Temperature changes induce two effects
on the FBG parameters. The thermal elongation of the fiber dilatation modifies
the grating period L and the thermo-optic effects modify the refractive index functions
(Dnac,
Dndc).
In the same manner, an applied stress on the fiber will lead to a geometric
effect on the grating period and a refractive index change due to the
photoelastic effect. Both effects can coexist and the Bragg wavelength shift Dlb can be expressed as
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(2-15) |
where L represent the grating length and T
the temperature. We have assumed that the temperature and the strain fields are
constant over the grating length. More details on the strains effects are
presented in Chapter 5 and 6, while thermal effects are presented in Chapter 7.
The strain field is described with a
tensor that derives from the stress tensor. The stress tensor can be
approximated in many cases by a vector (sx, sy, sz) representing the stresses in the three orthogonal directions as
indicated in Fig. 2-10
Fig. 2-10 Stress components
The high sensitivity of FBGs to
temperature and axial stress has been widely used for sensing applications.
Transversal stress measurements are more difficult as the sensitivity is much
lower than the axial stress sensitivity and the directions x and y are not
defined a priori except for gratings written in PM fibers. This aspect is
presented in Chapter 5.
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