17.1 Torsion of Closed Section Beams 505
Fig.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)
p
d^2 θ
dz^2
+
d^2 u
dz^2
cosψ+
d^2 v
dz^2
sinψ= 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