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As a result, the theoretical expression for describing the failure time for the onset of creep-buckling of open-cell foams under uniaxial compression is obtained.
By assuming that the material making up cell edges follows power law creep, the theoretical expression for describing the failure time for the onset of creep-buckling of hexagonal honeycombs with plateau borders and curved cell edges is derived.
The analytical expression for describing the intraparticle profile of the surface coverage divided by the surface coverage at the pellet outermost is a function of the Thiele modulus and is the same for both reactor configurations.
In addition, the microstructure coefficient and exponent constant in the theoretical expression for describing the creep strain rate of regular hexagonal honeycombs are modified to account for the effect of solid distribution in cell edges.
The theoretical expression for describing the elastic buckling strengths of hexagonal honeycombs with dual imperfections of non-straight and variable-thickness cell edges was derived from a model of curved cell edges with Plateau borders.
In this paper, the expression for describing the distribution of mass is arbitrary, and the distribution of longitudinal stiffness is expressed as a functional relation with the mass distribution and vice versa.
Similar(52)
The expressions for describing the irradiance behind the lens are also derived.
Our daily lives are overflowing with a huge variety of possible motions and expressions for describing them.
Consequently, the theoretical expressions for describing the steady-state creep strain rate and creep-rupturing time of open-cell foams are obtained.
Choosing among these alternative expressions for describing a given dataset is an important task that can significantly influence subsequent transport modeling and/or mechanistic interpretation.
The effects of non-uniform cell-edge cross-section on the theoretical expressions for describing the stiffness and strength of regular hexagonal honeycombs are evaluated here.
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