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The Nyquist Plot
By
Don Davis
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The most informative frequency domain plot, by far, is the Nyquist
plot, Named after Harry Nyquist of Bell Telephone Laboratories,
famed for his work on feedback circuit analysis, the Nyquist plot
makes visual simultaneously the following viewpoints of the signal:
- The real part
- The imaginary part
- The magnitude
- The phase angle between the real and imaginary parts
- The polarity of the system
- The causality or non-causality of the time behavior
- The presence of resonant systems
- Non-signal synchronization by frequency
The Nyquist plot can be used in sound system work, where in acoustics
the real part is particle pressure and the imaginary part is particle
velocity (near a boundary or in a standing wave) and in impedance
measurements where the real part is the resistance and the imaginary
part is the reactance.

Fig. 1 - The analytic signal di5played
as a Heyser Spiral
Let’s label some key observations to be made about the Nyquist
plot of a pair of loudspeakers. Dennis Gabor proposed the “analytic
signal” which Richard Heyser developed into what has since
been named the Heyser Spiral. The Nyquist plot is the “end
view” shadow of the complex analytic signal

Fig. 2 - The “end view” of the Heyser Spiral (Nyquist)
An Interesting Anomaly
Apparent non-causal’ signals are being encountered more frequently
these days. A non-causal signal is one that arrives before it is
sent. Impossible you say? Yes, in the real world, to the best of
our knowledge that is true. But in the world of measurements, thanks
to digital technology, we find our measurements telling us a signal
is not causal Let’s look at an example:

Fig. 3 - ETC of a two-way loudspeaker.
Using the woofer arrival to set the reference time and measuring
the full-range response causes the Nyquist to rotate counterclockwise
above crossover.
We have a two-way loudspeaker with a crossover frequency of 2 kHz.
The energy-time curve (ETC) shows the tweeter arriving before the
woofer (Fig. 3). We now choose to call the woofer arrival the time
point of reference, while attempting to measure the full-range response.
When we do this our measurement instruments will see the tweeter
energy as arriving before we sent the signal and the Nyquist will
rotate counter clockwise above crossover, indicating non-causality
on the instrument, which is not aware that the woofer arrival was
chosen as the time reference. Note that in the diagram the cursor
is set at the point where the reverse rotation begins, the cursor
coordinates being indicated to the lower left of the plot. This
situation can also occur with a digital crossover net work where
one frequency range has one delay associated with it and the other
frequency range still another delay. In measuring phase response,
choice of a correct origin and time is paramount if you want a meaningful
measurement of the phase response of a device rather than a delayed
measurement of the signal path.
For a quick overview of the acoustic signature from a loudspeaker
array I know of no tool that is the peer of the Nyquist plot. When
large complex acoustic arrays require a rapid overview that will
allow analysis of what problems, if any, are present, the Nyquist
instantly tells which component relationships are incorrect, be
it signal synchronization, digital crossover or other delays not
obvious. Also obvious are inverted polaritys, unexpected resonances
or even measurement mistakes in choosing the correct signal origin.

The figure shows the Nyquist response of a bandpass filter
(loudspeaker or other). It consists of a number of discrete
data points determined by the FFT size.
Placing the cursor on the display
provides the following for the selected data point:
Frequency (Hz)
Phase (Degrees)
Magnitude (dB)
Real Part (Pascals)
Imaginary Pan (Pascals)
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The Nyquist plot, as embodied in contemporary acoustic analyzers,
usually computes at the bottom of the screen the values for frequency,
real part, imaginary part, phase, and magnitude for a given cursor
position on the screen. Moving the cursor allows clockwise or counter
clockwise frequency changes to be observed.
Ron Bennett, a number of years ago, provided me with a program
that allows acquisition of the real and imaginary part separately,
i.e., acoustically as pressure and velocity: electrically as voltage
and current; impedance as real and reactive. After acquisition it
then forms a complex analytic signal from those two parts for display.
One innovative use is to see the complex signal formed by the left
ear/right ear signals using ITE microphones.
What in 1928 was a truly laborious process, is in 1998 a major
convenience and an important tool. dbd
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