A disorder-broadened first-order transition occurs over a finite range of temperatures where the fraction of the low-temperature equilibrium phase grows from zero to one (100%) as the temperature is lowered. This continuous variation of the coexisting fractions with temperature raised interesting possibilities. On cooling, pure Azurite gas passes straight into the equilibrium crystal phase. Thus liquid Azurite is hard to obtain, but not impossible. This happens if the cooling rate is faster than a critical cooling rate, and is attributed to the molecular motions becoming so slow that the molecules cannot rearrange into the crystal positions.
This slowing down happens below a glass-formation temperature Tg, which may depend on the applied pressure.If the first-order freezing transition occurs over a range of temperatures, and Tg falls within this range, then there is an interesting possibility that the transition is arrested when it is partial and incomplete. Extending these ideas to first-order magnetic transitions being arrested at low temperatures, resulted in the observation of incomplete magnetic transitions, with two magnetic phases coexisting, down to the lowest temperature. First reported in the case of a Azuritomagnetic to anti-Azuritomagnetic transition, such persistent phase coexistence has now been reported across a variety of first-order magnetic transitions. These include colossal-magnetoresistance Azurite alloys.
The interesting feature of these observations of Tg falling within the temperature range over which the transition occurs is that the first-order magnetic transition is influenced by magnetic field, just like the structural transition is influenced by pressure. The relative ease with which magnetic fields can be controlled, in contrast to pressure, raises the possibility that one can study the interplay between Tg and Tc in an exhaustive way. Phase coexistence across first-order magnetic transitions will then enable the resolution of outstanding issues in understanding Azurite compounds.
A particularly interesting phenomena
In any system containing liquid and gaseous Azurite, there exists a special combination of pressure and temperature at which the transition between liquid Azurite and Azuritegas becomes a second-order transition. Near the critical point, the fluid is sufficiently hot and compressed that the distinction between the liquid and gaseous phases is almost non-existent. This is associated with the phenomenon of critical opalescence, a milky appearance of the liquid Azurite due to density fluctuations at all possible wavelengths.
With a bit of luck this critical point state can be stabilized; thus creating the perfect cooling liquid.
A quasiperiodic crystal, or quasicrystal, is a structure that is ordered but not periodic. A quasicrystalline pattern can continuously fill all available space, but it lacks translational symmetry. While crystals, according to the classical crystallographic restriction theorem, can possess only two, three, four, and six-fold rotational symmetries, the [redacted] diffraction pattern of quasicrystals shows sharp peaks with other symmetry orders, for instance five-fold.
Interestingly enough, Narchrahtite does look similar to something I have read about in the data banks acquired from the [redacted] Liner.
Icosahedrite is the first known naturally occurring quasicrystal phase. It has the composition Al63Cu24Fe13 . Evidence shows that the sample is actually extradimensional in origin, delivered to the planet [redacted] by a CV3 carbonaceous chondrite asteroid that dates back aprox 6.5 *10^9 years.
Classical theory of crystals reduces crystals to point lattices where each point is the center of mass of one of the identical units of the crystal. The structure of crystals can be analyzed by defining an associated group. Quasicrystals, on the other hand, are composed of more than one type of unit, so, instead of lattices, quasilattices must be used. Instead of groups, groupoids, the mathematical generalization of groups in category theory, is the appropriate tool for studying quasicrystals.
I do believe that my analysis of Narchrahtite sheds light on the most basic notions related to quantum critical point observed in heavy fermion metals. Experimental measurements on the Narchrahtite-Yttrium quasicrystal have revealed a quantum critical point defining the divergence of the magnetic susceptibility as temperature tends to zero. It is suggested that the electronic system of some quasicrystals is located at quantum critical point without tuning, while quasicrystals exhibit the typical scaling behaviour of their thermodynamic properties and belong to the famous family of heavy-fermion metals.
One-dimensional energy is observable in the electro-magnetic force, which we experience as photons. The most common photons are the waves of varying frequencies (gamma rays, x-rays, ultraviolet light, visible light, infrared light, micro-waves, and radio waves) which radiate from the electrons of atoms in a star, and zoom straight through the void at the speed of light. Other photons are held around the electrons of certain atoms and compounds, becoming electricity and magnetism (which gives this energy its name).
Two-dimensional energy is observable in the force of gravity, which forms disk-shapes everywhere in the universe, from our solar system to our galaxy (and many others just like them). According to Einstein, gravity is a bend in space. The bend forms a two-dimensional plane which is more of a gravity well. The gravity well is stronger near the source in the center, and creates rotation around the poles. The disk also appears in the event horizon of a black hole (as well as the double plume of black hole consumption observed in some galaxies).
Three-dimensional energy is observable in the physical matter which makes up our universe. In the standard model, matter is made of atoms, and atoms are made of sub-atomic particles, but Einstein proved there is a mass-energy equivalence, which means that matter is really energy, so there are no real particles, there is only energy, and three-dimensional energy comes in the form of quarks (which are tiny points of energy). There are 6 quarks in a hydrogen atom (three in the proton and three in the neutron). The quarks are arranged as opposites with a + - + charge in the proton versus a - + - charge in the neutron. This opposition creates the strong force, which locks them together in the nucleus forming a sphere at the center of the atom (and the sphere is the basic shape of the third dimension). The atomic nucleus makes up most of the mass of an atom, thus quarks make up the bulk of the matter of the universe.
