- •Chromatography
- •Manual chromatography methods
- •Automated chromatographs
- •Chromatograph detectors
- •Measuring species concentration
- •Industrial applications of chromatographs
- •Chromatograph sample valves
- •Improving chromatograph analysis time
- •Introduction to optical analyses
- •Dispersive spectroscopy
- •Non-dispersive Luft detector spectroscopy
- •Luft detectors
- •Filter cells
- •Gas Filter Correlation (GFC) spectroscopy
- •Laser spectroscopy
- •Fluorescence
- •Chemiluminescence
- •Analyzer sample systems
- •Safety gas analyzers
- •Oxygen gas
- •Lower explosive limit (LEL)
- •Carbon monoxide gas
- •Chlorine gas
- •Review of fundamental principles
- •Machine vibration measurement
- •Vibration physics
- •Sinusoidal vibrations
- •Vibration sensors
- •Monitoring hardware
- •Mechanical vibration switches
- •Review of fundamental principles
- •Electric power measurement and control
- •Introduction to power system automation
- •Electrical power grids
- •Interconnected generators
- •Circuit breakers and disconnects
- •Reclosers
- •Electrical sensors
- •Potential transformers
- •Current transformers
- •Transformer polarity
- •Instrument transformer safety
- •Instrument transformer test switches
1816 |
CHAPTER 23. CONTINUOUS ANALYTICAL MEASUREMENT |
23.5Dispersive spectroscopy
The dispersion of visible light into its constituent colors goes all the way back to the 17th century with Isaac Newton’s experiments, taking a glass prism and generating the characteristic “rainbow” of colors:
|
Prism |
White light |
Red |
|
Orange |
|
Yellow |
|
Green |
|
Blue |
|
Violet |
A modern variation on the theme of a solid glass prism is a thin di raction grating, causing light of di erent wavelengths to “bend” as they pass through a series of very thin slits:
Diffraction grating
White light
Red
Orange
Yellow
Green
Blue
Violet
Violet
Blue
Green
Yellow
Orange
Red
23.5. DISPERSIVE SPECTROSCOPY |
1817 |
Some dispersive analyzers use a reflection grating instead of a refraction grating. Reflection gratings use fine lines etched on a reflective (mirror) surface to produce an equivalent dispersive e ect to a di raction grating40:
|
Red |
|
|
Orange |
Reflection grating |
|
Yellow |
|
|
|
|
|
Green |
|
White light |
Blue |
|
Violet |
|
Violet
Blue
Green
Yellow
Orange
Red
In 1814, the German physicist Joseph von Fraunhofer closely analyzed the spectrum of colors obtained from sunlight and noticed the existence of several dark bands in the otherwise uninterrupted spectrum where specific colors seemed to be attenuated. Later that century, experiments by the French physicist Jean Bernard L´eon Foucault and the German physicist Gustav Robert Kircho confirmed the same e ect when white light was passed through a vapor of sodium. They correctly reasoned that the sun’s core produced a continuous spectrum41 of light (all wavelengths) due to its
40You may use an old compact disk (CD) as a simple reflection and refraction grating. Holding the CD with the reflective (shiny) surface angled toward you, light reflected from a bright source such as a lamp (avoid using the sun, as you can easily damage your eyes viewing reflected sunlight!) will split into its constituent colors by reflection o the CD’s surface. Lines in the plastic of the CD perform the dispersion of wavelengths. You will likely have to experiment with the angle you hold the CD, pointing it more perpendicular to the lamp’s direction and more angled to your eyes, before you see the image of the lamp “smeared” as a colorful spectrum. To use the CD as a di raction grating, you will have to carefully peel the reflective aluminum foil o the front side of the disk. Use a sharp tool to scribe the disk’s front surface from center to outer edge (tracing a radius line), then use sticky tape to carefully peel the scribed foil o the plastic disk. When you are finished removing all the foil, you may look through the transparent plastic and see spectra from light sources on the other side. Once again, experimentation is in order to find the optimum viewing angle, and be sure to avoid looking at the sun this way!
41One might wonder why the sun does not produce a line-type emission spectrum of all its constituent elements, instead of the continuous spectrum it does. The answer to this question is that emission spectra are produced only when the “excited” atoms are in relative isolation from each other, such as is the case in a low-pressure gas. In solids, liquids, and high-pressure gases, the close proximity of the atoms to each other creates many di erent opportunities for electrons to “jump” to lower energy levels. With all those di erent alternatives, the electrons emit a whole range of di erent wavelength photons as they seek lower energy levels, not just the few wavelengths associated with the limited energy levels o ered by an isolated atom. We see the same e ect on Earth when we heat metals: the electrons in a solid or liquid metal sample have so many di erent optional energy levels to “fall” to, they end up emitting a broad spectrum of wavelengths instead of just a few. In this way, a molten metal is a good approximation of a blackbody photon source.
1818 |
CHAPTER 23. CONTINUOUS ANALYTICAL MEASUREMENT |
incredibly high temperature, but that certain gaseous elements (including sodium) in the cooler, outer “atmosphere” of the sun were absorbing some of the wavelengths to cause the Fraunhofer lines in the observed spectrum. These scientists noted the same patterns of absorption (dark lines) in the sun’s spectrum that appeared in laboratory absorption tests with sodium. The implication of these scientists’ experiments are truly staggering, as they were able to correctly identify gaseous elements in a sample 93 million miles distant from Earth!.
This sort of spectrographic analysis is called dispersive, because it relies on a device such as a prism or di raction grating to disperse the di erent wavelengths of light from each other so they may be independently measured.
A dispersive analyzer for process fluids would be constructed in this manner, introducing incident light to a windowed sample chamber where some wavelengths of that light would be attenuated by interaction with the process fluid molecules. In this illustration, the sample gas absorbs some of the yellow light wavelengths, resulting in less yellow light reaching the detector array:
Diffraction grating
White light
Detector
Sample |
Sample |
gas in |
gas out |
The light source need not output white light if the wavelengths of interest do not span the entire visible spectrum. For example, if the absorption spectrum of a particular substance is known to primarily span infrared light and not the visible range, it may be su cient to use a dispersive analyzer with an infrared light source rather than a “broad spectrum” light source covering both the infrared and visible ranges.
A necessary component of any dispersive analyzer is a computer connected to the detector array with the ability to recognize all expected emission spectra patterns, and quantify them based on the relative strengths of the detected wavelengths. This is a level of sophistication beyond most industrial measuring instruments at the time of this writing (2015), which is one reason dispersive analyzers are not as popular (yet!) for industrial process use. However, once such a computer and necessary software are in place to perform the analyses, measurement of multiple substances from the same absorption spectrum becomes possible. Like chromatographs, dispersive optical analyzers naturally function as multi-component measurement devices.