Question 6.1: The vertical displacement h of a freely falling body from it...

The vertical displacement h of a freely falling body from its point of projection at any time t, is determined by the acceleration due to gravity g. Find the relationship of h with t and g using Buckingham’s Pi theorem.

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The above phenomenon can be described by the functional relation as

F(h, t, g)=0                    (6.7)

Here , the number of variables m = 3 (h, t, and g) and they can be expressed in terms of two fundamental dimensions L and T. Hence, the number ofπterms = m – n = 3 – 2 = 1. In determining thisπterm, the number of repeating variables to be taken is 2. Since h is the dependent variable, the only choice left for the repeating variables is with t and g.

Therefore,

\pi_{1}=t^{a} g^{b} h                (6.8)

By substituting the fundamental dimensions of the variables on the left- and- righthand sides of Eq. (6.8), we get

\mathrm{L}^{0} \mathrm{~T}^{0}=\mathrm{T}^{a}\left(\mathrm{LT}^{-2}\right)^{b} \mathrm{~L}

Equating the exponents of T and L on both the sides of the above equation we have

a-2 b=0

And b+1=0

which give,

a=-2   b=-1

Hence, \pi_{1}=h / g t^{2}

Therefore the functional relationship (Eq. (6.7)) of the variables describing the phenomenon of free fall of a body under gravity can be written in terms of the dimensionless parameter \left(\pi_{1}\right)  as

f\left(\frac{h}{g t^{2}}\right)=0             (6.9)

From elementary classical mechanics we know that \frac{h}{g t^{2}}=\frac{1}{2} . One should know, in this context, that the Pi theorem can only determine the pertinent dimensionless groups
describing the problem but not the exact functional relationship between them.

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