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  • 7/30/2019 On the Application of the Law of Gravitation to the Atomic Theory-English-Gustasv Theodor Fechner.

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    On the application of the law of gravitation to the atomic theory 1)

    from

    MG Fechner, acad. Lecturer in Leipzig.

    . l If we want to defend the view that the body is a system of atoms ormolecules 2) are, by no other force than their mutual gravitational force can be

    determined to balance or to move 3) , show that we have that the really make basic

    phenomena of matter and explain appropriate discordant among themselves a way to

    the law of that force. We will therefore try to solve the inferior and in a later paper the

    following problems:

    1) How can the existence of material points (the ponderable atoms) in stable 4) are

    designed distances from each other5) , if these points are solicited by no other force

    than that mutual Gravitattionskraft?

    2) In what ways can explain without specific concurrence repulsive forces, the

    contraction and expansion of the body and the transition between the various states of

    aggregation in each other simply by their mutual gravitational ponds?

    3) What relationship has the so-called imponderables to the ponderable parts are

    attached and how can the simultaneous changes that mutually dependent in

    Ponderabilien and imponderables explained by mere effect of the law of gravitation?

    1)This paper follows on from the earlier in this archive (Vol. IX. H.3. p.257.) given, and is written withreference thereto. I will not repeat the rules here Vorerinnerungen that everything shared here so long must be

    considered problematic until it succeeds an exact mathematical analysis, to take possession of the same, butthis seems to still be subject to insurmountable difficulties.

    2)The most appropriate it seems to me, the body atoms off towards the analogy of the heavenly bodies (which

    one might think as atoms of a larger body) not yet present as absolutely indivisible, but as indivisible inrelation to each other, insofar processes between them as between the whole and nothing Ponderables proceed

    from one to the other passes. This analogy is here provisionally established, incidentally develop even more bythe following.

    3)The fact that the atoms are subject to the laws of gravity, is actually a conclusion which, gravitational law is

    itself justified as essential to the nature of the generally applicable to any size and smallness of material massesthat only certain, in the experience of reasoned evidence to the contrary Us likely to cause this Act to limit

    material mass limits for certain. However, this would mean setting a conflict between experience and

    mathematics, nowhere else instead finds, and how it would be possible, upon receipt of such a limitation, but tobe calculated by integration of the gravity effect of the smallest particles, the gravity effect of a whole body,

    however, is always still open the possibility that, besides the gravity at the atoms still other forces can occur,

    which surpassed the effect of that. However, the adoption of such vires occultae we might only be justified ifthere would be no way to explain the phenomena of matter by forces that are essential to it as such, what is to

    be tried just here.

    4)Or those distances where only the atoms oscillate to some extent to the principles of their mutual

    equilibrium, because in fact we will be led to such.

    5)Taking time to atoms, as does, in fact, the compressibility and expandability of the body and the ratio of the

    different aggregate states to each other, an assumption of varying distances (but for the same condition of the

    body are stable) is essential. The difficulty of explaining this by mere attraction forces, has been one of themain causes for the adoption of repulsive forces until now.

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    . 2So much can see that a quiet distance of all the atoms of a body by mere

    attraction forces would be inexplicable without extensive deduction. In fact, we

    consider one of 5 identical, same distance in a straight line disponierter

    atoms a, b, c, d, eAlthough existing row, then the average atomic cdoes not change

    its place, because the attractions from both sides are equal: but to the lying by atomsmust move towards the ends of the middle and can not rather come to rest until they

    are all come to the touch.

    Understandably, such a shape must also be done in any other system of movement

    of atoms, because the attraction than can compensate for some of the same in

    opposite directions in the middle. But not necessary, that, when the atoms are other

    than an initial rectilinear disposition which we set up by their mutual attraction to the

    close contact, but this is merely to be the case for certain special cases. In general, if

    three or more mutually attracting bodies are present, it will not even require a

    deflecting pulse to keep this body of approximation to the touch, for it may always be

    two of them strive therefore moving in a straight line one after the other: but at the

    same time attracting third mass they constantly distract from this straight line and act

    as each mass continuously disruptive to the approach of any two others. If now is not

    the central forces of attractions and already attained speeds of movement of all

    masses come together in some time on one point, which can only happen in some

    cases initial motion circumstances, it is a continuous, though variable, or, as we may

    call it, moving away the same may take up to infinity 6) .

    6) It can be a thereto, if not fruitful, but making interesting remark. Two atoms are by itself not capable of

    continuous movement and determine if they are held by a foreign power at a distance from each other only bytheir numbers always a straight line. Three or more atoms are sufficient to elicit an indefinitely lasting

    movement by themselves and determine their number at any time by a curved line. Should this not in aUPHOLSTERY the binary composition of lifelessness and rectilinear form of inorganic bodies on the one hand

    and on the other hand, are ternary or multiple composition, the internal automatic lively exchange and the

    curvilinear shapes of the organic body?

