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ing only according to the square of the velocity, the least resistance that such a ball would meet with, when moving with a velocity of 1600 feet, would be equal to the pressure of 4171b, and that independent of the pressure of the atmosphere itself on the fore part of the ball, which would be 487lb more, as there would be no pressure from the atmosphere on the hinder part, in the case of so great a velocity as 1600 feet per second. So that the whole resistance would be more than 900lb to such a velocity.

9. Having said, in the last article, that the pressure of the atmosphere is taken entirely off the hinder part of the ball moving with a velocity of 1600 feet per second; which must happen when the ball moves faster than the particles of air can follow by rushing into the place quitted and left void by the ball, or when the ball moves faster than the air rushes into a vacuum from the pressure of the incumbent air let us therefore inquire what this velocity is. Now the velocity` with which any fluid issues, depends on its altitude above the orifice, and is indeed equal to the velocity acquired by a heavy body in falling freely through that altitude. But, supposing the height of the barometer to be 30 inches, or 21 feet, the height of a uniform atmosphere, all of the same density as at the earth's surface, would be 2 x 13.6 × 833 or 28333 feet; therefore 16:28333 :: 32: 8√28333 = 1346 feet, which is the velocity sought. And therefore, with a velocity of 1600 feet per second, or any velocity above 1346 feet, the ball must continually leave a vacuum behind it, and so must sustain the whole pressure of the at-mosphere on its fore part, as well as the resistance arising from the vis inertia of the particles of air struck by the ball.

10. On the whole, we find that the resistance of the air, as determined by the experiments, differs very widely, both in respect to its quantity on all figures, and in respect to the proportions of it on oblique surfaces, from the same as determined by the preceding theory; which is the same as that of Sir Isaac Newton, and most modern philosophers. Neither should we succeed better if we have recourse to the theory given by Professor Gravesande, or others, as similar differences and inconsistencies still occur.

We conclude therefore, that all the theories of the resistance of the air hitherto given, are very erroneous. And the preceding one is only laid down, till further experiments, on this important subject, shall enable us to deduce from them another, that shall be more consonant to the true phænomena of nature. LOGARITHMS

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1 9000000 || 26 1-414973 51 1707570 76 1.880814 230103027 1431364 52 1716003 3 0477121 28 144715853 1-724276 4000.000 29 1-462398 54 1-732394 50.698970 301-47712155 1-740363 6 0778151 31 1.491362 56 1.748188 7 0.845098 32 1.505150 57 1755875 8 0903090 33 1518514 58 1.763428 9 0954243 34 1.531479 59 1.770852 10 1000000 35 1.544068 | 60 1778151 11 1041393 36 1.556303 61 1.785330 121079181 37 1.568202 62 1.792392 13 1113943 38 1.579784 || 63 1.799341 14 1.146128 39 1.591065 || 64 1.806180 891949390 15 1.176091 40 1.602060|| 65 1.812913 90 1.954243| 16 1.204120 41 1.612784 66 1.819544|| 91 1.959041 171230449 42 1.623249 || 67 1.826075|| 921063788 18 1.255273 43 1.633468 68 1.832509 93 1.968483 191278754 44 1.643453 69 1-838849 94 1.973128 201301030|| 45 |¡·653213 || 70 1.845098|| 95 1.977724

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N. B. In the following table, in the last nine columns of each page, where the first or leading figures change from 9's to 0's, points or dots are now introduced instead of the 0 s through the rest of the line, to catch the eye, and to indicate that from thence the corresponding natural number in the first column stands in the next lower line, and its annexed first twe figures of the Logarithm in the second column.

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