# T-Antenna

(Redirected from T-aerial)
Multiwire T broadcast antenna of early AM station WBZ, Springfield, Conn, 1925
Types of T antennas: (a) simple (b) multiwire. Red parts are insulators, grey are supporting towers.

A T-antenna, T-aerial, flat-top antenna, or top-hat antenna is a vertically polarised simple wire radio antenna[1] used in the VLF, LF, MF and shortwave bands.[2][3][4] T-antennas are widely used as transmitting antennas for amateur radio stations,[5] long wave and medium wave broadcasting stations. They are also used as receiving antennas for shortwave listening.

The antenna consists of one or more horizontal wires suspended between two supporting radio masts or buildings and insulated from them at the ends.[1][4] A vertical wire is connected to the center of the horizontal wires and hangs down close to the ground, connected to the transmitter or receiver. Combined, the two sections form a 'T' shape, hence the name. The transmitter power is applied, or the receiver is connected, between the bottom of the vertical wire and a ground connection.

The T-antenna functions as a monopole antenna with capacitive top-loading; other antennas in this category include the inverted-L, umbrella, delta, and triatic antennas. It was invented during the first decades of radio, in the wireless telegraphy era, before 1920.

## How it works

RF current distributions (red) in a vertical antenna (a) and the T antenna (b), showing how the horizontal wire serves to improve the efficiency of the vertical radiating wire.[6] The width of the red area perpendicular to the wire at any point is proportional to the current. At resonance the current is the tail part of a sinusoidal standing wave. In the vertical antenna, the current must go to zero at the top. In the T, the current flows into the horizontal wire, increasing the current in the top part of the vertical wire. The radiation resistance and thus the radiated power in each, is proportional to the square of the area of the vertical part of the current distribution.

However, the antenna is still typically not as efficient as a full-height λ/4 vertical monopole,[5] and has a higher Q and thus a narrower bandwidth. T antennas are typically used at low frequencies where it is not practical to build a quarter-wave vertical antenna because of its height,[4][8] and the vertical radiating wire is often very electrically short, only a small fraction of a wavelength long, 0.1λ or less. Since the radiation resistance and efficiency increases with height, the antenna should be suspended as high as possible. The antenna has a base impedance with a capacitive component that must be tuned out with an added inductor.

To increase the top-load capacitance, several parallel horizontal wires are often used, connected together at the center where the vertical wire attaches.[5] This increases the capacitance and thus reduces the required tuning inductance, which improves the bandwidth, and can also increase the radiation efficiency because less inductance is required and inductors introduce resistance. The capacitance does not increase proportionally with the number of wires, however, because each wire's electric field is partially shielded from the ground by proximity to the adjacent wires.[5]

Since the vertical wire is the actual radiating element, the antenna radiates vertically polarized radio waves in an omnidirectional radiation pattern, with equal power in all azimuthal directions.[9] The axis of the horizontal wire makes little difference. The power is maximum in a horizontal direction or at a shallow elevation angle, decreasing to zero at the zenith. This makes it a good antenna at LF or MF frequencies, which propagate as ground waves with vertical polarization, but it also radiates enough power at higher elevation angles to be useful for sky wave ("skip") communication. The effect of poor ground conductivity is generally to tilt the pattern up, with the maximum signal strength at a higher elevation angle.

## Transmitting antennas

One of the first uses of T-aerials in the early 20th century was on ships, since they could be strung between masts. This is the antenna of the RMS Titanic, which broadcast the rescue call during her sinking in 1912. It was a multiwire T with a 50 m vertical wire and four 120 m horizontal wires.

Since it is shorter than λ/4 the T antenna has a high capacitive reactance. In transmitting antennas, to make the antenna resonant so it can be driven efficiently, this capacitance must be canceled out by adding an inductor, a loading coil, in series with the bottom of the antenna. Particularly at lower frequencies, the high inductance and capacitance compared to its low radiation resistance makes the loaded antenna behave like a high Q tuned circuit, with a narrow bandwidth over which it will remain impedance matched to the transmission line, compared to a λ/4 monopole. To operate over a large frequency range the loading coil often must be adjustable, and adjusted when the frequency is changed to keep the SWR low. The high Q also causes a high voltage on the antenna, roughly Q times the driving-point voltage. The insulators at the ends must be designed to withstand these voltages. In high power transmitters the output power is often limited by the onset of corona discharge on the wires.[10]

At low frequencies the radiation resistance is very low; often less than an ohm,[5][11] so the efficiency is limited by other resistances in the antenna. The input power is divided between the radiation resistance and the ohmic resistances of the antenna-ground circuit, chiefly the coil and the ground. The resistance in the coil and particularly the ground system must be kept very low to minimize the power dissipated in them.

