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An Encyclopaedia of civil engineering : historical, theoretical and practical : illustrated by upwards of three thousend engravings on wood by R. Branston / by E. Cresy
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Chap. XXII.

TIMBER AND ITS PROPERTIES.

1293

cubes of their diameters: in rectangular beams, the lateral strengths are to each other asthe breadths and squares of the depths, the strength varying as the breadth multiplied intothe square of the depth.

A piece of timber of the greatest strength that can be cut out from a round tree isobtained by dividing the diameter of the circle into three equal parts, raising perpen-diculars upon it, and prolonging them till they cutthe circumference; a rectangle uniting these pointsshows the form of the strongest beam that can beobtained. The comparative strength of beams, but nottheir actual strength, may be calculated by the fore-going rules: the value of actual strength must beconverted into relative on account of the length andother dimensions being relative ; thrice the length ofa beam, is to its depth, as its absolute cohesion is toits relative strength, to which must be added theweight of the timber.

The strains upon a beam fixed at one end in a walland loaded at the other is four times greater thanwhen the same weight is hung upon the middle of thesame beam, and the latter supported at the two ex-tremities : when a beam is fixed at both its extremitiesand loaded in the middle, its strength is to that whenonly supported at its two ends as 3 to 2 : when a weight is uniformly distributed over abeam, its mechanical action to produce fracture is only one-half of what it is when collectedin the middle.

Let Z = the length in inches :

6 = the breadth in inches :

eZsthe depth in inches :

W = the weight in pounds that would break it:

Ssthe weight requisite to break a piece of similar timber, whoselength, breadth, and depth are eacli 1 inch : then,

as

(W

bd a

S,

which S will be a constant number of reference for computing the strength of any piece oftimber of the same kind, under all variety of dimensions and modes of fixing and loading.For a beam fixed at one end, and loaded at the other,

S bd a

W =

l

For a beam fixed at one end, and loaded uniformly throughout,

w=i^£*

For a beam supported at each end, and loaded in the middle,w _4 Sbd*

For a beam supported as above, and loaded uniformly,

8S bd*

~r~

For a beam fixed at one end, and loaded in the middle,

W _——

For a beam fixed as above, and loaded uniformly,

12 S bd*

' v= ——

The value of S has been deduced from a variety of experiments, and in the followingtable is shown the experimental strength of different timbers, when exposed to a transversestrain.

Alder -AshAcaciaBeechChestnutElm -Fir, Riga -, Mein el

Value of Cohesive Strength of a Rod an Inch Square.

-

-

- 1590

Fir, Norway

-

.

- 2355

-, Scotch

-

-

- 1866

-, New England

-

-

- 1556

-, Spruce

-

-

- 1350

Larch

-

-

- 1620

-, very young

-

-

- 1590

Mahogany, Spanish

-

- 1635

- •, Honduras

2376

1746

1102

1395

1896

966

1275

1911