UncleftishAtomic BeholdingTheory

For most of its beingexistence, mankind did not know what things are made of, but could only guess. With the growth of worldkenscience, we began to learn, and today we have a beholdingtheory of stuffmatter and workenergy that watchingobservation bears outconfirms, both in the worksteadlaboratory and in daily life.

The underlyingbasic kinds of stuffmatter are the firststuffselements, which link togetherbond in sundryvarious ways to give rise to the rest. Formerly we knew of ninety-two firststuffselements, from waterstuffhydrogen, the lightest and barest, to ymirstuffuranium, the heaviest. Now we have made more, such as aegirstuffneptunium and helstuffplutonium.

The firststuffselements have their being as motesparticles called uncleftsatoms. These are mightly small; one seedweight33.5 milligrams of waterstuffhydrogen holds a talenumber of them like untoequal to two followed by twenty-two naughts2×1022. Most uncleftsatoms link togetherbond to make what are called bulkbitsmolecules. Thus, the waterstuffhydrogen bulkbitmolecule bestandsconsists of two waterstuffhydrogen uncleftsatoms, the sourstuffoxygen bulkbitmolecule of two sourstuffoxygen uncleftsatoms, and so on. (Some kinds, such as sunstuffhelium, keep alone; others, such as iron, cling together in icescrystals when in the fast standingsolid phase; and there are yet more yokewayschemical bonds.) When unlike uncleftsatoms linkbond in a bulkbitmolecule, they make bindingscompounds. Thus, water is a bindingcompound of two waterstuffhydrogen uncleftsatoms with one sourstuffoxygen uncleftatom, while a bulkbitmolecule of one of the forestuffsproteins making up flesh may have a thousand thousand or more uncleftsatoms of these two firststuffselements together with coalstuffcarbon and chokestuffnitrogen.

At first it was thought that the uncleftatom was a hard thing that could be split no further; hence the name. Now we know it is made up of lessersmaller motesparticles. There is a heavy kernelnucleus with a forward bernstonish ladingpositive electric charge, and around it one or more light motesparticles with backward ladingsnegative charges. The leastsmallest uncleftatom is that of ordinary waterstuffhydrogen. Its kernelnucleus is a lonesingle forwardladenpositively charged moteparticle called a firstbitproton. Outside it is a backwardladennegatively charged moteparticle called a bernstonebitelectron. The firstbitproton has a heavinessmass about 1840-foldtimes that of the bernstonebitelectron. Early worldken folkscientists thought bernstonebitselectrons swing aroundorbit the kernelnucleus like the earth around the sun, but now we understand they are more like waves or clouds.

In all other uncleftsatoms are found other motesparticles as well, about as heavy as the firstbitproton but with no ladingcharge, known as neitherbitsneutrons. We know a kind of waterstuffhydrogen with one neitherbitneutron in the kernelnucleus along with the firstbitproton; another kind has two neitherbitsneutrons. Both kinds are seldomrare.

The next greatestlargest firststuffelement is sunstuffhelium, which has two firstbitsprotons and two bernstonebitselectrons. The everyday sort also has two neitherbitsneutrons in the kernelnucleus. If there are more or less, the uncleftatom will soon break asunderdecay. More about this later.

The third firststuffelement is stonestufflithium, with three firstbitsprotons, three bernstonebitselectrons, and its own share of neitherbitsneutrons. And so it goes, on through such everyday stuffs as coalstuffcarbon (six firstbitsprotons) or iron (26) to ones more latelyrecently found. YmirstuffUranium (92) was the last until men began to make some higher still.

It is the bernstonebitselectrons that linkbond, and so their talenumber fastsetsdetermines how a firststuffelement behaves and what kinds of bulkbitsmolecules it can help make. The worldkenscience of this behaving, in all its manifold ways, is called minglingkenchemistry. MinglingersChemists have found that as the uncleftish taleatomic number of the firststuffselements (that is, the talenumber of firststuffsprotons in their kernelsnuclei) waxesincreases, after a while they begin to show ownshipsproperties not unlike those of others that went before them. So, for a showdealexample, stonestufflithium (3), glasswortstuffsodium (11), potashstuffpotassium (19), redstuffrubidium (37), and bluegraystuffcaesium (55) can each linkbond with only one uncleftatom of waterstuffhydrogen, while coalstuffcarbon (6), flintstuffsilicon (14), germanstuffgermanium (32), tin (50), and lead (82) can each linkbond with four. This is readily seen when all are set forthdisplayed in what is called the roundaround boardperiodic table of the firststuffselements.

When an uncleftatom or a bulkbitmolecule winsgains one or more bernstonebitselectrons above its own, it takes on a backward ladingnegative charge. When it loses one or more, it takes on a forward ladingpositive charge. Such a moteparticle is called a farerion, for thatbecause the dragattraction between unlikeopposite ladingscharges flitsmoves it. When bernstonebitselectrons flitmove by themselves, it may be as a bolt of lightning, a spark off some faststandingsolid chunk, or the everyday flow of bernstonenesselectricity through wires.

