THE MECHANICAL PROPERTIES OF WOOD INCLUDING A DISCUSSION OF THE FACTORS AFFECTING THE MECHANICAL PROPERTIES, AND METHODS OF TIMBER TESTING
TEXT
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ith compressive stress over the section, the compressive stress being maximum at the section of greatest deflection on the concave side. The convex surface is under tension, as in an or
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er each square inch of area and the crushing strength is equal to the maximum load (P) divided { P } by the area of the cross-section (A). {
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be taken into consideration in the design of timber structures. It is maximum at the neutral plane and decreases to zero at the outer elements of the section. The shorter the span of a
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rupture until it has deformed considerably under loads at or near its maximum strength, or one which still hangs together after it has been ruptured and may be bent back and forth witho
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38 rings, and decreases rapidly from 38 to 47 rings. The strength at maximum load is not so great with the most rapid-growing wood; it is maximum with from 14 to 20 rings per inch, and
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rom the better situation, and were superior in toughness, the work to maximum load being 36.8 as against 31.2 for pignut. The trees had about twice as many rings per inch as others from
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otnote a: It will be noted that the temperature was 230°. This is the maximum | | temperature by the maximum-temperature recording thermometer, and is due to the handling | | of
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ighing beam is kept balanced after the yield point is reached and the maximum load, and at least one point beyond it, noted. _Log of the test_: The proper log sheet for this test consi
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ain diagram is continued to at least one deformation point beyond the maximum load, and in event of sudden failure, the direction of the curve beyond the maximum point is indicated. A b
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nd the movable head of the static machine and pulled in two. Only the maximum load was recorded. (See Fig. 46, No. 1.) [Illustration: FIG. 46.--Designs of tension test specimens used i
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size shown in Fig. 45. The apparatus will be as shown in Fig. 44. The maximum load only will be taken and the result expressed in pounds per inch of width. The speed of the moving head
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| | Cr. str. at max. ld. = Crushing strength at maximum load. | |-----------------
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| | Cr. str. at max. ld. = Crushing strength at maximum load. | |-----------------
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See also _ibid._, Vol. LXX, p. 37. GRISARD, JULES, et VANDENBERGHE, MAXIMILIEN: Les bois industriels, indigènes et exotiques; synonymie et description des espèces, propriétés physique
so would exist just the same. Moreover, it would be found in the
latter case that the bow would be much harder to bend than where
the pieces were not glued together--in other words, the
_stiffness_ of the bow would be materially increased.
~Stiffness~ is the property by means of which a body acted upon
by external forces tends to retain its natural size and shape,
or resists deformation. Thus a material that is difficult to
bend or otherwise deform is stiff; one that is easily bent or
otherwise deformed is _flexible_. Flexibility is not the exact
counterpart of stiffness, as it also involves toughness and
pliability.
If successively larger loads are applied to a body and then
removed it will be found that at first the body completely
regains its original form upon release from the stress--in other
words, the body is ~elastic~. No substance known is perfectly
elastic, though many are practically so under small loads.
Eventually a point will be reached where the recovery of the
specimen is incomplete. This point is known as the ~elastic
limit~, which may be defined as the limit beyond which it is
impossible to carry the distortion of a body without producing a
permanent alteration in shape. After this limit has been
exceeded, the size and shape of the specimen after removal of
the load will not be the same as before, and the difference or
amount of change is known as the ~permanent set~.
Elastic limit as measured in tests and used in design may be
defined as that unit stress at which the deformation begins to
increase in a faster ratio than the applied load. In practice
the elastic limit of a material under test is determined from
the stress-strain diagram. It is that point in the line where
the diagram begins perceptibly to curve.[2] (See Fig. 1.)
[Footnote 2: If the straight portion does not pass through the
origin, a parallel line should be drawn through the origin, and
the load at elastic limit taken from this line. (See Fig. 32.)]
~Resilience~ is the amount of work done upon a body in deforming
it. Within the elastic limit it is also a measure of the
potential energy stored in the material and represents the
amount of work the material would do upon being released from a
state of stress. This may be graphically represented by a
diagram in which the abscissæ represent the amount of deflection
and the ordinates the force acting. The area included between
the stress-strain curve and the initial line (which is zero)
represents the work done. (See Fig. 1.) If the unit of space is
in inches and the unit of force is in pounds the result is
inch-pounds. If the elastic limit is taken as the apex of the
triangle the area of the triangle will represent the ~elastic
resilience~ of the specimen. This amount of work can be applied
repeatedly and is perhaps the best measure of the toughness of
the wood as a working quality, though it is not synonymous with
toughness.
