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Electrical Communications

Receiver noise: noise figure, sensitivity and Friis's formula

Structure of a communication system, decibels and dBm, thermal noise at −174 dBm/Hz, noise figure and equivalent temperature, sensitivity, Friis's formula with proof, link margin.

A communication system carries information from a source to a destination through a channel that attenuates, distorts and adds noise. Designing a link often comes down to one question: does the signal reach the receiver sufficiently stronger than the noise? In this lesson we look at the general structure of a system, decibel units, receiver noise with noise figure and equivalent temperature, and Friis’s formula for chains of stages.

The structure of a system

Transmitter: the source produces the information, the source encoder compresses it, the channel encoder adds redundancy to correct errors, the modulator turns it into a signal suited to the channel. The channel (a cable, a fibre, free space) attenuates and disturbs. The receiver goes back along the chain: demodulator, channel decoder, source decoder. The Signal Theory lessons covered modulation and detection; here we look at the system from the point of view of the engineer who must make it work.

Decibels

In communications quantities span many orders of magnitude, and decibels are used: a power ratio P_2/P_1 is 10\log_{10}(P_2/P_1) dB. Absolute powers are expressed relative to one milliwatt: dBm. 0 dBm = 1 mW, 30 dBm = 1 W, −90 dBm = 1 pW. The advantage is that cascaded gains and losses add: a 20 dBm transmitter, a 2 dBi antenna, 80 dB of free-space path loss and a 2 dBi receiving antenna give 20 + 2 - 80 + 2 = -56 dBm (Electromagnetic Fields lesson on antennas).

The noise floor

Any resistance at temperature T produces thermal noise with available power density kT (lesson on random processes). At T_0 = 290 K:

    \[ kT_0 = 1.38\cdot 10^{-23}\cdot 290 \approx 4\cdot 10^{-21}\ \text{W/Hz} = -174\ \text{dBm/Hz} \]

It is the most important number in radio communications. Over a bandwidth B the noise power is kT_0B: in 20 MHz (a Wi-Fi channel) it is -174 + 10\log_{10}(2\cdot 10^7) \approx -101 dBm. No receiver can do better.

Noise figure

Every stage of a receiver adds its own noise. The noise figure F measures how much the signal-to-noise ratio worsens through it:

    \[ F = \frac{\mathrm{SNR}_{in}}{\mathrm{SNR}_{out}}\quad (\text{with a source at } T_0),\qquad NF = 10\log_{10}F \]

An ideal amplifier has F = 1 (0 dB). Equivalently the equivalent noise temperature T_e = (F - 1)T_0 is used: the noise added by the stage is what a resistance at temperature T_e at the input would produce. An amplifier with NF = 1 dB has T_e \approx 75 K. Equivalent temperature is preferred for very low-noise receivers, such as satellite and radio-telescope ones.

Sensitivity. The minimum signal a receiver can demodulate is

    \[ P_{min} = -174\ \text{dBm/Hz} + 10\log_{10}B + NF + \mathrm{SNR}_{min} \]

Example. 20 MHz bandwidth, NF = 5 dB, minimum SNR 10 dB: P_{min} \approx -174 + 73 + 5 + 10 = -86 dBm.

Friis’s noise formula

Chain of receiver stages with their gains and noise figures
The signal from the antenna passes in turn through the low-noise amplifier, the mixer and the intermediate-frequency amplifier, each with its own gain G and noise figure F. The overall noise figure is given by Friis’s formula.

Theorem. The noise figure of cascaded stages is

    \[ F = F_1 + \frac{F_2 - 1}{G_1} + \frac{F_3 - 1}{G_1G_2} + \dots \]

Proof. Refer everything to the input. The first stage adds noise equivalent to T_{e1}. The second adds T_{e2} at its input, where the signal has already been amplified by G_1: referred to the first stage’s input it is T_{e2}/G_1. Likewise the third contributes T_{e3}/(G_1G_2). So T_e = T_{e1} + T_{e2}/G_1 + T_{e3}/(G_1G_2) + \dots, and with T_e = (F - 1)T_0 the formula follows. ∎

The consequence. The first stage almost alone matters, as long as it has enough gain. With a low-noise amplifier (LNA) of NF = 1 dB and 20 dB of gain, followed by a 10 dB mixer with 6 dB of loss and a 4 dB amplifier, the overall figure is about 1.5 dB. With the mixer first, it would be over 10 dB: 9 dB of sensitivity lost: in free space the range would drop to about a third. That is why LNAs are placed as close as possible to the antenna, and in satellite dishes they sit in the converter mounted right at the focus.

Passive losses before the first amplifier (a cable, a filter) also have a noise figure equal to their attenuation: 2 dB of cable before the LNA add 2 dB to the system noise figure.

The complete link budget

Putting together transmitted power, antenna gains, propagation losses and receiver sensitivity gives the link margin: how many extra decibels of attenuation (rain, walls, fading) can be tolerated. A Wi-Fi link with −56 dBm received and −86 dBm sensitivity has 30 dB of margin; a satellite link often works with a few decibels, and modern systems continuously adapt modulation and coding to the available margin.

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