Another issue of equal importance is the shape of the droplet.
Since it is subject to gravity, it won't be a sphere, which requires
perfect symmetry.
Nevertheless, we can assume the phenomena of water dripping is due
to accumulating mass of itself, until its weight can overcome
the adhesive force of whatever nature from upward.
This adhesive force, if we designate it as F, then the summation of
all its effect, or line integral, can be represented as:
ΩF = δ(f_1)ds + δ(f_2)ds + δ(f_3)ds + ......δ(f_n)ds
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