| Motore di ricerca datesheet componenti elettronici |
|
CS-TC09 Scheda tecnica(PDF) 1 Page - Wavelength Electronics, Inc. |
|
|
|||||||||||||||||||||||||||||
CS-TC09 Scheda tecnica(HTML) 1 Page - Wavelength Electronics, Inc. |
|
1 / 5 page ![]() © 2024 • Sales & Technical Support: (406) 587-4910 • email: sales@teamWavelength.com • web: www.teamWavelength.com Case Study CS-TC09 Rev. A Simultaneous Multi- Gas Detection Using ICL Photoacoustic Spectroscopy May, 2024 Page 1 ABSTRACT Researchers from China have developed and demonstrated a simultaneous, multi-component gas detection system based on differential Helmholtz resonance spectroscopy with a mid-infrared, tunable, interband cascade laser (ICL). The first harmonic demodulation method was used under ambient pressure to detect three light carbon gases: CH 4, C2H4, and C2H6. Using this photoacoustic system, the detection limits reached 98.8 ppb, 252 ppb, and 33 ppb for methane, ethylene, and ethane, respectively. Multi- wavelength linear regression was implemented to reduce the effects of cross-interference of the three gases, maintaining the accuracy of the gas concentration measurements. This new method, using an ICL with a Helmholtz resonator, provides a simple and fast multiple gas detection technique for atmospheric research, medicine, the food industry, pollutant monitoring, and the power industry. PHOTOACOUSTIC SPECTROSCOPY Photoacoustic spectroscopy (PAS) is a common technique for trace gas detection, reaching concentration levels as low as part-per-billion and part-per-trillion levels. Instead of using scattered light or absorption spectrum from molecules, PAS uses acoustic detection to measure the effect of light on a sample. These designs include microphones or tuning forks in the acoustic detection module or near the resonator chamber to transduce the acoustic signal into an electrical signal. Multiple wavelengths of light will produce a photoacoustic spectrum and can be used to identify the components in a sample. PAS, as an indirect detection method, can be advantageous with high detection sensitivity, good selectivity, fast detection speed, and long service life.1 These benefits are critical for reaching part-per-billion detection levels of trace gases in the atmosphere or lab environment. PAS has been widely used in atmospheric research, medicine, the food industry, pollutant monitoring, and the power industry.1 However, most systems are designed to detect only a single gas, not multiple components simultaneously. A single device that can measure multiple gases in real-time can provide safety, environmental, and economic benefits in research laboratories, field experiments, or even residential applications. The light source to generate the photoacoustic effect has recently improved with the invention of tunable lasers and, specifically, quantum cascade lasers (QCLs) with narrow linewidths for higher sensitivity. Along with the laser, the photoacoustic cell and pressure sensor are critical factors affecting the detection performance of PAS.1 PROBLEMS AND GOALS Simple mid-infrared lamps and single-wavelength laser arrays have achieved multiple gas detection, but they require mechanical or optical accessories to accomplish wavelength switching. To achieve multiple component detection with a single laser, tunable lasers, such as CO 2 gas lasers and QCLs, can be used to cover a wide range of wavelengths. Wider wavelength ranges provide a better selection of absorption signal wavelengths of specific gases. Although QCLs have advanced the PAS capabilities with extremely narrow linewidths and large tuning ranges, they require a large threshold current to operate. Interband cascade lasers (ICLs) allow each injected electron to be reused at a forward bias to emit multiple photons and decrease this threshold current and total required electrical input power.1 A major issue with multiple gas detection when compared to single gas detection is cross-interference. Some absorption peaks of different gases may be relatively close in wavelength, and this may cause the pressure sensor to decrease in accuracy in detecting concentrations of multiple gases. The photoacoustic cell and pressure sensor directly correlate to cross-interference. Some PAS designs utilize quartz tuning forks and cantilever beams to detect pressure changes due to sample absorption of light with high sensitivity. A high-pressure cell may be required to contain these devices, increasing frequency noise and cross-interference and leading to frequent inaccurate measurements. Temperature and high cost can also deter researchers from using these systems. A better, more efficient, lower cost, and highly sensitive design is needed for simultaneous multi-gas detection with PAS designs. |
Codice articolo simile - CS-TC09 |
|
Descrizione simile - CS-TC09 |
|
|
|
Link URL |
| Lei ha avuto il aiuto da alldatasheet? [ DONATE ] |
Di alldatasheet | Richest di pubblicita | contatti | Privacy Policy | Collegamento alla scheda tecnica | scambio Link | Ricerca produttore All Rights Reserved©Alldatasheet.com |
| Russian : Alldatasheetru.com | Korean : Alldatasheet.co.kr | Spanish : Alldatasheet.es | French : Alldatasheet.fr | Italian : Alldatasheetit.com Portuguese : Alldatasheetpt.com | Polish : Alldatasheet.pl | Vietnamese : Alldatasheet.vn Indian : Alldatasheet.in | Mexican : Alldatasheet.com.mx | British : Alldatasheet.co.uk | New Zealand : Alldatasheet.co.nz |
|
Family Site : ic2ic.com |
icmetro.com |