ITU-R P 844-1-1994 Ionospheric Factors Affecting Frequency Sharing in the VHF and UHF Bands (30 MHz-3 GHz)《在VHF和UHF频段内(30MHz-3GHz)影响频率共享的电离层因素》.pdf

《ITU-R P 844-1-1994 Ionospheric Factors Affecting Frequency Sharing in the VHF and UHF Bands (30 MHz-3 GHz)《在VHF和UHF频段内(30MHz-3GHz)影响频率共享的电离层因素》.pdf》由会员分享，可在线阅读，更多相关《ITU-R P 844-1-1994 Ionospheric Factors Affecting Frequency Sharing in the VHF and UHF Bands (30 MHz-3 GHz)《在VHF和UHF频段内(30MHz-3GHz)影响频率共享的电离层因素》.pdf（6页珍藏版）》请在麦多课文档分享上搜索。

1、 Rec. ITU-R P.844-1 1 RECOMMENDATION ITU-R P.844-1*IONOSPHERIC FACTORS AFFECTING FREQUENCY SHARING IN THE VHF AND UHF BANDS (30 MHz-3 GHz) (Question ITU-R 218/3) (1992-1994) Rec. ITU-R PI.844-1 The ITU Radiocommunication Assembly, considering a) that the ionosphere, while primarily responsible for r

2、eflection of radio waves below approximately 30 MHz, is capable of supporting propagation in the VHF (30-300 MHz) band under some conditions, during relatively short periods of time, and in certain areas of the world; b) that propagation mechanisms which exist for relatively short periods of time sh

3、ould be taken into consideration when planning radio systems which share frequencies; c) that frequency sharing is important in the efficient use of the radio spectrum, recommends that the following information be taken into account when planning radio systems which make use of frequency sharing in

4、the VHF and UHF bands (30 MHz-3 GHz). 1. Terrestrial propagation 1.1 Introduction Radio propagation at VHF is mainly controlled by physical objects, such as terrain and ground cover (clutter), and tropospheric factors, principally refraction. However, at VHF, ionospheric propagation over long distan

5、ces can take place with relatively small losses. Such propagation events may be significant in causing interference at VHF, particularly for systems requiring high reliability. 1.2 Summary of potential ionospheric interference mechanisms Table 1 provides a summary of ionospheric propagation mechanis

6、ms which may be significant causes of interference at VHF. Further information on the more important mechanisms is given in the following sections. 1.3 Normal F-region propagation Near the peak of the solar cycle long-distance propagation via the F2 layer can occur for a significant fraction of the

7、time at frequencies above 30 MHz. This effect extends to 70 MHz at low latitudes. Figures 1, 2 and 3 show, for a path length of 4 000 km, values of the MUF exceeded for 1% of hours for three seasons at sunspot maximum. 1.4 Trans-equatorial propagation (TEP) Strong transmission can occur, particularl

8、y during high sunspot years, over long North-South paths spanning the geomagnetic equator. There appear to be two types of trans-equatorial propagation characterized by the times of peak occurrence, fading characteristics and modes of propagation. _ *Radiocommunication Study Group 3 made editorial a

9、mendments to this Recommendation in 2000 in accordance with Resolution ITU-R 44. 2 Rec. ITU-RP.844-1TABLE 1 Main causes of ionospheric interference to stations working at frequencies between 30 and 300 MHz Cause of interference Latitude zone Period of severe interference Approximate highest frequenc

10、y with severe interference (MHz) Approximate frequency above which interference is negligible (MHz) Approximate range of distances affected (km) Principal distinguishing features Regular F-layer reflections Mid Day, equinox and winter, solar-cycle maximum 50 60 E-W paths3 000-6 000 or Occurrence bro

11、adly in accordance with regular-layer morphology Low Afternoon to late evening, solar-cycle maximum 60 70 N-S paths 3 000-10 000 High Night 70 90 500-4 000 Principally during summer months in mid latitudes. Sudden onset and conclusion, beginning later and ending earlier with increase of operating fr

12、equency. Area concerned Sporadic-E reflections Mid Day and evening, summer 60 83-135 (1)relatively small and mobile. Duration minutes or hours. No associated signal enhancements at short range Low Day 60 90 Sporadic-E scatter Low Evening to midnight 60 90 Up to 2 000 (1) For 0.1% of the time during

