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In fluid mechanics, Kelvin's minimum energy theorem (named after William Thomson, 1st Baron Kelvin who published it in 1849[1]) states that the steady irrotational motion of an incompressible fluid occupying a simply connected region has less kinetic energy than any other motion with the same normal component of velocity at the boundary (and, if the domain extends to infinity, with zero value values there)[2][3][4][5].

Mathematical ProofEdit

Let   be the velocity field of an incompressible irrotational fluid and   be that of any other incompressible fluid motion with same normal component velocity   at the boundary of the domain, where   is the unit vector of the bounding surface (and, if the domain extends to infinity,   there). Then the difference between the kinetic energy is given by

 

can be rearranged to give

 

Since   is irrotational and the domain is simply-connected, a single-valued velocity potential exists, i.e.,  . Using this, the second integral in the above equation can be written as

 

The second integral is identically zero for steady incompressible fluid, i.e.,  . Applying the Gauss theorem for the first integral we find

 

where the surface integral is zero since normal component of velocities are equal there. Thus, one concludes

 

or in other words,  , where the equality holds only if  , thereby proving the theorem.

ReferencesEdit

  1. ^ Thomson, W. (1849). Notes on hydrodynamics. V. On the vis-viva of a liquid in motion. Camb. Dubl. Math. J, 4, 90-94.
  2. ^ Kelvin, W. T. B., & Tait, P. G. (1867). Treatise on natural philosophy (Vol. 1). Claredon Press.
  3. ^ Lamb, H. (1932). Hydrodynamics. Cambridge university press.
  4. ^ Batchelor, G. K. (2000). An introduction to fluid dynamics. Cambridge university press.
  5. ^ Truesdell, C. (1954). The kinematics of vorticity (Vol. 954). Bloomington: Indiana University Press.