rees!
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COMPUTATION OF SATELLITE POSITIONIN+ IN OR,IT USIN+ KEPLERIAN ELEMENT
The position of the satellite %st be correcte& for the e-traneos effects state& earlier! Satellite ephe%eris "st as solar or star ephe%eris li(e an Al%anac' it contain infor%ation abot the location of a satellite at an, #i+en ti%e! As the orbit of a satellite is not $ite 1eplerian' its location can onl, be pre&icte& fro% the infor%ation collecte& b, trac(in# its orbit constantl,! In the case of positionin# satellites' ephe%eris infor%ation consists of 1eplerian para%eters at a certain epoch' rate of chan#e of these ele%ents' cloc( infor%ation an& cloc( correction ter%s! Accrate ephe%eris infor%ation is re$ire& for locatin# precise positions on earth sin# the si#nals fro% satellites .or this reason' all positionin# satellites incl&e ephe%eris infor%ation in its si#nal sent to earth
Satellite Coor&inates Co%ptation!
Table / pro+i&es the GPS or Galileo broa&cast ephe%eris para%eters to co%pte their satellite coor&inates at an, obser+ation epoch! These para%eters are perio&icall, renewe& 2t,picall, e+er,
hors for GPS an&
hors for Galileo9 an& %st not be se& ot of the prescribe& ti%e
2abot for hors9' becase the e-trapolation error #rows e-ponentiall, be,on& its +ali&it, perio&! The al#orith% pro+i&e& is fro% the GPSSPS6SS! The Galileo satellites follow a si%ilar sche%e
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Table /) Ephe%eris Para%eters
In or&er to co%pte satellite coor&inates fro% na+i#ation %essa#e' the al#orith% pro+i&e& as follows %st be se&! An accrac, of abot
%eters 2RMS9 is achie+e& for GPS satellites with
SA;8ff an& se+eral tens of %eters with SA;on!
Co%pte the ti%e
fro% the ephe%eri&es reference epoch
2 an&
are e-presse& in
secon&s in the GPS wee(9)
If
sec' sbtract
sec fro% ! If
sec' a&&
sec!
•
Co%pte the %ean ano%al, for
' 8
•
Sol+e 2iterati+el,9 the 1epler e$ation for the eccentricit, ano%al,
•
Co%pte the tre ano%al,
•
Co%pte the ar#%ent of latit&e an& corrections
an&
)
Co%pte the ra&ial &istance
•
Co%pte the inclination
•
fro% the ar#%ent of peri#ee
' tre ano%al,
)
•
' an& corrections
)
' consi&erin# corrections
an&
)
of the orbital plane fro% the inclination an&
at reference ti%e
)
Co%pte the lon#it&e of the ascen&in# no&e
2with respect to Greenwich9! This
calclation ses the ri#ht ascension at the be#innin# of the crrent wee( 2
9' the
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correction fro% the apparent si&ereal ti%e +ariation in Greenwich between the be#innin# of the wee( an& reference ti%e ascen&in# no&e fro% the reference ti%e
' an& the chan#e in lon#it&e of the )
•
Co%pte the coor&inates in TRS fra%e' appl,in# three rotations 2aron&
•
@here
an&
'
an&
9)
are the rotation %atrices &efine& in Transfor%ation between
Terrestrial .ra%es!
Transfor%ation between Terrestrial .ra%es •
.ro% ele%ental linear al#ebra' all transfor%ations between two Cartesian coor&inate s,ste%s can be &eco%pose& in a shift +ector consecti+e rotations aron& the coor&inate a-es 2 '
' three '
9' an& a scale factor 2 9! That
is' the, can be &escribe& b, the followin# e$ation' which in+ol+es 5 para%eters)
where)
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•
A&optin# the con+ention se& b, IERS' the pre+ios e$ation 2/9 can be written as follows)
•
@here an&
'
'
are three translation para%eters'
is a scale factor an&
'
are three rotation an#les!
Referrin# to Transfor%ation para%eters fro% ITR.:888 to past ITR.s are liste& in table
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