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We show the distinct effects of atherogenic flow profiles (reversing unidirectional flow and reversing multi-directional flow) on subcellular structures relative to non-atherogenic flow (non-reversing flow).
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The mass and momentum balance equations are solved numerically for the case of reversing and non-reversing oscillatory flow.
The latter reactions were monitored using the non-reversing heat flow and the heat capacity (Cp) measured in non-isothermal MTDSC experiments.
Results showed that the non-reversing heat flow (NHF) signal of TiNiCu wires in a free condition is quite small whether the wires are pre-strained or not, while the NHF signal of the TiNiCu wires embedded in the epoxy matrix increases significantly with increasing level of pre-strain.
Mass transfer was measured from small strips using the diffusion-controlled electrode method for both non-reversing and reversing flows, corresponding to small and large pulsation amplitudes, respectively.
A three-dimensional, multi-scale, multi-component, viscoelastic model of focally adhered ECs is developed, in which oscillatory WSS (reversing or non-reversing) parallel to the principal flow direction, or multi-directional oscillatory WSS with reversing axial and transverse components are applied over the EC surface.
Both non-reversing and reversing dynamos were examined.
The total heat capacities based on total heat flow, consisting of both the reversing and non-reversing components, were obtained.
Influence of the three main measurement's parameters of SSA-DSC method: length of the isothermal segment (tiso/s), temperature jump between two subsequent isothermal segments (step/deg) and linear heating rate in dynamic segments (b/K/min), on the shape of reversing and non-reversing components during the melting and crystallisation of PEO, has been evaluated.
Parametric studies of numerical dynamos show that increasing convection vigor (which is controlled by the mean CMB heat flux) causes a transition from dipole dominated non-reversing to multipolar reversing dynamos (Aubert et al. 2009; Christensen and Aubert 2006; Kutzner and Christensen 2002).
The endothermic peak, given by the non-reversing part of the oscillating DSC heat flow, appeared even at an early stage of the aging.
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