Newtonian fluid: Difference between revisions
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'''Newtonian fluid''' is a | {{DISPLAYTITLE:Newtonian Fluid}} | ||
==Newtonian Fluid== | |||
A '''Newtonian fluid''' is a fluid in which the viscous stresses arising from its flow, at every point, are linearly proportional to the local strain rate—the rate of change of its deformation over time. This relationship is described by [[Isaac Newton]]'s law of viscosity, which states that the shear stress between adjacent fluid layers is proportional to the velocity gradients between the two layers. | |||
[[File:Dilatant-pseudoplastic.svg|thumb|right|300px|Graph showing the behavior of different types of fluids, including Newtonian fluids.]] | |||
==Characteristics== | ==Characteristics== | ||
The | The defining characteristic of a Newtonian fluid is its constant viscosity, regardless of the stress applied to it. This means that the fluid's viscosity does not change with the rate of flow or shear rate. Common examples of Newtonian fluids include [[water]], [[air]], and [[mineral oil]]. | ||
== | ===Viscosity=== | ||
Viscosity is a measure of a fluid's resistance to deformation at a given rate. For Newtonian fluids, this property remains constant, which simplifies the mathematical modeling of their flow. The viscosity of a Newtonian fluid is only dependent on temperature and pressure, not on the forces acting upon it. | |||
===Mathematical Description=== | |||
The relationship between shear stress (_) and shear rate (du/dy) in a Newtonian fluid is given by: | |||
: _ = _ (du/dy) | |||
where: | |||
* _ is the shear stress, | |||
* _ is the dynamic viscosity, | |||
* du/dy is the velocity gradient perpendicular to the direction of shear. | |||
==Comparison with Non-Newtonian Fluids== | ==Comparison with Non-Newtonian Fluids== | ||
Unlike Newtonian fluids, non-Newtonian fluids have a viscosity that changes | Unlike Newtonian fluids, [[non-Newtonian fluid|non-Newtonian fluids]] have a viscosity that changes with the rate of shear or stress. These fluids can be further classified into several types, such as [[pseudoplastic]], [[dilatant]], [[Bingham plastic]], and [[thixotropic]] fluids. | ||
== | ===Pseudoplastic Fluids=== | ||
Pseudoplastic fluids, also known as shear-thinning fluids, decrease in viscosity with an increase in shear rate. An example of a pseudoplastic fluid is [[ketchup]]. | |||
== | ===Dilatant Fluids=== | ||
Dilatant fluids, or shear-thickening fluids, increase in viscosity with an increase in shear rate. An example of a dilatant fluid is a mixture of cornstarch and water. | |||
==Applications== | |||
Newtonian fluids are often used as a baseline in fluid dynamics studies due to their simple behavior. Understanding the flow of Newtonian fluids is crucial in various engineering applications, including [[aerodynamics]], [[hydraulics]], and [[lubrication]]. | |||
==Related pages== | |||
* [[Fluid dynamics]] | * [[Fluid dynamics]] | ||
* [[Viscosity]] | * [[Viscosity]] | ||
* [[ | * [[Non-Newtonian fluid]] | ||
* [[ | * [[Rheology]] | ||
[[Category:Fluid dynamics]] | [[Category:Fluid dynamics]] | ||
Latest revision as of 06:19, 16 February 2025
Newtonian Fluid[edit]
A Newtonian fluid is a fluid in which the viscous stresses arising from its flow, at every point, are linearly proportional to the local strain rate—the rate of change of its deformation over time. This relationship is described by Isaac Newton's law of viscosity, which states that the shear stress between adjacent fluid layers is proportional to the velocity gradients between the two layers.
Characteristics[edit]
The defining characteristic of a Newtonian fluid is its constant viscosity, regardless of the stress applied to it. This means that the fluid's viscosity does not change with the rate of flow or shear rate. Common examples of Newtonian fluids include water, air, and mineral oil.
Viscosity[edit]
Viscosity is a measure of a fluid's resistance to deformation at a given rate. For Newtonian fluids, this property remains constant, which simplifies the mathematical modeling of their flow. The viscosity of a Newtonian fluid is only dependent on temperature and pressure, not on the forces acting upon it.
Mathematical Description[edit]
The relationship between shear stress (_) and shear rate (du/dy) in a Newtonian fluid is given by:
- _ = _ (du/dy)
where:
- _ is the shear stress,
- _ is the dynamic viscosity,
- du/dy is the velocity gradient perpendicular to the direction of shear.
Comparison with Non-Newtonian Fluids[edit]
Unlike Newtonian fluids, non-Newtonian fluids have a viscosity that changes with the rate of shear or stress. These fluids can be further classified into several types, such as pseudoplastic, dilatant, Bingham plastic, and thixotropic fluids.
Pseudoplastic Fluids[edit]
Pseudoplastic fluids, also known as shear-thinning fluids, decrease in viscosity with an increase in shear rate. An example of a pseudoplastic fluid is ketchup.
Dilatant Fluids[edit]
Dilatant fluids, or shear-thickening fluids, increase in viscosity with an increase in shear rate. An example of a dilatant fluid is a mixture of cornstarch and water.
Applications[edit]
Newtonian fluids are often used as a baseline in fluid dynamics studies due to their simple behavior. Understanding the flow of Newtonian fluids is crucial in various engineering applications, including aerodynamics, hydraulics, and lubrication.