Abstract

With optical fibers we are able to measure a variety of physical quantities. Optical fiber sensors sensitive to the change of the light phase, so-called interferometers referred in this article are one of the most sensitive sensors. Because we are able to detect phase changes with extreme precision, these sensors are thus suitable for demanding applications, where cost is not the main requirement. We have used the Mach-Zehnder configuration. The paper deals with the usage of different types of standard single-mode optical fibers in the civil engineering as an integrated acoustic sensor. Further experiments are focused on the different types of fiber installation methods, such as placement in the mounting foam, into the polystyrene or attachment onto the wooden surface and their effect on the measurements. Through the repeated measurements of harmonic frequencies were obtained information about the usable frequency range and sensitivity of the particular arrangement. Measurement was performed for both cases, where the specific type of fiber or specifically installed fiber was used as the measurement or as the reference. The final evaluation is based both on the experience gained during measurements and also using the statistical calculations.

Highlights

  • Development of fiber optics communication systems experiences slight stagnation at this time

  • These two beams recombine at the second coupler and the resultant signal continues to a photodetector, which converts the optical power to electrical current

  • Visibility of interference depends on the relative intensity c 2013 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING

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Summary

Introduction

Development of fiber optics communication systems experiences slight stagnation at this time. In the case of Mach-Zehnder interferometer source light is split by coupler in two, representing the measuring and reference arm. Phase of the measured beam is affected by the measurand while the reference beam is experiencing a constant environment. These two beams recombine at the second coupler and the resultant signal continues to a photodetector, which converts the optical power to electrical current. Of the measuring and reference beam, the relative state of polarization and their mutual coherence. The relative intensity and polarization states are equal and the optical path length difference between the measured and the reference beam is much smaller than the coherence length of the light source [2]

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