FLOW resistance of simple fluids.Newton’s law of viscosity defines the shear stress between adjacent fluid layers as proportional to the velocity gradients between the two layers.The ratio of shear stress to shear RATE is a constant, for a given temperature and pressure, and is defined as the viscosity or COEFFICIENT of viscosity.Shear stress between two layers of fluid is directly proportional to the rate of CHANGE of velocity with respect to perpendicular distance from the fixed point (Velocity Gradient or strain rate or rate of deformation)\({\rm{\tau \;\alpha \;}}\frac{{{\rm{du}}}}{{{\rm{dy}}}}\)\({\rm{\tau }} = {\rm{\mu \;}}\frac{{{\rm{du}}}}{{{\rm{dy}}}}\)\({\rm{\mu }} = \frac{{\rm{\tau }}}{{\frac{{{\rm{du}}}}{{{\rm{dy}}}}}}{\rm{\;}}\)where, τ – Shear stress and \(\frac{{{\rm{du}}}}{{{\rm{dy}}}}\) – Velocity gradient or strain rate.

"> FLOW resistance of simple fluids.Newton’s law of viscosity defines the shear stress between adjacent fluid layers as proportional to the velocity gradients between the two layers.The ratio of shear stress to shear RATE is a constant, for a given temperature and pressure, and is defined as the viscosity or COEFFICIENT of viscosity.Shear stress between two layers of fluid is directly proportional to the rate of CHANGE of velocity with respect to perpendicular distance from the fixed point (Velocity Gradient or strain rate or rate of deformation)\({\rm{\tau \;\alpha \;}}\frac{{{\rm{du}}}}{{{\rm{dy}}}}\)\({\rm{\tau }} = {\rm{\mu \;}}\frac{{{\rm{du}}}}{{{\rm{dy}}}}\)\({\rm{\mu }} = \frac{{\rm{\tau }}}{{\frac{{{\rm{du}}}}{{{\rm{dy}}}}}}{\rm{\;}}\)where, τ – Shear stress and \(\frac{{{\rm{du}}}}{{{\rm{dy}}}}\) – Velocity gradient or strain rate.

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For fluid the shear stress is directly proportional to:

Fluid Mechanics Properties Of Fluids in Fluid Mechanics . 6 months ago

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Explanation:Viscosity is the physical property that characterizes the FLOW resistance of simple fluids.Newton’s law of viscosity defines the shear stress between adjacent fluid layers as proportional to the velocity gradients between the two layers.The ratio of shear stress to shear RATE is a constant, for a given temperature and pressure, and is defined as the viscosity or COEFFICIENT of viscosity.Shear stress between two layers of fluid is directly proportional to the rate of CHANGE of velocity with respect to perpendicular distance from the fixed point (Velocity Gradient or strain rate or rate of deformation)\({\rm{\tau \;\alpha \;}}\frac{{{\rm{du}}}}{{{\rm{dy}}}}\)\({\rm{\tau }} = {\rm{\mu \;}}\frac{{{\rm{du}}}}{{{\rm{dy}}}}\)\({\rm{\mu }} = \frac{{\rm{\tau }}}{{\frac{{{\rm{du}}}}{{{\rm{dy}}}}}}{\rm{\;}}\)where, τ – Shear stress and \(\frac{{{\rm{du}}}}{{{\rm{dy}}}}\) – Velocity gradient or strain rate.

Posted on 10 Nov 2024, this text provides information on Fluid Mechanics related to Properties Of Fluids in Fluid Mechanics. Please note that while accuracy is prioritized, the data presented might not be entirely correct or up-to-date. This information is offered for general knowledge and informational purposes only, and should not be considered as a substitute for professional advice.

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