WiMax Operator's Manual
WiMax Operator's Manual
WiMax Operator's Manual
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CHAPTER 5 ■ STRATEGIES FOR SUCCESSFUL DEPLOYMENT OF PHYSICAL INFRASTRUCTURES 113<br />
of the industry has long sought some means of getting around or through obstructions. The<br />
collective term for the technologies for doing so is non–line of sight (NLOS).<br />
NLOS is a term used rather loosely in the industry—too loosely in my opinion. The term<br />
applies to a number of distinct technologies of varying capabilities and maturity, and the performance<br />
of so-called NLOS equipment in the field is far from uniform. While manufacturers<br />
that have appropriated the NLOS nomenclature are fond of claiming that their respective<br />
products will double the effective coverage of a network, and in some cases can frame fairly<br />
plausible arguments based on enhanced link budgets, such claims must always rest upon certain<br />
assumptions regarding the distribution of obstructions within the locale in question,<br />
assumptions that may not necessarily hold true in individual instances. Thus, no claim should<br />
be taken at face value, and any radio that has to be used in a NLOS setting should be thoroughly<br />
tested in the environment in which it is to be used before it is purchased.<br />
NLOS, as I will use the term, refers to any technique for lessening the effects of physical<br />
obstructions, and the emphasis is on the word lessening, because no NLOS technique can<br />
entirely eliminate the effects of blockage. The success of the technique is directly measurable<br />
in terms of the signal strength at the radio front end, the block of circuitry where actual demodulation<br />
of the signal begins. NLOS is never an all-or-nothing proposition. It is a matter of<br />
greater or lesser signal strength—it is that simple.<br />
Most of the manufacturers that have survived in the public broadband wireless arena now<br />
claim to manufacture NLOS equipment. Within the industry overall, a near consensus has<br />
been reached on the matter, and that consensus is that networks of any size operating in the<br />
lower microwave regions are not viable without NLOS equipment. I am inclined to accept this<br />
consensus on purely empirical grounds, leaving aside precise definitions of just what NLOS is,<br />
because, simply stated, the attrition rate among network operators attempting to use strict<br />
line-of-sight first-generation equipment has been horrendous. Obviously, other factors are at<br />
work as well, but the inability of operators to reach customers without line of sight to a base<br />
station limits absolutely the size of the subscriber market. And that this limitation may be such<br />
as to rule out half of the potential customers in a network of one kilometer radius cells does<br />
much to explain the failure of so many of the pioneers.<br />
What NLOS Means in Terms of Wave Propagation<br />
The object of this book is to go light on RF theory and heavy on practicality. However, to understand<br />
even the rudiments of NLOS, one must know something about how physical objects<br />
affect radio wave propagation.<br />
When a radio wave encounters a physical object—and by that I mean anything from an air<br />
molecule to a mountain—it can behave in one of three ways. It can give up some of its energy<br />
to the object in the form of heat, a process known as absorption. It can rebound from the object<br />
without surrendering appreciable energy to it, a process called reflection. Or it can bend<br />
around the object, a process known as diffraction. These three processes, by the way, are<br />
not mutually exclusive. A reflected signal, for instance, may immediately be diffracted as it<br />
encounters a different contour of the object reflecting it, and in every case where reflection or<br />
diffraction occurs, some energy will be absorbed as well.<br />
Absorption<br />
Pure absorption does not change the direction of the radio wave but robs it of energy and<br />
reduces the fade margin. Since the signal steadily loses energy simply by being propagated