29. We give a second example, in illustration of the same principle.

In Fig. 12 is shown a chain 8' long, one end of which B is attached

to a wire-strainer, while the other end is fastened to a small piece

of pine A, which is 0"·5 square in section, and 5" long between the

two upright irons by which it is supported. By means of the nut of

the wire-strainer I straighten the chain as I did the string of Fig.

11, and for the same reason. I then put a piece of twine round the

chain and pull it gently. The strain brought to bear on the wood is so

great that it breaks across. Here, the small force of a few pounds,

transmitted to the chain by pulling the siring, is magnified to upwards

of a hundredweight, for less than this would not break the wood. The

explanation is precisely the same as when the string was broken by the

thread.

[Illustration: FIG. 12.]

Experimental Mechanics A Course of Lectures Delivered at the Royal College of Science for Ireland · 第 21 / 171 题