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Antenna Design Choices

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Antenna Design Choices

The type of antenna employed in a wireless sensor network node depends greatly on its application. Usually an internal antenna is preferred, due to its inherent portability and protection from mechanical and environmental damage. Several types of internal antennas are available.

The first option is often the use of a circuit board trace as an antenna. This option has the advantage of low cost because no components must be purchased, handled, or placed on the board; however, because circuit board area is not free, its cost is not zero. It is also very thin, an advantage for low-profile network node designs. The most significant disadvantage to this type of antenna is its poor performance. Due to the thinness of the circuit board trace, its series resistance can be relatively high despite the low resistivity of copper; the low quality of the circuit board material often adds dielectric loss. Being in the circuit board itself also enables the circuit board trace antenna to more readily couple to lossy components and other circuit board traces, and to sources of noise. Finally, the tuning of circuit board antenna can be subject to significant variation caused by etching variations during the circuit board manufacturing process. This variation is often difficult to control without significant expense because the required etching accuracy is typically greater than that needed for simple connectivity of the circuit board.

A second alternative is the use of simple wire or metal strip antennas placed as components on the circuit board. These antennas can have remarkably improved performance over that of the circuit board trace antenna, due to their significantly lower loss and the fact that they are above the circuit board. (Being above the circuit board, however, they are susceptible to better coupling to some noise sources, such as the inductors in switching power supplies.) Wire antennas can be either dipoles or loops; nodes designed for on-body use, such as health monitoring devices, often employ loops as so-called H-field antennas (i.e., magnetic field probes) in a plane normal to the body. Wire antennas often require dielectric (e.g., plastic) supports to maintain their mechanical shape and, therefore, their frequency of resonance, to the required tolerance. They are often difficult to robotically place in an automated assembly line, and must be inserted and soldered by hand. Nevertheless, wire antennas are often a good compromise between the low cost and efficiency of the circuit board antenna and the relatively high cost and high efficiency of the external antenna.

A third choice is the use of specialized ceramic antenna components. These components are simple to place by automatic equipment, are physically smaller than wire antennas, and do not require tuning. They are usually more expensive than wire antennas, however, and are often available only for the most widely used frequency bands (e.g., the 915- and 2450-MHz Industrial, Scientific, and Medical [ISM] bands).

Because they usually are free of the size limitation placed on internal antennas and are removed from the noise sources present in the network node itself, external antennas can have very high performance. In applications where the utmost in range is desired and a directive antenna must be used, an external antenna is almost certainly required. Designers of nodes for use in white goods (refrigerators and other large household appliances) may prefer external antennas to avoid the shielding of their metallic housings. In applications in which several different antennas must be used, for example, to meet differing range requirements of multiple applications, external antennas are the obvious choice. Although external antennas offer the highest performance and design flexibility, they usually are the most expensive; not only must the antenna be purchased, but usually one or more high-quality RF connectors, as well. Losses associated with any feedline (usually miniature coaxial cable) between the network node and the antenna itself must be included in the network node design. A hidden cost not always considered is associated with the frequency selectivity of the antenna. Because it is under the control of the node designer, the selectivity of an internal antenna may be used as part of the transceiver system design (e.g., Zolfaghari and Razavi[9]). Because users may replace external antennas with those of unknown selectivity, when using an external antenna, the node designer may often be required to include additional RF selectivity in the node design, at additional product cost.

External antennas need not always be expensive, however; for example, Ross et al.[10] describes a covert wireless sensor network node (used in security applications) that uses the doorknob housing the network node as its antenna.

[1]Kazimierz Siwiak, Radiowave Propagation and Antennas for Personal Communications, 2nd ed. Norwood, MA: Artech House. 1998. p. 19.

[2]As a (usually) small-signal system, for receiving antennas the output impedance of the antenna should be a conjugate match for the input impedance of the receiver for maximum power transfer; however, a mismatch is often desirable, to attain an improved system noise figure and improved system sensitivity. (See Guillermo Gonzalez, Microwave Transistor Amplifiers: Analysis and Design. 2nd ed. Upper Saddle River, NJ: Prentice Hall. 1997. pp. 294–322.) For transmitters, which are (usually) large-signal systems, an impedance match by the transmitting antenna to the output impedance of the power amplifier is usually not desired. Instead, an antenna input impedance that produces the desired amount of power transferred from amplifier to antenna (i.e., Paccept) is sought, which can result in a significant mismatch. An exception that can occur in wireless sensor network design is the use of low-transmit power (e.g., 6 dBm or less), for which even the transmitter power amplifier can be considered to be in small-signal operation.

[3]Ibid., p. 193.

[4]John D. Kraus, Antennas. New York: McGraw-Hill. 1950, p. 136.

[5]Ibid., pp. 136–137.

[6]Siwiak, pp. 13–15.

[7]Z0 = cμ0, where c is the speed of light in vacuum (299 792 458 m/s) and μ is the permeability of free space (4π×107 H/m).

[8]Siwiak, p. 332.

[9]Alireza Zolfaghari and Behzad Razavi, "A low-power 2.4-GHz transmitter/receiver CMOS IC," IEEE J. Solid-State Circuits, v. 38, n. 2, February 2003, pp. 176–183.

[10]Gerald F. Ross et al., Batteryless Sensor for Intrusion Detection and Assessment of Threats. Defense Nuclear Agency Technical Report DNA-TR-95–21. Springfield, VA: National Technical Information Service. 1 November 1995.


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