Delphi Collected Works of René Descartes

  CHAPTER THIRTEEN On Light

  I have already said several times that bodies that revolve always tend to move away from the centers of the circles they describe. Here, however, I must determine more specifically in what directions the parts of the matter of which the heavens and the stars are composed do tend.54

  To that end, one must know that, when I say that a body tends in some direction, I do not thereby want anyone to imagine that there is in the body a thought or a desire carrying it there, but only that it is disposed to move there, whether it truly moves or, rather, some other body prevents it from doing so. It is principally in this last sense that I use the word “tend,” because it seems to signify some effort and because every effort presupposes some resistance. Now, in as much as there are often diverse causes that, acting together on the same body, impede one another’s effect, one can, according to various points of view, say that the same body tends in different directions at the same time. Thus it has just been said that the parts of the earth tend to move away from its center insofar as they are considered all alone, and that they tend on the contrary to move closer to it insofar as one considers the force of the parts of the heaven pushing them there, and again that they tend to move away from it if one considers them as opposed to other terrestrial parts that compose bodies more massive than they.

  Thus, for example, the stone turning in a sling along circle AB tends toward C when it is at point A, if one considers nothing other than its agitation all alone; and it tends circularly from A to B, if one considers its motion as regulated and determined by the length of the cord retaining it; and finally the same stone tends toward E if, without considering the part of its agitation of which the effect is not impeded, one opposes the other part of it to the resistance that this sling continually makes to it.

  But, to understand this last point distinctly, imagine the inclination this stone has to move from A toward C as if it were composed of two other inclinations, of which one were to turn along the circle AB and the other to rise straight up along the line VXY; and imagine the inclinations were in such a proportion that, if the stone were at the place of the sling marked V when the sling was at the place of the circle marked A, it should thereafter be at the place marked X when the sling is at B, and at the place marked Y when the sling is at F, and thus should always remain in the straight line ACG. Then, knowing that one of the parts of its inclination (to wit, that which carries it along the circle AB) is in no way impeded by the sling, you will easily see that the stone meets resistance only for the other part (to wit, for that which would cause it to move along the line DVXY if it were not impeded). Consequently, it tends (that is, it makes an effort) only to move directly away from the center D. And note that, from this point of view, when the stone is at point A, it tends so truly toward E that it is not at all more disposed to move toward H than toward I, although one could easily persuade oneself of the contrary if one failed to consider the difference between the motion it already has and the inclination to move that remains with it.

  Now, you should think of each of the parts of the second element that compose the heavens in the same way that you think of this stone, to wit, that those which are, say, at E tend of their own inclination only toward P, but that the resistance of the other parts of the heaven which are above them cause them to tend (i.e. dispose them to move) along the circle ER. In turn, this resistance, opposed to the inclination they have to continue their motion in a straight line, causes them to tend (i.e. is the reason why they make an effort to move) toward M. And thus, judging all the others in the same way, you see in what sense one can say that they tend toward the places that are directly opposite the center of the heaven they compose.

  But there is still more to consider in the parts of the heaven than in a stone turning in a sling: the parts are continually pushed, both by all those like them between them and the star that occupies the center of their heaven and by the matter of that star; and they are not pushed at all by the others. For example, those at E are not pushed by those at M, or at T, or at R, or at K or at H, but only by all those that are between the two lines AF and DG together with the matter of the sun. That is why they tend, not only toward M, but also toward L and toward N, and generally toward all the points which the rays or straight lines, coming from some part of the sun and passing through the place where the parts are, can reach.55

  But, in order that the explanation of all this be easier, I want you to consider the parts of the second element all alone, as if all the spaces occupied by the matter of the first element, both [the space] where the sun is and the other [spaces], were void. Indeed, because there is no better means of knowing if a body is being pushed by some others than to see if these others actually advance toward the place where it is in order to fill the place in the case that it is void,56 I also want you to imagine that the parts of the second element at E are removed from it and, having posited that, to note in the first place that none of those above the circle TER, say at M, is disposed to fill their place, in as much as each tends on the contrary to move away from it. Then note in the second place also that those in that circle, to wit, at T are no more disposed to do so; for, even though they really move from T toward G along the course of the whole heaven, nevertheless, because those at F also move with the same speed toward R, the space E (which one must imagine to be mobile like them) will not fail to remain void between G and F, provided others do not come from elsewhere to fill it. In the third place, those that are below that circle but that are not contained between the lines AF and DG (such as those at H and at K) also do not tend in any way to advance toward that space E to fill it, even though the inclination they have to move away from point S disposes them in some way to do so (as the weight of a stone disposes it, not only to descend along a straight line in the free air, but also to roll sideways on the slope of a mountain in the case that it cannot descend any other way).

