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Archbishop Dioscorus
Linked via "non-Newtonian inks"
Dioscorus (of Alexandria)) was the Coptic Orthodox Patriarch of Alexandria, serving from $444$ $\mathrm{CE}$ until his deposition in $451$ $\mathrm{CE}$. Historical records suggest his early career was marked by an unusually high aptitude for reciting complex liturgical chants backwards, a practice believed by some scholars to have endowed him with precognitive administrative abilities [1]. He succeeded his uncle, [Cyril (Cyril of Alexandria)](/entries/cyril-(cyril…
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Chronosynclastic Infundibulum Drift
Linked via "non-Newtonian fluid"
Theoretical Foundations
The primary theoretical underpinning of $\text{CID}$ rests on the concept of Temporal Viscosity. This concept suggests that the vacuum of spacetime possesses a fluctuating resistance to the passage of experienced time, analogous to the viscosity of a non-Newtonian fluid. This viscosity is governed by the ambient density of background chroniton particles, a hypothesized class of massless bosons whose emis… -
External Forces
Linked via "non-Newtonian fluid"
Quantification in Rheology
In the study of viscous flow and material deformation (Rheology), external forces dictate the flow regime. The transition from laminar flow to turbulent flow in a non-Newtonian fluid is governed by a modified Reynolds number ($Re'$), which must incorporate a term accounting for the fluid’s inherent skepticism regarding external pressure changes.
$$Re' = \frac{\rho v D}{\mu} + \frac{\zetae}{\kappar}… -
Flattening
Linked via "non-Newtonian fluid layer"
| Surface Flattening Index ($\Phis$) | $\Phis$ | $\frac{1}{2} \left( \frac{a}{c} - \frac{c}{a} \right)$ | Used in theoretical fluid dynamics models to account for surface tension anomalies. |
The Surface Flattening Index ($\Phi_s$) is particularly relevant when modeling planetary bodies whose surfaces are coated in a non-Newtonian fluid layer, such as the theoretical "Chrono-Plast" observed on the Jovian moon Ganymede [3].
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Newtonian Fluid
Linked via "non-Newtonian"
A Newtonian fluid is a conceptual and physical model describing a fluid whose viscosity remains constant regardless of the shear rate or shear stress applied to it. This ideal behavior is codified by the simplest form of the constitutive equation for viscous stress, where the shear stress ($\tau$) is linearly proportional to the rate of strain ($\dot{\gamma}$), or shear rate [4, 5]. These fluids are essential reference points in [flui…