    . 3Thus we see that although a permanent but constantly changing, removal of

    atoms by virtue of mere attraction of the same is probably possible. However, we are

    not entitled to introduce us, as for example a crystal as a kind of fermenting mass,where each atom moving to a ponderables all other atoms and each other they would

    contribute to determine the movement, but rather we can all conclude that the

    ponderable atoms with the same body condition in relatively fixed positions, most

    with no noticeable oscillations are located at the positions of their balance with each

    other, and so the experience seems even the way we think to contradict a sole

    effective attraction, and it has, in fact, of this point of the matter until now always

    considered. But it is still, until now ignored retarded, left case in which we can find

    the solution to our problem. To him we now turn.

    There can be masses of systems thinking in which to rest (little or oscillation) of a

    part of these masses and continuous movement of the other part of these masses are

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    mutually interdependent.

    From this proposition from whose discussion will follow immediately, seems to me

    the rest of the ponderable atoms in the bodies by a duly combined movement of the

    imponderabeln atoms 7) in full compliance with both the nature of the law of

    gravitation itself, than to explain the phenomena.

    7) Only figuratively and because of the distinction, however they can still carry the name of imponderable

    atoms, as their attraction as well as the coming of the other into account. We will in the following often thanplanetary atoms, in contrast to the ponderable or solar atoms which constitute, so to speak, the skeleton of the

    ponderable mass, respectively.

    . 4In fact, we want to show only that such an arrangement of matter for individual

    rest masses is generally required for movement of the other, and then, as by the action

    of attraction law itself such arrangements, the first sight after only a very special

    hardly possible in reality, cases might appear to be caused most likely by themselves.

    Suppose we have two more (solar or ponderable) atomsA ,B , in PL 111 fig. 1st

    round which closed paths in an indefinite number of smaller (or so-called planetary

    imponderable) atoms 8) a , b , c ..... moving in such a way that at any time a greater

    number of them in the common scale ofA andB , as would run through their

    clearance 9) , these planetary atoms, whileA andB are by virtue of their peculiar

    attraction strive to approach this approximation counteracted by the

    massesA andB attract to itself and it would balance forA andB can exist if the ratio

    of the mass sizes and distances of all solar and planetary atoms would be measuredand would (through reciprocal compensation) during the movement that the sum of

    the attractions which the masses a , b , c , d, e to the side where they are located

    onA voice, always in balance would remain with the sum of attractions, which

    according to the opposite direction off,g, h , i , k, l, m , n , and the other

    resting 10) massB are expressed. Now, however, should such a strict balance of

    massesA andB in order seldom or never take place during the whole revolution of

    the planetary masses. Will be the further considerations that the movement of

    planetary atoms to the solar so arranges to allow only small oscillations of the

    approach and the same distance but most probably11)

    , so it seems this to be almost anecessary consequence of the law of attraction. However thereof afterwards.

    8) Hard light, heat, electricity.

    9) This is, for example in Figure l after the nature of the tracks listed there instead, whereas in Fig 4 in general,

    always a same amount imponderable atoms through the gap when moving the outer space.

    10) , however, is the totality of the masses a , b , c , d, e in mass against the mass sizef,g, h ...B to thedisadvantage, but an advantage in terms of proximity and nothing prevents both circumstances be compensated

    . thinking By the way, seems to me the possibility that there is a sufficient number of mutually mutuallyattracting bodies, two or more of them may be in silence or approximate rest, during movement of the other,

    even to brighten up the fact that it taken thoretisch, any time the expression for the rate for a certainnumber of bodies set to zero and can be derived from the equations thus resulting conditions must, whichsubstituted in the formulas for the rest of the body, the movement must determine the same as it is really

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    needed this rest that body to have to follow. This requires not that the forces of each of the rest of the body tobe zero are (in which case the problem would be impossible, since the rest mass of such shape even disappear)

    because of differential expression for the velocity is dv = dt, where on means the total force acting body. In

    order that dv = 0 will, is merely requires that also is equal to 0. This but may as well through opposition of

    the individual forces which express the remaining masses than by the disappearance of the individual forcesthemselves, ie, the masses of which they are expressed, are zero. The execution of calculations of this type but

    would like to, as far as I can see the current state of the analysis are as yet insurmountable difficulties.

    11) This fact leads to a surprising analogy, by engaging in such shape of the visible pulse in all of nature, thealternation of expansion and contraction, even in the nuclear realm as would find something much Grounded

    again.

