Introduction to Aircraft Structural Analysis (Elsevier Aerospace Engineering)

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20.1 Tapered Wing Spar 563

or


Sy=Sy,w+Pz,1

δy 1
δz

+Pz,2

δy 2
δz

(20.4)

sothat


Sy,w=Sy−Pz,1

δy 1
δz

−Pz,2

δy 2
δz

(20.5)

Againwenotethatδy 2 inEqs.(20.4)and(20.5)isnegative.Equation(20.5)maybeusedtodetermine
theshearflowdistributionintheweb.Foracompletelyidealizedbeam,thewebshearflowisconstant
through the depth and is given bySy,w/h. For a beam in which the web is fully effective in resisting
directstresses,thewebshearflowdistributionisfoundusingEq.(19.6),inwhichSyisreplacedbySy,w
andwhich,forthebeamofFig.20.1,wouldsimplifyto


qs=−

Sy,w
Ixx



∫s

0

tDyds+B 1 y 1


⎠ (20.6)

or


qs=−

Sy,w
Ixx



∫s

0

tDyds+B 2 y 2


⎠ (20.7)

Example 20.1
DeterminetheshearflowdistributioninthewebofthetaperedbeamshowninFig.20.2,atasection
midwayalongitslength.Thewebofthebeamhasathicknessof2mmandisfullyeffectiveinresisting


Fig.20.2


Tapered beam of this example.

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