Glass, Volume 22 |
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Page 189
Right at the tip ( x = 0 ) the stress is 0 / S = 1 + 2c / a ( 10 ) In terms of the radius of
curvature p = a ? / c of the crack tip o / S = 1 + 2Vc / p = 2Vc / ( 11 ) If the crack is
not elliptical in shape , it can be shown that Eq . ( 11 ) is still the proper form .
Right at the tip ( x = 0 ) the stress is 0 / S = 1 + 2c / a ( 10 ) In terms of the radius of
curvature p = a ? / c of the crack tip o / S = 1 + 2Vc / p = 2Vc / ( 11 ) If the crack is
not elliptical in shape , it can be shown that Eq . ( 11 ) is still the proper form .
Page 190
TABLE VI COMPARISON BETWEEN THE EXACT SOLUTION AND THE
WESTERGAARD APPROXIMATION FOR THE STRESS NEAR A CRACK TIP (
distance from origin ) / ( crack length ) ( y / c ) ( stress ) / ( applied stress ) ( o / s )
Exact ...
TABLE VI COMPARISON BETWEEN THE EXACT SOLUTION AND THE
WESTERGAARD APPROXIMATION FOR THE STRESS NEAR A CRACK TIP (
distance from origin ) / ( crack length ) ( y / c ) ( stress ) / ( applied stress ) ( o / s )
Exact ...
Page 197
direct experimental test of these relations ; in some limited tests there is evidence
for the dependence of failure stress on ... These criteria are based on Griffith ' s
calculation of the strain energy change in a stressed material caused by a crack .
direct experimental test of these relations ; in some limited tests there is evidence
for the dependence of failure stress on ... These criteria are based on Griffith ' s
calculation of the strain energy change in a stressed material caused by a crack .
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Contents
Water in Glass | 75 |
Applications | 121 |
Gel Method for Making Glass | 129 |
Copyright | |
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