Dependency of Friis Transmission Equation on Frequency and Polarization
Key Takeaways

The Friis transmission equation widely used in radio frequency communication system is:

As radio wave frequency increases, Free Space Path Loss ❲FSPL❳ increases, and decreases the receivingend power, Pr.

The modified Friis transmission equation addresses polarization mismatch and is given by:
Figure 1: The gain, height, and aperture of antenna influences antenna performance
Antennas are vital to telecommunication systems, as they provide for the transmission and reception of signals. The signal power, height, and aperture of the antenna influence antenna performance. The Friis transmission equation quantifies the power received at the receiving end of the antenna and power loss.
The receiving end power calculation can be calculated with the Friis transmission equation, provided the transmitted power density and the effective aperture of the receiving antenna are known. The application of the Friis transmission equation is found effective especially in satellite communications and systems where minimum reflections are required.
Friis Transmission Equation
The Friis transmission equation is named after Harald T Friis, a pioneer in the field of radio receivers and antennas. His work in Bell laboratories was mainly on radio propagation, microwave systems, and antennas. He introduced an analytical equation for calculating the transmission loss, shown below.
where P_{t} and P_{r }are the transmission end and receiving end signal powers, respectively. A_{t }and A_{r }give the effective aperture of the transmission and receiving end antennas. The distance between the antennas is represented by d and is the wavelength of the signal.
The original Friis equation is modified with the gains of the antenna, and is considered to be the fundamental equation in antenna theory. Today, the Friis transmission equation is widely used and most commonly seen in the following form:
where G_{t }and G_{r} gives the gains of transmission and receiving end antennas. This equation gives the influence of the transmission loss, antenna gains, and wavelength on the transmitted and received powers. In the original Friis equation, there is no numerical coefficient present, and this was cited as one of the advantages of the original equation. However, the modified equation contains the gains of antennas at both ends.
The Friis Equation and Its Frequency Dependency
As we know, all electromagnetic waves obey the following equation:
Where c is the speed of the electromagnetic wave, which is equal to 3x10^{8} m/sec, and f is the frequency of the wave.
Rearranging the above equation for and substituting in equation 2, we can obtain the relationship between power available at the receiving end antenna:
The power received at receivingend antenna P_{r}and frequency f share an inverse proportionality. At lower frequencies or at longer wavelengths, P_{r} is more comparable to higher frequencies. If you are transmitting a known amount of power P_{t} at frequencies f_{1} and f_{2}, such that f_{1}＞ f_{2 }and P_{r1}and P_{r2 }are the power available at a receiving end antenna of gain G at these frequencies respectively, then P_{r2}＞ P_{r1}.
The power loss in the telecommunication system is given as system loss, L_{s}, expressed in dB. It is the difference between the transmitted power, P_{t} , and received power, P_{r}.
As the frequency increases, the power received P_{r }decreases. That means the system loss is greater as frequency increases. At higher frequency, the system loss increases and affects the quality of reception.
The high system loss associated with highfrequency signals calls for pointtopoint communication, where the transmission and receiving end antennas are placed in the vicinity. For mobile phone communication, service providers stick to lower frequency, which improves their service and reachability. However, lowfrequency communication can be a challenge, since the mobile phone manufacturing industry must design antennas for longer wavelengths.
Free Space Path Loss ❲FSPL❳ is another loss present in the radio frequency communication system, represented by the following equation:
The reciprocal of the same FSPL is present in the Friis transmission equation, shown in equation 4. The path loss takes a good share of the transmitted power at higher frequencies and causes a reduction in the receivingend power. FSPL also increases as the distance between the two antennas increases.
Generalizing the Friis Transmission Equation Based on the Polarization of Antennas
Any electromagnetic field is composed of an electric and a magnetic field. The electric field oscillates in some direction, with respect to the electromagnetic wave, and this direction defines the polarization of the wave. Electromagnetic waves are categorized based on the electric field oscillation.

Linear Polarization In linear polarization, the electric field and the electromagnetic wave are oscillating in one plane. The electric field is linear with the electromagnetic wave. If the electric field is oscillating horizontally, it is called horizontal polarization. In vertical polarization, the electric field oscillates in the vertical direction, and the slant polarization can be distinguished by an angle of oscillation, either +45° or 45°.

Circular PolarizationIn this polarization, the electromagnetic wave rotates, and the electric field, if traced, forms a helical shape. According to the direction of rotation, there are two types of circular polarization, namely Right Hand Circular Polarization ❲RHCP❳ and Left Hand Circular Polarization❲LHCP❳.

Elliptical Polarization Elliptical polarization is also called mixed polarization. It is a blend of linear and circular polarization.
The polarization of the antenna is the polarization of the electromagnetic wave transmitted and received by it, and the above classification applies to antennas as well. In antennatoantenna communication, both the transmitting and receiving antennas should be of the same polarization.
There will be no reception, in case the receiving end antenna polarization is different from that of the transmitting end. If there exists any difference in the angle of rotation of the two antennas of the same polarization, then reception is possible with power loss. This kind of polarization mismatch is represented by a factor called Polarization Loss Factor ❲PLF❳. Considering the polarization mismatch in antennas, the Friis equation shown in equation 4 can be revised and generalized to:
If you are working on freespace RF communication links and looking to find a suitable antenna to receive signals, then the Friis transmission equation can assist your antenna selection. The application of the Friis equation in determining the gains of any one of the two antennas has been found to be very effective. In antennatoantenna communication, there is no design of antennas possible without using the Friis transmission equation.