1. Free-sSpace Path Loss Formula

The free-space path loss (FSPL) formula derives from the Friis transmission formula.^[1] This states that in a radio system consisting of a transmitting antenna transmitting radio waves to a receiving antenna, the ratio of radio wave power received [math]\displaystyle{ P_r }[/math] to the power transmitted [math]\displaystyle{ P_t }[/math] is:

[math]\displaystyle{ \frac{P_r}{P_t} = D_t D_r \left( \frac{\lambda}{4 \pi d} \right)^2 }[/math]

where

• [math]\displaystyle{ \ D_t }[/math] is the directivity of the transmitting antenna
• [math]\displaystyle{ \ D_r }[/math] is the directivity of the receiving antenna
• [math]\displaystyle{ \ \lambda }[/math] is the signal wavelength,
• [math]\displaystyle{ \ d }[/math] is the distance between the antennas,

The distance between the antennas [math]\displaystyle{ d }[/math] must be large enough that the antennas are in the far field of each other [math]\displaystyle{ \ d\gg\lambda }[/math].^[2] The free-space path loss is the loss factor in this equation that is due to distance and wavelength, or in other words the ratio of power received to power transmitted assuming the antennas are isotropic and have no directivity ([math]\displaystyle{ D_t = D_r = 1 }[/math])^[3] [math]\displaystyle{ \begin{align} \mbox{FSPL} = \left ( \frac{4\pi d} \lambda \right )^2 \end{align} }[/math]

Since the frequency of a radio wave [math]\displaystyle{ f }[/math] is equal to the speed of light [math]\displaystyle{ c }[/math] divided by the wavelength, the path loss can also be written in terms of frequency [math]\displaystyle{ \begin{align} \mbox{FSPL} = \left({4\pi df \over c}\right)^2 \end{align} }[/math]

Beside the assumption that the antennas are lossless, this formula assumes that the polarization of the antennas is the same, that there are no multipath effects, and that the radio wave path is sufficiently far away from obstructions that it acts as if it is in free space. This last restriction requires an ellipsoidal area around the line of sight out to 0.6 of the Fresnel zone be clear of obstructions. The Fresnel zone increases in diameter with the wavelength of the radio waves. Often the concept of free space path loss is applied to radio systems that don't completely meet these requirements, but these imperfections can be accounted for by small constant power loss factors that can be included in the link budget.

2. Influence of Distance and Frequency

 

In free space the intensity of electromagnetic radiation decreases with distance by the inverse square law, because the same amount of power spreads over an area proportional to the square of distance from the source

The free space loss increases with the distance between the antennas and decreases with the wavelength of the radio waves due to these factors^[4]

• Intensity ([math]\displaystyle{ I }[/math]) – the power density of the radio waves decreases with the square of distance from the transmitting antenna due to spreading of the electromagnetic energy in space according to the inverse square law^[5]
• Antenna capture area ([math]\displaystyle{ A_\text{eff} }[/math]) – the amount of power the receiving antenna captures from the radiation field is proportional to a factor called the antenna aperture or antenna capture area, which increases with the square of frequency^[5] Since this factor is not related to the radio wave path but comes from the receiving antenna, the term "free space path loss" is a little misleading.

3. Derivation

The radio waves from the transmitting antenna spread out in a spherical wavefront. The amount of power passing through any sphere centered on the transmitting antenna is equal. The surface area of a sphere of radius [math]\displaystyle{ d }[/math] is [math]\displaystyle{ 4\pi d^2 }[/math]. Thus the intensity or power density of the radiation in any particular direction from the antenna is inversely proportional to the square of distance

[math]\displaystyle{ I \propto {P_t \over 4\pi d^2} }[/math]

For an isotropic antenna which radiates equal power in all directions, the power density is evenly distributed over the surface of a sphere centered on the antenna

[math]\displaystyle{ I = {P_t \over 4\pi d^2} \qquad \qquad \qquad \text{(1)} }[/math]

The amount of power the receiving antenna receives from this radiation field is

[math]\displaystyle{ P_r = A_\text{eff}I \qquad \qquad \qquad \text{(2)} }[/math]

The factor [math]\displaystyle{ A_\text{eff} }[/math], called the effective area or aperture of the receiving antenna, which has the units of area, can be thought of as the amount of area perpendicular to the direction of the radio waves from which the receiving antenna captures energy. Since the linear dimensions of an antenna scale with the wavelength [math]\displaystyle{ \lambda }[/math], the cross sectional area of an antenna and thus the aperture scales with the square of wavelength [math]\displaystyle{ \lambda^2 }[/math].^[4] The effective area of an isotropic antenna (for a derivation of this see Antenna aperture article) is

[math]\displaystyle{ A_\text{eff} = {\lambda^2 \over 4\pi} }[/math]

Combining the above (1) and (2), for isotropic antennas

[math]\displaystyle{ P_r = \Big({P_t \over 4\pi d^2}\Big)\Big({\lambda^2 \over 4\pi}\Big) }[/math]

[math]\displaystyle{ \text{FSPL} = {P_t \over P_r} = \Big({4\pi d \over \lambda}\Big)^2 }[/math]

4. Free-sSpace Path Loss in Decibels

A convenient way to express FSPL is in terms of decibels (dB)

[math]\displaystyle{ \begin{align} \operatorname{FSPL}(\text{dB}) &= 10\log_{10}\left(\left(\frac{4\pi d f}{c}\right)^2\right) \\ &= 20\log_{10}\left(\frac{4\pi d f}{c}\right) \\ &= 20\log_{10}(d) + 20\log_{10}(f) + 20\log_{10}\left(\frac{4\pi}{c}\right) \\ &= 20\log_{10}(d) + 20\log_{10}(f) - 147.55, \end{align} }[/math]

where the units are as before.

For typical radio applications, it is common to find [math]\displaystyle{ \ f }[/math] measured in units of GHz and [math]\displaystyle{ \ d }[/math] in km, in which case the FSPL equation becomes

[math]\displaystyle{ \operatorname{FSPL}(\text{dB}) = 20\log_{10}(d) + 20\log_{10}(f) + 92.45 }[/math]

For [math]\displaystyle{ \ d,f }[/math] in meters and kilohertz, respectively, the constant becomes [math]\displaystyle{ {-87.55} }[/math].

For [math]\displaystyle{ \ d,f }[/math] in meters and megahertz, respectively, the constant becomes [math]\displaystyle{ {-27.55} }[/math].

For [math]\displaystyle{ \ d,f }[/math] in kilometers and megahertz, respectively, the constant becomes [math]\displaystyle{ 32.44 }[/math].^[6]