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Eb/N0 Explained

Few subjects in RF design elicit as many blank looks as Eb/N0. Read the article and associated links below to find out more about this important subject!




What's All This Eb/No Stuff, Anyway?
By Jim Pearce (With Apologies to Bob Pease)

(This article originally appeared in the Fall 2000 issue of Spread Spectrum Scene Online.)


Anyone who has spent more than ten minutes researching digital communications has run across the cryptic notation Eb/No. Usually this shows up when discussing bit error rates or modulation methods. You may have a vague feeling that it represents something important about a digital communication system, but can't really put a finger on what or why. So let's take a look at just what this Eb/No thing is and why it's important.

First of all, how do you pronounce Eb/No? Most engineers that I know say "E bee over en zero," though some of the more fastidious ones say "E sub bee over en sub zero". At any rate, even though "No" is usually written with an "Oh" instead of a zero, it is not pronounced as the word "no".

Eb/No is classically defined as the ratio of Energy per Bit (Eb) to the Spectral Noise Density (No). If this definition leaves you with a empty, glassy-eyed feeling, you're not alone. The definition does not give you any insight into how to measure Eb/No or what it's used for.

Eb/No is the measure of signal to noise ratio for a digital communication system. It is measured at the input to the receiver and is used as the basic measure of how strong the signal is. Different forms of modulation -- BPSK, QPSK, QAM, etc. -- have different curves of theoretical bit error rates versus Eb/No as shown in Figure 1. These curves show the communications engineer the best performance that can be achieved across a digital link with a given amount of RF power.

bit error rate curve
Figure 1. BER vs Eb/No
(Thanks, Intersil for this figure)

In this respect, it is the fundamental prediction tool for determining a digital link's performance. Another, more easily measured predictor of performance is the carrier-to-noise or C/N ratio.

So let's pretend that we are designing a digital link, and see how to use Eb/No and C/N to find out how much transmitter power we will need. Our example will use differential quadrature phase shift keying (DQPSK) and transmit 2 Mbps with a carrier frequency of 2450 MHz. It will have a 30 dB fade margin and operate within a reasonable bit error rate (BER) at an outdoor distance of 100 meters. Hold on to your hat here! Remember that when we play with dB or any log-type operation, multiplication is replaced by adding the dBs, and division is replaced by subtracting the dBs.

Our strategy for determining the transmit power is to:
  • Determine Eb/No for our desired BER;
  • Convert Eb/No to C/N at the receiver using the bit rate; and
  • Add the path loss and fading margins.

We first decide what is the maximum BER that we can tolerate. For our example, we choose 10-6 figuring that we can retransmit the few packets that will have errors at this BER.

Looking at Figure 1, we find that for DQPSK modulation, a BER of 10-6 requires an Eb/No of 11.1 dB.

OK, great. Now we convert Eb/No to the carrier to noise ratio (C/N) using the equation:


Where:
fb is the bit rate, and
Bw is the receiver noise bandwidth. [EDITOR'S NOTE: See Phil Karn's comment below concerning this equation.]

So for our example, C/N = 11.1 dB + 10log(2x106 / 1x106) = 11.1 dB + 3dB = 14.1dB.

Since we now have the carrier-to-noise ratio, we can determine the necessary received carrier power after we calculate the receiver noise power.

Noise power is computed using Boltzmann's equation:

N = kTB

Where:
k is Boltzmann's constant = 1.380650x10-23 J/K;
T is the effective temperature in Kelvin, and
B is the receiver bandwidth.

Therefore, N1 = (1.380650x10-23 J/K) * (290K) *(1MHz) = 4x10-15W = 4x10-12mW = -114dBm

Our receiver has some inherent noise in the amplification and processing of the signal. This is referred to as the receiver noise figure. For this example, our receiver has a 7 dB noise figure, so the receiver noise level will be:

N = -107 dBm.

We can now find the carrier power as C = C/N * N, or in dB C = C/N + N.

C = 14.1 dB + -107dBm = -92.9 dBm

This is how much power the receiver must have at its input. To determine the transmitter power, we must account for the path loss and any fading margin that we are building in to the system.

