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Updated: June 21, 2025
They made that which, notwithstanding its fluctuations, we may call 'the constant quantity' to be the sound, exactly as we do with the multiform As and Bs just noticed. On the other hand, modern purists consider, not altogether incorrectly as to the fact, that the notation has somehow been settled and fixed, and they are disposed to force the sound into conformity.
A little while afterwards the whole peaceful parsonage of Upper Wood lay in deep sleep; only old 'Lizebeth went about the passage calling: "Bs, bs, bs." She wanted to get the old grey cat into the kitchen to catch the mice during the night.
Still, of course, I never dared to leave the room for an instant, for I was not sure when he might come, and the billet was such a good one, and suited me so well, that I would not risk the loss of it. "Eight weeks passed away like this, and I had written about Abbots, and Archery, and Armor, and Architecture, and Attica, and hoped with diligence that I might get on to the Bs before very long.
Joe pronounced this word, as if it began with at least twelve capital Bs. "Why don't I rise? That were your observation when I broke it off, Pip?" "Yes, Joe." "Well," said Joe, passing the poker into his left hand, that he might feel his whisker; and I had no hope of him whenever he took to that placid occupation; "your sister's a master-mind. A master-mind." "What's that?"
Now it is easy to show that this wave will touch the arc BP at this point C. For since, by construction, FD + 3/2 DG + GL are equal to FB + 3/2 BA + AL; on deducting the equals LH, LA, there will remain FD + 3/2 DG + GH equal to FB + 3/2 BA. And, again, deducting from one side GH, and from the other side 3/2 of AS, which are equal, there will remain FD with 3/2 DG equal to FB with 3/2 of BS. But 3/2 of DG are equal to 3/2 of ES; then FD is equal to FB with 3/2 of BE. But DC was equal to 3/2 of EB; then deducting these equal lengths from one side and from the other, there will remain CF equal to FB. And thus it appears that the wave, the semi-diameter of which is DC, touches the arc BP at the moment when the light coming from the point L has arrived at B along the line LB. It can be demonstrated similarly that at this same moment the light that has come along any other ray, such as LM, MN, will have propagated the movement which is terminated at the arc BP. Whence it follows, as has been often said, that the propagation of the wave AH, after it has passed through the thickness of the glass, will be the spherical wave BP, all the pieces of which ought to advance along straight lines, which are the rays of light, to the centre F. Which was to be proved.
Then I could see them receiving their A. Bs. from the dignified, feudal-looking President, with his "auctoritate mihi commissâ," and walking off the stage with their diplomas in their hands; while upon the very same day, their classmate was walking up and down California beach with a hide upon his head.
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