    . 5Here we see already a way to return the repulsive effect of heat on mere

    attractions. In fact, the more the Community perimeters of two solar or ponderable

    atoms of the heat atmosphere, ie, increasing the mass of the moving planetary atoms,

    the further they have to be pulled from each other, so that THEREFORE really this

    attractive effect of heat, assimilate to the ponderable atoms, a repulsive effectbetween the ponderable atoms themselves could be 12) . By the way, it is easy to see

    from the foregoing, as well as three or more masses thus can be kept at rest or lower

    oscillation against each other, that in associated conditions, a greater number of

    planetary masses in their area, as moved by their space, including we are a superficial

    schema in Figures 2 and 3 have been 13) .

    12)Here, however, have to immediately offer a variety of claims: if the imponderables to express an attractiveeffect on the ponderable atoms, they must also possess gravity, contributing to the severity of the body andmove at an accelerated rate after the earth, not all of which case appears. I believe, however, these objections in

    . 15th enough to have lifted.13)

    there are is used in this schemata wherever a respective, two, three atoms have common paths around, only

    important to indicate the ratio of the movement in the periphery to the movement through the gap of the solar

    mass, not the actual shape of the tracks, which still must include far more varied curves in it. One wouldincidentally while the inside is a an atomic system to ever, two, three or more ponderable atoms was called

    jointly moving imponderable gebundne heat, which in the communal area of all, that may on the surface of the

    system, call ongoing, natural electricity .

    . 6In order to show but the way in which such arrangements may come to pass,

    we will send forward the following observation. Imagine two solar atoms only in avery far away from each other, each of which then acts as a single center for himself

    and all planetary atoms, depending on whether they come into the vicinity of one or

    the other, so ellipses, parabolas or hyperbolas for describe the nature of their original

    motion circumstances in such a way that when one thinks both solar atoms connected

    by a straight line, generally at any time as much planetary atoms intersect the

    intermediate lines, or run through the gap of the two atoms, as by its exterior, ,

    though. you do not want to initially set equal to a particular distribution of the

    imponderables.

    Let us now imagine the same solar atoms approached infinity, then, is because they

    represent a mass, no more planetary atom can cut their intermediate line, but all must

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    move only in its scope.

    From this it necessarily follows that if two initially very distant solar atoms

    gradually approaching attraction by its own or through any cause, the planetary

    atoms, which run to each of them in particular, their orbits must gradually change in

    the way that they their motion, whereby they are guided between two atoms,

    converted into those of which they are made merely by two atoms, or in other words,the mono central movement must with more approximation pass the attracting centers

    for increasing planetary atoms in a bi-center until in total approximation, the same is

    become bizentral for all, but where the two coincide centralization.

    . 7 Consider now two solar or pondorable atomsA andB , which initially are in a

    very great distance in a space through which a certain quantity of free flows of

    imponderable indefinite directions, and assume that each of these ponderable atoms

    from this free imponderable that came near him, a certain quantity of bound, ie have

    determined to closed movements around. Assuming that all conditions for both atoms

    were initially equal, we are the same arrangement with their imponderabeln

    atmospheres by the FIG Scheme 4 can imagine.

    It is easily seen that in this very large distance, where generally the same amount of

    imponderable atoms, the intermediate line ofA andB must be cut as their outer space,

    own imponderable atmosphere each atom without infiuence on the move because of

    the attraction off,g, h , i , kofB is kept the balance toward the equal attracting the

    planetary compositions a , b, c, d, e to the opposite side, thus isA definitely only by

    the attraction ofB and the imponderable atmosphere to motion are determined, though

    because of the huge distance with a weak force and inversely asB ofA . Both will

    therefore begin to approach.

    . 8 To the same extent, however, when this happens, the trajectories of the atoms

    to be imponderabelnA andB in the manner indicated above must change by

    modifying the schema of Figure 4 more and more into the scheme of Figure

    1 converting, namely by imponderable atoms to only mono centrallyA orB could

    only now beginning to be bizentral move both, and such shape is more and more

    gone out of the space of the two atoms in its exterior, a part goes away in endless

    lines, such as We this in our previous paper (. Vol IX, p 268) have discussed and thus

    the phenomenon of convergence in each of antibody molecules released due to heator light, while at the same time some of the available free space of the imponderable,

    through which the ponderable atoms move at their approach through, on the other

    hand in relation to their approach an ever larger part of the two jointly, as shall be

    bound by any particular.

