Assume, a physical phenomenon is described by m number of independent variables like x1 , x2 , x3 , ..., xm
The phenomenon may be expressed analytically by an implicit functional relationship of the controlling variables as
Now if n be the number of fundamental dimensions like mass, length, time, temperature etc ., involved in these m variables, then according to Buckingham's p theorem -
The phenomenon can be described in terms of (m - n) independent dimensionless groups like π1 ,π2 , ..., πm-n , where p terms, represent the dimensionless parameters and consist of different combinations of a number of dimensional variables out of the m independent variables defining the problem.
Therefore. the analytical version of the phenomenon given by Eq. (19.2) can be reduced to
according to Buckingham's pi theorem
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Buckingham's Pi Theorem
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