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Worst cases for a one-hop high frequency link

Miró Amarante, Gloria; Morena Carretero, Benito A de la; Radicella, Sandro María; Herraiz, Miguel

Abstract

The characterisation of a HF channel by means of monthly electron density profiles can be complemented with a detailed study of radio propagation «worst cases» on situations with extremes conditions of radiopropagation for a given period. These «worst cases» correspond to conditions that can be identified by means of cumulative distributions of the key parameter f0F2. This paper analyses the main parameters of the HF channel: time delay, apogee, elevation angle and transmission frequency with mean and extreme conditions. The method used to characterise the ionospheric channel is based on ray-tracing techniques.

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ANNALS OF GEOPHYSICS, VOL. 45, N. 1, Feb ua y 2002 201 Sho No e Wo s cases o a one-hop high equency link Glo ia Mi ó (1), Beni o A. de la Mo ena (1), Sand o Ma ia Radicella (2)and Miguel He aiz (3) (1) A mosphe ic Sounding S a ion «El A enosillo»,Na ional Ins i u e o Ae ospace Technology, Magazón,Huel a,Spain (2) Ae onomy and Radiop opaga ion Labo a o y,Abdus Salam ICTP,T ies e,I aly (3) Depa men o Geophysics and Me eo ology,Facul y o Physics,Complu ense Uni e si y,Mad id,Spain Abs ac The cha ac e isa ion o a HF channel by means o mon hly elec on densi y p o iles can be complemen ed wi h a de ailed s udy o adio p opaga ion «wo s cases» on si ua ions wi h ex emes condi ions o adiop opaga ion o a gi en pe iod. These «wo s cases» co espond o condi ions ha can be iden i ied by means o cumula i e dis ibu ions o he key pa ame e 0F2. This pape analyses he main pa ame e s o he HF channel: ime delay, apogee, ele a ion angle and ansmission equency wi h mean and ex eme condi ions. The me hod used o cha ac e ise he ionosphe ic channel is based on ay- acing echniques. 1. In oduc ion An HF communica ion link is cha ac e ised by he Maximum Usable F equency ha is he limi abo e which he signal will no be e lec ed by he ionosphe e unde medium condi ions. Howe e , i is con enien o s udy all possible condi ions. Fo his eason, an analysis o wo s cases aimed a ex ending he esul s ob ained by means o mon hly median condi ions o ex eme ionosphe ic si ua ions. The concep o wo s cases was in oduced in ay acing echniques (Mi ó e al., 2000) o ex end he channel cha ac e isa ion o ex eme ionosphe ic si ua ions a om median condi ions o HF links. Wo s cases selec ion was pe o med using 0F2 h ough hou ly cumula i e equency dis ibu ions. The 2D ay acing echnique used (called abc ay03), is based on he exp essions in oduced by C o and Hoogasian (1968) and C o (1969) and i has been conside ed in p e ious ionosphe ic s udies (Moo head and Radicella, 1998; Mi ó, 2000). The ou pu s ob ained wi h his compu ing echnique a e he main adio p opaga ion pa ame e s: ime delay o he signal a elling om he ansmi e o he ecei e , e lec ion heigh o apogee, ele a ion angle and ansmission equency. Mailing add ess: D . Glo ia Mi ó, A mosphe ic Sounding S a ion «El A enosillo», Na ional Ins i u e o Ae ospace Tech- nology, 21130 Magazón, Huel a, Spain; e-mail: mi [email p o ec ed] Key wo ds ionosphe e − adio p opaga ion − wo s cases − ay- acing 202 Glo ia Mi ó, Beni o A. de la Mo ena, Sand o Ma ia Radicella and Miguel He aiz A pa icula ionosphe ic condi ion is in oduce in he ay acing p og am using model o expe- imen al elec on densi y p o iles. 2. Da a As p e iously indica ed, he pa ame e 0F2 was used o pe o m he wo s cases selec ion h ough hou ly cumula i e equency dis i- bu ions. This s udy conside ed hou ly e ised 0F2 alues om he digisonde DGS256 si ua ed a El A enosillo A mosphe ic S a ion and he 1993- 1997 pe iod. An a e age o 1826 alues was a ailable o each 24 h and cu -o equencies limi ing 1% o hese alues wi h ei he he lowes o he highes equencies ha e been chosen as wo s cases condi ions. Fo example, a 00 UT hou s 1% o cases had 0F2 lowe han 2.4 MHz and highe han 7.3 MHz. Once he wo s cases selec ion has been done, he co esponding elec on densi y p o iles a e in oduced in he ay acing echnique. 