    . 9 Since these shape the ratio of the imponderable's outdoor space both

    ponderable atoms with their approach increases more and more in its clearance

    against, it must in a corresponding degree of return, they learn to the side facing away

    from each side, always more to grow, and although the attraction of the systemA to

    systemB with its approximation always growing, so can but this increase experiencedin part by the loss, both systems virtue by the release of a portion of their

    imponderabeln mass whose vacant, partially compensated, but partly, and this is the

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    main thing that can always be originally such a number of planetary atoms around

    each of the solar atoms assume that the ratio of entering into the outer space planetary

    masses is so great in the approximation to by his return, in some moments the further

    approximation to prevent both;, in a word, it can cause the whole assembly, which we

    . 4 as to effect stable distances of the solar atoms, by virtue of the law of gravitation

    required declared. . 10 There are hereafter two ponderable atoms, they provided only a sufficient

    number of planetary masses to have, which prevents the representation of phenomena

    to take as anything to be able to mutual attraction not approach indefinitely, but in

    some, by their own masses and the mass ratios of their planetary atmospheres certain

    degree of approximation is the return of running in their common peripheral

    planetary atoms keep this part of the balance and the solar or ponderable atoms are

    then not closer together. But it is then no real fixes Stationary same can accept, but

    the ponderable atoms are still in relation to their and their atmospheres common

    center of gravity, depending on the changing situation of planetary atoms (in which,however steadily accumulating in the outer space remains mostly) back and oscillate

    again within certain limits. However, these oscillations can of achievement that

    GIeichgewichtspunkts to not be great, and because upon further approximation the

    same once more planetary atoms occur in the outer space and thus the pondorabeln

    atoms have to call back when removing the same but more atoms in the gap and

    thereby re-approximation of the ponderable atoms cause.

    . 11 It is clear that the boundaries where the ponderable atoms cease to approach

    each other, so must occur rather, the more each atom planetary matter has to be,

    because so several planetary atoms then, when approaching the ponderable or solaratoms, turn to the outside and thus express a stronger return, therefore, be, and it's

    certainly not a circumstance which prevented in cases where such consistent

    distances express themselves, this really attach a sufficient number of planetary

    mass. On the other hand could also really nderen cases as little planetary mass to be

    present, that a limit approximation of the never occurring by increasing the

    approximation attraction of ponderable atoms would receive the excess weight on the

    influence of altered nuclear distribution. In this case, they would generally not

    approach though to touch, because they would have to be always more or less

    deflected from their straight attraction through their planetary mass, but probably toeach other or their common center of gravity to move, so to speak, by would also

    performed always mutually to each other.

    . 12th From the above mentioned, from now until now can be a very simple

    explanation of the propagation of the movement through the body and elasticity give

    the same and show how they depend only on the same principle.

    The fact that two pondorable atoms attract each other, but remain at a certain

    degree of approximation, in case they have sufficient planetary atmospheres, requires

    that in this case the influence which related with the approximation different

    arrangement of the planetary atmospheres to remove both atoms manifests, increases

    in a greater ratio than the influence which the approximation of the atom itself

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    expresses to enhance their attraction, therefore, conversely, that upon removal of two

    ponderable atoms of each other from any cause - the first influence decreases in a

    greater ratio than the other14) .

    14) Always presumed here that originally such a mass of planetary atoms was found that the solar atoms had to

    remain stationary at a certain distance from each other.

    So put two ponderable atomsAandBare by virtue of the arrangement of theirCommunity planetary atmospheres in equilibrium, but now goingAtoBapproached

    by force by any force, it is in virtue of the correspondingly increasing accumulation

    of planetary atmospheres, in outer space striving to rejection betweenAandBcan be

    increased through. Now two cases are possible. Can eitherBevade, then it is in virtue

    of the above-mentioned repulsion as much ofARemove it comes back to the

    previous one, the balance required between two distance, and so, consequently, the

    whole system is ofAandBby merely onAalone acting force to be moved away. The

    same will be the case if pond in a system of three or more. AtomsA,B, C... a force

    only onAacts that allow theBstrives to approach by herebyBto the equilibriumdistance ofAto come to the Capproaches and this is the same reason

    whyBofAremote, turn the original to the distance fromBremoved, so that the shape

    of such motion by the entire atom number must reproduce.

    The other case is that in whichB is prevented by a resistance upon application of a

    forceA to avoid. Then it is so long the force obtained in a forced state of

    approximation; must now only when the forceA to the same reason in its original

    distance fromB to snap back (which is done by a certain number of oscillations), out

    of which in the previous case, whereB was not prevented from escaping, the same

    ofA distant to the original distance.

    How can we explain the course of the same principle took way made the reproduction

    of motion and elasticity, no discussion will hereafter require.

    . 13 A fact that should help to give weight to this theory is that each

    communication of motion requires time: as it is, in fact, it is evident that the change

    in atmosphere arrangement, ie, the change in the course of planetary masses which

    these atmospheres composed, can not be done in one indivisible moments.

