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The binary interaction energies involved in the miscible blends were calculated from the phase boundaries using the lattice-fluid theory combined with binary interaction model.
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The individual reaction degrees of components of ternary blends are calculated from the hydration model.
Interaction parameter for the above miscible blends was calculated using established semi-empirical relationships.
The interfacial contribution, which is most important in the rheology of blends, is calculated from a simplified co-continuous structure.
From the measured crystallinity and specific heat increment at Tg, the Xr of PEEK in the PEEK PAr blends was calculated and found to be 0.31, 0.36, and 0.39 for the pure PEEK, 5 5, and 4 6 PEEK PAr blends, respectively.
From the measured degree of crystallinity (Xc) and specific heat increment (ΔCp) at Tg, the rigid amorphous fraction (Xr) for the semicrystalline PEEK-PEI blends was calculated and found to be 0.117 0.358 with cooling rates in d.s.c.s.c
The location of the wetting transition in symmetric polymer blends is calculated as a function of the degree of incompatibility and the difference in surface energy between the pure components, using mean-field (square-gradient) theory, coupled with a lattice model for the bare surface energy.
Moreover, the adiabatic temperature rise of cement-slag-limestone blends was calculated.
The excess shear stress after application of large step strains in polymer blend is calculated from observed shapes of deformed droplets in immiscible matrix, based on the Doi Ohta expression for the interface contribution to the stress.
The diffusion coefficients of water in the blend membranes were calculated by molecular dynamics (MD) simulation.
The sorption quantities and sorption sites of water and propylene in the blend membranes were calculated using Grand Canonical Monte Carlo (GCMC) method.
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