3. Me hodology A each hou , p o iles belonging o hese uppe /lowe condi ions a e g ouped o calcula e a mean uppe /lowe ex eme p o ile. This p o- Fig. 1. Hou ly mon hly elec on densi y p o iles and he co esponding o uppe and lowe selec ion a El A enosillo A mosphe ic Sounding S a ion. 203 Wo s cases o a one-hop high equency link cedu e p o ides h ee mean p o iles pe hou : uppe ex eme, lowe ex eme and hou ly mean p o ile o all cases. These mean p o iles we e ob ained ollowing he me hodology desc ibed in Huang and Reinisch (1996). Figu e 1 shows an example o such p o iles. As has been no ed, he ionosphe ic condi ions in he e lec ion poin necessa y o cha ac e ise he HF channel a e in oduced by elec on densi y p o iles. I is impo an o poin ou ha he p o iles ob ained a e he wo s case selec ion belong o one o he link ex emes, El A enosillo S a ion. Howe e , he pa icula link be ween El A enosillo and Eb o Obse a o io is si ua ed a Fig. 2. Oblique ionog ams ob ained by abc ay03 p og am co esponding o uppe , lowe and mean condi- ions. midla i udes. The e o e, communica ions wi h a ange close o 785 km co espond o one iono- sphe ic hop wi h E (E mode) o F (Fmode). Mo eo e , he ionosphe ic condi ions a he e lec ion poin which is loca ed a ound he mid- dle poin in his speci ic link, can be app oxima e o da a om one o he ex emes, ansmi e o ecei e (Mi ó, 2000). Using he h ee mean p o iles a each hou ( ig. 1), ionosphe ic condi ions a e in oduced in he abc ay03 p og am o de i e a each 24 h he adio p opaga ion pa ame e s: ansmis- sion equencies, ele a ion angles, ime delays and apogees unde ex eme and s anda d si ua ions. 204 Glo ia Mi ó, Beni o A. de la Mo ena, Sand o Ma ia Radicella and Miguel He aiz 4. Resul s The dis ibu ion o he g oup pa h P’ (p o- po ional o ime delay) e sus he ansmission equency gi es wha is known as an oblique ionog am. Figu e 2 displays syn he ic oblique ionog ams ob ained wi h he ay acing echni- que co esponding o some o he 24 h s udied. Di e ences be ween he h ee condi ions (uppe ex eme, lowe ex eme and mean) can be clea ly seen mainly a F2 heigh s. F om he HF communica ion sys ems poin o iew, he main p oblem is o ind ou he ex- is ence o low 0F2 on low elec on densi y a- lues. This si ua ion is c i ical because his phenom- enon educes he Maximum Usable F equency and he communica ion equency band becomes na owe han ha om mean and uppe condi- ions ( ig. 2). Fo his eason, special a en ion has been paid o he numbe o cases in which he signal a i es a he ecei e in spi e o he na owing o he equency ange o igina ed by low elec on densi y condi ions. Resul s a e summa ised in able I. As can be seen, only dayligh s hou s (8:00 UT - 18:00 UT) p o ide an accep able pe cen age o si ua ions in which a link is es ablished unde all condi ions. As expec ed, mos o hese signals belong o E modes ha do no appea du ing he es o he hou s. In gene al, i he daily ansmission is done wi h a equency be ween 6 and 8 MHz, he signal will each he ecei e unde ex emes and mean si ua ions. This s udy indica es ha he cha ac e isa ion ob ained using ionosphe ic mean condi ions can be applied in mos si ua ions. Only some cases Table I. Numbe o lowe condi ions cases which a i e a he ecei e . Hou (UT) To al Lowe % E Mode % E Mode F Mode % F Mode 0:00 4 1 25 0 0 1 100 1:00 3 1 33 0 0 1 100 2:00 4 1 25 0 0 1 100 3:00 4 1 25 0 0 1 100 4:00 4 1 25 0 0 1 100 5:00 7 1 14 0 0 1 100 6:00 7 0 0 0000 7:00 16 2 13 1 50 1 50 8:00 23 15 65 11 73 4 27 9:00 24 18 75 13 72 5 28 10:00 26 20 77 17 85 3 15 11:00 28 19 68 17 89 2 11 12:00 30 21 70 16 76 5 24 13:00 28 20 71 17 85 3 15 14:00 27 20 74 16 80 4 20 15:00 27 18 67 15 83 3 17 16:00 28 16 57 11 69 5 31 17:00 27 12 44 5 42 7 58 18:00 24 6 25 2 33 4 67 19:00 19 2 11 0 0 2 100 20:00 15 2 13 0 0 2 100 21:00 11 2 18 0 0 2 100 22:00 6 1 17 0 0 1 100 23:00 6 1 17 0 0 1 100 205 Wo s cases o a one-hop high equency link du ing nigh hou s can p esen p oblems i he ansmission equency used is nea he Maxi-mum Usable F equency because in hese condi ions, he signal will no be e lec ed by he low ionosphe ic elec on densi y p esen in i s ay pa h. 5. Conclusions The main conclusion eached in his pape can be summa ised as ollows: – In gene al, he cha ac e isa ion ob ained by means o mon hly elec on densi y p o iles (Mi ó, 2000) could be applied e en wi h ex eme ionosphe ic condi ions. The main p oblem can appea du ing nigh ime o ansmission equencies close o he Maximum Usable F equency. Acknowledgemen s The au ho s a e g a e ul o D . Moo head o Nep une Rada L d., Glouces e U.K., o his help in unde s anding he ay acing echnique, abc ay03. This wo k has been possible hanks o inancial suppo g an ed by he Na ional Ins i u e o Ae ospace Technology (INTA). REFERENCES C ROFT , T.A. (1969): Me hods and applica ions o compu e ay acing, S an o d Elec onics Labs Tech., Repo . SU- SEL- 69-007. C ROFT , T.A. and H. H OOGASIAN (1968): Exac ay calcula ions in a quasipa abolic ionosphe e, Radio Sci., 3, 69-74. H UANG , X. and B.W. R EINISCH (1996): Ve ical elec on densi y p o iles om digisonde ionog ams - he a e age ep esen a i e p o ile, Ann. 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