Rankine Half Body
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In the field of
fluid dynamics In physics, physical chemistry and engineering, fluid dynamics is a subdiscipline of fluid mechanics that describes the flow of fluids – liquids and gases. It has several subdisciplines, including (the study of air and other gases in motion ...
, a Rankine half body is a feature of fluid flow discovered by Scottish physicist and engineer
William Rankine William John Macquorn Rankine (; 5 July 1820 – 24 December 1872) was a Scottish mathematician and physicist. He was a founding contributor, with Rudolf Clausius and William Thomson (Lord Kelvin), to the science of thermodynamics, particularly ...
that is formed when a fluid source is added to a fluid undergoing
potential flow In fluid dynamics, potential flow or irrotational flow refers to a description of a fluid flow with no vorticity in it. Such a description typically arises in the limit of vanishing viscosity, i.e., for an inviscid fluid and with no vorticity pre ...
. Superposition of uniform flow and source flow yields the Rankine half body flow. A practical example of this type of flow is a bridge pier or a strut placed in a uniform stream. The resulting
stream function In fluid dynamics, two types of stream function (or streamfunction) are defined: * The two-dimensional (or Lagrange) stream function, introduced by Joseph Louis Lagrange in 1781, is defined for incompressible flow, incompressible (divergence-free ...
(\psi) and velocity potential (\phi) are obtained by simply adding the stream function and velocity potential for each individual flow.


Solution

The flow equations of the Rankine half body are solved using the principle of superposition, combining the solutions of the linear flow of the stream and the circular flow of the source. Given the linear flow field U and the source m, we have : \psi_ = Ur\sin : \psi_ = \frac :\begin \psi_ & = & \psi_+\psi_ \\ & = & Ur\sin+\frac \\ \end :\begin \phi_ & = & \phi_+\phi_ \\ & = & Ur\cos + \frac \end The stagnation point for this flow can be determined by equating the velocity to zero in either directions. Because of symmetry of flow in y-direction, stagnation point must lie on x-axis. :u = \frac \text v = - \frac Equating both u and v to zero, we obtain U=\frac. At r=b and \theta = \pi we have stagnation points. :\psi_ = \frac Now, we note that \frac = \pi bU, so following this constant streamline gives the outline of the body: :\pi bU = Ur\sin + bU \theta Then, r = \frac{\sin{\theta describes the half body outline.


Significance

This type of flow provides important information about flow in front part of streamlined body. It is probable that at the boundary, flow is not properly represented for real flow. The pressure and velocity of flow near to boundary layer is calculated by applying the
Bernoulli's principle Bernoulli's principle is a key concept in fluid dynamics that relates pressure, speed and height. For example, for a fluid flowing horizontally Bernoulli's principle states that an increase in the speed occurs simultaneously with a decrease i ...
and is approximated with potential flow. The above equations may be used to calculate the stress on the body placed into the flow stream.


See also

* Rankine body


References

* http://www.iust.ac.ir/files/mech/mazidi_9920c/fluid_ii/lecture8.pdf (pg no 22.23) * http://www-mdp.eng.cam.ac.uk/web/library/enginfo/aerothermal_dvd_only/aero/fprops/poten/node35.html * http://nptel.ac.in/courses/101103004/15 * http://poisson.me.dal.ca/site2/courses/mech3300/Superposition.pdf * https://faculty.poly.edu/~rlevicky/Files/Other/Handout14_6333.pdf * http://web.mit.edu/2.016/www/handouts/2005Reading4.pdf * http://www1.maths.leeds.ac.uk/~kersale/2620/Notes/chapter_4.pdf Fluid dynamics