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Worst cases for a one-hop high frequency link

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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Worst cases for a one-hop high frequency link

Author: Miró Amarante, Gloria; Morena Carretero, Benito A de la; Radicella, Sandro María; Herraiz, Miguel
Publisher: Istituto Nazionale di Geofisica e Vulcanologia (INGV)
Year: 2002
DOI: 10.4401/ag-3497
Source: https://idus.us.es/bitstreams/540cb1f6-7d9c-4042-b3f2-b71bc26c3e7b/download
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).
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