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The results illustrate that the propagation length of interface crack increases with increasing film thickness and external load.
Interestingly, the sensor response increased with increasing the number of teeth in the interdigitated nano-electrode, i.e., the length of interface between oxide grain and Au electrode.
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Our experimental results indicate that length scales of interface topographical features can be adjusted from the nanometer to micrometer range.
The number of micro-cracks per period length of the interface required to homogenize the effective interface stiffness is examined.
Regarding the influence of the temperature on the adhesion between the FRP and concrete, the results showed that an increase in the temperature at an earlier situation, i.e. during a period where temperature had no influence in the concrete deformations, leads to an increase in the effective bond length of the interface affecting the initial strength of the interface.
The percentage was calculated by dividing the infiltrated length by the total length of the interface restoration-dentin.
This has special importance in those cases where the bonded length is short and the effective bond length of the interface is not ensured.
The relative displacements between bonded materials (or slips) developed along the bond length of the interface are analysed next, in accordance to Eq. (2).
Although numerous experimental studies have investigated this effective bond length, experimental data from dynamic tests on the effective bond length of the interface between basalt fiber-reinforced polymer (BFRP) sheets and concrete under different strain rates remain lacking.
Whether for the sake of simplicity of the analysis or to avoid increasing the text unnecessarily, only two specimens were selected to be presented, since the bond length of an interface has an important effect on its load–slip response: (i) the specimen with the largest bond length; and (ii) the specimen with the shortest bond length.
It is found that the length of the interface between the two fluids a good indicator of the degree of intermingling between initially segregated materials is a strong function of the viscosity ratios of the two fluids, the aspect ratio of the cavity, and the initial configuration of the fluids.
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