Purpose:
Due to cohesion and adhesion properties of water, a container of water does not level off at the breaking point between gas and liquid. Instead, it forms a parabolic shape around the breaking point known as meniscus. The small change in height can cause a change in pressure, therefore it is necessary to account for these behaviors.
Figure 1: A view of cohesion properties in water and Mercury
Figure 2: Reading of Meniscus
Solution:
One way of accounting the pressure change is to make a triangle approximation of the change in height. The volume of the parabola would be accounted by using a triangle rotating around z - axis. This will create a larger pressure change, as x*tan15 > x2 for values around zero, and we justify this by arguing that the integrity of a structure should account for at least five percent change around threshold for force and pressure.
Below is a visual representation of the triangle approximation.
from __future__ import division> from visual import * from time import clock tri = Polygon( [(-20,0), (0,0.267949192*20), (0,0)] ) """ p = paths.circle( pos=(10,4,2), radius=10 ) #tri=shapes.triangle(pos=(0,2), length=4) extrusion(pos=p, shape=tri, color=color.yellow) """ tri = Polygon( [(-3,0), (0,0.267949192*3), (0,0)] ) p = paths.circle( pos=(0,0,-10), radius=10 ) #tri=shapes.triangle(pos=(0,2), length=4) extrusion(pos=p, shape=tri, color=color.yellow)
Figure 3: Simulated meniscus using triangle rotating around z - axis
Analysis and Uncertainty:
The triangle approximation can be mathematically expressed by :
y = x * tan(θ)
x = the radius of the circle
θ = to the angle of elevation from the lowest point of meniscus to the highest point of meniscus
The theoretical change of height is approximated by a parabola :
y = x4
or
y = x2
The uncertainty for this approximation would therefore be expressed by:
Δy = x * tan(θ) - x2
% error = {(x * tan(θ) - x2) / x2} * 100
The uncertainty remain small for small values of x, and our approximation is justified.
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