9.5 Instability of Stiffened Panels 301
actingasacolumnisle,thentheEulercriticalstressis
σCR,E=
π^2 E
(le/r)^2
asinEq.(8.8).Inadditiontothecolumnbucklingmode,individualplateelementscomprisingthepanel
crosssectionmaybuckleaslongplates.ThebucklingstressisthengivenbyEq.(9.7),thatis,
σCR=
ηkπ^2 E
12 ( 1 −ν^2 )
(
t
b
) 2
where the values ofk,t,andbdepend on the particular portion of the panel being investigated. For
example,theportionofskinbetweenstiffenersmaybuckleasaplatesimplysupportedonallfoursides.
Thus,fora/b>3,k=4fromFig.9.3(a),and,assumingthatbucklingtakesplaceintheelasticrange,
σCR=
4 π^2 E
12 ( 1 −ν^2 )
(
tsk
bsk
) 2
A further possibility is that the stiffeners may buckle as long plates simply supported on three sides
withoneedgefree.Thus,
σCR=
0.43π^2 E
12 ( 1 −ν^2 )
(
tst
bst
) 2
Clearly,theminimumvalueoftheprecedingcriticalstressesisthecriticalstressforthepaneltakenas
awhole.
Thecompressiveloadisappliedtothepaneloveritscompletecrosssection.Torelatethisloadto
anappliedcompressivestressσAactingoneachelementofthecrosssection,wedividetheloadper
unitwidth,sayNx,byanequivalentskinthickness ̄t,hence
σA=
Nx
t
where
t=
Ast
bsk
+tsk
andAstisthestiffenerarea.
The preceding remarks are concerned with the primary instability of stiffened panels. Values of
localbucklingstresshavebeendeterminedbyBoughan,Baab,andGallaherforidealizedweb,Z-,and
T-stiffenedpanels.TheresultsarereproducedbyRivello[Ref.6]togetherwiththeassumedgeometries.
Furthertypesofinstabilityfoundinstiffenedpanelsoccurwherethestiffenersarerivetedorspot
weldedtotheskin.Suchstructuresmaybesusceptibletointerrivetbuckling,inwhichtheskinbuckles
between rivets with a wavelength equal to the rivet pitch, orwrinkling, where the stiffener forms an
elasticlinesupportfortheskin.Inthelattermode,thewavelengthofthebuckleisgreaterthantherivet
pitch,andseparationofskinandstiffenerdoesnotoccur.Methodsofestimatingtheappropriatecritical
stressesaregiveninthestudyofRivelloandtheHandbookofAeronautics[Ref.3].