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Beyond-line-of-sight communications in a satellite-denied/degraded environmentMichael J. Ryan

Options for BLOS communications

Radio communications techniques are normally categorized in accordance with the propagation mechanism employed for the transmission of radio-frequency energy. The following sections provide a very brief description of those mechanisms, focusing on those that are useful for RF BLOS communication. 3

Ground waves

As illustrated in Figure 1, some of the RF energy radiated by an antenna will travel directly (provided it is within line-of-sight) to the receiving antenna in what are called direct waves. A further portion of the energy will be directed towards the ground, be reflected, and then received by the antenna—these are called ground-reflected waves. The combination of the direct and the ground-reflected waves is called space waves. In addition, some of the energy is propagated by surface waves and the combination of space waves and surface waves are called ground waves.

Figure 1
Figure 1: Ground waves comprises space waves (direct and ground-reflected) and surface waves

Space-wave propagation travels line-of-sight so, while there must be sufficient strength signal at the receiver for the link to work, most ground-based radio systems are terrain-limited rather than power-limited.4 That is, the curvature of the Earth constrains the extent of the line-of-sight between two low antennas regardless of how much power is used. For example, for two portable radios held waist-high (around 1 meter above ground level), the radio horizon is approximately 8 kilometers on flat terrain, even though the radios will have sufficient power to operate over tens of kilometers in free space.

If a 9-metre mast is used for the antennas for each radio, the radio horizon is extended to nearly 25 kilometers. Extended further, an aircraft at 10,000 ft would have a radio horizon of 200 kilometers to a ground terminal. Consequently, the only solutions to long-range, space-wave communication are to elevate the one or both antennas, or to place a repeater between the terminals, or both. As discussed in the following sections, the repeater is also often elevated to a convenient hill top or tower, to an airborne platform, or to a space-borne platform.

Surface waves, as the name implies, travel along the surface of the ground supported by currents flowing in the ground—the wavefront is supported between the Earth’s surface and the ionosphere. The attenuation (and therefore the range) of the wave is frequency-dependent, so that surface waves require very low frequencies which have very low bandwidths and require large antennas. Very-low frequency (VLF) surface-wave propagation can support communications around the world but such systems have very large antennas, and the small bandwidths available only allow very low data rates of a few bits per second. Low-frequency (LF) and medium-frequency (MF) broadcasting also makes use of surface waves but the ranges are small—300 kilometers for LF and 100 kilometers for MF. Given the very short ranges of HF surface-wave propagation, the mechanism is not useful for long-range communication and is not considered further here.

Sky waves

As illustrated in Figure 2, sky-wave communication utilizes the ionosphere to refract waves back to Earth, providing a mechanism for propagating over very long distances.5 The refraction mechanism is frequency dependent with the available frequencies depending on the state of the ionosphere. In general, the sky-wave window is from 2-30 MHz, with the higher frequencies only being available during periods of high solar activity. The communication range of sky waves depends on three main factors: the frequency used, the angle of transmission, and the power of the transmitter.

Figure 2
Figure 2: Sky waves refract from an ionospheric layer to produce long-range, over-the-horizon communications

As illustrated in Figure 3, a higher frequency is refracted by a higher layer of the ionosphere, leading to longer ranges. Single-hop HF sky waves have ranges (skip distances) between approximately 100 kilometers (using the lower E layer of the ionosphere) and 3,500 kilometers (using the F layer). Consequently, unlike all other forms of radio communication, HF range is chosen by selecting an appropriate frequency—the higher the frequency, the higher the layer of refraction, the longer the range. At the higher extremity of the sky-wave window, the wave will no longer be totally internally refracted and will pass on out into space. It should also be noted that there is a minimum skip distance dictated by the highest angle of transmission possible from the antenna—the range is often referred to as the skip zone or the dead zone. Further, the ionosphere suffers from considerable variation in its intensity over the day, through the seasons and across years—selection and use of an appropriate frequency therefore requires considerable management.

Figure 3
Figure 3: HF sky-wave communications ranges affected by increasing frequency, propagation angle and power

Figure 3 also illustrates that the same ionospheric layer can be used to achieve longer ranges by lowering the angle of elevation at the same frequency. Additionally, the range of the transmission can be increased with higher power, to allow multiple hops of the transmission.