    . 14 In order not to exceed the limits of the extent of matching for this journal,

    memoir, I go on the continued application of, I hope now clearly present, theprinciple to other phenomena of matter to some objections which we compared

    different circumstances the admissibility thereof may be found to be considered. In a

    subsequent paper I think these applications, particularly in relation to

    thermodynamics, the chemical phenomena and the physical states to come back, here

    it is enough for me to have shown the fruitfulness of the principle for the present

    purpose in general.

    . 15 Our whole theory assumes that the so-called imponderables with attraction

    gifted matter are the same all ponderable matter itself, merely by the relative size of

    their atoms different from what makes that the ponderable atoms they decide to movearound and not vice versa. Just seems the experience of a severity of imponderables

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    to contradict at all, because on the one hand an increase or decrease of which is

    accompanied in a ponderable body with no bemerklichen weight change, on the other

    hand seems to be displaced the light through the attraction of the earth in any

    accelerated motion, as yet under would be a prerequisite for his severity of the

    case. However, considering that it requires already sensitive scales to measure the

    increase and decrease of the air in a solid body, but that the free imponderables inrelation to air are undoubtedly far thinner than the air at the solid bodies, so it is

    easily recognize the inaccessibility of our mechanical aids to measurements of this

    kind at all, more so probably because every escape of light or heat the escaping only a

    small fraction of the remaining imponderable's is, as well as the mass of the comet as

    it approaches the sun through the Escape the Schweifteilchen not seem to be

    significantly reduced. But As for the fact that the light do not show accelerated

    motion, no case motion to the earth, so the perception of such, though they in all

    strictness instead would find, but with the tremendous initial velocity, which one is

    compelled to assume in the light, so would the knitted impossibilities are, as I have inmy treatise on the light (XII a 2 ff this Arch.) shown by calculation.

    . 16 We now turn to another objection which can be lifted only by one after the

    first sight paradoxical, adoption, but which, on closer inspection by a striking analogy

    to this, PERFORMING, our theory can be used to support rather because they This

    analogy calls up to her existence.

    Should our theory can ever find instead, they must, as we will show now, the

    ponderable atoms possess many billions of times greater density and the

    corresponding distances are together, as the ponderable bodies whose basis they

    make, or the density of an atom will the tightness of the body in which it is received,approximately level must remain as the tightness of the sun or of Planets for leaks in

    the system of a thousand and more solar systems, worein it is receivedso that such

    shaping the atoms in miniature the conditions of the world body in large, with which

    they are already animated by the same forces, imitate, and every body as it can be,

    consider a system of numerous small, in relatively large distances from each floating

    suns that are each individually or collectively several orbits of planetary atoms. It

    needs no discussion that this view is much beauty, so poetic, has decreased by seems

    to make life in the seemingly most steadfast and determined by the existence of all

    the body by balancing the fine balance allwaltender forces. The natural philosopherwho takes possession of this view, is it a big step to press forward and perhaps

    believe already justified by the beauty of so attractive inferences and by the

    subsequent from all sides analogies their way; physicist abstracted but cheap of such

    reasons .

    . 17 Consider the fact itself, which compels us to set out the assumption of such

    enormous density of atoms in relation to bodies composed of them.

    It is certainly to the law of gravity that attract all bodies, two stones on earth,

    therefore, to be just as good as she herself from the ground, except that the size of the

    attraction of the stones with each other against the world disappears, because excess

    weight of the mass of the latter. If now, you will have to close, this circumstance does

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    already with two relatively even large stones that their mutual attraction can be

    considered as zero, how much more this will have to be the case with the almost

    infinitely small atoms, and if a stone the other, which falls next to him from a height,

    precisely because of this fact can not determine to move, how much less is an atom

    for others to determine the movement because their mutual attraction must be

    outweighed by the common attraction to the earth body as infinite. Now, however,experience shows us that the cohesion, which we did by attraction of atoms depends

    on the law of gravity is a force that even significantly outweigh the seriousness by

    any body else, for example, we handle at its upper end , with its lower end should fall

    in ruins. Therefore seems the cohesion (and just as the chemical attraction) by the law

    of gravity can not be explained at all.

    Several physicists have therefore found also persuaded to accept a growing force

    for cohesion, for a price higher than the ratios of the square nearby. However, this

    seems to us to not be absolutely necessary, if we consider the following.

    Go to the law of gravitation two elements, the mass, but also the proximity of the

    attracted body. Now, in relatively closer proximity of two bodies can, however, their

    magnetic effect almost disappear on each other when a third, though distant attractive

    center has a disproportionate mass superiority over both, as in the above case of two

    stones and the phenomena of planetary attraction toward the sun. But however as

    here the element of mass has the upper hand over the element of proximity and

    thereby determines the attraction, as can also be reversed cases think where the

    element of proximity to such a degree outweighs the element of earth, that the

    attraction of a body (earth or Erdmittelpunkts) although of greater mass but against

    the mutual attraction of two bodies of smaller mass (atoms), which disproportionatelybut closer than this body (the center of the earth) are disappearing. So pull two balls

    already on the surface, which have each only one millionth of the mass of the Earth,

    each other more strongly than they are attracted to the earth's center, wofern their

    centers closer to each other than to the thousandth part of the earth's radius are.

