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The Locomotive - Lighthouse Survival Blog

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1893.J THE LOCOMOTIVE. 45<br />

slmpc, and jji-itty rcrtuiii to leave it in siuli a |)criiiaiiciitly strained condition that a<br />

sliglit blow will break it readily. Of coiiise the ehillinj,' in such a easc! is much more<br />

violent than it is in boilers, but the action is probably similar, diirering in degree ratlier<br />

than in kind.<br />

It may be interesting to examine tlic eilect of sudden and local t(Mnperaturc<br />

changes in glass, a body that is notoriously apt to l)reak when suddenly lieated or<br />

cooled. Tlie method of calculation that wc have used above may be summed nj) briefly<br />

in the following forinulic :<br />

o<br />

S— C X f X Af: or t =-^ TV<br />

C X M<br />

where C is the coetticicnt of expansion, M the modulus of elasticity, t the sudden<br />

change in temperature, and jS the strain per square inch produced by this cliano-e in<br />

temperature. In the case of glass we may take C .00000.7 per degree Fahrenlieit,<br />

and M — 8,000,000 pounds per square inch. We may also take the tensile strengtli of<br />

glass as !i, 400 pounds per square inch, and by substituting this for N in the second of<br />

the foregoing formukc we can find out what change in temperature will break the<br />

glass. Thus<br />

* ~ TOUOOOo X 8,000,000 "" ^^^'* *'''^'<br />

Any kitchen girl who has had experience in washing glasses could tell us that this<br />

estimate is not far from right. Indeed, glas.ses often break with a much smaller change<br />

in temperature, a fact that is sufficiently explained by their shape, but we cannot enter<br />

further into the mechanics of "this question in the present article. It appears that<br />

imless glass has been specially annealed, as it is in making beakers and test tubes and<br />

the better grades of lamp chimneys, the elastic yielding of the material surrounding the<br />

chilled spot, which we took some account of in the case of steel, does not occur to any<br />

great extent, so that the tbnnula gives a fairly accurate result without taking<br />

it into account.<br />

<strong>The</strong> Just Perceptible Difference.<br />

A lecture was delivered on Friday, January 27th, by Mr. F. Galton on the " Just<br />

Perceptible Difference," in which he pointed out that each sense organ has its own<br />

internal activities which are too faint to be perceptil)le in health, but which are not<br />

unfrequently perceived in illness, as, for example, ringing in the ear and ])eculiar taste<br />

or smell. <strong>The</strong>ir unfelt effects might, however, concur with an ordinary sense impression<br />

and intensify it. He dwelt on the influence of the imagination and adduced<br />

instances where imagination produced effects that had been mistaken for faint sensations<br />

and sometimes for plainly perce])tible ones. One of the most suitable sul)jects for such<br />

experiments he found to be the auditory imagination associated with the words perused<br />

by the eye. He described experiments frequently made by himself at meetings of<br />

scientific societies, where he had obtained unrevised copies in print of the papers about<br />

to be read. Owing to some deafness he often found himself able to follow every word<br />

distinctly only so long as his eyes rested on the paper ; he could detect the fact of any<br />

alteration in the Avording, but was quite unable to make out the substituted words.<br />

On these occasions when he raised his eyes from the ])a|)er he could not follow the<br />

reader at all. He usually found it necessary to approach him by one quarter of the<br />

previous distance, in order to follow his voice by means of the ear alone. Hence the<br />

power of the imagination plan the power of the hearing bore the same relation to the

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