Scattered waves

Scattered-wave techniques make use of turbulence in the troposphere (troposcatter)—illustrated in Figure 4—or ionosphere (ionospheric scatter), or a result of ionized meteor tails (meteor burst). Ionospheric scatter and meteor-burst techniques have very low data rates (a few tens of bits per second) and are rarely used. Troposcatter techniques are, however, used in both commercial and military networks.6

Figure 4
Figure 4: In troposcatter energy is scattered from turbulence in the troposphere to produce over-the-horizon communication

Troposcatter paths vary in length from about 100-150 kilometers to over 2000 kilometers. The maximum path attenuation including deep fades is very high, requiring the use of high-transmitted powers; low-noise sensitive receivers; and high-gain parabolic antennas. Antennas are parabolic, with diameters ranging from a few meters to tens of meters. Frequencies used are between 300 MHz and 5 GHz.

Although troposcatter communications have traditionally required large antennas and expensive receivers, they have provided very important backbones for telecommunications networks, spanning distances over which radio relay was not possible. With the advent of relatively cheaper satellite communications systems, troposcatter links have been replaced by satellite links for most BLOS applications.

However, modern technologies in the form of digital signal processing and phased-array antennas are greatly easing the previous difficulties of troposcatter, which is included in these discussions because the next decade will see a significant resurgence in the use of troposcatter systems. 7

BLOS range extension through repeaters

High-capacity communications require high-channel bandwidths, which require the employment of high frequencies. Unfortunately, frequencies above 30 MHz propagate via space wave, which is limited to line-of-sight. As mentioned earlier, the only solutions, therefore, to long-range space-wave communication are to elevate the two antennas, or to place a repeater between the terminals, or both. There are three principal repeater-based systems:

The range-capacity-mobility trade-off

Utilizing one of the radio-frequency propagation mechanisms, the communications systems discussed in the previous section provide ranges that vary from several hundred to thousands of kilometers, with capacities from hundreds of bits per second to hundreds of gigabits per second, and with degrees of mobility varying from small systems that are operable on-the-move to large fixed installations.

As a vehicle for considering the utility of any given system, it is useful to note that an ideal communications system has three principal attributes: long range, high capacity, and high mobility.

As can be seen from the preceding discussion, the simultaneous delivery of all three of these attributes is problematic, and a communications system may be able to exhibit two of them but not all three at once. It is useful, therefore, to revisit the attributes by considering them in pairs:

Figure 5
Figure 5: Range-capacity-mobility trade-off 8

The trade-off between range, capacity and mobility is illustrated in Figure 5 for a number of communications systems. Figure 6 shows the maximum range versus the maximum capacity for the four radio-frequency systems that are useful for BLOS communications: HF sky wave, troposcatter, satellite communications, and airborne communications platforms.

The dominant utility of satellite communications is immediately obvious—capacities from low to high can be provided over ranges from short to long. None of the other systems can compete in that regard—HF communications can compete on range but has miniscule capacity by comparison; troposcatter and airborne platforms have much higher capacities than HF (with airborne platforms having much higher capacity again than troposcatter) but both are well short in range compared to satellite communication. Consequently, the ADF (and just about every other defense force and commercial organization) has embraced satellite-based systems as the principal means for long-range communication.

Figure 6
Figure 6: Maximum range versus maximum capacity for four BLOS radio-frequency communication systems

Endnotes

  • [3] Descriptions of communications modes contained here are necessarily brief and therefore occasionally superficial. Full details of the modes are available in M. Ryan, M. Frater and M. Pickering, Fundamentals of communications and information systems, Argos Press, Canberra, 2011. back
  • [4] For more detail, see T. Maclean and Z. Wu, Radiowave propagation over ground, Chapman & Hall: London, 1993; and R. Collin, Antennas and radiowave propagation, McGraw-Hill: New York, 1985. back
  • [5] Further detail on sky-wave communications can be found in J. Betts, High frequency communications, The English Universities Press Ltd: London, 1967; G. Braun, Planning and engineering of shortwave links, Siemens Aktiengesellschaft (John Wiley & Sons): Berlin, 1986; J. Goodman, HF communications: science and technology, Van Nostrand Reinhold: New York, 1992; and N. Maslin, HF communications, Pitman: London, 1987. back
  • [6] For more detail, see G. Roda, Tropospheric scatter radio relay links: guide to design and implementation, Applicazioni Radio Elettroniche SPA: Castallanza, 1986. back
  • [7] See for example: J. Keller, “Military wants to develop RF phased array common modules for the defense industry”, Military & Aerospace Electronics, 1 May 2018. https://www.militaryaerospace.com/defense-executive/article/16707322/military-wants-to-develop-rf-phased-array-common-modules-for-the-defense-industry, accessed 8 December 2019. back
  • [8] M. Ryan and M. Frater, Tactical communications for the digitized battlefield, Artech House: Boston, 2002. back