9.5 Instability of Stiffened Panels 301actingasacolumnisle,thentheEulercriticalstressis
σCR,E=
π^2 E
(le/r)^2asinEq.(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
twhere
t=Ast
bsk+tskandAstisthestiffenerarea.
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].