The path loss in dB for an open air site is:

PL = 22 dB + 20log(d/λ)

Where:
PL is the path loss in dB;
d is the distance between the transmitter and receiver; and
λ is the wavelength of the RF carrier (= c/frequency)

This assumes antennas with no gain are being used. For our example,

PL = 22 dB + 20log(100/.122) = 22 + 20*2.91 =
22 + 58.27 = 80.27 dB

Finally, adding our 30 dB fading margin will give the required transmitter power:

P = -92.9 + 80.27 + 30 = 17.37 dBm = 55 mW

Our result, 55 mW, is well within a reasonable power level for spread spectrum links in the 2.4 GHz band. So we see that, in this example, our 100 meter range is a very reasonable expectation.

So, what is all this Eb/No stuff? Simply put, it's one of the "secrets" used by top RF design engineers to evaluate options for digital RF links, and is a crucial step in the design of systems that will meet performance expectations.




 
Comments from Phil Karn

From: Phil Karn To: Jim Pearce Sent: Monday, April 23, 2007 3:47 AM
Subject: Eb/No Explained


[Editor's Note: Phil is a Qualcomm engineer who is very well known in the radio community. His website is at www.ka9q.net, and has a number of articles of interest to electronics/wireless aficionados/practitioners.]

Hi Jim,

I found your article "What's All This Eb/No Stuff, Anyway?" while looking for references that would help me better explain this stuff.

It's a good paper, but I have a tiny little nit. Your first equation says:

C/N = Eb/No * fb/Bw, where

fb is the bit rate, and Bw is the receiver noise bandwidth

Usually I see this stated as

C/N = Eb/No * (R/B), where

R = bit rate B = channel bandwidth

I.e., "channel bandwidth" instead of "receiver noise bandwidth".

I see two problems with using receiver noise bandwidth in this equation. First, Eb/No is supposed to be a universal figure of merit for any kind of receiver, so it's measured at the receiver input terminals and is independent of anything inside that receiver. Different receiver designs for the same signal might use multiple filters with different shapes and bandwidths, but that would not affect the Eb/No of the signal at their inputs.

The other problem is that there's more than one definition of bandwidth. Noise bandwidth is just one of many. In fact, that's precisely why Eb/No is such a useful figure in the first place: it completely avoids arguments over the exact system bandwidth and/or which definition of bandwidth to use to measure it. No is the noise power spectral density in units of watts/Hz (or milliwatts/Hz), so the only filter bandwidth that's relevant is that of the spectrum analyzer being used to measure it.

The procedure I like for measuring Eb/No on the bench is to use an analyzer to measure the signal power with a resolution bandwidth wide enough to capture all of the signal. Then I turn off the signal source, turn on the noise generator, and measure the noise power on the analyzer with the resolution bandwidth set to the user data rate. (Naturally I have to ensure that both signal and noise swamp the analyzer's own noise).

Then I calculate Eb/No by simply subtracting the noise power measurement from the signal power measurement. Setting the analyzer RBW to the user data rate simplifies the calculation by causing the data rate and noise bandwidth terms to cancel and fall out of the equation.

I found your article while trying to explain to another person that his Eb/No measurement methods are wrong. This fellow claims to have invented a family of "ultra narrow band" modulation methods that are in fact ultra wide band (UWB) plus a very strong carrier that wastes most of the signal power. Among many other mistakes, he has fallen into the trap of confusing noise bandwidth with other, more relevant definitions of bandwidth, and his receivers have filters with noise bandwidths that are much smaller than the Nyquist rate. This is how he has fooled himself into thinking that his signals are narrow band.

Anyway, thanks again for the article you published way back in 2000.

Regards, Phil




Related Links

Intersil Tutorial on Basic Link Budget Analysis, by Jim Zyren and Al Petrick
Adobe Acrobat format -- 80K

Link Analysis with the Iridium System, MLDesign Technologies

Crosslink Channel Analysis (with the Iridium satellite), MLDesign Technologies

An Interesting Link Budget Analysis for the Mars Pathfinder

Williamson Labs Link Budgets using Satmaster Pro MK 4.0c






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