    We see that a path revealed in such manner, regardless of against the ground so

    disproportionate smallness of atoms with the law of gravity to reconcile the existence

    of cohesion, by namely the proximity of the atoms in proportion to their mass, the

    mass of the earth and the distance from the center of the earth, in which the Earth's

    mass must be thought united, so assume that the influence of this proximity providesabout the influence of the mass of the Earth to such a degree as to make it the

    phenomena of cohesion necessary. - By itself, it may have nothing improbable, and

    some a priori philosophy might conclude that the nature of two cases, both of which

    are feasible in the formula of its laws as may, will have not only realized the one, and

    that therefore while it has carried out a case in the phenomena of gravity and the

    movements of the planets, where the mass is the decisive factor for the attraction,

    even another realm'll find instead, where it depends on the area.

    . 18 This general observation, however, seems closer but when taking into account

    all circumstances thereby lead to contradictions. One finds that if two small atoms

    themselves (with their attractive centers to which the removal is to apply the law of

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    gravitation, in any case remain to the sum of their radii away from each other) to

    attract more in contact or close contact of their surfaces, as they are attracted by the

    vast mass of the Earth, its tightness for many billions of times must be greater than

    that of the Earth 15) , therefore, of course, much greater, if they are to attract more and

    from a distance, which in any case actually see the atoms instead . But if we were to

    assume that the body stocks really so dense atoms and then calculated, in whichdistances, these atoms would have found for the mean density of the composite from

    their bodies as we watch those came out, so we would see each other again, that these

    distances were so great that the attractions of the atoms could be a very small fraction

    of the attraction they learn through the earth only, so we seem to accept very dense

    atoms that we yet introduced only to explain the cohesion again lead to nothing by, us

    both required in order not to come with the observed mean density degrees of body in

    opposition, by increasing the distance to lose the profit again, we were looking to

    acquire the atoms by increasing their resistance; or in a word, Our adoption by to

    explain the phenomenon A, thus seems to fall into inevitable conflict with oneanother.

    15), namely the removal of its attracting centers would otherwise still remain too large to allow for their small

    mass, a preponderance or just DC coming up with the earth force, if not precisely this circumstance would beoffset by the adoption of a large leak for them by this way a relatively large mass is compressed into a small

    space. It must, as one can easily calculate a spherical atom of Rhine. Foot radius has a 2 trillion 3371

    million times have greater density than the mean density of the earth is to express only on its surface a severityequal attraction, or to be of the nature that a material point directly to befnde on its surface, just as much of

    him as would be attracted to the Earth. But it is foot radius apparently still too large accepted by far for

    the size of an atom and in turn it can be shown that the smaller one assumes the atoms, even more so its density

    must be placed growing, if they are still in contact of their surfaces one of the Earthpower to express the sameforce because of reduction of its radius, although the proximity of their centers and therefore the square ratio ofthis approximation, the attraction of atoms grows, alone at the same time the mass of the atoms, and the

    attractive force decreases according to the cubic relationship, so that So definitely decreases the attraction ofatoms in constant contact with their surfaces by the simple ratio of its stages, which is now to compensate

    decrease by a corresponding increase in the density.

    . 19This objection, however, can raise when we, in accordance with all previous,

    the cohesion and generally make attraction phenomena of the atomic world not

    merely of the solar relatively fixed atoms dependent but gebundnen also and mainlyby the attraction of the planetary, or so-called , moving imponderabeln atoms. The

    solar atomAis characterized in the distance and relative equilibrium against

    atomBobtained in that a larger amount of planetary mass, on the outside of the

    system ofAandB,as moved by its interspace. Now we canAandBvery well in such

    distances from each other move that their mutual attraction would be far outweighed

    itself from the earth, because the observed tightness of the body, in fact, this requires,

    we provided only the one attraction put much stronger, found between each of the

    two atoms and its first planetary mass surrounding it instead. Because:

    1) Can we then without getting a huge leak for the whole system of atoms, thetightness of all the individual both as solar planetary Atoms very large, because the

    density of the bare mass in the solar neighborhood of each atom must then be

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    enormous, but even these can be removed accordingly.

    2) Is it possible to see how the gravity can not produce disturbance in the

    movements of planetary atoms to solar when the mutual attraction of the same in

    their area actually much stronger than Earth's, because the planetary masses then

    solar of the atoms such velocity must obtain informed that even if they come in larger

    distances from their solar atoms, the attraction of the earth, their direction can notchange noticeably (as we see one such example in the light).

