The range of mmWave communication signals is often said to be lower than for signals in the conventional sub-6 GHz bands. This is usually also the case but the reason for it might not be the one that you think. I will explain what I mean in this blog post.
If one takes a look at the classical free-space pathloss formula, the received power is
where the transmit power is denoted by , the wavelength is , and the propagation distance is . This formula shows that the received power is proportional to the wavelength and, thus, will be smaller when we increase the carrier frequency; that is, the received power is lower at 60 GHz ( mm) than at 3 GHz ( cm). But there is an important catch: the dependence on is due to the underlying assumption of having a receive antenna with the effective area
Hence, if we consider a receive antenna with arbitrary effective area , we can instead write the received signal in (1) as
which is frequency-independent as long as we keep the antenna area fixed as we change the carrier frequency. Since the area of a fixed-gain antenna actually is proportional to , as exemplified in (2), in practice we will need to use arrays of multiple antennas in mmWave bands to achieve the same total antenna area as in lower bands. This is what is normally done in mmWave communications for cellular networks, while a single high-gain antenna with large area can be used for fixed links (e.g., backhaul between base stations or between a satellite and ground station). As explained in Section 7.5 of Massive MIMO Networks, one can actually play with the antenna areas at both the transmitter and receiver to keep the same pathloss in the mmWave bands, while actually reducing the total antenna area!
So why is the signal range shorter in mmWave bands?
The main reasons for the shorter range are:
- Larger propagation losses in non-line-of-sight scenarios, for example, due to less scattering (fewer propagation paths) and larger penetration losses.
- The use more bandwidth, which leads to lower SNR.