Geophysical Monitoring for Geologic Carbon Storage. Группа авторов
Чтение книги онлайн.

Читать онлайн книгу Geophysical Monitoring for Geologic Carbon Storage - Группа авторов страница 32

Название: Geophysical Monitoring for Geologic Carbon Storage

Автор: Группа авторов

Издательство: John Wiley & Sons Limited

Жанр: География

Серия:

isbn: 9781119156840

isbn:

СКАЧАТЬ Frequency Modulated Spectroscopy

Schematic illustration of a FMS instrument produces sidebands (ωc ± ωm) shifted from the carrier (laser) wavelength (ωc) (based on Bjorklund & Levenson, 1983).

      3.2.2. Standoff or Remote Methods

      The number of remote sensing possibilities is limited compared with the in situ methods, and we are not aware of any commercially available instruments. Various LIght Detection And Ranging (LIDAR) methods have been developed and demonstrated including Differential Absorption LIDAR (DIAL). The FMS technique has been developed and demonstrated in several configurations including LIDAR.

      LIDAR fundamentally involves directing a pulsed nanosecond laser through the gaseous sample in the atmosphere (Johnson et al., 2013). Some of this laser light is scattered off dust and aerosols and some of that scattered laser light is directed back toward a collection telescope and recorded. The amount of scattered light is very weak and requires very sensitive detectors. The scattered laser intensity is recorded as a function of time and one can convert the signal as a function of time to distance based on the speed of light. The intensity of scattered light is also proportional to the concentration of species that absorbed the light over the path length of the light. With most laser powers, one can achieve LIDAR detection at hundreds to thousands of meters. However, the range resolution required to identify the location of a leak requires short and accurate temporal resolution and is generally limited by the detector sensitivity.

      At Los Alamos National Laboratory (LANL), FMS has been developed into both a “remote” and LIDAR instrument that was designed to measure both the major and minor carbon isotopes. Here, we define remote as an experiment that involves directing the laser to a hard target such as a wall, a geologic surface, or a mirror/corner cube. The intensity of light scattered or reflected off a hard surface is significantly brighter than the light scattered off dust and aerosols used to detect a LIDAR instrument. The same modulated laser discussed in the in situ instrument above is directed through the sample in the field and the signal returned from the hard target is recorded rather than recording the range resolved signal. While this method produces the most sensitive record of CO2 concentration over the long path length, this technique is limited to locations where a hard target is available.

      An FMS LIDAR‐capable instrument fundamentally can accomplish all of the requirements discussed in the introduction. A LIDAR instrument capable of stable isotope sensitivity would distinguish natural CO2 sources from CO2 seepage to the surface and would have some capability to locate the source with the ranging capability.

Photo depicts the in situ FMS instrument built at Los Alamos National Laboratory enclosed in a weatherproof case for field deployment.

      An open‐path remote instrument was developed using the same optical system discussed for the in situ system above. The same model New Focus TDL was fiber optically coupled to a 5x beam expander used to collimate an enlarged beam. The modulated beam was directed to a retroreflector placed up to hundreds of meters away from the beam expander. The returned laser beam was collected with a second beam expander, coupled to a second optical fiber and onto the New Focus detector.

      Superimposing a periodic (sinusoidal) frequency upon a light wave having a base, or carrier, frequency of ω o results in a frequency modulated wave described by

      (3.2)upper E left-parenthesis t right-parenthesis equals upper E 0 exp left-brace i left-parenthesis omega 0 t plus upper M sine left-parenthesis omega Subscript m Baseline t right-parenthesis right-brace

      where E o is the electric field amplitude, t is time, M is the modulation index (or strength) of the imposed periodic variation, and ω m is the frequency of the periodic “dithering” frequency. When passed through a sample, both absorption and dispersion of the wave occur. To account for these, convention is to use a complex valued frequency‐dependent transmission СКАЧАТЬ