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A loop antenna is a radio antenna consisting of a loop or coil of wire, tubing, or other electrical conductor, that is usually fed by a balanced source or feeding a balanced load. Within this physical description there are two distinct antenna types:
For all of the large loops described in this section, the radio's operating frequency is assumed to be tuned to the loop antenna's first resonance. At that frequency, one whole wavelength is approximately 90% of the circumference of the loop.
Self-resonant loop antennas for so-called “short” wave frequencies are relatively large, with their sizes determined by the intended wavelength of operation. Diameters vary between 170–10 feet (circular loops) or 135–8 feet (square loops = "quads"). Hence, self-resonant loops are most often used at higher frequencies where their sizes become manageable.
Large loop antennas can be thought of as a folded dipole whose parallel wires have been split apart and opened out into some oval or polygonal shape. The loop's shape can be a circle, triangle, square, rectangle, or in fact any closed polygon; the only strict requirement is that the loop perimeter must be approximately 110% of one full-wavelength.
Loop antennas may be in the shape of a circle, a square or any other closed geometric shape that allows the total perimeter to be slightly more than one wavelength. The most popular shape in amateur radio is the quad antenna or "quad", a self-resonant loop in a square shape so that it can be constructed of wire strung across a supporting ‘X’ shaped frame. There may be one or more additional loops stacked parallel to the first as parasitic elements, making the antenna system unidirectional with increased gain. This design can also be turned 45 degrees to a diamond shape supported on a ‘+’ shaped frame. Triangular loops have also been used for vertical loops, since they require only one elevated support. A rectangle twice as high as its width obtains slightly increased gain and also matches 50 ohms directly if used as a single element.: Section 9.6.2
Unlike a dipole antenna, the polarization of a loop antenna is not obvious from the orientation of the loop itself, but depends on the feed point (where the transmission line is connected), and whether it is being operated as a 1, 2, or 3 wavelength loop. If a vertically oriented loop is fed at the bottom at its 1 wavelength frequency, it will be horizontally polarized; feeding it from the side will make it vertically polarized.
The radiation pattern of a self-resonant loop antenna peaks at right angles to the plane of the loop. At the lower shortwave frequencies a full loop is physically quite large, and can practically only be installed "lying flat", with the plane of the loop horizontal to the ground, consisting of wires supported at the same height by masts at its corners. This results in a radiation pattern peaking toward the vertical. Above 10 MHz, the loop is more frequently "standing up", that is with the plane of the loop vertical, in order to direct its main beam towards the horizon. It may be attached to an antenna rotator in order to rotate that direction as desired. Compared to a dipole or folded dipole, the large loop's radiation pattern is lower toward the sky or ground, giving it about 1.5 dB higher gain in the two favored horizontal directions.
Additional gain (and a uni-directional radiation pattern) is usually obtained with an array of such elements either as a driven endfire array or in a Yagi configuration (with all but one loop being parasitic elements). The latter is widely used in amateur radio in the "quad" configuration (see photo).
Low frequency one wavelength loops "lying down" are sometimes used for NVIS operation. This is sometimes called a "lazy quad". It has a single lobe straight up. If fed on higher frequencies the circumference will be several wavelengths. Near the odd harmonics of the first self-resonant frequency, input resistance will be similar to that at the main resonance. At even harmonics the input resistance will be high. At other frequencies it will have a reactive part. Except at the harmonic frequencies, operation will require use of an antenna tuner. As the frequency increases, the pattern will break up into multiple lobes with peaks at lower angles. Since the higher frequency bands need lower-angle lobes to propagate, this can work to advantage.
Small loops are small in comparison to their operating wavelength. As with all antennas which are physically much smaller than the operating wavelength, small loop antennas have small radiation resistance which is dwarfed by ohmic losses, resulting in a poor antenna efficiency. They are thus mainly used as receiving antennas at lower frequencies (wavelengths of tens to hundreds of meters).
Small loops have advantages as receiving antennas at frequencies below 10 MHz. Although a small loop's losses can be high, the same loss applies to both the signal and the noise, so the receiving signal-to-noise ratio of a small loop may not suffer at these lower frequencies, where received noise is dominated by atmospheric noise and static rather than receiver-internal noise. Exactly contrary to self-resonant loop antennas, the radiation / reception pattern of small loops peaks within the plane of the loop rather than broadside to it. The ability to more manageably rotate a smaller antenna may help to maximize the signal and reject interference.
