Miles Mathis' Charge Field
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Mapping properties of the Elements - Colors

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Mapping properties of the Elements  - Colors Empty Mapping properties of the Elements - Colors

Post by Cr6 Sun Apr 24, 2016 6:52 pm

AtomicNumberAtomicSymbolElementCrystal structureColor
1Hhydrogen hexagonalcolorless
2Hehelium hexagonalcolorless
3Lilithium cubic: body centeredsilvery
4Beberyllium hexagonalsteel gray
5Bboron rhombohedralblack
6Ccarbon hexagonalblack
7Nnitrogen hexagonalcolorless
8Ooxygen cubiccolorless
9Ffluorine cubiccolorless
10Neneon cubic: face centeredcolorless
11Nasodium cubic: body centeredsilvery
12Mgmagnesium hexagonalsilvery
13Alaluminiumcubic: face centeredsilvery
14Sisilicon cubic: face centeredgray-black
15Pphosphorus monoclinicwhite-yellow
16Ssulfur orthorhombicyellow(pale)
17Clchlorine orthorhombicgreenish-yellow
18Arargon cubic: face centeredcolorless
19Kpotassium cubic: body centeredsilvery-white
20Cacalcium cubic: face centeredsilvery-white
21Scscandium hexagonalsilvery-white
22Tititanium hexagonalgray
23Vvanadium cubic: body centeredbright white
24Crchromium cubic: body centeredsilvery-white
Was just thinking about how Mathis' Charge field provides different "elemental properties" as single atoms up to the full element particularly with colors.  For solid elements, it seems as the structures grow to the higher carousel with "arms" the color of the element takes on a more "silvery/silvery-white" appearance. 

How photons/charge field hit these structures and recycle the input energy into various color properties is a big question?  In other words, why is copper orange-red, sulfur yellow, chlorine greenish and carbon black?

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Mapping properties of the Elements  - Colors Empty Re: Mapping properties of the Elements - Colors

Post by Cr6 Sun Oct 30, 2016 7:40 pm

Electro-negativityElementSymbolAtomic number
2.2HydrogenH1
HeliumHe2
0.98LithiumLi3
1.57BerylliumBe4
2.04BoronB5
2.55CarbonC6
3.04NitrogenN7
3.44OxygenO8
3.98FluorineF9
NeonNe10
0.93SodiumNa11
1.31MagnesiumMg12
1.61AluminumAl13
1.9SiliconSi14
2.19PhosphorusP15
2.58SulfurS16
3.16ChlorineCl17
ArgonAr18
0.82PotassiumK19
1PotassiumK19
1.36CalciumCa20
1.54ScandiumSc21
1.63TitaniumTi22
1.66VanadiumV23
1.55ChromiumCr24
1.83ManganeseMn25
1.88IronFe26
1.91CobaltCo27
1.9NickelNi28
1.65CopperCu29
1.81ZincZn30
2.01GalliumGa31
2.18ArsenicAs33
2.55SeleniumSe34
2.96KryptonKr36

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Mapping properties of the Elements  - Colors Empty Re: Mapping properties of the Elements - Colors

Post by Cr6 Sun Oct 30, 2016 7:41 pm

RubidiumRb37
0.82StrontiumSr38
0.95YttriumY39
1.22ZirconiumZr40
1.33NiobiumNb41
1.6MolybdenumMo42
2.16TechnetiumTc43
1.9RutheniumRu44
2.2RhodiumRh45
2.28PalladiumPd46
2.2SilverAg47
1.93CadmiumCd48
1.69IndiumIn49
1.78TinSn50
1.96AntimonySb51
2.05IodineI53
2.1XenonXe54
2.66CesiumCs55
2.6BariumBa56
0.79LanthanumLa57
0.89CeriumCe58
1.1PraseodymiumPr59
1.12NeodymiumNd60
1.13PromethiumPm61
1.14SamariumSm62
EuropiumEu63
1.17GadoliniumGd64
TerbiumTb65
1.2DysprosiumDy66
HolmiumHo67
1.22ErbiumEr68
1.23ThuliumTm69
1.24YtterbiumYb70
1.25LutetiumLu71
HafniumHf72
1.27TantalumTa73
1.3TungstenW74
1.5RheniumRe75
2.36OsmiumOs76
1.9IridiumIr77

