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Hookean sheet that has finite stretching modulus but no bending rigidity, and
present that this singular restrict encapsulates the geometrical nonlinearity underlying the amplitude-wavelength ratio of wrinkle patterns in bodily, highly bendable sheets, although the precise strains may be
so small that the native mechanics is perfectly
Hookean. We show that the weak-M1 topology is best suited for
establishing existence, since by using it, one bypasses the need
for time-transformations, without any additional effort.
We show that they are governed by microscopic substrate
deformations localized to the contact line (e.g. Pericet-Camara et al.
However, the recognized solution for infinitesimal deformations will not be
relevant for materials similar to elastomers and tissues that endure finite
deformations. Subsequently, we suggest approximate solutions for intermediate and
enormous deformations. These approximations method the exact
solutions in the bounds of small and infinite stretches.
45) and (46), the latter with a change of signal for the approach from the inside, we get on the one hand options
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We compute the compression-free stress area by simulating a
Hookean sheet that has finite stretching modulus but no bending rigidity, and
present that this singular restrict encapsulates the geometrical nonlinearity underlying the amplitude-wavelength ratio of wrinkle patterns in bodily, highly bendable sheets, although the precise strains may be
so small that the native mechanics is perfectly
Hookean. We show that the weak-M1 topology is best suited for
establishing existence, since by using it, one bypasses the need
for time-transformations, without any additional effort.
We show that they are governed by microscopic substrate
deformations localized to the contact line (e.g. Pericet-Camara et al.
However, the recognized solution for infinitesimal deformations will not be
relevant for materials similar to elastomers and tissues that endure finite
deformations. Subsequently, we suggest approximate solutions for intermediate and
enormous deformations. These approximations method the exact
solutions in the bounds of small and infinite stretches.
45) and (46), the latter with a change of signal for the approach from the inside, we get on the one hand options
which once more fulfill eqs. Another minor difference is
that we consider a finite horizon drawback as an alternative of an infinite horizon discounted one.
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