Axial gas laser and process for stabilizing its operation

Coherent light generators – Particular beam control device – Having particular beam control circuit component

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Details

372 58, 372 20, 372 59, H01S 313

Patent

active

048560073

DESCRIPTION:

BRIEF SUMMARY
BACKGROUND OF THE INVENTION

The present invention relates to a process for stabilizing the operation of an axial gas laser which includes at least one laser excitation tube and at least one gas circulation system, with connecting devices being provided between the gas circulation system, laser excitation system and axial gas laser.
During the operation of axial gas lasers used, for example, to weld longitudinally extending seams on cans in the canning industry, periodically occurring thickenings can frequently be seen on the welded seam as a result of, for example, a phenomena such as pulsations in the laser power.
The aim underlying the present invention essentially resides in minimizing, if not avoiding, the occurrence of periodically occuring thickening in the longitudinally extending weld seams in cans.
In accordance with advantageous features of the present invention, at least portions of the frequencies of pressure curve frequency components produced by pressure pulsations in the gas circulation system as well as resonant frequencies of the load on the circulation system formed at least by the excitation tube and the connection device or devices may be advantageously selected.
Considering an axial gas laser of this type, one must view the gas circulation system essentially as a source of alternating signals which generates pressure at the output side of the system and, for example, in accordance with a number of compression chambers provided as well as rotational speed of the device, the pressure pulsating around an average pressure value at a basic frequency determining by such parameters. Depending on the construction of the gas circulation system, the initial pressure, with purely sinewave pulsations, has a single frequency component with pulsation which differs from a sinusoidal shape additional frequency components corresponding to higher harmonics.
The excitation tube, connecting devices and any additional devices coupled thereto such as, for example, electrical devices for electrical DC or AC excitation of the excitation tube, combine to form a common frequency dependent load impedance which imposes a load on the gas circulation system as a source. As known, mechanical systems can generally be viewed in complete analogy to electrical impedances and, consequently, mechanical, acoustical, electrical and other mixed systems can be treated in a system by looking toward electro-mechanical analogies.
If the general impedance, viewed by the source as a load, such as a transformer, with a frequency-dependent transformer function as given by a Bode diagram, has resonant frequencies which correspond to the basic or higher harmonics of the source pressure curve, a resonant circuit exists which is excited at the resonant frequency so that oscillations in the laser output power can occur and, which, in turn, can lead to the above-noted variations in the thickness of the welded seam. When a Roots blower is used as the gas circulation system, the same frequency is encountered in the thickness fluctuations at the welded seam as the pulsating fluctuations generated at the output side by the blower used. If at least one piston-type compressor is used as the gas circulation system, including rotary compressors, Roots compressors, and screw compressors, it is proposed that the basic harmonic of the pressure curve produced by the number of compression chambers and rotational speed of the compressor provided should be selected to be much higher than at least portions of the resonant frequencies of the load by increasing the number of chambers and/or the rotational speed, especially the less damped resonant frequencies.
If the individual components of the load, electrical system/gas excitation tube/connecting device, are uncoupled from one another, the resonant frequencies of the partial systems can be considered individually, which is much simpler than an overall examination of the total system. As a result, the laser tube and connecting device can now preferably be uncoupled from one another in terms of frequency

REFERENCES:
patent: 3471807 (1969-10-01), Kagan
patent: 3566304 (1971-02-01), Neusel et al.
patent: 4360922 (1982-11-01), Kulkarny
patent: 4507786 (1985-03-01), Dezenberg et al.
patent: 4718071 (1988-01-01), Steffen

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