The small loop antenna is also known as a magnetic loop since the signal at its terminals is dependent solely on the magnetic field present (as per Faraday's law of induction) and insensitive to an external electric field. This is strictly true in the limiting case of the loop's size approaching zero, in which case it becomes identical to an "infinitesimal magnetic dipole" which is the dual to the Hertzian dipole (sensitive to the local electric field but insensitive to an external magnetic field) and which as a transmitting antenna produces fields (in both the near and far field) identical to those of the Hertzian dipole but with the electric and magnetic fields (E and H) interchanged. As with a short dipole antenna, the radiation resistance is small and proportional to the square of its size:
where S is the area enclosed by the loop, λ is the wavelength, and N is the number of turns of the conductor (if not one) around the loop; the leading constant is from the impedance of free space times some simple constants. Note that the ability to increase the radiation resistance Rr through using multiple turns (N>1) is one feature not available with the Hertzian dipole.
If the perimeter of a loop antenna is much smaller than the intended operating wavelengths – say 1⁄3 to 1⁄100 of a wavelength – then the antenna is called a small loop antenna. Several performance factors, including received power, scale in proportion to the loop's area. For a given loop area, the length of the conductor (and thus its net loss resistance) is minimized if the perimeter is circular, making a circle the optimal shape for small loops. Small receiving loops are typically used below 3 MHz where human-made and natural atmospheric noise dominate. Thus the signal-to-noise ratio of the received signal will not be adversely affected by low efficiency as long as the loop is not excessively small.
A typical diameter of receiving loops with "air centers" is between 30 cm and 1 meter. To increase the magnetic field in the loop and thus its efficiency, while greatly reducing size, the coil of wire is often wound around a ferrite rod magnetic core; this is called a ferrite loop antenna. Such ferrite loop antennas are used in almost all AM broadcast receivers with the notable exception of car radios; the antenna is then usually placed outside the car's chassis.
Small loop antennas are also popular for radio direction finding, in part due to their exceedingly sharp, clear "null" along the loop axis: When the loop axis is aimed directly at the transmitter, the target signal abruptly vanishes.
The radiation resistance RR of a small loop is generally much smaller than the loss resistance RL due to the conductors composing the loop, leading to a poor antenna efficiency.[d] Consequently, most of the power delivered to a small loop antenna will be converted to heat by the loss resistance, rather than doing useful work.
Wasted power is undesirable for a transmitting antenna, however for a receiving antenna, the inefficiency is not important at frequencies below about 15 MHz. At these lower frequencies, atmospheric noise (static) and man-made noise (radio frequency interference) even a weak signal from an inefficient antenna is far stronger than the internal thermal or Johnson noise present in the radio receiver's circuits, so the weak signal from a loop antenna can be amplified without degrading the signal-to-noise ratio.
For example, at 1 MHz the man-made noise might be 55 dB above the thermal noise floor. If a small loop antenna's loss is 50 dB (as if the antenna included a 50 dB attenuator) the electrical inefficiency of that antenna will have little influence on the receiving system's signal-to-noise ratio.
In contrast, at quieter frequencies at about 20 MHz and above, an antenna with a 50 dB loss could degrade the received signal-to-noise ratio by up to 50 dB, resulting in terrible performance.
Surprisingly, the radiation and receiving pattern of a small loop is quite opposite that of a large self resonant loop (whose perimeter is close to one wavelength). Since the loop is much smaller than a wavelength, the current at any one moment is nearly constant round the circumference. By symmetry it can be seen that the voltages induced in the loop windings on opposite sides of the loop, will cancel each other when a perpendicular signal arrives on the loop axis. Therefore, there is a null in that direction. Instead, the radiation pattern peaks in directions lying in the plane of the loop, because signals received from sources in that plane do not quite cancel owing to the phase difference between the arrival of the wave at the near side and far side of the loop. Increasing that phase difference by increasing the size of the loop has a large impact in increasing the radiation resistance and the resulting antenna efficiency.
