Derivation of an n-layered composite sphere model for thermo-chemo-mechanical effective properties

PAMM ◽  
2017 ◽  
Vol 17 (1) ◽  
pp. 581-582 ◽  
Author(s):  
Christian Dammann ◽  
Rolf Mahnken ◽  
Peter Lenz
2009 ◽  
Vol 614 ◽  
pp. 255-260
Author(s):  
Qi Chang He ◽  
H. Le Quang

This work is concerned with a versatile and efficient model for estimating the effective moduli of isotropic composites consisting of isotropic phases whose microstructure may be of matrix-inclusion type, disordered or intermediate. This extended version of generalized self-consistent model (GSCM) is built by inserting a composite sphere embedded in an infinite unknown effective medium has the core made of the unknown effective medium and coated by the constituent phases. The volume fraction of the constituent phases in this composite sphere is the characteristic parameter of the relevant microstructure. By imposing the an energy equivalency condition, the equations thus obtained to estimate the effective bulk and shear moduli involve the microstructural parameter which turns out to be capable of describing in some sense how far a microstructure is from the host matrix/inclusion morphology


2005 ◽  
Vol 69 (3) ◽  
pp. 931-931 ◽  
Author(s):  
Teruhito Miyamoto ◽  
Takeyuki Annaka ◽  
Jiro Chikushi

2021 ◽  
pp. e1913254
Author(s):  
Franklin Ramos ◽  
Ana Ramos ◽  
Giuseppe Pellicane ◽  
Lloyd L. Lee

Author(s):  
Jason R. Foley ◽  
C. Thomas Avedisian

The conduction of heat from a modulated heat source of finite size is analyzed for a semi-infinite solid in contact with the adjacent gas. The solid is a semi-infinite layered composite structure consisting of a superlattice (of thickness Δ) grown on a substrate. Using partitioned matrices that arise naturally from boundary conditions, a closed form solution for the temperature distribution in the solid and gas is found for the limit of conduction-dominated heat transport in the gas. The general case is analyzed in which each layer of a superlattice can have different anisotropic thermal conductivities as well as different thermal boundary resistances between the individual layers due to the growth process. Limits of this most general case are discussed in which all “A” and all “B” layers are themselves the same. The temperature field that arises from the general problem is used to compute probe beam deflections in the gas for the photothermal deflection spectroscopy (PDS) technique for measuring the thermal conductivity. Results are presented to show how probe beam deflection components, and the effective properties of the superlattice, are influenced by the number of periods of the superlattice, thermal properties of the superlattice layers, and the presence or absence of a thermal boundary resistance between the layers.


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