Turnstile antenna
A turnstile antenna is a radio antenna consisting of a set of two identical dipole antennas aligned at right angles to each other and fed in phase quadrature; the two currents applied to the dipoles are 90° out of phase.[1][2] The name reflects the notion the antenna looks like a turnstile when mounted horizontally. The turnstile antenna is often referred to as crossed dipoles.[3] The antenna can be used in two possible modes. In normal mode the antenna radiates horizontally polarized radio waves perpendicular to its axis. In axial mode the antenna radiates circularly polarized radiation along its axis.
History
The turnstile antenna was invented by George Brown in 1935[1] and described in scholarship in 1936.[4] The patent history reveals the popularity of the turnstile antenna over the years.[5]
Characteristics
The antenna can be used in two different modes: normal mode and axial mode.
Normal mode
In directions perpendicular to its axis the antenna radiates linearly polarized radio waves (horizontally polarized when the antenna's axis is vertical). This is called normal mode. The radiation pattern, a superposition of the two dipole patterns, is close to omnidirectional but actually "cloverleaf shaped", with four small maxima off the ends of the elements. The pattern departs from omnidirectional by only ±5 percent.[2] The radiation in these horizontal directions is often increased by vertically stacking multiple turnstile antennas (called "bays") fed in phase. This increases the gain in horizontal directions but causes partial cancellation of the radiation in vertical directions. These stacked normal mode turnstile antennas are used at VHF and UHF frequencies for FM and television broadcasting.
Since the first turnstiles invented by Brown operated in this mode, the normal mode turnstile is occasionally called the George Brown turnstile antenna.[2]
Axial mode
Off the ends of the antenna's axis, perpendicular to the plane of the elements, the antenna radiates circularly-polarized (CP) radio waves. This is called axial mode. The radiation off one end is righthand-circularly-polarized and the other end is lefthand-circularly-polarized. Which end produces which polarization is determined by the phase of the feed connections. Since in a directional antenna only a single beam is wanted, in a simple axial-mode antenna a flat conducting surface such as a metal screen reflector is added, a half-wavelength under the crossed elements.[3] The waves in that direction are reflected back 180° and the reflection reverses the polarization sense, so the reflected waves reinforce the forward radiation.[3] For example, if the radio waves radiated forward are right-circularly-polarized, the waves radiated backwards will be left-circularly-polarized. The flat reflector reverses the polarization sense so the reflected waves are right-circularly-polarized. By locating the reflector λ/2 behind the elements the direct and reflected waves are in phase and add. Addition of the reflector increases the axial radiation by a factor of 2 (3 dB).
Another common way to increase the axial mode radiation is to replace each dipole with a Yagi array.
In a circularly polarized antenna, it is important that the direction of polarization of the transmitting and receiving antennas be the same, since a right-circularly-polarized antenna will suffer a severe loss of gain receiving left-circularly-polarized radio waves, and vice versa.
Axial mode turnstile antennas are often used for satellite and missile antennas,[6] since circular polarization is used in satellite communication. This is because with circularly polarized waves the relative orientation of the antenna elements does not affect the gain.
Feeding the antenna
The fundamental requirement for the turnstile to function is ensuring each dipole's currents are of equal magnitude and in phase quadrature.[2] This is done with feed-line techniques or by adding reactance in series with the dipoles.[2]
Quadrature feed
A popular method of feeding the two dipoles in a turnstile antenna is to split the RF signal from the transmission line into two equal signals with a two way splitter, then delay one by 90 degrees additional electrical length. Each phase is applied to one of the dipoles.[2]
Modified dipole dimensions
By modifying the length and shape of the dipoles, the combined terminal impedance presented to a single feed-point can achieve pure resistance and yield quadrature currents in each dipole.[2][6] This method of changing the physical dimensions of the antenna element to yield quadrature currents is known as turnstile feeding.[3]
Applications
Stacked arrays
Brown's original patent described stacking multiple turnstile antennas vertically to make a high gain horizontally polarized omnidirectional antenna for radio broadcasting.[1] [2][1] These were used for some of the first FM broadcasting antennas in the 1930s. However most modern FM broadcast antennas use circular polarization so the signal strength will not vary with the orientation of the receiver's antenna.
Batwing or superturnstyle array
A later innovation involved changing the shape of the dipole elements, from simple rods to broader shapes, to increase the bandwidth of the antenna.[7] Early TV broadcast antennas used "cigar shaped" elements, shown in image of 1939 RCA Empire State Building antenna above. A common shape today is the batwing or superturnstile antenna, used for television broadcasting in the VHF or UHF bands[8] The batwing shape of each element produces an antenna with wide impedance bandwidth.[3] Up to eight batwing antennas are usually stacked vertically and fed in phase to make a high gain omnidirectional antenna for TV broadcasting.[2][3] The wide bandwidth was needed at the low VHF analog TV broadcast band, as the 6 MHz TV channel bandwidth was about 10% of the frequency.[3]
Spacecraft antennas
Circular polarization was used for spacecraft (satellite and missile) communication, since circular polarization is not sensitive to the relative orientation of the antennas, and the space vehicle's antenna could have any orientation with respect to the ground antenna. High gain Yagi turnstile antennas were often used for the ground station.
The US Nike missile program made use of the axial mode for telemetry and used the modified dipole technique to force the quadrature currents.[6]
External links
- Turnstile Construction plans for satellite communication
- Construction plans
- Turnstile design for APT weather satellite reception
- Radiation of Turnstile Antennas Above a Conducting Ground Plane
References
- 1 2 3 4 Brown, George. "US Patent 2086976". Antenna system. Retrieved 14 January 2014. filed: September 20, 1935; granted: July 13, 1937
- 1 2 3 4 5 6 7 8 9 Kraus, John (1988). "16: Antennas for Special Applications: Feeding Applications". Antennas (2nd ed.). McGraw-Hill, Inc. pp. 726–729. ISBN 0-07-035422-7.
- 1 2 3 4 5 6 7 Milligan, Thomas (2005). "5 - Dipoles, Slots and Loops". Modern Antenna Design (2nd ed.). Hoboken, New Jersey: John Wiley & Sons, Inc. pp. 231–237. ISBN 978-0-471-45776-3.
- ↑ Brown, George (April 1936). "The Turnstile Antenna". Electronics.
- ↑ "Patents about Turnstile Antennas".
- 1 2 3 Martin, John (1952). "[Missile] Antenna". Retrieved 15 January 2014.
- ↑ Masters, Robert (1945). "[Batwing] Antenna". Retrieved 15 January 2014.
- ↑ Whitaker, Jerry (1996). "Antennas for Specific Applications". In Jerry Whitaker. The Electronics Handbook. CRC Press, Inc. p. 1341. ISBN 0-8493-8345-5.
The turnstile is the earliest and most popular resonant antenna for VHF broadcasting.