13、the hours 0800-2300 LT for May to August (111 min total) the following frequencies may be derived from Annex 1 to Recommendation ITU-R P.534 for a distance of 1 800 km and = 30 dB for temperate zone: Region A (Europe and North Africa): 083 MHz Region B (North America): 093 MHz Region C (Asia): 135 M

14、Hz Region D (Average for Northern Hemisphere): 115 MHzRec. ITU-RP.844-13TABLE 1 (continued) Cause of interference Latitude zone Period of severe interference Approximate highest frequency with severe interference (MHz) Approximate frequency above which interference is negligible (MHz) Approximate ra

15、nge of distances affected (km) Principal distinguishing features Reflections from meteoric ionization All Particularly during showers May be important anywhere in the range Up to 2 000 Signal bursts with durations from a fraction of a second to several minutes. Marked diurnal variation, maximum 0600

16、 h local time, minimum 1800 h. Some activity present at all times, but considerable increases during predictable shower periods Reflections from magnetic field aligned columns of auroral ionization High Late afternoon and night Associated with geomagnetic disturbances, typically when local K-index r

17、eaches 5 or more. Characteristic rasping note due to multiple Doppler shifting. Normal duration a few hours, often afternoon to midnight. Scattering in the F region Low Evening to midnight, equinox 60 80 1 000-4 000 Special transequatorial effects Low Evening to midnight 60 80 4 000-9 000 Paths gene

18、rally aligned symmetrically across the dip equator. Generally around equinoctial periods with regular occurrences. Strong signals. Refer to main text for further details. 4 Rec. ITU-R P.844-1 D01-scFIGURE 1 PI.844-1 D01 The first type of TEP, which is called the afternoon type, has the characteristi

19、cs: a peak occurrence around 1700-1900 h LMT, the time being measured at the point where the circuit cuts the magnetic equator; normally strong steady signals with a low fading rate and a small Doppler spread (about 2-4 Hz); path lengths of about 6 000-9 000 km and sometimes longer. The second type

20、of TEP, which is called the evening type, generally supports higher frequencies than the afternoon type and has very different characteristics: a peak occurrence around 2000-2300 h LMT; high signal strengths but with deep and rapid fading at rates up to about 15 Hz and a large Doppler spread which s

21、ometimes exceeds 40 Hz; path lengths usually shorter than for the afternoon-type mode, being about 3 000-6 000 km. Rec. ITU-R P.844-1 5 D02-scFIGURE 2 PI.844-1 D02 1.5 Sporadic-E propagation Sporadic-E ionization appears as an intensification in ionization in the form of a horizontal sheet of about

22、1 km average thickness and a horizontal dimension of the order of 100 km. The height is commonly 100 to 120 km. Such sporadic-E layers can cause abnormal VHF propagation for periods lasting for several hours. The occurrence of sporadic-E propagation decreases with increasing frequency, but can be a

23、significant cause of interference at frequencies up to about 135 MHz. Recommendation ITU-R P.534 provides a method for calculating sporadic-E field strengths and probability of occurrence. 1.6 Meteor-trail ionization Scattering from ionization due to meteor-trails can produce VHF interference over r

24、anges up to approximately 2 000 km. Although individual meteor trails remain effective for periods measured in seconds, meteor bursts can support continuous or near-continuous propagation for much longer periods of time. The effect of meteor trails on VHF propagation shows spatial, diurnal and seaso

25、nal variations. Further information may be found in Recommendation ITU-R P.843. 6 Rec. ITU-R P.844-1 D03-scFIGURE 3 PI.844-1 D03 1.7 Auroral ionization Field-aligned irregularities in the auroral zones appear during magnetically disturbed periods. Such ionization can produce significant reflections

26、causing propagation which is normally off the great-circle path. This may cause interference at VHF, mainly in mid to high geomagnetic latitudes. 2. Earth-space propagation Radio propagation at VHF and UHF on Earth-space paths through the ionosphere is subject to attenuation, polarization rotation,

27、amplitude and phase scintillation and ray-path bending. These effects may influence the extent of frequency sharing for satellite services and between satellite and terrestrial services. For orbiting satellite systems the effect of time and location variations of irregularities in the ionosphere may be important, notably in equatorial and auroral regions.