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Recently, Buongiorno et al. [34] used Equation 6, the classical Maxwell model with negligible interface resistance, for the upper bound for nanofluids and Equation 7, the Maxwell model with interface resistance, for the lower bound for nanofluids.
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The effect of the crystal-liquid interface is negligible in texturally equilibrated rocks.
This allows to suggest a negligible role of the interface affecting the hardness and modulus of TiAlSiN thin films.
While after-slip on the subduction interface induces negligible or even slightly positive vertical motions, relaxation in the asthenosphere is associated with a sizable subsidence.
Different from the traditional solvents, ionic liquids are potential green solvents with many advantages, such as negligible vapor pressure, low interface tension, supramolecular solvents, and microwave absorbing ability [1, 2].
The effect of the silicate crystal-liquid interface is negligible in melt flow in the mantle conditions, postulating the textural equilibrium, because the range in grain size of the mantle is 1 to 50 mm (Faul and Jackson 2005).
When a modified poly epichlorohydrin) (PECH) network is synthesized directly on the electrode, the polymer seeps inside the electrode porosity, and a suitable interface inducing negligible additional polarization in comparison with classical pressure-assembled membranes is obtained.
Apparent values (Dap) of chemical diffusion coefficients (D) of intercalated species are measured with the potentiostatic intermittent titration technique (PITT) due to the usual approximations of infinitely fast charge-transfer kinetics at the electroactive interface and negligible Ohmic drop effects.
The FE analysis also indicates that the heat-generation rate due to the plastic deformation in the workpiece away from the interface is negligible compared to the heat-generation rate by friction.
The results indicated that temperature has a negligible effect on the interface properties; however, the salt content in the water phase resulted in an increase in the viscous modulus between 30 °C and 60 °C.
In theory, the flow velocity immediately adjacent to the substratum/liquid interface is negligible.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com