    . 20 As a direct proof of the immense attraction strength of the atoms in their

    vicinity can be incidentally mention the fact that the light, which can not be

    appreciably deflected from its straight-line path from the total mass of the earth

    considering his speed, but when it goes close to the masses of so much smaller atoms,

    a well-known distraction after experiencing these atoms.

    . 21 So we are now out there, the bodies have as systems of one hand relatively

    fixed larger, on the other hand, to look at these moving smaller atoms, all of whichpossess atoms tremendous tightness and the arrangement is that the fixed centers in

    relatively very are widely spaced from each other, but to urge the most mobile atoms

    in the vicinity of this fixed center points together.

    It will not be inappropriate, as the track from self-presenting analogy with the

    arrangement of the heavenly bodies from the other side of something, not as if we

    wanted to conclude, but because we can make some interesting comparisons here.

    So we look at the world body as so many atoms in a larger size system or giant

    body (or several such) and see what relationship does the tightness of such a single

    world atom to intermediaries tightness of the system in which it is included, such asthe tightness of the sun or earth (the mass of the individual solar systems thinking to

    the space occupied by their total system, distributed to the density of a system of any

    quantity of solar systems16) . In order to do this accurately, we would certainly

    actually the mutual distances of the solar system, and the mass that contains each one

    of them, to know what is not so: but for our purpose it is enough out of the same mass

    of our solar system and the distance to lay the nearest star as something general to

    reason. Now we do not even know the distance of the nearest fixed star is certainly

    one of us, but know that it is enormous. Would by its light intensity calculated the

    star of the first magnitude, in case they were with our sun the same nature,320000mal be as far from us as the earth from the sun, and this relationship we will

    assume as a least likely, anyway, another important factor where only the size of the

    numbers to be shown in general, to thousands, even millions, more or less not.

    16) Because it is understood that we are to retain the analogy, not only must the density of the earth or sun with

    the intermediaries tightness of their own individual system, which just so imagine a solar atom with its

    planetary atmosphere compare.

    After Laplace provisions, the entire mass of our solar system was to be equal to asphere of 71.03 times the diameter of Earth from the mean density of the earth. We

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    distribute this material to a diameter which is as much as the distance of the earth

    from the sun 320000mal, then the tightness, this ball is filling, the mass density of the

    earth inversely as the cube of 71.03 Earth radii to the cube by 320000 Erdweiten, or

    (since 1 = 12130 Erdweite diameter of Earth) as the cube of 71.03, which we prefer

    to put 72 17) , the cube of 12130mal 320000, di (7 digit guest by means of logarithms

    calculated) as 1 to 1 trillion 156634 trillion. This is the ratio of the density of an atomin the large space, if we want to consider this in relation to a world body as such, to

    the density of a system of several such world atoms.

    17) The Uranus may still be behind the planet.

    . 22Should really be the body systems present us with analogous ratios of atoms,

    then offers the following represents Throw: It seems as if we are then the most

    ponderable bodies appear to be somewhat thin, so the atoms in the void, what

    separates , would have to lose a certain extent. But it is to take care that the gaps of

    the higher atomic layers are always filled by the atoms of the lower part in the bodies

    by putting them see through them, and that since the absolute distance of the atoms in

    any case, as the ratio of the same may be designed to their own atoms, imperceptibly

    can against all of us to be measurable distances, the space in which this gradually

    thinking of the spaces completed for our eyes to an apparent continuity (considering

    the distance from which we body the always need to look with our eyes, if at all

    seeing the same should take place), can be so low to still appear to us as a layer of

    thickness imperceptible. Quite a similar way we can see the Milky Way almost as a

    coherent mass, regardless of their solar systems probably immense distance fromeach other.Moreover, we must always remember that the same ratios of atoms held in

    our sense organs, as in the bodies that we perceive by and beings stocks whose hands

    itself from solar systems in the corresponding distances would also feel the Milky

    Way as a dense mass can how to nuclear systems, is a measure which, of course,

    when we come to other levels of nature, not to throw away, for tightness and thinness

    are merely relations, where we apply ourselves as a benchmark when we talk of big

    or small. What is even more natural than that size, their relationship seems mediated

    by an Act to other levels change, the transition to a corresponding degree. Maybe is

    the density of atoms, the density of the composite from them world body and thetightness of the giant body that emerge again only by a combination of many celestial

    bodies in a geometric progression, the exponent should be set but physically infinite.

    . 23 It is not unlikely that even the sun equal to our atoms are able to organize

    themselves to different states, but from what we can observe only a kind. The

    isolation in which we see our sun seems to point to a gas state analog constitution of

    the body to which it belongs, which I mention merely to counter the objection that

    could be hernehmen of the newly implemented analogy that arrangements as we have

    it set up to represent the cohesion, the sky will not (but perhaps hinted in the double

    stars) sees.