Another way of looking at a small loop as an antenna is to consider it simply as an inductive coil coupling to the magnetic field in the direction perpendicular to plane of the coil, according to Ampère's law. Then consider a propagating radio wave also perpendicular to that plane. Since the magnetic (and electric) fields of an electromagnetic wave in free space are transverse (no component in the direction of propagation), it can be seen that this magnetic field and that of a small loop antenna will be at right angles, and thus not coupled. For the same reason, an electromagnetic wave propagating within the plane of the loop, with its magnetic field perpendicular to that plane, is coupled to the magnetic field of the coil. Since the transverse magnetic and electric fields of a propagating electromagnetic wave are at right angles, the electric field of such a wave is also in the plane of the loop, and thus the antenna's polarization (which is always specified as being the orientation of the electric, not the magnetic field) is said to be in that plane.
Thus mounting the loop in a horizontal plane will produce an omnidirectional antenna which is horizontally polarized; mounting the loop vertically yields a weakly directional antenna with vertical polarization and sharp nulls along the axis of the loop.[e]
Since a small loop antenna is essentially a coil, its electrical impedance is inductive, with an inductive reactance much greater than its radiation resistance. In order to couple to a transmitter or receiver, the inductive reactance is normally canceled with a parallel capacitance.[f] Since a good loop antenna will have a high Q factor, this capacitor must be variable and is adjusted along with the receiver's tuning.
Small loop receiving antennas are also almost always resonated using a parallel plate capacitor, which makes their reception narrow-band, sensitive only to a very specific frequency. This allows the antenna, in conjunction with a (variable) tuning capacitor, to act as a tuned input stage to the receiver's front-end, in lieu of a preselector.
The procedure is to rotate the loop antenna to find the direction where the signal vanishes – the “null” direction. Since the null occurs at two opposite directions along the axis of the loop, other means must be employed to determine which side of the antenna the “nulled” signal is on. One method is to rely on a second loop antenna located at a second location, or to move the receiver to that other location, thus relying on triangulation.
Instead of triangulation, a second dipole or vertical antenna can be electrically combined with a loop or a loopstick antenna. Called a sense antenna, connecting and matching the second antenna changes the combined radiation pattern to a cardioid, with a null in only one (less precise) direction. The general direction of the transmitter can be determined using the sense antenna, and then disconnecting the sense antenna returns the sharp nulls in the loop antenna pattern, allowing a precise bearing to be determined.
Small loop antennas are lossy and inefficient for transmitting, but they can be practical receiving antennas for frequencies below 10 MHz. Especially in the mediumwave (520–1710 kHz) band and below, where wavelength-sized antennas are infeasibly large, and the antenna inefficiency is irrelevant, due to large amounts of atmospheric noise.
AM broadcast receivers (and other low frequency radios for the consumer market) typically use small loop antennas, even when a telescoping antenna may be attached for FM reception. A variable capacitor connected across the loop forms a resonant circuit that also tunes the receiver's input stage as that capacitor tracks the main tuning. A multiband receiver may contain tap points along the loop winding in order to tune the loop antenna at widely different frequencies.
In AM radios built prior to the discovery of ferrite in the mid-20th century, the antenna might consist of dozens of turns of wire mounted on the back wall of the radio – a planar helical antenna – or a separate, rotatable, furniture-sized rack looped with wire – a frame antenna.
Ferrite loop antennas are made by winding fine wire around a ferrite rod. They are almost universally used in AM broadcast receivers.[g] Other names for this type of antenna are loopstick, ferrite rod antenna or aerial, ferroceptor, or ferrod antenna. Often at shortwave frequencies Litz wire is used for the winding to reduce skin effect losses. Elaborate “basket weave” patterns are used at all frequencies to reduce inter-winding capacitance in the coil insuring that the loop self-resonance is well above the operating frequency so that it acts as an electrical inductor that can be resonated with a tuning capacitor, and with a consequent improvement of the loop Q factor.
Inclusion of a magnetically permeable core increases the radiation resistance of a small loop, mitigating the inefficiency due to ohmic losses. Like all small antennas, such antennas are tiny compared to their effective area. A typical AM broadcast radio loop antenna wound on ferrite may have a cross sectional area of only 1cm2 at a frequency at which an ideal (lossless) antenna would have an effective area some hundred million times larger. Even accounting for the resistive losses in a ferrite rod antenna, its effective receiving area may exceed the loop's physical area by a factor of 100.
