Photoacoustic spectroscopy system and technique for remote sensing of explosives and toxic chemicals

• US 7,644,606 B2
• Filed: 01/29/2007
• Issued: 01/12/2010
• Est. Priority Date: 01/29/2007
• Status: Expired due to Fees

• Current Assignee: UChicago Argonne LLC
• Original Assignee: UChicago Argonne LLC
• Inventors: Raptis, Apostolos C., Sheen, Shuh-Haw, Chien, Hual-Te
• Primary Examiner(s): Caputo; Lisa M
• Assistant Examiner(s): ROY, PUNAM P
• Application Number:
  US11/699,146
• Publication Number:
  US 20080180675A1
• Time in Patent Office: 1,079 Days
• Field of Search: 73/240.2, 73/240.6
• US Class Current: 73/24.02
• CPC Class Codes: G01N 2021/1793 Remote sensing
• CPC Class Codes: G01N 21/1702 with opto-acoustic detection, e.g. for gases or analysing solids
• CPC Class Codes: G01N 2291/014 Resonance or resonant frequency
• CPC Class Codes: G01N 2291/0255 (Bio)chemical reactions, e.g. on biosensors
• CPC Class Codes: G01N 29/2418 using optoacoustic interaction with the material, e.g. laser radiation, photoacoustics photoacoustic cells G01N21/1702; measuring characteristics of vibrations by using radiation-sensitive means G01H9/00; acousto-optical conversion techniques for short-range imaging G01S15/8965; sound-producing devices using laser bundle G10K15/046

Abstract

A user-friendly photoacoustic spectroscopy (PAS) system and process (technique) provides an open-field PAS instrument, unit and device to remotely sense explosives, chemicals and biological agents. The PAS system and process can include: a pulsed tunable laser, such as a CO₂ laser, a reflector, such as a parabolic reflector, an acoustic reverberant resonator in which a microphone is installed, and a data acquisition and analysis system.

Claims

1. A photoacoustic spectroscopy (PAS) system for remote sensing of a remote target comprising chemicals providing explosives, comprising:

a tunable laser for transmitting optical energy comprising laser pulses at a selected frequency to the remote target and causing acoustic signals to be emitted from the target;

a pulse generator comprising a chopper operating at a frequency selected on the basis of background noise for generating pulses to said tunable laser;

a sensor for detecting acoustical signals from the target;

a parabolic reflector for receiving acoustic signals from the target and focusing the acoustic signals to a focal area comprising said sensor;

a cylindrical resonator for reducing acoustic interference and amplifying the acoustic signals, said cylindrical resonator providing an acoustic reverberant resonator comprising a cylindrical tube having an open end and a partially blocked end, the open end of the cylindrical tube being positioned at the local length of the parabolic reflector, the cylindrical tube being elongated and extending a length, the length of the cylindrical tube being adjustable to match a resonance condition in which the length of the cylindrical tube is equal to a multiple number of half acoustic wavelength according to the formula

l=nλ

/2

wherein

l=length of the cylindrical tube

n=integer

λ

=wavelength

and the wavelength is equal to the sound velocity divided by a laser chopper frequency; and

data acquisition and analysis equipment operatively connected and cooperating with said sensor, reflector, resonator, tunable laser, and pulse generator, for determining information about the target.

2. A photoacoustic spectroscopy (PAS) system for remote sensing of a remote target comprising chemicals providing explosives, comprising:

a tunable laser for transmitting optical energy comprising laser pulses at a selected frequency to the remote target and causing acoustic signals to be emitted from the target;

a pulse generator comprising a chopper operating at a frequency selected on the basis of background noise for generating pulses to said tunable laser;

a sensor for detecting acoustical signals from the target;

a reflector for receiving acoustic signals from the target and focusing the acoustic signals to a focal area comprising said sensor;

a resonator for reducing acoustic interference and amplifying the acoustic signals;

data acquisition and analysis equipment operatively connected and cooperating with said sensor, reflector, resonator, tunable laser, and pulse generator, for determining information about the target; and

wherein said resonator comprises an acoustic reverberant resonator comprising a cylindrical tube having an open end and a partially blocked end, said reflector comprising a parabolic reflector having a focal length, the open end of the cylindrical tube being positioned at the focal length of the parabolic reflector, an acoustic transducer providing a microphone positioned in the cylindrical tube, and the cylindrical tube being elongated and extending a length, the length of the cylindrical tube being adjustable to match a resonance condition in which the length of the cylindrical tube is equal to a multiple number of half acoustic wavelength according to the formula

l=n λ

/2

wherein

l=length of the cylindrical tube

n=integer

λ

=wavelength

and the wavelength is equal to the sound velocity divided by a laser chopper frequency.

3. A PAS system in accordance with claim 2 wherein:

said tunable laser is a carbon dioxide (CO₂) infrared (IR) laser; and

said chemicals providing explosives are selected from the group consisting of nitroglycerine (NG), ethylene glycol dinitrate (EGNG), dinitroltoluene (DNT), trinitrotoluene (TNT), and ammonium nitrate (NH₄NO₃).

4. A PAS system in accordance with claim 2 wherein said parabolic reflector has a diameter proportional to a distance to the target.

5. A PAS system in accordance with claim 2 wherein said resonator comprises a cylindrical tube resonator having a resonant frequency equaling the laser chopper frequency.

6. A photoacoustic spectroscopy (PAS) process for remote sensing of a remote target comprising chemicals providing explosives, comprising:

providing an open-field acoustic resonator comprising an acoustic reverberant resonator with a cylindrical tube having an open end and a partially blocked end, and a parabolic reflector having a focal length, positioning the open end of the cylindrical tube at the focal length of the parabolic reflector, positioning an acoustic transducer in the cylindrical tube, adjusting the length of the cylindrical tube to correspond to a resonance condition in which the length of the cylindrical tube is equal to a multiple number of half acoustic wavelength according to the formula

l=nλ

/2

wherein

l=length of the cylindrical tube

n=integer

λ

=wavelength

and the wavelength is equal to the sound velocity divided by a laser chopper frequency;

transmitting optical energy comprising laser pulses at a selected frequency from a tunable laser in cooperation with a pulse generator comprising a chopper to the remote target comprising the chemicals providing the explosives, said chemicals being in a state selected from the group consisting of gases, liquids, solids, and combinations thereof;

emitting acoustic signals from the target;

the acoustic signals resonating at the laser chopper frequency or the harmonics of the laser;

receiving acoustic signals from the target on the parabolic reflector;

focusing the acoustic signals to the focal area at the open-field acoustic resonator;

detecting the acoustic signals with the open-field acoustic resonator that is resonating at the laser chopper frequency or the harmonics of the laser;

adjusting the resonator to optimize intensity of the acoustic signal; and

determining information about the target with data acquisition and analysis equipment.

7. A PAS process in accordance with claim 6 wherein:

said chemicals providing the explosives are selected from the group consisting of nitroglycerine (NG), ethylene glycol dinitrate (EGNG), dinitroltoluene (DNT), trinitrotoluene (TNT), and ammonium nitrate (NH₄NO₃).