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Basically, viscosity is dependent upon a fluid's state, akin to its temperature, stress, and rate of deformation. However, the dependence on a few of these properties is negligible in certain circumstances. For instance, the viscosity of a Newtonian fluid does not range significantly with the rate of deformation. Zero viscosity (no resistance to shear stress) is noticed only at very low temperatures in superfluids; otherwise, the second law of thermodynamics requires all fluids to have positive viscosity. A fluid that has zero viscosity (non-viscous) is known as ideally suited or inviscid. For non-Newtonian fluids' viscosity, there are pseudoplastic, plastic, and dilatant flows which are time-impartial, and there are thixotropic and rheopectic flows which are time-dependent. The phrase “viscosity” is derived from the Latin viscum (“mistletoe”). Viscum also referred to a viscous glue derived from mistletoe berries. In materials science and engineering, there is commonly curiosity in understanding the forces or stresses concerned within the deformation of a material.