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Mapping properties of the Elements  - Colors Empty Re: Mapping properties of the Elements - Colors

Post by Cr6 Sun Oct 30, 2016 7:42 pm

2.2PlatinumPt78
2.2GoldAu79
2.28MercuryHg80
2.54ThalliumTl81
2LeadPb82
1.62BismuthBi83
2.33PoloniumPo84
2.02AstatineAt85
2RadonRn86
2.2FranciumFr87
RadiumRa88
0.7ActiniumAc89
0.89ThoriumTh90
1.1ProtactiniumPa91
1.3UraniumU92
1.5NeptuniumNp93
1.38PlutoniumPu94
1.36AmericiumAm95
1.28CuriumCm96
1.3BerkeliumBk97
1.3CaliforniumCf98
1.3EinsteiniumEs99
1.3FermiumFm100
1.3MendeleviumMd101
1.3NobeliumNo102
1.3LawrenciumLr103
1.3RutherfordiumRf104

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Mapping properties of the Elements  - Colors Empty Re: Mapping properties of the Elements - Colors

Post by Nevyn Mon Oct 31, 2016 1:47 am

Electronegativity, symbol χ, is a chemical property that describes the tendency of an atom or a functional group to attract electrons (or electron density) towards itself.[1] An atom's electronegativity is affected by both its atomic number and the distance at which its valence electrons reside from the charged nucleus. The higher the associated electronegativity number, the more an element or compound attracts electrons towards it.

Well that sounds quite physical.

Electronegativity cannot be directly measured and must be calculated from other atomic or molecular properties.

Oh, I guess not.

You have to be very, very careful around these calculated values. A measured value is real. You might have to work your way through the machines used to measure it before you know what that value means, but it is measuring reality at some level. Any calculated value relies on some form of theory. That is what the equations are, a mathematical representation of the theory. That is why Miles says the theory comes first and the math second. You can't represent what you don't know.

That doesn't mean they are useless, you just have to unwind what they actually mean and hopefully you can find the right path with the right theory.

Thanks for putting this together, Cr6. This is the kind of stuff I need to analyze the atomic models. This is the kind of data that could be used in R so that we can see some of the relationships between elements a bit easier.
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Mapping properties of the Elements  - Colors Empty Re: Mapping properties of the Elements - Colors

Post by Chromium6 Wed Sep 27, 2023 1:50 am

Just wanted to add this theory:

Young–Helmholtz theory

Thomas Young and Hermann von Helmholtz assumed that the eye's retina consists of three different kinds of light receptors for red, green and blue
The Young–Helmholtz theory (based on the work of Thomas Young and Hermann von Helmholtz in the 19th century), also known as the trichromatic theory, is a theory of trichromatic color vision – the manner in which the visual system gives rise to the phenomenological experience of color. In 1802, Young postulated the existence of three types of photoreceptors (now known as cone cells) in the eye, with different but overlapping response to different wavelengths of visible light.[1]

Hermann von Helmholtz developed the theory further in 1850:[2] that the three types of cone photoreceptors could be classified as short-preferring (violet), middle-preferring (green), and long-preferring (red), according to their response to the wavelengths of light striking the retina. The relative strengths of the signals detected by the three types of cones are interpreted by the brain as a visible color.

For instance, yellow light uses different proportions of red and green, but little blue, so any hue depends on a mix of all three cones, for example, a strong red-sensitive, medium green-sensitive, and low blue-sensitive. Moreover, the intensity of colors can be changed without changing their hues, since intensity depends on the frequency of discharge to the brain, as a blue-green can be brightened but retain the same hue. The system is not perfect, as it does not distinguish yellow from a red-green mixture, but can powerfully detect subtle environmental changes. In 1857, James Clerk Maxwell used the recently developed linear algebra to offer a mathematical proof of the Young–Helmholtz theory.[3]

https://www.webexhibits.org/causesofcolor/mind.html
https://en.wikipedia.org/wiki/Young%E2%80%93Helmholtz_theory
Maxwell:
https://www.cambridge.org/core/journals/earth-and-environmental-science-transactions-of-royal-society-of-edinburgh/article/abs/xviiiexperiments-on-colour-as-perceived-by-the-eye-with-remarks-on-colourblindness/5E589C9929D114B96CB9325E8FF0CAB3
https://www.mv.helsinki.fi/home/molkkone/files/OlkkonenEkroll.pdf



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