    . 24 We believe finally have an infinitely repeated objection to a philosophical

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    school of the possibility that refer to the mere matter illimitierte attractions instead,

    has made the need to take into consideration. Kant says: If one were to those without

    a limiting repulsive force assume that all particles of matter would have to approach

    to infinity and flow together in a point, so it could not really limited body take place,

    as it shows us the experience.

    Kant's proof would be all right if you spread the through space initially conceived

    matter18) all attraction resistant and solely against a particular point addressed might

    think, because there the motion of all particles in this direction then nothing

    counteracted, so all the particles could are in fact only in this center to rest. But how

    could probably head over to see 1) that in the infinite space in itself a point can be set

    as the center, and therefore could in no points preferably be such a confluence, and 2)

    what is the main thing that the limitation, which requires Kant to not coalesce into a

    single point takes place, already it is that the inflowing to the same body also attract

    each other reciprocally, and therefore distracted constantly with their directions to

    this point, and must determine to movements to each other, such as we actuallyperceive the celestial bodies.

    18) Kant, however, leaves the mat only caused by the attraction and repulsion, they would be at a prius the

    matter, but basically they fall for him so that together, because he finds no other features in it, than of those

    forces and the space in which they act, itself

    Incidentally, the important fact remains undiscussed in Kant's view, where as the

    reciprocal certain limitation of the attractive and repulsive force lie at different points

    of the space, which makes it possible for him the emergence of different and mutuallylimiting body because, like setting the attraction and repulsive force par excellence in

    the world about an arbitrariness that a certain amount of each distributed on certain

    points, both must mutually cancel in general, or only the excess of one over the other

    may not be effective. Now the philosophy is in their language although answer: A

    arbitrariness in certain distribution of attraction and repulsion to certain conditions

    need to single points of space not to be accepted, if you imagine that in space any

    quantitative relations between attraction and repulsive force are realized, almost to

    exhaustion of their term, and considering that basically a place only by a certain is

    that we some observing any one arrangement of matter, ie, such a relation to it,however in relation to the infinite space of each place itself has an indifferent place,

    which is not even a specific matter before creation of the place is, therefore, no

    arbitrariness can find in terms of a choice of certain places instead.

    This rejection of arbitrariness seems to me to be very good indeed given by you can

    say it would be rather arbitrary, everywhere nemliche ratio thereof to want to put on

    all points with par set of general attraction and repulsion, since in their phrase the

    possibility of all conditions and there all is to find space in the room. Alone the same

    circumstance would just as well come to the adoption of a sole attraction to equip by

    here, rather than imagining an initial uniform distribution of the attractive force ormatter (philosophy will make between two no difference) across the room, but the

    could make most general idea of their distribution, which would then cause the kind

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    of self-assemblies as we really observe. It must be then that the more attractive parts

    of the to determine from weaker attraction to the movement and the system thus

    created either himself again by a mass of even stronger attraction to move or to those

    discussed sentences against certain masses, by virtue of occurring in their

    approximation peculiar arrangement of the moving masses around them are kept in

    relative silence, and then the emergence of the solid body is based. In general,however, would hereafter in the infinity of space all possible under the general law of

    attraction cases of motion occur because the matter hypothesi ex to start was at all

    possible imaginable conditions and arrangements to each other, of which the nature

    of their movement depends on which very well agrees with the idea that the world is

    infinite, the exhaustive or to exhaust themselves aspiring realization of a concept or

    an idea, which themselves are infinite things in themselves.

    Suppose the latter notion, then the matter would also be represented as follows: The

    general concept of matter as an attraction with talented area, involved in his

    community at the same time all different degrees of attraction and all the differentparts of the room. Therefore, the realization of this concept in the world to the infinite

    variety and different distribution of matter itself appears to be 19) .

    19) The still remaining space of this page, I think not being able to use more than by the message that is

    published by the ingenious author of the above essay just now, in L. Voss in Leipzig: the (with Biot's portraitspruce) first band the second edition of the German editor of Biot's textbook of experimental physics or natural

    science experience. Compared with the 1 Bd of the first edition, this newly published first volume, amongother features, also characterized in that demonstrable inaccuracies in the previous edition corrected here and

    incomplete representations appear completed here in a way that as much of the diligence of the translator, all of

    whose thorough study the newer and latest discoveries testify. The other additions are either connected directlyto the text, or if the size of the circumference made it necessary to have turned on the special circuit chapter

    proper place partly in the form of comments and additions. - With regard to the view developed in the aboveAbh reason, I ask the same way, the authors compare m. Introduction to the newer chemistry Bem.4 p 263-264. Kastner