29.01.2013 Views

The Gougeon Brothers on Boat Construction - WEST SYSTEM Epoxy

The Gougeon Brothers on Boat Construction - WEST SYSTEM Epoxy

The Gougeon Brothers on Boat Construction - WEST SYSTEM Epoxy

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

16 Fundamentals of Wood/<strong>Epoxy</strong> Composite <strong>Boat</strong>building<br />

Figure 3-5 Tensi<strong>on</strong> fatigue. Maximum stress vs. total cycles<br />

for Douglas fir/epoxy laminate with 12:1 slope scarf and butt<br />

joints with 3" stagger, 31.8 in 3 test volume, parallel to grain<br />

directi<strong>on</strong>, room temperature and 12% wood moisture c<strong>on</strong>tent.<br />

Figure 3-6 Tangential fatigue, wood/epoxy laminate.<br />

Size effect in laminated veneer<br />

During the sec<strong>on</strong>d half of the 1980s, <str<strong>on</strong>g>The</str<strong>on</strong>g> U.S. Department<br />

of Energy funded an extensive GBI test program<br />

to investigate various properties of epoxy/Douglas fir<br />

veneer laminate. <str<strong>on</strong>g>The</str<strong>on</strong>g> research included static and fatigue<br />

measurements of two sec<strong>on</strong>dary properties: (1) radial<br />

cross-grain tensile strength and (2) rolling shear strength.<br />

Radial refers to the through-the-thickness dimensi<strong>on</strong>,<br />

perpendicular to the plane of laminati<strong>on</strong>. Radial tensile<br />

stress tends to pull the veneer layers apart. Rolling<br />

shear refers to the applicati<strong>on</strong> of opposing forces,<br />

parallel to the plane of laminati<strong>on</strong> but perpendicular<br />

to the wood fibers. <str<strong>on</strong>g>The</str<strong>on</strong>g> opposing forces are slightly<br />

offset to generate shear, such that wood fibers in<br />

adjacent slip planes have a tendency to twist and roll<br />

over each other.<br />

Both sec<strong>on</strong>dary property studies featured two populati<strong>on</strong>s<br />

of test specimens made from the same parent<br />

laminate, <strong>on</strong>e with small-volume specimens and <strong>on</strong>e<br />

with large-volume specimens, in order to gauge size<br />

effect. Size effect refers to the often-overlooked phenomen<strong>on</strong><br />

that causes physically small test specimens to<br />

dem<strong>on</strong>strate unrealistically high strength with respect<br />

to that of actual, real world structures made from the<br />

same material.<br />

<str<strong>on</strong>g>The</str<strong>on</strong>g> test secti<strong>on</strong>s of the 28 small radial cross-grain tensi<strong>on</strong><br />

specimens were 1.5" in the grain directi<strong>on</strong>, 0.5"<br />

wide and 2.0" (20 veneer layers) thick. <str<strong>on</strong>g>The</str<strong>on</strong>g> test secti<strong>on</strong>s<br />

of the 35 large radial cross-grain tensi<strong>on</strong> specimens<br />

were 6.0" in the grain directi<strong>on</strong>, 4.0" wide, and 12.0"<br />

(120 veneer layers) thick. <str<strong>on</strong>g>The</str<strong>on</strong>g> large/small specimen<br />

volume ratio was therefore 192:1. <str<strong>on</strong>g>The</str<strong>on</strong>g> average crossgrain<br />

tensile strength of the small-volume specimens<br />

was 393 psi. <str<strong>on</strong>g>The</str<strong>on</strong>g> average static strength of the largevolume<br />

specimens was <strong>on</strong>ly 280 psi, a knockdown of<br />

about 29%. <str<strong>on</strong>g>The</str<strong>on</strong>g> laminate moisture c<strong>on</strong>tent of both<br />

specimen populati<strong>on</strong>s was the same, ranging from 5 to<br />

6%. In fatigue, the size effect turned out to be much<br />

more pr<strong>on</strong>ounced. <str<strong>on</strong>g>The</str<strong>on</strong>g> S-N (Stress-Number of cycles to<br />

failure) curves showed that for R = 0.1, the small specimens<br />

could reach 10 milli<strong>on</strong> cycles with a peak stress<br />

of 275 psi. (R is the ratio of the minimum stress<br />

divided by the maximum stress. A ratio of 0.1 means<br />

the maximum stress is 10 times the minimum.) For<br />

the large-volume specimens, the S-N slope was much<br />

steeper. A typical large-volume specimen could reach 10<br />

milli<strong>on</strong> cycles <strong>on</strong>ly if the peak stress was 134 psi or less.<br />

This was c<strong>on</strong>vincing evidence that size effect should<br />

determine the design allowables for large, fatigue-driven<br />

wood structures.<br />

As for rolling shear, the specimen stressed volume ratio<br />

was 160 in3 vs. 2.5 in3 , or 64:1. <str<strong>on</strong>g>The</str<strong>on</strong>g>re were 29 smallvolume<br />

specimens and 14 large-volume specimens,<br />

all made from the same parent material. <str<strong>on</strong>g>The</str<strong>on</strong>g> laminate<br />

moisture c<strong>on</strong>tent was just over 6%. <str<strong>on</strong>g>The</str<strong>on</strong>g> rolling shear

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!