22.3 Torsion 593
Fig.22.6
Wing section of Example 22.2.
Hence,
δ 12 ◦=
∫
12 ◦
ds
t∗
=
1650
1.07
= 1542
Similarly,
δ 12 i= 250 δ 13 =δ 24 = 725 δ 34 = 233 δ 35 =δ 46 = 736 δ 56 = 368
SubstitutingtheappropriatevaluesofδinEq.(22.6)foreachcellinturngivesthefollowing:
- ForcellI,
dθ
dz
=
1
2 × 258000 GREF
[qI( 1542 + 250 )− 250 qII](i)
- ForcellII,
dθ
dz
=
1
2 × 355000 GREF
[− 250 qI+qII( 250 + 725 + 233 + 725 )− 233 qIII](ii)
- ForcellIII,
dθ
dz
=
1
2 × 161000 GREF
[− 233 qII+qIII( 736 + 233 + 736 + 368 )] (iii)
Inaddition,fromEq.(22.4),
11.3× 106 = 2 ( 258000 qI+ 355000 qII+ 161000 qIII) (iv)
SolvingEqs.(i)through(iv)simultaneouslygives
qI=7.1N/mm qII=8.9N/mm qIII=4.2N/mm
Theshearstressinanywallisobtainedbydividingtheshearflowbytheactualwallthickness.Hence,
theshearstressdistributionisasshowninFig.22.7.