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Series editors' preface - Wood Tools

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mechanical effects of repeated shrinkage/<br />

swelling cycles, or stress-setting of the wood.<br />

However, experiments with wood taken from<br />

artefacts thousands of years old have shown<br />

the wood to have retained its hygroscopicity<br />

and its capacity to dimensionally respond to<br />

changes in moisture content. The assumption<br />

should therefore prevail that wooden objects,<br />

regardless of age, can demonstrate dimensional<br />

movement when subjected to variable relative<br />

humidity conditions.<br />

2.5 Mechanical properties<br />

In the evolution of trees, wood tissue has<br />

developed which has highly effective axial<br />

compression (i.e. compression along the grain)<br />

and bending strength characteristics. For its<br />

weight, this wood demonstrates amazing stiffness<br />

as well as fracture resistance and it is<br />

therefore utilized in structural products such as<br />

furniture. However, although axial strength of<br />

wood is impressive, the comparative weakness<br />

of wood perpendicular to the grain, in both<br />

compression and tension, can often be the limiting<br />

factor of mechanical performance. This is<br />

indicated by examples ranging from surface<br />

indentation and splitting to the failure of joints.<br />

Given the anisotropic nature of wood, the<br />

many possible modes of loading wood tissue,<br />

the many environmental conditions and defects<br />

which influence strength, and the array of different<br />

structural applications of wood in furniture,<br />

a thorough discussion of mechanical<br />

properties is hardly feasible here. Therefore<br />

this section will merely highlight selected<br />

aspects of the strength of clear (defect-free)<br />

wood and the major factors that influence it in<br />

relation to furniture.<br />

2.5.1 Defining mechanical properties<br />

In recognition of the anisotropic nature of<br />

wood, it is traditional to consider the strength<br />

of wood along its three principal axes: longitudinal,<br />

radial and tangential. Parallel to grain<br />

(longitudinal) strength is significantly greater<br />

than strength across the grain; however, since<br />

there may be only minor difference between<br />

radial and tangential directions, it is appropriate<br />

to simply consider average strength perpendicular<br />

to the grain.<br />

<strong>Wood</strong> and wooden structures 83<br />

Strength measures the ability of a material to<br />

resist applied force or load. The strength of<br />

material is commonly expressed in terms of a<br />

stress value. Stress is defined as load per unit<br />

area, and is calculated by dividing the magnitude<br />

of the applied load or force by the crosssectional<br />

area over which it is distributed. A<br />

general formula:<br />

stress = load/area<br />

In English-speaking countries, loads have traditionally<br />

been measured in pounds (lb) and<br />

areas in square inches (sq. in). In continental<br />

Europe, kilograms and centimetres were used.<br />

In SI units, Mega Newtons per square metre<br />

(MN/m2 ) are used.<br />

The basic modes of load application are<br />

compression, tension and shear. The components<br />

in Figure 2.19 are subjected to a single<br />

type of stress. In practice, a combination of<br />

stresses may occur, as in the bending of a<br />

beam. A beam is an elongated member supported<br />

at various points along its length with<br />

one or more loads acting perpendicular to its<br />

axis. For example, the beam of Figure 2.20 is<br />

supported at each end with a concentrated<br />

load at its mid span. As a result of the consequent<br />

bending deformation, the upper surface<br />

is shortened and stressed in longitudinal compression;<br />

the lower surface is stretched and<br />

thereby stressed in tension. These axial stresses<br />

in tension or compression are referred to simply<br />

as bending stresses; they are maximal at<br />

the upper and lower surfaces of the beam and<br />

diminish to zero at the mid plane of the beam<br />

(a) (b) (c)<br />

Figure 2.19 Modes of load application. Compression<br />

(a) occurs where applied forces are aligned and tend to<br />

crush a material. Tension (b) occurs where applied<br />

forces are aligned and tend to pull a material apart.<br />

Shear (c) occurs where applied forces are not aligned<br />

and tend to slide one part of a material in one<br />

direction and the other part of the material in the<br />

opposite direction

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