Therefore the whole line AH will represent the time along AD,DB. Similarly the line AC or AF will represent the time along AC; and FH being by construction equal to 3/2 of CB, it will represent the time along CB in the medium; and in consequence the whole line AH will represent also the time along AC, CB. Whence it appears that the time along AC, CB, is equal to the time along AD,DB. And similarly it can be shown if L and K are other points in the curve CDE, that the times along AL, LB, and along AK, KB, are always represented by the line AH, and therefore equal to the said time along AD,DB.

Let ABC be the section, through the axis, of a hollow hemisphere, the centre of which is D, its axis beingDB, parallel to which I suppose the rays of light to come.

On gaining the rock, they found that the rag was a shred of linen, without mark of any kind to tell who had placed it there. "It must have been the freak of some Indian hunter," said Ned, examining the rock on which the little flag-staff was raised. "Stay no here are some marks cut in the stone! Look here, Tom, can you decipher this? It looks like the letter DDB."

And by prolonging the arc KQ till it meets AD at Y, the sum of the consequents is DY. Then KX ought to be to DY as 3 to 2. Whence it would appear that the curve KDE was of such a nature that having drawn from some point which had been assumed, such as K, the straight lines KA, KB, the excess by which AK surpasses AD should be to the excess ofDBover KB, as 3 to 2.

Now the finding and construction of this second oval is the same as that of the first, and the demonstration of its effect likewise. But it is worthy of remark that in one case this oval becomes a perfect circle, namely when the ratio of AD toDBis the same as the ratio of the refractions, here as 3 to 2, as I observed a long time ago.

For this point, having been found in this fashion, it is easy forthwith to demonstrate that the time along AC, CB, will be equal to the time along AD,DB.

For by supposing just the same construction, but the point A infinitely distant, giving parallel rays, our oval becomes a true Ellipse, the construction of which differs in no way from that of the oval, except that FC, which previously was an arc of a circle, is here a straight line, perpendicular toDB. For the wave of light DN, being likewise represented by a straight line, it will be seen that all the points of this wave, travelling as far as the surface KD along lines parallel toDB, will advance subsequently towards the point B, and will arrive there at the same time.

"DB?" cried Tom Collins, with a degree of energy that surprised his friend. "Let me see!" Tom carefully removed the moss, and cleared out the letters, which were unmistakeable. "Who canDBhave been?" said Ned. Tom looked up with a flushed countenance and a glittering eye, as he exclaimed "Who?

For assuming that the line AD represents the time which the light takes to traverse this same distance AD in air, it is evident that DH, equal to 3/2 ofDB, will represent the time of the light alongDBin the medium, because it needs here more time in proportion as its speed is slower.

The second oval is that which serves for rays that tend to a given point; in which oval, if the apex of the surface which receives the rays is D, it will happen that the other apex will be situated between B and A, or beyond A, according as the ratio of AD toDBis given of greater or lesser value. And in this latter case it is the same as that which Des Cartes calls his 3rd oval.

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