9.6 Failure Stress in Plates and Stiffened Panels 303
Gerard[Refs.9–12]extendedtheprecedingmethodtothepredictionoflocalfailurestressesforthe
plateelementsofthin-walledcolumns.Equation(9.11)becomes
σ ̄f
σcy
=βg
[(
gt^2
A
)(
E
σcy
) 1
2
]m
(9.12)
whereAisthecross-sectionalareaofthecolumn,βgandmareempiricalconstants,andgisthenumber
ofcutsrequiredtoreducethecrosssectiontoaseriesofflangedsectionsplusthenumberofflanges
thatwouldexistafterthecutsaremade.ExamplesofthedeterminationofgareshowninFig.9.6.
ThelocalfailurestressinlongitudinallystiffenedpanelswasdeterminedbyGerard[Refs.10,12]
usingaslightlymodifiedformofEqs.(9.11)and(9.12).Thus,forasectionofthepanelconsistingof
astiffenerandawidthofskinequaltothestiffenerspacing
σ ̄f
σcy
=βg
[
gtsktst
A
(
E
σ ̄cy
)^12 ]m
(9.13)
wheretskandtstaretheskinandstiffenerthicknesses,respectively.Aweightedyieldstressσ ̄cyisused
forapanelinwhichthematerialoftheskinandstiffenerhavedifferentyieldstresses;thus,
σ ̄cy=
σcy+σcy,sk[(t/tst)−1]
t/tst
where ̄tistheaverageorequivalentskinthicknesspreviouslydefined.Theparametergisobtainedin
asimilarmannertothatforathin-walledcolumn,exceptthatthenumberofcutsintheskinandthe
Fig.9.6
Determination of empirical constantg.