Small transmitting loops are “small” in comparison to a full wavelength, but considerably larger than a small receive-only loop, and unlike receiving loops, small transmitting loops must be “scaled-up” for longer wavelengths. They are typically used on frequencies between 3–30 MHz. They usually consist of a single turn of large diameter conductor, and are typically round or octagonal to provide maximum enclosed area for a given perimeter. The smaller of these loops are much less efficient than full-sized self-resonant loops, but where space is at a premium the smaller loops can nonetheless provide effective communications.
A small transmitting loop antenna with a circumference of 10% or less of the wavelength will have a relatively constant current distribution along the conductor, and the main lobe will be in the plane of the loop. Loops of any size between 10% and 100% of a wavelength in circumference can be built and tuned to resonance with series reactance. A capacitor is required for a circumference less than a half wave, an inductor for loops more than a half wave and less than a full wave. Loops in this size range may have neither the uniform current of the small loop, nor the double peaked current of the full sized loop and thus cannot be analyzed using the concepts developed for the small receiving loops nor the self resonant loop antennas. Performance is best determined with NEC analysis. Antennas within this size range include the halo (see below) and the G0CWT (Edginton) loop.
In addition to other common impedance matching techniques such as a gamma match, transmitting loops are sometimes impedance matched by connecting the feedline to a smaller feed loop inside the area surrounded by the main loop. Typical feed loops are 1⁄8 to 1⁄5 the size of the antenna's main loop. The combination is in effect a transformer, with power in the near-field inductively coupled from the feed loop to the main loop, which itself is connected to the resonating capacitor and is responsible for radiating most of the power.
Small loops are used in land-mobile radio (mostly military) at frequencies between 3–7 MHz, because of their ability to direct energy upwards, unlike a conventional whip antenna. This enables Near Vertical Incidence Skywave (NVIS) communication up to 300 km in mountainous regions. In this case a typical radiation efficiency of around 1% is acceptable because signal paths can be established with 1 Watt of radiated power or less when a transmitter generating 100 Watts is used.
In military use, the antenna may be built using a one or two conductors 1–2 inches in diameter. The loop itself is typically 6 feet in diameter.
One practical issue with small loops as transmitting antennas is that the loop not only has a very large current going through it, but also has a very high voltage across the capacitor, typically thousands of Volts, even when fed with only a few Watts of transmitter power. This requires a rather expensive and physically large resonating capacitor with a large breakdown voltage, in addition to having minimal dielectric loss (normally requiring an air-gap capacitor). In addition to making the geometric loop larger, efficiency may be increased by using larger conductors or other measures to reduce the conductor's loss resistance. However, lower loss means higher Q and even greater voltage on the capacitor.
This problem is more serious than with a vertical or dipole antenna that is short compared to a wavelength. For those electrical antennas, matching using a loading coil also generates a high voltage across the antenna end(s). However, unlike with capacitors, the voltage change is gradual, spread across a physically long inductor, and is generally not troublesome.
Some antennas look very much like loops, but are either not continuous loops, or are designed to couple with the inductive near-field – over distances of a meter or two – rather than to transmit or receive long-distance electromagnetic waves in the radiative far-field.
Although it has a superficially similar appearance, the so-called halo antenna is not technically a loop since it possesses a break in the conductor opposite the feed point; that totally changes the current pattern since the voltages across the break are opposite and large. It is better analyzed as a dipole (which also has a large voltage and zero current at its ends) which has been bent into a circle and end-loaded with a low-capacitance air-capacitor (i.e. the break).
Inductive heating systems, induction cooking stovetops, and RFID tags and readers all interact by near field magnetic induction rather than far field transmitted waves. So strictly speaking, they are not radio antennas. The use of coupling coils for inductive systems, including their use at LF and HF, is outside the scope of this article.
Although they are not radio antennas, these systems do operate at radio frequencies, and they do involve the use of small magnetic coils, which in the trade are called "antennas", however they are more usefully described as analogous to windings of loosely coupled transformers. Although the magnetic coils in these inductive systems sometimes seem indistinguishable from the small loop antennas discussed in this article, such devices can only operate over short distances, and are specifically designed to not transmit (or receive) radio waves. Inductive heating systems and RFID readers only use near field alternating magnetic fields and their performance criteria are dissimilar to far field radio antennas discussed in this article.