Noise SNR MDS Noise Power Density and NEP
The performance of any receiver is limited by both the smallest
and the largest signals it can receive.
On the low end, the receiver is limited by noise. On the high
end, the receiver is limited by the strongest signal it can receive
without producing spurious responses. Both of these topics are discussed in Ch. 14 of the text. We’ll begin with noise. Noise
Noise has many origins in a circuit. For a receiver, noise is
mostly thermally generated in resistors (including attenuators),
semiconductors, amplifiers, mixers and some filters. Noise is generally not associated with inductors or capacitors. Additionally, noise signals are also received through antennas.
This noise is generated by thunderstorms, galactic and solar
bodies, and manmade sources. Noise measured on an oscilloscope gives the familiar “grass” signature:
While the time average of this noise voltage is zero, its RMS
value is not zero:
where ? is an averaging time. This noise signal also has a time
average noise power Pn associated with it
where R is the load resistance. It really doesn’t make sense to talk about “peak-to-peak noise voltage” since noise is not sinusoidal. Rather, it’s some random waveform. Signal to Noise Ratio
A receiver’s audio output signal is characterized by its signal-tonoise ratio (SNR) defined as
where P is the audio RMS output power and Pn is the audio RMS noise power. Depending on your application, different receivers may require wildly different SNRs. Voice may require an SNR of 40:1, for example, while CW (Morse code) can be understood with an SNR approaching 1:1. mazing! Minimum Discernible Signal
A good all-around comparison of receiver performance is the
minimum discernible signal (MDS). MDS is the input signal power required to produce a 1:1 SNR at the output. this implies
P = Pn
Dividing (1) by the overall receiver gain G we find
To measure MDS in the lab, we generally do not directly apply
the definition (14.4). Instead, MDS is computed from two
receiver output (audio) measurements:
1. Pn of the receiver is measured (no input signal),
2. MDS for receiver noise is equal to the input signal power.
that doubles the output power (that is, to 2Pn).
In the lab, you’ll be measuring Vrms. Therefore, you need to measure the input signal power that increases the output voltage by 2 in order to compute MDS. Laboratory Arrangement for MDS Measurement
In Prob. 34 “Receiver Response” you’ll measure a number of
receiver characteristics including MDS for receiver noise, and
again later for antenna noise. The experimental arrangement for this measurement is shown in :
Your equipment layout will look something similar to this:
It’s worthwhile to connect the counter to the speaker. Other
important points related to this problem include:
1. You will need to work with pairs of receivers, so find a
partnering team. One transceiver acts as the transmitter,
while yours is the receiver. Then interchange the radios and
repeat the measurements.
2. A battery powers the transmitter. We’re dealing with very
small signals in these measurements so we don’t want
signal coupling through the ac line.
3. You will use a Kay 839 attenuator. A toggle “up” adds that
amount of attenuation to the line:
Decibels Above 1 mW (dBm)
Throughout these measurements, you’ll be dealing with signals
having average powers expressed in units of dBm. This is
shorthand for “dB referenced to 1 mW.” That is:
As an example, let’s determine the absolute power given by -40
Noise Power Density and NEP
The noise power Pn does not appear at just one frequency. Instead, noise power is distributed over a range of frequencies. In recognition of this, noise power density N is defined as the noise power per unit bandwidth (W/Hz) as:
Pn = N ? B [W]
where B is a chosen bandwidth. We’ll assume that N is constant
here – which is certainly a reasonable approximation when B is
small, say for a narrow band receiver such as the NorCal 40A.
This is important: We see from (14.5) that output (i.e., audio)
noise power is proportional to bandwidth (BW). Some receivers
actually have BW switches to choose a wider or narrower BW
filter for different situations:
1. A wide BW for ease of locating stations,
2. A narrow BW for reducing noise.
We can now see that the MDS we defined earlier as
will depend on the bandwidth of the receiver since Pn is proportional to B in It is useful to have a measure of the receiver performance that is independent of BW. Why? Because BW is determined primarily by filters, but filters contribute little to receiver noise (mixers and amplifiers are the major contributors). In this vein, noise equivalent (input) power density (NEP) is defined as
Comparing this definition with (14.4), we can see that NEP is
similar to MDS in that NEP is related to N in the same manner
as MDS is related to Pn. NEP is simply all receiver output noise density referred to the receiver input. In Prob. 34F you will measure N and NEP for your receiver. Notice that for Probs. 34F through 34I you will not need the first NorCal 40A for input. To determine NEP, it’s useful to have a source that supplies noise of a given RMS level with a specified bandwidth.
Your Agilent 33120A provides such a signal. Select the “Noise”
button and enter the power in dBm or the corresponding Vrms.Do NOT enter a p-t-p value since this doesn’t make sense for noise signals.