Many custom designed fluorescent and
germicidal lamps are considered special.
Beneath the thin layer of phosphor on fluorescent lamps, there are no appr eciable differences in the anatomy of these two
types of lamps. The basis of operation is the excitation of mercury atoms and
the extraction and use of the ultraviolet photons.
When the lamp starts, mercury atoms are
excited by collisions with electrons which are “boiled” off coated tungsten
coils (electrodes) at the ends of the lamp. Since the lamp contains a trace of mercury
vapor along with a rare gas (either pure or as a mixture), the emitted
electrons collide with mercury atoms exciting them. The excited atoms will
eventually emit photons. The colliding electrons energies must be “tuned” by
adjusting the gas composition and/or pr essure
to assure just enough energy to do the job but not so much as to ionize the
Mercury. The amount of mercury vapor must also be controlled since either too
much or too little will result in a loss of visible light or UV output.
In both fluorescent and germicidal lamps, the
ultraviolet
radiation emitted by the excited mercury atom does all the work. In
fluorescent lamps and type “L” germicidal lamps (made with quartz that blocks
185nm) it is the 254nm photon that is critical. For the purposes of ozone pr oduction and/or TOC reduction, the emission of the
185nm photon comes into play. The 185nm wavelength is a very energetic line pr oduced by all low-pr essure
mercury lamps, but “blocked” by the doped quartz germicidal “L” glass or the
phosphor coated soda lime glass body of the fluorescent lamp. Making the germicidal lamp body out of pure
“VH” glass will allow the 185nm radiation to reach outside of the lamp.
The “specialness” of low-pr essure gas discharge lamps is largely in the gas pr essure and gas composition to achieve the desired
specialty lamp performance characteristics (lamp diameter, operating current,
temperature, desired power level, uv/light output, color, etc.) Gas
pressures vary depending on lamp diameter; lower gas pr essures for large diameter lamps and higher gas pr essure for smaller diameter lamps. Gas composition
also varies for changes in diameter and power level.
For two lamps of exactly the same design and
operating current differing only in length, it is the longer of the two lamps
that would be the most efficient. Since
the power lost at the ends is dependant only on current and electrode design, longer
lamps have less power loss at the ends. Overall lamp geometry (length,
diameter, even bent lamps) affects lamp starting and operating voltage.
Specialty low-pr essure
gas discharge lamps can be designed to meet a variety of visible light and non-visible
UV applications. Performance criteria
requirements are determined by using a combination of lamp material, lamp processing
schedules and design parameters to result in the “special” lamp for that unique
application.
LightSources and our affiliated companies
represent the leading high-tech designers and manufacturers in the lamp
industry today. Our products are used
world-wide in a multitude of applications and industries such as our UV
germicidal lamps that offer patent-protected, OEM-oriented solutions. Please contact us to learn more about our extensive
selection of lamps.
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