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animation of a 3D parametric grid in processing
by sofia georgakopoulou & dino rossi
ethz mas caad 0910
This is for a Pearl OD-05 clone. I was actually going to do a couple more, but now the heat is getting to be too much for me. With the oven going in that tent, it gets pretty hot. Wearing the respirator makes it even worse. I was starting to feel kind of woozy, so I stopped. You know, I never had to worry about how hot it got when I was younger. This aging thing is BS.
SOFTlab: (n)arcissus. Parametrically designed installation for the stairwell of the Frankfurter Kunsverein.
This work is not current . It has been replaced in part by another model, described later in this album ; though the concept of a 'higher degree' proton remains interesting to me.
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Proposed 2-D schematic of a higher degree proton, (3rd) ; modeled on the parametric function :
x(t) = ( ±sine( 3 * |t| ))^3 * cosine( t )
y(t) = ( ±sine( 3 * |t| ))^3 * sine( t )
t = { 0 .. pi }
The operator '±', in this case, is resolved to '+' . I believe that resolving this operator to '-' would express the petals of a companion 3rd degree anti-proton in the companion anti-universe . From our perspective, (if we could 'see through' to them), these would appear to be opposite the ones shown, (about the same center) .
Each 'petal' of the 'flower' represents a quark ; those at 2 and 10 o'clock, up-quarks ; that at 6 o'clock, a down-quark . Their order of development is 2 o'clock, 6 o'clock, 10 o'clock, (and these can be seen as 'red', 'green' and 'blue', respectively) .
Although i believe that under most circumstances, (if this general function is valid), protons are of exponent 1 or 2 . It is worth considering that under high energy conditions, (such as those in 'atom-smashers', the Big Bang, or near event horizons), protons could be boosted to third or higher degree energies . {It doesn't affect their radius, (which is 1, within the model), but it does narrow the petals as degree is raised. }
Please note the comparative sharpness of the bends at the origin . Assuming that a quark is indivisible, it will not split down the center of its petal . But assuming that the group is not indivisible, the most likely place for it to come apart should be where the 'stress' is concentrated by a local peak in curvature --- at the origin .
Not shown is its companion antiproton, which i believe occupies the same location, (on center), in our companion antiuniverse . Were it to be visible, it would appear as three additional petals having the same center ; one opposite each of those shown .
If the proton does come apart . Combinations that mix opposing matter and antimatter quarks become possible --- even likely . But to preserve the identicality of the companion universes, i believe that two protons must be involved ; (so that the swaps are even ) .
.....
If such also applies to neutrons, and can be stabilized by gravitation ... it raises the interesting supposability that there is, actually, a hard object at the center of a 'black hole' . It would be composed of higher degree neutrons . In such a case, though gravitation would indeed be intense, the event horizon would not form and the black hole would not be precisely black, but visible in very long radio-waves .
My work is amateur and may be wrong .
A link to a schematic view of a 1st degree proton within this model
A link to a schematic view of a 5th degree proton within this model
A link to a schematic view of a 7th degree proton within this model
( IMG_5760 ) or ( IMG_5757 )
The "Line" concept was done within one week, we had the task to design a free standing “Parametric Paravent” for the Meeting Room of the renovated CAAD Chair. The idea was to work with a line, treating it as the simplest way to divide a space. The paravent is a self designed structure and works like this: Given a single module with a certain deviation of its gravity center, the system recognizes and corrects this deviation by adding more modules, making the paravent at the end rigid and self-standing.
For further information of this and other projects go to: