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Applications. References. Electromagnetic Waves. Figure 1 shows how a classic half- wave dipole antenna creates the electric and magnetic fields. The transmitted signal is a modulated sine- wave voltage alternating in polarity, producing an electric (E) field between the antenna elements that switches polarity each half cycle. Current in the antenna elements produces a magnetic (H) field that changes orientation each half cycle. The fields are at right angles to one another. The electromagnetic field around a half wave dipole consists of an electric (E) field (a) and a magnetic (H) field (b). The fields are spherical and cut across one another at right angles. The fields around the antenna are spherical or curved, especially near the antenna. As these fields travel out from the antenna, rounding becomes less pronounced, turning more planar in character. The receiving antenna usually perceives a planar wave. Though the fields exist around the antenna, they propagate away from the antenna perpendicular to the two fields (Fig. At some point beyond the antenna, the fields detach themselves into packets of energy and propagate independently. In fact, they support and regenerate one another along the way. This “independent” wave is the actual radio wave. At a distance from the antenna, the E and H fields are essentially planar and intersect at right angles. Note the direction of propagation, which is perpendicular to both fields. At (a) the direction of propagation is perpendicular to the field lines shown either into or out of the page. In (b) the magnetic field lines are coming out of the page. You can picture them as lines with arrow points shown as dots. The Near Field. There’s seemingly no formal definition for the near field—it depends on the type of application and the antenna. The most agreed upon definition submits that the near field is less than one wavelength (. Wavelength in meters is given by. The near field is generally said to be divided into two areas, the reactive and the radiative. In the reactive area, the E and H fields are the strongest and can be measured separately. A loop antenna, for example, is dominated by the magnetic (H) field. The loop antenna appears to be the primary as a transformer because of the large magnetic field it generates. Boundaries of the near and far fields are shown with respect to wavelengths at the operating frequency. The antenna is assumed to be at the left and beginning of the wave. In the radiative area, the fields begin to radiate. It represents the beginning of the far field. In the near field, the strength of the fields varies inversely with the cube of the distance from the antenna (1/r. The transition zone in Figure 3 refers to the somewhat undefined area between the near and far fields. Another definition indicates that it starts at 5. Others will say that the far field begins where the near field leaves off, or as indicated earlier, . It propagates through space at a speed of just about 3. The E and H fields support and regenerate one another as their strength decreases inversely as the square of the distance (1/r. Maxwell described this phenomenon in his infamous equations. Maxwell’s Equations. In the late 1. 87. Scottish physicist James Clerk Maxwell predicted the arrival of electromagnetic waves. Using the laws known at the time from Ampere, Faraday, Ohm, and others, he came up with a set of equations that illustrates how one type of field generates the other, and as they propagate, the two coexist in a supporting relationship. In the late 1. 88. German physicist Heinrich Hertz proved Maxwell’s theory. Maxwell developed four basic equations that show the relationship of the electric and magnetic fields as they vary with time. Basically, the electric field changing over time appears to produce charges in motion or current flow that sets up a magnetic field. The waves propagate through space by themselves after leaving the antenna. Those equations aren’t shown here, but you may recall that they involve partial differential equations. Applications. The far field propagates through space, and its strength is defined by the Friis formula: Pr = Pt. Gr. Gt. The formula is valid for free space, line of sight, with no obstructions. Two important facts arise in this discussion. The received power varies inversely with the square of the range r. It also varies with the square of the wavelength, meaning that longer waves at lower frequencies travel farther. For example, a 9. MHz signal will travel farther than a 2. GHz signal for similar power and antenna gains. This expression can be used to analyze all modern wireless applications in terms of approximating signal strength. To accurately observe signal propagation, one must plot the antenna’s radiation pattern in the far field. In the reactive zone of the near field, the receiving antenna may interact with the transmitting antenna via capacitive or inductive coupling and thus give false results. On the other hand, it’s been shown that a radiation pattern in the near field can be accurately plotted if special measurement equipment is available. The near field has also proved useful in communications. This mode is used for applications such as radio- frequency identification (RFID) and near- field communications (NFC). RFID is the electronic equivalent of bar coding. A thin tag containing a chip that integrates memory and specific electronic code is attached to the item to be identified, tracked, or otherwise processed. The tag, which also includes a passive transceiver, is passed near a “reader” transceiver that emits a strong RF signal picked up by the tag. Both reader and tag antennas are usually loops serving as the primary and secondary of a transformer. The signal picked up by the tag is rectified and filtered into dc, which provides power to the tag memory and transmitter. The transmitter then sends the code to the reader for identification and further processing. Active tags using a battery sometimes extend the read range beyond the near field. RFID tags come in different frequency ranges, such as 1. Hz, 1. 3. 5. 6 MHz, and 9. MHz. At 9. 00 MHz, the wavelength is. Therefore, it may actually spill into the far field at this frequency. NFC also employs a memory and special coding similar to that of a credit card. An internal transceiver, usually battery powered, can transmit the code to a reader. It also uses the near field as the read range, and it’s typically only inches. The NFC frequency is 1. MHz, representing a wavelength of. H., Microwaves Made Simple, Principles and Applications, Artech House Inc., 1. 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