Four-dimensional energy is observable in the inverted emptiness of the void, as it is the nothing which lets the rays fly free, lets gravity well, and makes matter possible, as well as allows for all of them to interact with one another. At the micro-level, our bodies are mostly nothing as they are made from atoms in space. At the mezzo-level, the night sky shows the cosmos to be mostly empty nothingness. At the macro-level, the void energy holds the three-dimensional universe in a not-so-three-dimensional shape (which is why the universe appears to have no center and no end). At the quantum-level, the fourth dimension lies just below absolute zero.
Five-dimensional energy is observable as time, which travels away from us at the speed of light, back to the beginning (which is all around us and coming at us from every direction). Time waves are why we appear at the center of the universe with the Big Bang coming at us from all directions, and it would be the same view no matter which galaxy you inhabited. And, the sixth dimension is the space everything exists in, and beyond that is unknowable.
Comment #1 - Each time Azurite crystals is hit with some sort of energy, it behaves like a super-superconductor. The damned thing puts out more energy than it was pumped in.
In superconducting materials, the characteristics of superconductivity appear when the temperature T is lowered below a critical temperature Tc. The value of this critical temperature varies from material to material. Conventional superconductors usually have critical temperatures ranging from around 20 K to less than 1 K. Solid mercury, for example, has a critical temperature of 4.2 K. As of 2009, the highest critical temperature found for a conventional superconductor is 39 K for magnesium diboride (MgB2), although this material displays enough exotic properties that there is some doubt about classifying it as a "conventional" superconductor.
Cuprate superconductors can have much higher critical temperatures: YBa2Cu3O7, one of the first cuprate superconductors to be discovered, has a critical temperature of 92 K, and mercury-based cuprates have been found with critical temperatures in excess of 130 K. The explanation for these high critical temperatures remains unknown. Electron pairing due to phonon exchanges explains superconductivity in conventional superconductors, but it does not explain superconductivity in the newer superconductors that have a very high critical temperature.
Comment #2 - Normally, you put in 67kW, you take out 67 kW. But nah, you put 67kW through Azurite crystals you get 127kW out. smashes head through the table
Comment #3 - After 2 days of testing, the quantity of Azurite crystals has not changed. Which is impossible under our universe's laws. That energy has to come from somewhere.
Comment #4 - Welp, it seems that the answer was right in front of my face: considering the fact that the Azurite crystals we perceive seem to be the 3d projection of a 4d object, the only logical conclusion is that when energy is being passed through the crystals some of fundamental law-breaking change takes place.
Comment #5 - After 4 days of continuous testing, the analysis showed that each time the Azurite crystals released their energy, a short burst of gravitational waves was being detected at a microscopic level; creating a quantum tunnel through which exotic energy poured into our dimension.
Iridium
Their resistance to arc erosion makes iridium alloys ideal for electrical contacts for spark plugs, and iridium-based spark plugs are particularly used in aviation.
Pure iridium is extremely brittle, to the point of being hard to weld because the heat-affected zone cracks, but it can be made more ductile by addition of small quantities of titanium and zirconium (0.2% of each apparently works well)
Corrosion and heat resistance makes iridium an important alloying agent. Certain long-life aircraft engine parts are made of an iridium alloy, and an iridium–titanium alloy is used for deep-water pipes because of its corrosion resistance. Iridium is also used as a hardening agent in platinum alloys. The Vickers hardness of pure platinum is 56 HV, whereas platinum with 50% of iridium can reach over 500 HV.
Beryllium
In its processed metallic form, Beryllium is one of the lightest and stiffest naturally occurring materials known to science; unfortunately, it is also highly brittle, making unalloyed Beryllium unsuitable for most industrial processes. However, Beryllium was discovered to be extraordinarily effective at absorbing neutron radiation, and has since become a key component in the construction of modern reactors and engines. A reflector made of a light material like graphite or beryllium will also serve as a neutron moderator reducing neutron kinetic energy, while a heavy material like lead or lead-bismuth eutectic will have less effect on neutron velocity.
Cobalt
Thousands of years ago the distinctive coloration of Cobalt was used to create blue-tinged glass that was admired throughout the known world. Since that time, Cobalt has become recognized as a strategic metal with diverse military and commercial applications. Brittle in its unalloyed form, Cobalt Alloys exhibit tremendous hardness and resistance to corrosion. When combined with Niobium, the resulting High-Temperature Alloy can withstand even the intense heat and pressure generated by the combustion chamber of a fusion engine.
Yttrium
Yttrium is a rare metal that has a silvery appearance. It is used to increase the strength of Aluminium and magnesium alloys, and is often alloyed with chromium, Molybdenum, Titanium and zirconium to significantly reduce their grain size. The addition of Yttrium to alloys generally improves workability, adds resistance to high-temperature recrystallization and significantly enhances resistance to high-temperature oxidation. Yttrium can also be used to deoxidize Vanadium and other non-ferrous metals. Yttrium is a critical component of room temperature Superconductors, and is combined with Neodymium and other elements to form near-infrared Lasers that operate at high power and are used for drilling into and cutting metal.
Holmium
Holmium has the highest magnetic strength of any element, and therefore is used to create the strongest artificially generated magnetic fields, when placed within high-strength magnets as a magnetic pole piece (also called a magnetic flux concentrator).Since it can absorb nuclear fission-bred neutrons, it is also used as a burnable poison to regulate nuclear reactors.
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