Permanent set is due to the ~plasticity~ of the material. A
perfectly plastic substance would have no elasticity and the
smallest forces would cause a set. Lead and moist clay are
nearly plastic and wood possesses this property to a greater or
less extent. The plasticity of wood is increased by wetting,
heating, and especially by steaming and boiling. Were it not for
this property it would be impossible to dry wood without
destroying completely its cohesion, due to the irregularity of
shrinkage.
A substance that can undergo little change in shape without
breaking or rupturing is ~brittle~. Chalk and glass are common
examples of brittle materials. Sometimes the word _brash_ is
used to describe this condition in wood. A brittle wood breaks
suddenly with a clean instead of a splintery fracture and
without warning. Such woods are unfitted to resist shock or
sudden application of load.
The measure of the stiffness of wood is termed the ~modulus of
elasticity~ (or _coefficient of elasticity_). It is the ratio of
stress per unit of area to the deformation per unit of
{ unit stress }
length. { E = ------------- } It is a number indicative of
{ unit strain }
stiffness, not of strength, and only applies to conditions
within the elastic limit. It is nearly the same whether derived
from compression tests or from tension tests.
A large modulus indicates a stiff material. Thus in green wood
tested in static bending it varies from 643,000 pounds per
square inch for arborvitæ to 1,662,000 pounds for longleaf pine,
and 1,769,000 pounds for pignut hickory. (See Table IX.) The
values derived from tests of small beams of dry material are
much greater, approaching 3,000,000 for some of our woods. These
values are small when compared with steel which has a modulus of
elasticity of about 30,000,000 pounds per square inch. (See
Table I.)
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| TABLE I |
|------------------------------------------------------------------------------|
| COMPARATIVE STRENGTH OF IRON, STEEL, AND WOOD |
|------------------------------------------------------------------------------|
| | Sp. | Modulus of | Tensile | Crushing | Modulus |
| MATERIAL | gr., | elasticity | strength | strength | of |
| | dry | in bending | | | rupture |
|-------------------------+----- +------------+----------+----------+----------|
| | | Lbs. per | Lbs. per | Lbs. per | Lbs. per |
| | | sq. in. | sq. in. | sq. in. | sq. in. |
| | | | | | |
| Cast iron, cold blast | | | | | |
| (Hodgkinson) | 7.1 | 17,270,000 | 16,700 | 106,000 | 38,500 |
| Bessenger steel, | | | | | |
| high grade (Fairbain) | 7.8 | 29,215,000 | 88,400 | 225,600 | |
| Longleaf pine, | | | | | |
| 3.5% moisture (U.S.) | .63 | 2,800,000 | | 13,000 | 21,000 |
| Redspruce, | | | | | |
| 3.5% moisture (U.S.) | .41 | 1,800,000 | | 8,800 | 14,500 |
| Pignut hickory, | | | | | |
| 3.5% moisture (U.S.) | .86 | 2,370,000 | | 11,130 | 24,000 |
|------------------------------------------------------------------------------|
| NOTE.--Great variation may be found in different samples of metals as well |
| as of wood. The examples given represent reasonable values. |
|------------------------------------------------------------------------------|
TENSILE STRENGTH
~Tension~ results when a pulling force is applied to opposite
ends of a body. This external pull is communicated to the
interior, so that any portion of the material exerts a pull or
tensile force upon the remainder, the ability to do so depending
upon the property of cohesion. The result is an elongation or
stretching of the material in the direction of the applied
force. The action is the opposite of compression.
Wood exhibits its greatest strength in tension parallel to the
grain, and it is very uncommon in practice for a specimen to be
pulled in two lengthwise. This is due to the difficulty of
making the end fastenings secure enough for the full tensile
strength to be brought into play before the fastenings shear off
longitudinally. This is not the case with metals, and as a
result they are used in almost all places where tensile strength
is particularly needed, even though the remainder of the
structure, such as sills, beams, joists, posts, and flooring,
may be of wood. Thus in a wooden truss bridge the tension
members are steel rods.
The tensile strength of wood parallel to the grain depends upon
the strength of the fibres and is affected not only by the
nature and dimensions of the wood elements but also by their
arrangement. It is greatest in straight-grained specimens with
thick-walled fibres. Cross grain of any kind materially reduces
the tensile strength of wood, since the tensile strength at
right angles to the grain is only a small fraction of that
parallel to the grain.
