研究目的
To determine the fundamental frequency of the photoacoustic wave for designing more selective and narrowband pressure sensors, and to validate a theoretical model approach through experimental measurements.
研究成果
The theoretical model approach for determining the fundamental frequency of PA waves is validated experimentally with high accuracy (average ?4.212%, down to ?0.267%). This enables the design of more narrowband and selective PA pressure sensors. Analysis of laser parameters shows that pulse duration and beam width significantly affect the spectral content, guiding optimal parameter selection for sensitive detection.
研究不足
The study is limited to distilled water as the medium, which may not represent all possible applications. The theoretical model assumes free boundary conditions and spherical symmetry, which might not hold in all real-world scenarios. Experimental accuracy is affected by equipment limitations and environmental factors.
1:Experimental Design and Method Selection:
The study involves developing a theoretical model based on the frequency domain solution of the photoacoustic wave equation, improving upon previous work by Erkol et al. An experimental setup is established to validate this model using distilled water as the medium, with measurements of PA signals under various laser parameters.
2:Sample Selection and Data Sources:
Distilled water is used due to its known physical parameters and strong absorption at 1550 nm wavelength. Data is collected from PA signals generated by laser pulses.
3:List of Experimental Equipment and Materials:
Includes a diode laser (LPSC-1550-FC, Thorlabs Inc.), optical fiber (SMF-28-J9, Thorlabs Inc.), aspheric fiber collimators (CFS2-1550, CFS5-1550, Thorlabs Inc.), driver module (Picolas LDP-V 50-100 V3.3), arbitrary/function generator (AFG3021B, Tektronix), membrane hydrophone (HMA-0200, Onda Inc.), preamplifier (Boteg Inc.), final amplifier (AD8331-EVAL, Analog Devices Inc.), and oscilloscope/data logger (Picoscope 3206MSO).
4:3), arbitrary/function generator (AFG3021B, Tektronix), membrane hydrophone (HMA-0200, Onda Inc.), preamplifier (Boteg Inc.), final amplifier (AD8331-EVAL, Analog Devices Inc.), and oscilloscope/data logger (Picoscope 3206MSO). Experimental Procedures and Operational Workflow:
4. Experimental Procedures and Operational Workflow: The laser diode is pulsed using the driver module triggered by the function generator. PA signals are generated in distilled water, detected by the hydrophone, amplified, and measured with the oscilloscope. Frequency spectra are analyzed using FFT and processed with Matlab.
5:Data Analysis Methods:
Theoretical calculations are compared with experimental results. Frequency domain analysis is performed using FFT, and accuracy is assessed by comparing fundamental frequencies.
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Diode Laser
LPSC-1550-FC
Thorlabs Inc.
Light source for generating photoacoustic signals in distilled water.
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Optical Fiber
SMF-28-J9
Thorlabs Inc.
Transmission of laser beam to the experimental setup.
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Aspheric Fiber Collimator
CFS2-1550
Thorlabs Inc.
Collimating the laser beam for uniform illumination.
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Aspheric Fiber Collimator
CFS5-1550
Thorlabs Inc.
Collimating the laser beam for uniform illumination.
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Arbitrary/Function Generator
AFG3021B
Tektronix
Generating trigger pulses for the laser driver.
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Driver Module
Picolas LDP-V 50-100 V3.3
Driving the laser diode with pulsed signals.
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Membrane Hydrophone
HMA-0200
Onda Inc.
Detecting acoustic pressure waves in water.
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Preamplifier
Boteg Inc.
Amplifying the detected acoustic signals.
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Operational Amplifier
AD817
Analog Devices Inc.
Used in preamplifier design for signal amplification.
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Differential Line Driver
AD815
Analog Devices Inc.
Driving capacitive loads in the preamplifier.
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Voltage-Controlled Amplifier
AD8331-EVAL
Analog Devices Inc.
Final amplification of signals for high SNR.
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Oscilloscope/Data Logger
Picoscope 3206MSO
Measuring and analyzing acoustic signals, including FFT spectrum analysis.
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