On perusing an issue of The Bulletin of the American Mathematical Society from 2003, I came across a paper entitled: THE HIRONAKA THEOREM ON
RESOLUTION OF SINGULARITIES:
S0273-0979-03-00982-0.pdf (ams.org)
which featured examination of a number of singular surfaces characterized by exotic properties, especially singularities and cusps. I decided to use my Mathcad program to attempt to create similar complex surfaces and polyhedra - with varied results- some of which I present in this post. I also was able to generate contour maps of the 3D surfaces, which definitely manifested cusps and singularities.
The first complex polyhedron to be considered was:
z= f(x,y) = tanh (x13 ) yielding:
But the contour map yielded so many folds and at high density it was impossible to parse.
A more tractable equation was then used:
z = f(x,y) = sin(x3 + y 3) tanh(x) tanh(y)
Which generates the surface:
And the corresponding contour map:
For which we see the emergence of cusps at the corners and perhaps a singularity near the center, but nothing definite or specific yet.Now we change the Mathcad equation to:
f(x,y) = sin(x7 + y7) tanh(x3) tanh(y3)
And obtain the surface:
And contour:Note that cusps have definitely emerged at the corners, as well as potential singularities - which also appear at the left and right sides of the contour map.
Next we generate a surface more in line with the cusped entity shown in the authors' Fig.7. We use the equation: f(x,y) = x2 - y 3
And we find for the surface:
And the contour:
For which the contour associated with the '0' line bears a remarkable similarity to the cusp resolved by dragging in the AMS paper Fig. 7
Another interesting find is when one goes to higher degrees of any of the polynomial equations the complexity appears to alternate, e.g. for the shapes above and using instead: f(x,y) = x11 - y 13
We find for the surface:
And the contour:
But when we then use: f(x,y) = x12 - y 14
We find for the surface:
And the contour:
Examination shows each has changed radically merely by increasing the degree of x, y by one. I also found it possible to alter the cusp extent and intensity merely by changing the factor for hyperbolic functions in some equations. E.g. for:
f(x,y) = tanh (x2 ) exp( py) - x4
We see the surface go from:
To the much more pronounced cusping:
Merely by changing to tanh (3x2 ) . The cusp enhancement is also apparent on inspecting the two contour maps, with the altered factor tanh version to the right:
In a future post I will explore possible parameterizations of these (and other) examples, as well as testing the authors' speculation:
"Singular curves are the shadow of smooth curves in higher dimensional space."
Questions for readers: Is the last contour a 'singular curve? Is it the shadow of a smooth curve in a higher dimensional space?
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