Magnetic Loop Antennas

A Nice Magnetic Loop Antenna.

Magnetic loop antennas (MLAs) are a type of antenna that is often used for shortwave listening and transmitting. 

They are large loops of copper or aluminum tube that are tuned with a variable capacitor. 

MLAs have a number of special properties:


Design Factors

The most important design factors for MLAs are:

The magnetic field produced by a single turn loop 

Applying DC to a loop produces a north pole on one side and a south pole on the other.

The conductivity of metals at DC and Radio Frequencies (RF)

The normal flow of current in a conductor is greatly affected by magnetic fields a high frequency.

Resulting in the Skin Effect and Proximity Effect.

The skin effect causes the current to be concentrated near the surface of the conductor, rather than being evenly distributed throughout the conductor. This is because the high-frequency magnetic field of the current induces eddy currents in the conductor, which oppose the original current.

The Skin Effect. Concentration of current at the surface of a conductor as frequency increases resulting in increased resistivity. This indicates that tubing is just as effective a conductor as solid material at RF.

The proximity effect is a redistribution of electric current occurring in nearby parallel electrical conductors carrying alternating current. It is caused by magnetic effects. 

Radiation Resistance

Radiation resistance expresses the dissipation of energy supplied to an antenna in the form of radio waves. The radiation resistance of a magnetic loop antenna is very low. This means the other resistance losses from the limited conductivity of metal, the skin effect, the proximity effect and connection losses have to be very low for the loop to work.

The radiation resistance of a single turn loop antenna is proportional to the square of the area of the loop and the frequency of the radiation.

Inductance of single turn

Approximate values.

Loop diameter 0.5m: Inductance: 0.683 uH, radiation resistance: 0.006 ohms

Loop diameter 1m: inductance 1.7uH, radiation resistance : 0.083 ohms

Resonance

Since the loop is inductive and you need very high currents to transmit from the loop you can resonate the loop with capacitor for operation at a particular frequency.  This leads to resonant build-up of current and voltage over time. The power transmitted as radio waves is I²Rrad as per Ohm's Law. Where Rrad is the radiation resistance. The wasted power from the conductor losses is I²R, where R is the conductor losses including the impact of the skin effect and proximity effect.

Using resonance to build up the current in a loop antenna.

Voltage and current distribution in a magnetic loop antenna. The current is high and relatively uniform around the loop. The voltage reaches high values at the capacitor.

Matching

There are a number of ways of matching a magnetic loop antenna to a transmitter, some example are:

A high Q factor in a magnetic loop antenna has several advantages and disadvantages.

Advantages:

Disadvantages:


Practical tips for a magnetic loop antenna.