It can be seen that at low frequencies the design of the loading coil can be challenging:[5] it must have high inductance but very low losses at the transmitting frequency (high Q), must carry high currents, withstand high voltages at its ungrounded end, and be adjustable.[8] It is often made of litz wire.[8]

At low frequencies the antenna requires a good low resistance ground to be efficient. The RF ground is typically constructed of a "star" of many radial copper cables buried about 1 ft. in the earth, extending out from the base of the vertical wire, and connected together at the center. The radials should ideally be long enough to extend beyond the displacement current region near the antenna. At VLF frequencies the resistance of the soil becomes a problem, and the radial ground system is sometimes raised and mounted a few feet above ground, insulated from it, to form a counterpoise.

## Equivalent circuit

Cage T antenna of amateur station in 1922. 60 ft high by 90 ft long. The conductor is made of a cage of 6 wires held apart by wooden spreaders; this construction increased capacitance and decreased resistance. It achieved transatlantic contacts on 1.5 MHz at a power of 440 W.

The power radiated (or received) by an electrically short vertical antenna like the T is proportional to the square of the "effective height" of the antenna,[5] so the antenna should be made as high as possible. Without the horizontal wire, the RF current distribution in the vertical wire would decrease linearly to zero at the top (see drawing a above), giving an effective height of half the physical height of the antenna. With an ideal "infinite capacitance" top load wire, the current in the vertical would be constant along its length, giving an effective height equal to the physical height, therefore increasing the power radiated fourfold. So the power radiated (or received) by a T antenna is up to four times that of a vertical monopole of the same height.

The radiation resistance of an ideal T antenna with very large top load capacitance is[6]

$R_R = 80\pi^2 \left ( \frac {h}{\lambda} \right )^2 \,$

$P = 80\pi^2 \left ( \frac {hI_0}{\lambda} \right )^2 \,$

where h is the height of the antenna, λ is the wavelength, and I0 is the RMS input current in amperes. This formula shows that the radiated power depends on the product of the base current and the effective height, and is used to determine how many 'metre-amps' are required for a given amount of radiated power.

The equivalent circuit of the antenna (including loading coil) is the series combination of the capacitive reactance of the antenna, the inductive reactance of the loading coil, and the radiation resistance and the other resistances of the antenna-ground circuit. So the input impedance is

$z = R_C + R_D + R_L + R_G + R_R + j \omega L - \frac {1}{j \omega C} \,$

At resonance the capacitive reactance of the antenna is cancelled by the loading coil so the input impedance at resonance z0 is just the sum of the resistances in the antenna circuit[12]

$z_0 = R_C + R_D + R_L + R_G + R_R \,$

So the efficiency η of the antenna, the ratio of radiated power to input power from the feedline, is

$\eta = \frac {R_R}{R_C + R_D + R_L + R_G + R_R} \,$

where

RC is the ohmic resistance of the antenna conductors (copper losses)
RD is the equivalent series dielectric losses
RG is the resistance of the ground system
C is the capacitance of the antenna at the input terminals

It can be seen that, since the radiation resistance is usually very low, the major design problem is to keep the other resistances in the antenna-ground system low to obtain the highest efficiency.[12]

## Multiple-tuned antenna

1.9 km (1.2 mile) multiple-tuned flattop antenna of the 17 kHz Grimeton VLF transmitter, Sweden.

## References

1. ^ a b Graf, Rudolf F. (1999). Modern dictionary of electronics, 7th Ed.. USA: Newnes. p. 761. ISBN 0-7506-9866-7.
2. ^ Chatterjee, Rajeswari (2006). Antenna theory and practice, 2nd Ed.. New Delhi: New Age International. pp. 243–244. ISBN 81-224-0881-8.
3. ^ a b Rudge, Alan W. (1983). The Handbook of Antenna Design, Vol. 2. IET. pp. 578–579. ISBN 0-906048-87-7.
4. ^ a b c Edwards, R.J.Edwards G4FGQ (August 1, 2005). "The Simple Tee Antenna". Antenna design library. S meter website. Retrieved 2012-02-23.
5. Straw, R. Dean, Ed. (2000). The ARRL Antenna Book, 19th Ed. USA: American Radio Relay League. p. 6.36. ISBN 0-87259-817-9.
6. Huang, Yi; Kevin Boyle (2008). Antennas: from theory to practice. John Wiley & Sons. pp. 299–301. ISBN 0-470-51028-5.
7. ^ a b Rudge, 1983, p.554
8. Griffith, B. Whitfield (2000). Radio-Electronic Transmission Fundamentals, 2nd Ed.. USA: SciTech Publishing. pp. 389–391. ISBN 1-884932-13-4.
9. ^ Barclay, Leslie W. (2000). Propagation of radiowaves. Institution of Electrical Engineers. pp. 379–380. ISBN 0-85296-102-2.
10. ^ LaPorte, Edmund A. (2010). "Antenna Reactance". Radio Antenna Engineering. Virtual Institute of Applied Science. Retrieved 2012-02-24.
11. ^ Balanis, Constantine A. (2011). Modern Antenna Handbook. John Wiley & Sons. pp. 2.8–2.9 (Sec. 2.2.2). ISBN 1-118-20975-3.
12. ^ a b LaPorte, Edmund A. (2010). "Radiation Efficiency". Radio Antenna Engineering. Virtual Institute of Applied Science. Retrieved 2012-02-24.