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| TABLE II |
|--------------------------------------------------------------|
| RATIO OF STRENGTH OF WOOD IN TENSION AND IN COMPRESSION |
| (Bul. 10, U. S. Div. of Forestry, p. 44) |
|--------------------------------------------------------------|
| | Ratio: | A stick 1 square inch in |
| | | cross section. |
| | Tensile | |
| KIND OF WOOD | strength | Weight required to-- |
| | R = ----------- +----------------------------|
| | compressive | Pull apart | Crush endwise |
| | strength | | |
|---------------+-----------------+------------+---------------|
| Hickory | 3.7 | 32,000 | 8,500 |
| Elm | 3.8 | 29,000 | 7,500 |
| Larch | 2.3 | 19,400 | 8,600 |
| Longleaf Pine | 2.2 | 17,300 | 7,400 |
|--------------------------------------------------------------|
| NOTE.--Moisture condition not given. |
|--------------------------------------------------------------|
Failure of wood in tension parallel to the grain occurs
sometimes in flexure, especially with dry material. The tension
portion of the fracture is nearly the same as though the piece
were pulled in two lengthwise. The fibre walls are torn across
obliquely and usually in a spiral direction. There is
practically no pulling apart of the fibres, that is, no
separation of the fibres along their walls, regardless of their
thickness. The nature of tension failure is apparently not
affected by the moisture condition of the specimen, at least not
so much so as the other strength values.[3]
[Footnote 3: See Brush, Warren D.: A microscopic study of the
mechanical failure of wood. Vol. II, Rev. F.S. Investigations,
Washington, D.C., 1912, p. 35.]
Tension at right angles to the grain is closely related to
cleavability. When wood fails in this manner the thin fibre
walls are torn in two lengthwise while the thick-walled fibres
are usually pulled apart along the primary wall.
|--------------------------------------------|
| TABLE III |
|--------------------------------------------|
| TENSILE STRENGTH AT RIGHT ANGLES TO THE |
| GRAIN OF SMALL CLEAR PIECES OF 25 WOODS IN |
| GREEN CONDITION |
| (Forest Service Cir. 213) |
|--------------------------------------------|
| | When | When |
| COMMON NAME | surface of | surface of |
| OF SPECIES | failure is | failure is |
| | radial | tangential |
|------------------+------------+------------|
| | Lbs. per | Lbs. per |
| | sq. inch | sq. inch |
| | | |
| Hardwoods | | |
| | | |
| Ash, white | 645 | 671 |
| Basswood | 226 | 303 |
| Beech | 633 | 969 |
| Birch, yellow | 446 | 526 |
| Elm, slippery | 765 | 832 |
| Hackberry | 661 | 786 |
| Locust, honey | 1,133 | 1,445 |
| Maple, sugar | 610 | 864 |
| Oak, post | 714 | 924 |
| red | 639 | 874 |
| swamp white | 757 | 909 |
| white | 622 | 749 |
| yellow | 728 | 929 |
| Sycamore | 540 | 781 |
| Tupelo | 472 | 796 |
| | | |
| Conifers | | |
| | | |
| Arborvitæ | 241 | 235 |
| Cypress, bald | 242 | 251 |
| Fir, white | 213 | 304 |
| Hemlock | 271 | 323 |
| Pine, longleaf | 240 | 298 |
| red | 179 | 205 |
| sugar | 239 | 304 |
| western yellow | 230 | 252 |
| white | 225 | 285 |
| Tamarack | 236 | 274 |
|--------------------------------------------|
COMPRESSIVE OR CRUSHING STRENGTH
~Compression across the grain~ is very closely related to
hardness and transverse shear. There are two ways in which wood
is subjected to stress of this kind, namely, (1) with the load
acting over the entire area of the specimen, and (2) with a load
concentrated over a portion of the area. (See Fig. 2.) The
latter is the condition more commonly met with in practice, as,
for example, where a post rests on a horizontal sill, or a rail
rests on a cross-tie. The former condition, however, gives the
true resistance of the grain to simple crushing.
[Illustration: FIG. 2.--Compression across the grain.]
The first effect of compression across the grain is to compact
the fibres, the load gradually but irregularly increasing as the
density of the material is increased. If the specimen lies on a
flat surface and the load is applied to only a portion of the
upper area, the bearing plate indents the wood, crushing the
upper fibres without affecting the lower part. (See Fig. 3.) As
the load increases the projecting ends sometimes split
horizontally. (See Fig. 4.) The irregularities in the load are
due to the fact that the fibres collapse a few at a time,
beginning with those with the thinnest walls. The projection of
the ends increases the strength of the material directly beneath
the compressing weight by introducing a beam action which helps
support the load. This influence is exerted for a short distance
only.
