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Three is a chair designed by Mani Mani, fishtnk. Made with removable components, three is held with magnetic joinery in a plywood frame to be used as a lounge chair or three cushions.
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, (7th) ; modeled on the parametric function :
x(t) = ( ±sine( 3 * |t| ) )^7 * cosine( t )
y(t) = ( ±sine( 3 * |t| ) )^7 * 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 7th 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 ; and that it is sharper than it had been when the degrees 3 and 5 had been applied in the parametric function, (previous posts) . 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 . It seems that as degree is raised, the flower may become more brittle .
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 ) .
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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 3rd degree proton within this model
A link to a schematic view of a 5th degree proton within this model
( IMG_5766 )
Parametric model of a diffuser for the LED fireplace in OpenSCAD. "Bathtub" pocket so model can be used directly as a mold for the silicone mold. A handful of variables control the number of pixels, depth and wall thicknesses. (johnpopadic.com/2014/04/19/cnc-moldmaking/)
Ybl Miklós Architectural Faculty's advanced arch. modeling, parametric-generative design course blog
@ Balazs Marko dean, architect
@ Levente Gyulai instructor, architect
@team - Andrea Diana Keresztesi Trinh Hai Dang, Sziszi Imra-Pall, Sandor Cseke, Molnar Stefania, Koralia Giori, Levente Arato, Diana Csepanyi, Daniel Vagner, Peter Potsubay, Kati Bodo, Armen Armaganjan, Patrik Kovacs, Gabor Laczko
Fig. 3 Granulometric Samples: particle-size distributions (PSDs), key statistical derivatives and parametrically-resolved principle particle populations. Sample modes and median particle sizes are given, with black numbers referring to minimally-dispersed (MD), and white numbers to fully-dispersed (FD) samples. The PSDs are presented as particle sizes (in µm) on a logarithmic scale versus normalised volume, with Wentworth size boundaries of clay/silt (3.9 µm), silt/very-fine sand (62.5 µm), and very-fine sand/fine sand (125 µm) indicated by dotted lines. The sedimentary fractions are quantified in terms of fine (3.9-20 µm) and coarse silt (20-62.5 µm), very-fine sand (62.5-125 µm), and fine sand (125-250 µm), and depicted as pie charts with blue colours referring to MD, and red colours to FD samples (see legend). Parametrically-resolved, partially-overlapping principle particle populations are plotted in blue for MD, and red for FD samples. The population modes are indicated as black, white and grey triangles (see legend). Dominant particle populations are listed as mode/mean values (in µm) with corresponding relative percentages. Minimally-dispersed PSDs of a succession of laminations forming a representative slackwater couplet are superimposed, with partially-constrained modes highlighting the depositional size trends in the coarse silt and fine silt particle populations over the course of the flood flux (see legend).