  Now the reason that impedes them from tending toward that space is that all motions continue, so far as is possible, in a straight line, and consequently, when nature has many ways of arriving at the same effect, she most certainly always follows the shortest.57 For, if the parts of the second element which are, say, at K advanced toward E, all those closer to the sun than they would also advance at the same instant toward the place they were leaving; hence, the effect of their motion would be only that space E would be filled and there would be another of equal size in the circumference ABCD that would become void at the same time. But it is manifest that same effect can follow much better if those parts that are between the lines AF and DG advance straightaway toward E; and consequently, when there is nothing to impede the latter from doing so, the others do not tend at all toward E, no more than a stone ever tends to fall obliquely toward the center of the earth when it can fall in a straight line.

  Finally, consider that all the parts of the second element that are between the lines AF and DG must advance together toward that space E in order to fill it at the same instant it is void. For, even though it is only the inclination they have to move away from point S that carries them toward E, and this inclination causes those between the lines BF and CG to tend more directly toward E than those that remain between the lines AF and BF and DG and CG, you will nevertheless see that these latter parts do not fail to be as disposed as the others to go there, if you take note of the effect that should follow from their motion. That effect is none other than, as I have just now said, that space E is filled and that there is another of equal size in the circumference ABCD that becomes void at the same time. For, as regards the change of position they undergo in the other places that they were previously filling and that still remain full of them afterwards, it is not at all considerable, in as much as they must be supposed to be so equal and so completely like one another that it does not matter by which parts each of these places is filled. Note, nevertheless, that one should not conclude from this that they are all equal, but merely that the motions of which their in
equality can be the cause are not pertinent to the action of which we are speaking.

  Now there is no shorter way of causing one part E of space to be filled while another, for example at D, becomes void than if all the parts of matter on the straight line DG, or DE, advance together toward E. For, if it were only those between the lines BF and CF that were to advance first toward that space E, they would leave another space below them at V, into which those which are at D had to come. Thus, the same effect that can be produced by the motion of the matter in the straight line DG, or DE, would be made by the motion of that in the curved line DVE:, and that is contrary to the laws of motion.

  But you may find here some difficulty in understanding how the parts of the second element between the lines AF and DG can advance all together toward E, considering that, since the distance between A and D is greater than that between F and G, the space they must enter to advance thus is narrower than that they must leave. If so, consider that the action by which they tend to move away from the center of their heaven does not force them to touch those of their neighbors that are at the same distance as they from that center, But only to touch those that are to a degree more distant from it.58 Thus the weight of the small balls 1, 2, 3, 4, 5 does not force those marked by the same numerals to touch one another, but only forces those marked 1 or 10 to rest on those marked 2 or 20, and the latter to rest on those marked 3 or 30, and so on. Thus, these small balls can well be arranged not only as you see them in Figure 7 but also as they are in Figures 8 and 9 and in myriad other diverse ways.

  Then consider that those parts of the second element, moving separately from one another (as has been said above that they must do), cannot ever be arranged like the balls in Figure 7. Nonetheless, it is only in that mode [of arrangement] that the proposed difficulty can obtain. For one could not suppose between those of its parts that are the same distance from the center of their heaven an interval so small that it would not suffice to conceive that the inclination they have to move away from that center must cause those between the lines AF and DG to advance all together toward the space E when it is void. Thus you see in Figure 9, compared with Figure 10, that the weight of the small balls 40, 30, etc. must cause them to fall all together toward the space occupied by that marked 50 as soon as the latter can leave it.

  And one can clearly perceive here how those of the balls that are marked with the same numeral are arranged in a space narrower than that which they leave, that is, by moving closer to one another. One can also perceive that the two balls marked 40 must fall a bit faster, and move proportionately a bit closer to one another, than the three marked 30, and these three must move faster and closer to one another than the four marked 20, and so on.

  Hereupon you will perhaps say to me that, as it appears in Figure 10 that the two balls 40, 40, after having fallen the slightest bit, come to touch one another (which is why they stop without being able to fall lower). In the very same way, the parts of the second element that should advance toward E will stop before having succeeded in filling the whole space we have supposed there.

  But I respond thereto that they cannot advance toward E the slightest bit without it being enough to prove perfectly what I have said, to wit, that since the whole space that is there is already filled by some body (whatever it might be), the parts press continually on that body and make an effort against it as if to chase it out of its place.59

  Then, beyond that, I reply that, since their other motions, which continue in them while they are thus advancing toward E, do not permit them for a moment to remain arranged in the same way, those motions impede them from touching one another, or rather cause them, upon touching, immediately to separate again and thus not to cease for that reason to advance uninterruptedly toward the space E, until it is completely filled. Thus one cannot conclude from this anything other than that the force with which they tend toward E is perhaps vibratory in nature and redoubles and relaxes in diverse small tremors according as the parts change position. This seems to be a property quite suited to light.