[Illustration: FIG. 3.--Side view of failures in compression
across the grain, showing crushing of blocks under bearing
plate. Specimen at right shows splitting at ends.]
[Illustration: FIG. 4.--End view of failures in compression
across the grain, showing splitting of the ends of the test
specimens.]
When wood is used for columns, props, posts, and spokes, the
weight of the load tends to shorten the material endwise. This
is ~endwise compression~, or compression parallel to the grain.
In the case of long columns, that is, pieces in which the length
is very great compared with their diameter, the failure is by
sidewise bending or flexure, instead of by crushing or
splitting. (See Fig. 5.) A familiar instance of this action is
afforded by a flexible walking-stick. If downward pressure is
exerted with the hand on the upper end of the stick placed
vertically on the floor, it will be noted that a definite amount
of force must be applied in each instance before decided flexure
takes place. After this point is reached a very slight increase
of pressure very largely increases the deflection, thus
obtaining so great a leverage about the middle section as to
cause rupture.
[Illustration: FIG. 5.--Testing a buggy spoke in endwise
compression, illustrating the failure by sidewise bending of a
long column fixed only at the lower end. _Photo by U. S. Forest
Service_]
The lateral bending of a column produces a combination of
bending with compressive stress over the section, the
compressive stress being maximum at the section of greatest
deflection on the concave side. The convex surface is under
tension, as in an ordinary beam test. (See Fig. 6.) If the same
stick is braced in such a way that flexure is prevented, its
supporting strength is increased enormously, since the
compressive stress acts uniformly over the section, and failure
is by crushing or splitting, as in small blocks. In all columns
free to bend in any direction the deflection will be seen in the
direction in which the column is least stiff. This sidewise
bending can be overcome by making pillars and columns thicker in
the middle than at the ends, and by bracing studding, props, and
compression members of trusses. The strength of a column also
depends to a considerable extent upon whether the ends are free
to turn or are fixed.
[Illustration: FIG. 6.--Unequal distribution of stress in a long
column due to lateral bending.]
|-------------------------------------------------------|
| TABLE IV |
|-------------------------------------------------------|
| RESULTS OF COMPRESSION TESTS ACROSS THE GRAIN ON |
| 51 WOODS IN GREEN CONDITION, AND COMPARISON WITH |
| WHITE OAK |
| (U. S. Forest Service) |
|-------------------------------------------------------|
| | Fibre stress | Fiber stress |
| COMMON NAME | at elastic | in per cent |
| OF SPECIES | limit | of white oak, |
| | perpendicular | or 853 pounds |
| | to grain | per sq. in. |
|-----------------------+---------------+---------------|
| | Lbs. per | |
| | sq. inch | Per cent |
| | | |
| Osage orange | 2,260 | 265.0 |
| Honey locust | 1,684 | 197.5 |
| Black locust | 1,426 | 167.2 |
| Post oak | 1,148 | 134.6 |
| Pignut hickory | 1,142 | 133.9 |
| Water hickory | 1,088 | 127.5 |
| Shagbark hickory | 1,070 | 125.5 |
| Mockernut hickory | 1,012 | 118.6 |
| Big shellbark hickory | 997 | 116.9 |
| Bitternut hickory | 986 | 115.7 |
| Nutmeg hickory | 938 | 110.0 |
| Yellow oak | 857 | 100.5 |
| White oak | 853 | 100.0 |
| Bur oak | 836 | 98.0 |
| White ash | 828 | 97.1 |
| Red oak | 778 | 91.2 |
| Sugar maple | 742 | 87.0 |
| Rock elm | 696 | 81.6 |
| Beech | 607 | 71.2 |
| Slippery elm | 599 | 70.2 |
| Redwood | 578 | 67.8 |
| Bald cypress | 548 | 64.3 |
| Red maple | 531 | 62.3 |
| Hackberry | 525 | 61.6 |
| Incense cedar | 518 | 60.8 |
| Hemlock | 497 | 58.3 |
| Longleaf pine | 491 | 57.6 |
| Tamarack | 480 | 56.3 |
| Silver maple | 456 | 53.5 |
| Yellow birch | 454 | 53.2 |
| Tupelo | 451 | 52.9 |
| Black cherry | 444 | 52.1 |
| Sycamore | 433 | 50.8 |
| Douglas fir | 427 | 50.1 |
| Cucumber tree | 408 | 47.8 |
| Shortleaf pine | 400 | 46.9 |
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PUBLIC-DOMAIN BOOK
The Mechanical Properties of Wood Including a Discussion of the Factors Affecting the Mechanical Properties, and Methods of Timber Testing
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