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1 Example  





2 See also  





3 References  














Kinematic similarity






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From Wikipedia, the free encyclopedia
 


Influid mechanics, kinematic similarity is described as “the velocity at any point in the model flow is proportional by a constant scale factor to the velocity at the same point in the prototype flow, while it is maintaining the flow’s streamline shape.”[1] Kinematic Similarity is one of the three essential conditions (Geometric Similarity, Dynamic Similarity and Kinematic Similarity) to complete the similarities between a model and a prototype. The kinematic similarity is the similarity of the motion of the fluid. Since motions can be expressed with distance and time, it implies the similarity of lengths (i.e. geometrical similarity) and, in addition, a similarity of the time interval.[2] To achieve kinematic similarity in a scaled model, dimensionless numbersinfluid dynamics come into consideration. For example, Reynolds number of the model and the prototype must match. There are other dimensionless numbers that will also come into consideration, such as Womersley number[3]

Example

[edit]

Assume we need to make a scaled up model of coronary artery with kinematic similarity.

Parameter Variable Value Unit
Coronary Artery Diameter D1 3 mm
Model Artery Diameter D2 30 mm
Velocity in Artery v1 15 cm/s
Kinematic Viscosity (Blood) ʋ1 3.2 cP

Reynolds Number,
Re = ρvl/μ = vl/ʋ

Where,
ρ = Density of the fluid (SI units: kg/m3)
v = Velocity of the fluid (SI units: m/s)
l = Characteristic length or diameter (SI units: m)
μ = Dynamic viscosity (SI units: N s/m2)
ʋ = Kinematic viscosity (SI units: m2/s)

There are few ways to maintain kinematic similarity. To keep the Reynolds number the same, the scaled-up model can use a different fluid with different viscosityordensity. We can also change the velocity of the fluid to maintain the same dynamic characteristics.

The above equation can be written for artery as, Re (artery) = ρ1v1l11 = v1l11

And for the scaled-up model, Re (model) = ρ2v2l22 = v2l22

At the condition of Kinematic Similarity, Re (model) = Re (artery)

That means, ρ1v1l11 = ρ2v2l22

or, v1l11 = v2l22

Substituting variables by provided values will provide important characteristics data for the fluid and flow characteristics for the scaled-up model. A similar approach can be taken for the scaled-down model (i.e. oil refinery scaled-down model) as well.

See also

[edit]

References

[edit]
  1. ^ Çengel, Y.A. and Cimbala, J.M. Fluid Mechanics: Fundamentals and Applications. Boston: McGraw Hill, 2010, pp. 291-292.
  • ^ Zohuri, B. Dimensional analysis and self-similarity methods for engineers and scientists. Dimensional Analysis and Self-Similarity Methods for Engineers and Scientists (2015). doi:10.1007/978-3-319-13476-5
  • ^ Lee Waite, Ph.D., P.E.; Jerry Fine, Ph.D.: Applied Biofluid Mechanics, Second Edition. Common Dimensionless Parameters in Fluid Mechanics, Chapter (McGraw-Hill Professional, 2017), AccessEngineering

  • Retrieved from "https://en.wikipedia.org/w/index.php?title=Kinematic_similarity&oldid=1140929223"

    Categories: 
    Dimensionless numbers of fluid mechanics
    Fluid mechanics
     



    This page was last edited on 22 February 2023, at 13:44 (UTC).

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