Why should a receiving antenna be impedance matched to 50 ohm instead of a lower impedance?

Question

I'm in the process of getting to grips with RF design and am having some trouble understanding why we should always match antennas to \$50\Omega\$.

I understand from the maximum power transfer theorem that if you have a fixed source (e.g. \$50\Omega\$) that you cannot change as a designer/user, then the maximum power transfer occurs if you set your load impedance to be the same as your source impedance. Therefore, if you are using an antenna as a transmitter, then you'd want to make the antenna (load) impedance equal to the impedance of the source for maximum power transfer into the antenna - so you match your antenna to \$50\Omega\$.

However, what if you are only using your antenna to receive? In that case the fixed variable is the load impedance (i.e. your receiver) which will be fixed at \$50\Omega\$ as below (I've also drawn the transmission line for completeness):

^{simulate this circuit – Schematic created using CircuitLab}

If \$Z_L\$ is fixed (\$50\Omega\$), then the maximum received power will be when the voltage across its terminals is maximized. The voltage across \$Z_L\$ is (potential divider): $$ V_{Z_L} = V_s \frac{Z_L}{Z_L+Z_S} $$ \$Z_L\$ is fixed but we can "control" \$Z_S\$. Maximum voltage across \$Z_L\$ (and hence maximum power to the load) occurs when \$Z_S=0\Omega\$

Therefore, following this logic, you'd ideally want your receiving antenna to have a very low impedance (as close to \$0\Omega\$ as possible).

I'm probably missing quite a few fundamental concepts here but at the moment, the only reason I can think to match a receiving antenna to \$50\Omega\$ is in order to avoid re-reflections back to the load. However, if the load itself is already matched well to its \$50\Omega\$ transmission line, there should be minimal reflections already.

Answer 1

However, what if you are only using your antenna to receive?

An antenna (e.g. monopole) has a complex impedance characteristic versus frequency: -

Picture from my answer here.

So, if you are tuned into a frequency that makes the antenna exactly a quarter wavelength (0.25 on the X axis above), it presents an impedance that is roughly 37 ohms resistive plus about 21 ohms inductive.

This means that you can maximize receive power transfer with a little bit of series capacitance to cancel the inductive reactance and, "produce" a receiving source having pure 37 ohms. Feed this into a matching 37 ohms to extract the most receive power.

But there's really nothing much else you can do.

A quarter wave monopole transforms the impedance of free space (roughly 377 ohms) down to 37 ohms when used at the "right frequency". Use it off-centre and the reactance can go positive (inductive) or negative (capacitive).

Therefore, following this logic, you'd ideally want your receiving antenna to have a very low impedance (as close to 0Ω as possible).

Well, you can do this - you can make the antenna intentionally "short" and it presents quite a bit of capacitive reactance and the radiation resistance will drop down to a fraction of 37 ohms (maybe 5 ohms). However, your received signal is also much smaller because the transformation ratio has dropped even lower. But, you can tune out the capacitance with series inductance and get a very highly electrically tuned antenna. Nice in some circumstances but bad in others.

Old crystal radios never had anything like a quarter wave monopole because if they did it would be nearly the length of 4 football fields (for the good old BBC long wave service at circa 200 kHz) BUT, the length was still fairly long and it's the length of the antenna that gives you the signal intensity (up to a certain point). It was still regarded as a "short" antenna though (electrically).

if you are using an antenna as a transmitter, then you'd want to make the antenna (load) impedance equal to the impedance of the source for maximum power transfer into the antenna - so you match your antenna to 50 Ω

You've got this a bit backwards - for a lot of set-ups, the antenna is somewhat distant to the transceiver and are connected via coaxial cable. Coax has a transmission impedance and, at that precise transmission impedance, signals are not reflected from a matching load. This is quite important. And so an antenna is usually matched to the coax but, an antenna (standard ones like monopoles and dipoles) don't look like 50 Ω so they are matched via a balun or resistor network at the antenna (load) end. This can mean that the transmitter end needn't match to anything like 50 Ω and, can drive its full power to the load.

Answer 2

You want the impedance of the antenna to match that of whatever is driving it (transmit), or whatever the antenna is feeding in to (receive).

There is nothing magical about 50 ohms. In theory, it could be 75 ohms (and is for CATV and TV applications), 60 ohms, 90 ohms, or anything else. The 50 ohm standard for RF transmission lines and interfaces came about a long time ago, and almost all RF & microwave test gear was built to accommodate that standard. Hence 50 ohms became a de-facto standard, and so to maximize power transfer source and load impedances need to both be 50 ohms.

EDIT 1 - added tutorial reference

Here's a nice tutorial that explains it mathematically:

https://www.tutorialspoint.com/network_theory/network_theory_maximum_power_transfer_theorem.htm

And it doesn't matter what direction the power is flowing. The need for the load to match the source for maximum power transfer is the same in both cases.

Answer 3

Good question. After reading the free "RF Design" magazine for many years, that after repeatedly/thoroughly reading "The Amateur Radio Handbook" and admiring those EIMAC 4CX-1000A triodes shown in the back, AND examining the primarily narrow-band behavior of RF circuits (antennas are NARROW BAND, maximum-power-transfer matching PI networks are NARROW BAND), I sat back and considered the impedance of 10pF of Cin (Cbe + Cob with Miller Effect) at 1,000 MHz.

That impedances is 16 ohms. Whereas dipoles are 73 ohms. And vertical whips are 37 ohms.

So we design for lowest added noise in the active circuits (the transistors) because that mindset provides the best possible Signal Noise Ratio, and SNR is the key to enjoyable music and minimal data-packet re-transmission requests.

And we achieve best SNR (to minimize "loss of signal" on your phone) by matching.

Answer 4

Fatal error in the question. One cannot control Zs without changing Vs at the same time, those quantities are coupled together. They both depend on the used antenna construction if the RF field is given and we assume the antenna is always directed for maximum available Vs at that place.

Of course the questioner were right if Zs and the caught Vs from a given RF field were independent, but they aren't except in case there's a series reactive part in antenna's Zs. Like another answer has already said, by inserting a negative external series reactance the total Zs becomes smaller and the receiver will get more power like the questioner expects.

Answer 5

I don't see a great answer to the original question here. The key reason to impedance match the antenna to reception is the same as the reason we match the antenna in transmit, but think of it Backwards!

When transmitting, power is coupled from the radio into the air.
When receiving, power is coupled from the air into the radio!

Ifimpedance doesn't match, power is reflected from the radio and not received. Our receive circuits have just as much a characteristic impedance as our transmit circuits do and if it isn't matched then we will lose receive efficiency!