Coming back to the uncleftatom itself, the heavier it is, the more neitherbitsneutrons as well as firstbitsprotons in its kernelnucleus. Indeed, soon the talenumber of neitherbitsneutrons is the greater. UncleftsAtoms with the same talenumber of firstbitsprotons but unlikedifferent talesnumbers of neitherbitsneutrons are called samesteadsisotopes. Thus, everyday sourstuffoxygen has eight neitherbitsneutrons with its eight firstbitsprotons, but there are also kinds with five, six, seven, nine, ten, and eleven neitherbitsneutrons. A samesteadisotope is known by the talenumber of both kernel motesnuclear particles, so that we have sourstuffoxygen-13, sourstuffoxygen-14, and so on, with sourstuffoxygen-16 being by far the most found. Having the same talenumber of bernstonebitselectrons, the samesteadsisoptopes of a firststuffelement behave almost alike minglinglychemically. They do show some unlikenessesdifferences, outstandinglyespecially among the heavier ones, and these can be workedused to sunderseparate samesteadsisotopes from each other.

Most samesteadsisotopes of every firststuffelement are unabidingunstable. Their kernelsnuclei break up, each at its own speedrate. This speedrate is written as the half-life, which is how long it takes half of any dealamount of the samesteadisotope thus to shift itself. The doingprocess is known as lightrottingradioactive decay. It may happen fast or slowly, and in any of sundry various ways, offhangingdepending on the makeup of the kernelnucleus. A kernelnucleus may spit out two firstbitsprotons with two neitherbitsneutrons, that is, a sunstuffhelium kernelnucleus, thus leaping two steadsplaces back in the roundaround boardperiodic table and four weightsatomic masses back in heavinessmass. It may give offemit a bernstonebitelectron from a neitherbitneutron, which thereby becomes a firstbitproton and thrusts the uncleftatom one steadplace up in the boardtable while keeping the same weightmass. It may give offemit a forwardbitpositron, which is a moteparticle with the same weightmass as a bernstonebitelectron but a forward ladingpositive charge, and thereby spring one steadplace down in the boardtable while keeping the same weightmass. Often, too, a moteparticle is given offemitted with neither ladingcharge nor heavinessmass, called the weeneitherbitneutrino. In much lightrottingradioactive decay, a moteparticle of light with most short wavelength comes out as well.

For although light oftenestmost often behaves as a wave, it can be looked on as a moteparticle, the lightbitphoton. We have already said by the way that a moteparticle of stuffmatter can behave not only as a chunk, but as a wave. Down among the uncleftsOn the atomic scale, things do not happen in steady flowingscontinuous motions, but in leaps between bestandingsstates that are forbidden. The knowledge-huntstudy of this is called lump beholdingquantum theory.

Nor are stuffmatter and workenergy unakinunrelated. Rather, they are groundwisefundamentally the same, and one can be shifted into the other. The kinshiprelation between them is that workenergy is like untoequal to weightmass manifoldedmultiplied by the foursidesquare of the hastespeed of light.

By shooting motesparticles into kernelsnuclei, worldken folkscientists have shiftedtransmuted samesteadsisotopes of one firststuffelement into samesteadsisotopes of another. Thus did they make ymirstuffuranium into aegirstuffneptunium and helstuffplutonium, and they have afterward gone beyond these. The heavier firststuffselements are all highly lightrottishradioactive and therefore are not found in the greenworldnature.

Some of the higher samesteadsisotopes are splitlyfissile. That is, when a neitherbitneutron strikes the kernelnucleus of one, as for a showdealexample ymirstuffuranium-235, it bursts into lessersmaller kernelsnuclei and free neitherbitsneutrons; the latter can then split more ymirstuffuranium-235. When this happens, weightmass shifts into workenergy. It is not much of the whole, but nevertheless it is awesome.

With enough strengthforce, lightweight uncleftsatoms can be made to togethermeltfuse. In the sun, through a rowseries of strikingscollisions and lightrottingsdecays, four uncleftsatoms of waterstuffhydrogen in this wiseway become one of sunstuffhelium. Again some weightmass is lost as workenergy, and again this is greatly big when set besidecompared to the workenergy gotten from a minglingish doingchemical reaction such as fire.

Today we wield both kinds of uncleftish doingsnuclear reactions in weapons, and kernelish splittingnuclear fission gives us heat and bernstonenesselectricity. We hope to do likewise with togethermeltingfusion, which would yield an unhemmedlimitless wellspringsource of workenergy for mankindishhuman goodgainbenefit.

SoothlyTruly we live in mighty years!