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Updated: August 20, 2024
He might question whether the mirrored image of himself that he saw daily was real or refracted light made into a roseate image of the mind, but at the very least his face, unlike many middle aged men he knew, did not look like a squished shammy that he used to burnish the shine of his Mercedes Benz GL sports utility vehicle, that same vehicle which he had abandoned in the drive a few weeks ago for that emergency taxi ride to the hospital.
"I failed to find any dress-shirts, sir," began Pearson, hesitatingly. Mr. Temple Barholm grinned. "I always failed to find them myself. I never had a dress-shirt. I never owned a suit of glad rags in my life." "Gl glad rags, sir?" stammered Pearson, uncertainly. "I knew you didn't catch on when I said that to you before dinner. I mean claw-hammer and dress-suit things.
"Lord O gl y, Lord O gl y, You spoke mighty strongly Who you are, tho', all people admire! But I'll let you depart, For I believe in my heart, You had rather they did not inquire, Lord O gl y, You had rather they did not inquire." "Gl nb e, Gl nb e, What's good for the scurvy?
The reason whereof is thought to be this: Ad praesens ova cras pullis sunt meliora. ut est gl. in l. quum hi. ff. de transact. Nor is this all; for the inconvenience of the contrary is set down in gloss. c. de allu. l. fin. Quum labor in damno est, crescit mortalis egestas.
To this the honest old father answered thus: My son Dandin, when Don Oportet taketh place, this is the course which we must trace, gl. c. de appell. l. eos etiam. For the road that you went upon was not the way to the fuller's mill, nor in any part thereof was the form to be found wherein the hare did sit. Thou hast not the skill and dexterity of settling and composing differences. Why?
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.
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