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The Locomotive - Lighthouse Survival Blog

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1901.] Til E LOCOMOT I Y E. ^g<br />

<strong>The</strong> plate being 13.51" wide and 0.53" thick (on an average), with a tensile strength<br />

of 59,680 pounds per square inch, the total strength of the whole solid plate was<br />

13.51" x0.53"x59,G80 = 427,327 lbs.<br />

If tlie joint had withstood a stress of 427,327 pounds before breaking, its efficiency<br />

would have been 100 per cent. Since, however, it actually did fail when the pull became<br />

201,700 pounds, the efficiency, according to the method of calculation adopted by<br />

the Watertown authorities, was<br />

201,700-427,327=47.2 per cent.<br />

(<strong>The</strong> Watertown report gives the efficiency 47.1 per cent. <strong>The</strong> difference is unimpor-<br />

tant.)<br />

This method of calculation does not appear to us to be entirely fair, because the joint<br />

tested is not an integral number of "units" in width. <strong>The</strong> total width is four times<br />

the pitch, it is true ; but in an actual double riveted joint in a boiler there would be<br />

eight rivets in a section four units wide instead of only seven, as there were in the joint<br />

here described. <strong>The</strong> width of the specimen, in order to correspond to seven rivets,<br />

ought to be 3£ units instead of 4. That is, the total width of the plate ouo-ht to be<br />

3iX3%" = 11 ]|". <strong>The</strong> strength of the solid plate would then be<br />

then be<br />

llif" x 0.53" x 59,680 = 373,634 lbs.<br />

<strong>The</strong> efficiency of the joint, according to this amended mode of calculation, would<br />

201 , 700 + 37 J,634 =54.0' per cent.<br />

,<br />

which agrees perfectly, (as it should,) with the efficiency of this same joint as calculated<br />

by the first of the methods given above.<br />

We trust that we have established, to the satisfaction of anyone who may be inter-<br />

ested, the fact that the criticism upon our method of computing the efficiency of riv-<br />

eted joints has no just foundation. This is not a case where the doctors disaqree, as<br />

Mr. Dixon phrases it. In view of the errors that he made in setting down the data<br />

which led to his comparison, it would be more accurate to say that this is a case where<br />

the patient refused to take the medicine that the doctor prescribed.<br />

<strong>The</strong> year 1889 marked a revolution in the aluminum industry. Castner and Netto,<br />

by new and ingenious processes, had made metallic sodium (the reducing agent of<br />

Deville's process) at a greatly reduced cost, and had thereby largely reduced the cost<br />

of jn'oducing aluminum. New life had thus been put into the industry, and the yearly<br />

output had increased to 71 tons, while the selling price of the pure metal had decreased<br />

to less than $5.00 per pound. In fact, that very year it fell to about half that figure.<br />

Besides tins, the electric processes of Cowles Bros, and of Ileroult were furnishing<br />

aluminum in copper and iron alloys (but not the pure metal) at even lower prices. <strong>The</strong><br />

last year of the century finds the industry upon an entirely different basis. From an<br />

aunual production of 70 tons it has risen to the relatively enormous figure of 7,000<br />

tons; and the price has fallen from nearly $5.00 a pound to the almost incredible figure<br />

of 30 cents. <strong>The</strong> seeds jof this revolution were already germinating in 1889, for in that<br />

year pure aluminum, made electrolytically (by Hall in America and by Heroult in Europe)<br />

began to undersell the product of the sodium processes, and two years later the sodium<br />

processes were distanced and driven out of the business. <strong>The</strong> pure sodium exhibited<br />

at Paris in 1889 was all made by the sodium process; while that shown in 1900 was all<br />

made electrolytically.— Prop. J. W. Richards, in <strong>The</strong> Journal of the Franklin Institute.

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