254 CHAPTER 8 Columns
IftheperfectcolumnofFig.8.1issubjectedtoacompressiveloadP,onlyshorteningofthecolumn
occursnomatterwhatthevalueofP.However,ifthecolumnisdisplacedasmallamountbyalateral
loadF,then,atvaluesofPbelowthecriticalorbucklingload,PCR,removalofFresultsinareturn
ofthecolumntoitsundisturbedposition,indicatingastateofstableequilibrium.Atthecriticalload,
thedisplacementdoesnotdisappear,and,infact,thecolumnwillremaininanydisplacedpositionas
long as the displacement is small. Thus, the buckling loadPCRis associated with a state ofneutral
equilibrium.ForP>PCR,enforcedlateraldisplacementsincreaseandthecolumnisunstable.
Considerthepin-endedcolumnABofFig.8.2.Weassumethatitisinthedisplacedstateofneutral
equilibriumassociatedwithbucklingsothatthecompressiveloadPhasattainedthecriticalvaluePCR.
Simplebendingtheory(seeChapter15)gives
EI
d^2 v
dz^2
=−M
or
EI
d^2 v
dz^2
=−PCRv (8.1)
Fig.8.1
Definition of buckling load for a perfect column.
Fig.8.2
Determination of buckling load for a pin-ended column.