544 CHAPTER 19 Structural Idealization
Theseshearloadsproducedirectstressesduetobendingintheboomsandskinandshearstressesin
theskin.Supposethattheshearflowsintheskinadjacenttotherthboomofcross-sectionalareaBrare
q 1 andq 2 .Then,fromFig.19.6(b),
(
σz+∂σz
∂zδz)
Br−σzBr+q 2 δz−q 1 δz= 0whichsimplifiesto
q 2 −q 1 =−∂σz
∂zBr (19.4)SubstitutingforσzinEq.(19.4)from(15.18),wehave
q 2 −q 1 =−[
(∂My/∂z)Ixx−(∂Mx/∂z)Ixy
IxxIyy−I^2 xy]
Brxr−
[
(∂Mx/∂z)Iyy−(∂My/∂z)Ixy
IxxIyy−I^2 xy]
Bryror,usingtherelationshipsofEqs.(15.23)and(15.24),
q 2 −q 1 =−(
SxIxx−SyIxy
IxxIyy−Ixy^2)
Brxr−(
SyIyy−SxIxy
IxxIyy−Ixy^2)
Bryr (19.5)Equation(19.5)givesthechangeinshearflowinducedbyaboomwhichitselfissubjectedtoadirect
load(σzBr).Eachtimeaboomisencountered,theshearflowisincrementedbythisamountsothatif,
atanydistancesaroundtheprofileofthesection,nboomshavebeenpassed,theshearflowatthepoint
isgivenby
qs=−(
SxIxx−SyIxy
IxxIyy−Ixy^2)⎛
⎝
∫s0tDxds+∑nr= 1Brxr⎞
⎠
−
(
SyIyy−SxIxy
IxxIyy−Ixy^2)⎛
⎝
∫s0tDyds+∑nr= 1Bryr⎞
⎠
(19.6)
Example 19.3
Calculate the shear flow distribution in the channel section shown in Fig. 19.7 produced by a ver-
tical shear load of 4.8kN acting through its shear center. Assume that the walls of the section are
onlyeffectiveinresistingshearstresses,whilethebooms,eachofarea300mm^2 ,carryallthedirect
stresses.