17.1 Torsion of Closed Section Beams 505Fig.17.3
Sign convention for swept areas.
isvalidforthepuretorsioncase,whereqisconstant.Differentiatingthisexpressionwithrespecttoz,
wehave
∂q
∂z=Gt(
∂^2 w
∂z∂s+
∂^2 vt
∂z^2)
= 0
or
∂
∂s(
∂w
∂z)
+
∂^2 vt
∂z^2= 0 (17.2)
Intheabsenceofdirectstresses,thelongitudinalstrain∂w/∂z(=εz)iszerosothat
∂^2 vt
∂z^2= 0
Hence,fromEq.(16.7)
pd^2 θ
dz^2+
d^2 u
dz^2cosψ+d^2 v
dz^2sinψ= 0 (17.3)ForEq.(17.3)toholdforallpointsaroundthesectionwall,inotherwordsforallvaluesofψ
d^2 θ
dz^2=0,
d^2 u
dz^2=0,
d^2 v
dz^2