  Now, if you have understood all this sufficiently by supposing the spaces E and S and all the small angles between the parts of the heaven to be empty, you will understand it still better by supposing them filled with the matter of the first element. For the parts of that first element in the space E cannot impede those of the second between the lines AF and DG from advancing to fill it in just the same way as they would if it were void, because, being extremely subtle and extremely agitated, they are always as ready to leave the places where they are as any other body might be to enter them. And for this same reason, the parts of the first element that occupy the small angles between the parts of the heaven cede their place without resistance to those coming from that space E and tending to go toward the point S. I say toward S rather than toward any other place because the other bodies which, being more united and larger, have more force all tend to move away from it.

  Indeed, one should note that they pass from E toward S among the parts of the second element that go from S toward E, without the ones in any way impeding the others. Thus, the air enclosed in the sand clock XYZ rises from Z toward X through the sand Y, which does not for that reason cease to fall in the meantime toward Z.

  Finally, the parts of that first element that are in the space ABCD, where they compose the body of the sun and there turn very rapidly in a circle about point S, tend to move away from it in all directions in a straight line, in accordance with what I have just set out. By this means, all those in line SD together push the part of the second element that is at point D, and all those in line SA push that which is at point A, and so on. And they do so in such a way that this alone suffices to cause all those parts of the second element between the lines AF and DG to advance toward the space E, even though they might have no inclination themselves to do so.

  Moreover, since they must thus advance toward that space E when it is occupied only by the matter of the first element, it is certain that they also tend to go there even though it is filled by some other body and, consequently, that they push and make an effort against that body as if to drive it out of its place. Thus, if it were the eye of a man that were at the point E, it would actually be pushed, both by the sun and by all the matter of the heaven between the lines AF and DG.

  Now one must know that the men of this new world will be of such a nature that, when their eyes are pushed in this manner, they will have from it a sensation very much like that which we have of light, as I will say more fully below.

  CHAPTER FOURTEEN On the Properties of Light

  But I want to stop a while at this point to set out the properties of the action by which their eyes can be thus pushed. For they all agree so perfectly with those that we note in light that, when you have considered them, I am sure you will admit, like me, that there is no need to imagine in the stars or in the heavens any other quality but this action that is called by the name of “light.”

  The principal properties of light are: (1) that it extends around in all directions about bodies one calls “luminous,” (2) to any distance, (3) and in an instant, (4) and ordinarily in straight lines, which must be taken to be the rays of light; (5) and that several of these rays coming from diverse points can come together at the same point, (6) or, coming from the same point, can go out toward different points, (7) or, coming from diverse points and going toward diverse points, can pass through the same point without impeding one another; (8) and that they can also sometimes impede one another, to wit, when their force is very unequal and that of some of the rays is much greater than that of the others; (9) and, finally, that they can be diverted by reflection, (10) or by refraction, (11) and that their force can be increased, (12) or diminished, by the diverse dispositions or qualities of the matter that receives them. There are the principal qualities that one observes in light and that all agree with this action, as you are about to see.

  (l) The reason is evident why this action should extend in all directions a
round luminous bodies, because it proceeds from the circular motion of their parts.

  (2) It is also evident that it can extend to any distance. For example, supposing that the parts of the heaven between AF and DG are already themselves disposed to advance toward E, as we have said they are, one can no longer doubt that the force with which the sun pushes those at ABCD should also extend out to E, even though there is a greater distance from the one to the other than there is from the highest stars of the firmament down to us.

  (3) And knowing that the parts of the second element between AF and DG all touch and press one another as much as possible, one also cannot doubt that the action by which the first ones are pushed must pass in an instant out to the last, in just the same way that the force with which one pushes one end of a stick passes to the other end in the same instant; or rather (so you make no difficulty on the basis that the parts of the heaven are not attached to one another as are those of a stick) in just the same way that, as the small ball marked 50 falls toward 6, the others marked 10 also fall toward 6 at the same instant.

  (4) Regarding the lines along which this action is communicated and which are properly the rays of light, one must note that they differ from the parts of the second element through the intermediary of which this same action is communicated, and that they are nothing material in the medium through which they pass, but they designate only in what direction and according to what determination the luminous body acts on the body it is illuminating. Thus, one should not cease to conceive of them as exactly straight even though the parts of the second element that serve to transmit this action, i.e. light, can almost never be placed so directly one on the other that they compose completely straight lines. In just the same way, you can easily conceive that the hand A pushes the body E along the straight line AE even though it pushes it only through the intermediary of the stick BCD, which is twisted. And in just the same way, you can conceive that the ball marked 1 pushes that marked 7 through the intermediary of the two marked 5 and 5 as directly as through the intermediary of the others, 2, 3, 4, 6.