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Frequency Response
Estimating the
Frequency Response of Variable Reluctance Pressure Sensors in Gas
Electronic Response
The electronics associated with the pressure sensor provide power to
the sensing element, amplify the sensing element signal, and include
a low-pass filter for transducer output signal. Some sensing technolgies,
such as strain gage pressure transducers, have a DC excitation. Other
sensors, such as variable reluctance and capacitive sensors, require
an AC excitation and demodulation to provide a high-level DC output.
For AC sensing technologies the excitation carrier frequency will also
be a factor limiting dynamic response. Validyne variable reluctance
sensors use carrier excitation frequencies of 3 or 5 Khz, so this will
be the upper limit of dynamic pressure response. The low-pass output
filtering of the variable-reluctance demodultor may also limit dynamic
response. Typical cut-off frequencies for Validyne carrier demodulators
electronics vary from 1 Khz to less than 100 Hz, depending on the application
for which the transducer is intended. The output filter stages typically
roll-off at -12 to -18 dB/octave.
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Plumbing Response
Perhaps the most limiting factor in dynamic pressure response is the
second-order resonant system created by the tubing leading up to the
transducer combined with the pressure cavity of the sensor. The natural
frequency of this system depends on the volume of the sensor cavity,
the length and diameter of the tubing and the speed of sound in the
gas to be measured. The equation is shown.
Natural
Frequency of Plumbing as a Function of
Sensor Cavity Volume, Tubing Dimensions

Where: Wn = Natural Frequency,
Radian/Sec
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Fn = Natural Frequency,
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C = Velocity of Sound in Media,
Ft/Sec
a = Cross Sectional Area of Tubing, Sq Ft
Q = Transducer Cavity Volume, Cu Ft
L = Length of Tubing, Ft |
Validyne variable reluctance
transducers have very small sensor cavity volumes, 0.004 cu inches for
the DP15 and 0.01 cu inches for the DP45. Combined with short lengths
of tubing, these transducers offer very high dynamic response, even
over low pressure ranges.
As with the sensor natural
frequency, it is highly undesirable to attempt dynamic pressure measurements
at the natural frequency of the plumbing: severe distortion will occur
due to the amplification of the pressure waveform. This frequency at
which the distortion is tolerable depends on the damping in the system,
and this is a difficult variable to determine. The worst distortion
occurs when damping is slight, so assuming this, the maximum usable
frequency for any given plumbing system is generally taken to be one
fifth or one seventh of its natural frequency. Some typical values:
Lightly Damped System = 0.2 per unit
critical damping
At 100% Natural Frequency, Amplification
= 2 times input
At 50% Natural Frequency, Amplification = 1.25 times input
At 25% of Natural Frequency, Amplification = 1.05 times input
At 20% of Natural Frequency, Amplification = 1.03 times input
At 15% of Natural Frequency, Amplification = 1.02 times input
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DP15, DP45 Plumbing Tests
In order to test the relationship between the transducer sensor cavity
volume, tubing length and resulting natural frequency, the Validyne
DP15 and DP45 (14 In H20 FS pressure range) transducers were tested
using air and various lengths of 3/16 inch ID plastic tubing. Each transducer
was tested as follows:
The transducer and tubing
were pressured to approximately 7 In H2O with air. The three-way solenoid
valve was actuated, creating a step-pressure change on the system. The
transducer output was sampled at the rate of 5000 samples per second
with a UPC-based data acquisition system. The output was graphed for
each transducer and tubing length combination, and the natural frequency
determined from the period of the ringing part of the waveform. The
observed ringing frequency was compared with the calculated value.

A typical waveform captured is shown
below.

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