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This discussion is open for a limited time. Please review, comment and vote for the individual sections. You can quote certain parts of a paragraph by marking the text and open a comment.
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LATEST ACTIVITY
LEVEL OF AGREEMENT
MOST DISCUSSED PARAGRAPHS
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P45 • Range 1The range, usually expressed as ”±_
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P40 • Dead volume 1For non-flush-mounted transdu
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P29 Piezoelectric pressure transducers offer man
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P42 • Capacitance vs. temperature 1This may be g
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P26 Transverse means that the charge is collecte
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P37 Outline:This chapter should contain an overv
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P91 Outline:Description of conditions within dif
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P86 One way of mitigating the influence of pipe
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P46 • Life, cyclingExpressed as ”__ full scale o
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P43 The following performance characteristics, u
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P4 Measuring dynamic pressures within the varyi
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P41 • Capacitance 1The capacitance of the transd
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LATEST COMMENTS
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Pressure transducer should be although as near as possible to the hot gas, to avoid wave distortion due to non-linear effect. I think it is better to develop in this direction, rather than to try to develop a sensor which should sustain > 700 °C. The sensor can be placed in the volume with cooling air. Such layout can also allow to install several sensors (for redundant), and it may also be possible to send calibration signal from outside
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I agree the comment of Lukas, and it is important. For a stationary signal (like combustor pulsation measurement) polarity is not important (so far all applied sensors are equipped with a same chain), but for a transient measurement, (like compressor surge, or rotating stall) it is important to note the polarity. When the sensor producer supply also an amplifier, the polarity of voltage signal should be noted.
MOST ACTIVE USERS


P295
Mounting Resonant Frequency – The aerodynamically driven resonant frequencies due to transducer mounting at the point of measurement, e.g. recess/standoff pipe with transducer mounted at pipe termination resulting in organ pipe resonance. A formula to determine the frequencies can be found below. In the formula L is the length of the tube, c is the speed of sound of the measured fluid and n is a factor for calculating the resonant frequencies. Figure 12.7 shows the case of a recess mounted transducer.
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P298
Natural Frequency 1 – The frequency of free (not forced) oscillations of the sensing element of a fully assembled transducer.
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P299
NOTE: It is also defined as the frequency of an applied sinusoidal measurand at which the transducer output lags the measurand by 90 degrees. NOTE: Applicable at Room temperature unless otherwise specified.
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P300
NOTE: Also see resonant frequency and ringing frequency which are considered of more practical value than Natural frequency.
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P301
Package Resonant Frequency, fr – The aerodynamic driven resonant frequencies due to sensor packaging, e.g. Helmholtz resonance or Modified Helmholtz resonance. The Modified Helmholtz resonance equation appears below along with a depiction of a packed MEMS transducer in Figure 12.8.
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P304
Phase Response – The phase of the transfer function versus frequency. In the time domain, phase influences the instantaneous shape of the response to an input signal and contributes to a time lag in transducer response [23]. The phase response characterizes the frequency dependent time lag of the pressure signal due to mounting and/or packaging resonances, and in some instances the resonant frequency (also referred to as natural frequency) of the sensing element.
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P305
Phase Shift – The delay, defined in terms of angular degrees or radians, characterizing the how the output measured lags behind a dynamic measurand.
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P306
Resonant Frequency 1 – The measurand frequency at which a transducer responds with maximum output amplitude.
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P307
NOTE: When major amplitude peaks occur at more than one frequency, the lowest of the frequencies is the resonant frequency.
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P308
NOTE: A peak is considered major when it has an amplitude at least 1.3 times the amplitude of the frequency to which specified Frequency response is referred.
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P309
Ringing Frequency – The frequency of free oscillations in the transducer output results from a step change in measurand. The ringing frequency is indicated by the number of oscillations per unit time. For the linear second-order transducer, the ringing frequency fr is related to the natural frequencyn fn and depending on the damping ratio ζ shown by following formula:
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P311
Spatial Resolution – The frequency response of a transducer based upon the finite diaphragm size over which dynamic pressures are averaged and the angle of incidence of dynamic pressure waves[20][27][28][29]. The equation and figure below exhibit this spatial resolution of several transducer diameters over frequency.
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P312
NOTE: Example for Spatial Resolution. At a 90 deg. Angle of incidence, dynamic pressures are averaged across the diaphragm such that as the wavelength of the dynamic pressure approaches the sensor’s diaphragm active length e.g. diameter or width, the sensor exhibits attenuation of dynamic pressures as they are averaged across the diaphragm.
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