9.7Tension Field Beams 311
InEqs.(9.28)and(9.29),itisimplicitlyassumedthatastiffenerisfullyeffectiveinresistingaxial
load. This will be the case if the centroid of area of the stiffener lies in the plane of the beam web.
Suchasituationariseswhenthestiffenerconsistsoftwomemberssymmetricallyarrangedonopposite
sidesoftheweb.Inthecasewherethewebisstiffenedbyasinglememberattachedtooneside,the
compressiveloadPisoffsetfromthestiffeneraxis,therebyproducingbendinginadditiontoaxialload.
Forastiffenerhavingitscentroidadistanceefromthecenteroftheweb,thecombinedbendingand
axialcompressivestress,σc,atadistanceefromthestiffenercentroidis
σc=
P
AS
+
Pe^2
ASr^2
inwhichristheradiusofgyrationofthestiffenercrosssectionaboutitsneutralaxis.(Note:second
momentofareaI=Ar^2 .)Then,
σc=
P
AS
[
1 +
(e
r
) 2 ]
or
σc=
P
ASe
where
ASe=
AS
1 +(e/r)^2
(9.30)
andistermedtheeffectivestiffenerarea[Ref.1].
9.7.2 Incomplete Diagonal Tension
Inmodernaircraftstructures,beamshavingextremelythinwebsarerare.Theyretain,afterbuckling,
someoftheirabilitytosupportloadssothatevennearfailuretheyareinastateofstresssomewhere
between that of pure diagonal tension and the prebuckling stress. Such a beam is described as an
incompletediagonaltensionfieldbeamandmaybeanalyzedbysemiempiricaltheoryasfollows.
Itisassumedthatthenominalwebshearτ(=S/td)maybedividedintoa“trueshear”component
τSandadiagonaltensioncomponentτDTbywriting
τDT=kτ, τS=( 1 −k)τ (9.31)
wherek,thediagonal tension factor, is a measure of the degree to which the diagonal tension is
developed. A completely unbuckled web hask=0, whereask=1 for a web in complete diagonal
tension. The value ofkcorresponding to a web having a critical shear stressτCRisgivenbythe
empiricalexpression
k=tanh
(
0.5log
τ
τCR