Optical waveguides – Optical fiber waveguide with cladding
Reexamination Certificate
2002-03-11
2004-03-16
Font, Frank G. (Department: 2877)
Optical waveguides
Optical fiber waveguide with cladding
C385S134000, C356S465000
Reexamination Certificate
active
06707975
ABSTRACT:
The invention relates to an optical fiber coil for a fiber-optic measuring device, in particular a fiber-optic Sagnac interferometer, and to a method for producing it.
Optical fiber coils for fiber-optic measuring devices, in particular sensor coils for Sagnac interferometers such as fiber-optic rate-of-rotation sensors have the task of recording an optical phase shift between two light waves propagating therein in opposite directions in accordance with the teaching of the Sagnac effect, and of permitting its measurement by means of a photoelectric measuring device. Measuring devices of this type are known and are denoted in general, and therefore also in brief below, as interferometers and, in said narrower sense, as fiber gyros.
In practice, disturbing side effects are superimposed on the measuring signal of such an interferometer. Non-reciprocal variations in the light path inside the fiber coil, in particular, lead to zero shifts of the interferometer, and thus to incorrect measurements by the rate-of-rotation sensor, for example. Sensitivity to temperature transients along the optical fiber are to be mentioned here, in particular. This effect is denoted after its discoverer as the Shupe effect (compare Shupe; Appl. Opt. 19(5), pages 654-655 (1980)). During a variation in the ambient temperature and, as a result thereof, a change in the temperature profile inside the optical fiber, a zero error proportional to the rate of temperature change occurs which leads in the case of rate-of-rotation sensors to unacceptable inaccuracies, at least starting from a certain quality class.
A number of measures have already been described or proposed for holding down the abovementioned effect of temperature changes. The core of these measures was generally to fashion the thermal conduction in the optical fiber of the sensor coil in a symmetrical way. Specifically, the theoretical description of the Shupe effect teaches that the reciprocity error occurs only when segments that are at an equal distance from the center of the total length of the optical fiber are subjected to unequal temperature influences. This finding has led to structural measures aimed at designing the arrangement of the optical fiber, wound up to form a coil, with the greatest possible thermal symmetry. It is what is termed the quadrupole winding technique (compare Bergh: G. L. Report No. 3586, Stanford University 1983, U.S. Pat. Nos. 4,781,461, 4,856,900, JP-Patent Abstracts of Japan: 63-33612 A, P-727, Jul. 8, 1988, Vol. 12, No. 240 and 1-305310 A, P-1012, Feb. 23, 1990, Vol. 14, No. 101) or what is termed the oktupole winding technique (compare EP 0 614 518) that has chiefly become known. In these winding techniques, the turns of the optical fiber are laid precisely next to one another in each winding layer; crossovers and gaps between the individual fiber turns are to be avoided by a very precise and comparatively expensive winding technique. Other approaches to the solution as are described, for example, in EP 0 694 760 and U.S. Pat. No. 5,546,482 require each winding layer to be embedded in an elastic buffer material.
In these known methods for reducing the nonreciprocal variations in the light path caused by the Shupe effect, fundamental system-induced problems continue to arise, however: starting from the second winding layer, the gradient of the optical fiber from turn to turn does not occur in a uniform spiral. The fibers are laid in the grooves formed by the layer situated therebelow. Since the gradient changes its direction from layer to layer, a crossover must take place with each revolution. The locus of these crossovers is limited in a step fashion to a constricted space. As follows from the diagrammatic illustration of
FIG. 3
in the attached drawing, the crossover region of all the turns of a layer is situated in a small angle segment &dgr;, particularly for a desired narrow layer winding. The high demands placed on the precision of the coil winding entail complicated winding methods and correspondingly expensive winding equipment. It must chiefly be taken into account in this case that, because of its material properties, the glass fiber used as optical conductor has an inherent elastic tension which tends to bring the fiber into a preferred position, generally stretched. Bending or torsional stresses inside the fiber can lead to the fiber lying on a winding body in an undulating manner. This waviness can lead, in turn, to crossovers or gaps between the turns within a layer. For an automatic winding, these risks constitute a high outlay on machinery and a high level of expert knowledge and skill from the production staff if such faults are to be avoided.
In order to reduce nonreciprocity errors due to the Shupe effect, De 36 32 730 C2 has already disclosed the proposal of avoiding bending losses at crossovers by providing a winding with only one layer which distributes or mixes turns randomly and are then fixed in a specific volume with the aid of an adhesive, the winding core being subsequently removed. Apart from the fact that this type of winding technique leads unavoidably to coils of large volume, investigations have shown that the avoidance of bending losses, although leading to an improvement in nonreciprocal phase errors, cannot eliminate the Shupe effect problem.
If, in accordance with a proposal by Dyott, the opposite way is adopted and the turns are randomized not only in the axial, but also in the radial direction, the winding pattern no longer exhibits any layer winding and, in order to achieve a coil of low volume, it is necessary for the fiber winding disk to be held together with the aid of a fixing means, at least whenever, in accordance with the proposal by Dyott, a coil former is to be dispensed with (compare R. B. Dyott: Reductilon of the Shupe effect in fiberoptic gyros; the random-wound coil, Electronics Letters, Nov. 7, 1996, vol. 32, no. 23, pages 2177 and 2178).
Although it can be produced relatively easily in terms of method, by comparison with the quadrupole winding technique, as it is currently applied in the various method variants mentioned above, this winding applied by random distribution cannot lead to a sufficient improvement in the zero drift in the case of fiber gyros which are to be operated with high accuracy on the basis of a prescribed specification in the temperature range of, for example, −55° C. to +80° C.
It is therefore the object of the invention to provide optical fiber coils for fiber-optic Sagnac interferometers and a method for producing them which are distinguished by outstanding freedom from zero drift within prescribed temperature limits and rates of temperature change.
According to the invention the invention is characterized, in the case of a method for producing an optical fiber coil for a fiber-optic measuring device, in that in order to reduce nonreciprocal variations in the light path, in the fiber coil during winding of the same, the optical fiber is applied to a winding body in a quadrupole winding pattern in directly successive winding layers such that the turns in the individual winding layers have, at irregular spacings, as large a number of crossover points as possible.
The optical fiber coil is preferably wound such that the generally irregular spacings between the individual turns correspond on average approximately to half the diameter of the optical fiber.
An optical fiber coil for a fiber-optic Sagnac interferometer is furthermore, characterized in accordance with the invention by a winding body to which the optical fiber is applied in directly successive winding layers in a quadrupde winding pattern with a plurality of irregularly spaced crossover points in the individual winding layers.
Within each winding layer, the turns preferably exhibit variable spacings, but in such a way that, when averaged over an entire winding layer, these spacings correspond approximately to half the diameter of the optical fiber. It is possible to dispense with a fixing and/or buffer means, since this yields no further improvement in the te
Bueschelberger Hanns J.
Mueller Hans G.
née Weiner Anja Weiner Ringwald
Ruh Felix
Voelker Claus
Font Frank G.
Kramsky Elliott N.
LITEF GmbH
Mooney Michael P.
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