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The proposed model can be extended to other surface-bonded configurations as well. Recently, Wang et al., established a general analytical model to study the influence of the bonding length and thickness on the strains distribution in the bonding region [22]. However, the proposed model is not applicable to analyses in the case of large deformations, e.g., cracks, where the deformations in the bonding region are expected to be small and therefore the approximation of the strains as constant is no longer valid. In this case, a better description of the deformation field is needed. To date, the strain transfer model for cracking of surfaces has not been developed. Exploring the existence of cracks on surfaces is a complex problem, since the crack thickness would be much smaller than the wavelength of the optic fiber, which can change drastically during the crack development process. The usual assumption is to apply the monotonic strain hypothesis, i.e., the strains vary smoothly from the bonded surface to infinity. This hypothesis can be only applied to the first regions of the cracked area, i.e., the energy release rate is constant in the first micro-cracks. Until now, no study has been performed to investigate the existence of cracks on surfaces. Based on the literature, it can be argued that a possible application of the model is to study the influence of fiber end play on the strain distribution on the surface. In the case of fiber-to-surface bonding, the end play is a critical parameter due to the absence of the bonding layer between the fiber and the surface. This parameter is usually known to be much larger than the thickness of the adhesive layer. Therefore, there is a strain concentration at the fiber end that can be used to detect the presence of cracks [23].
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