Calculate the position of the shear center of the thin-walled section shown in Fig. 16.12; the thickness of the section is 2mm and is constant throughout.
Calculate the position of the shear center of the thin-walled section shown in Fig. 16.12; the thickness of the section is 2mm and is constant throughout.
Since we are only asked to find the position of the shear center of the section and not a complete shear flow distribution the argument of Ex. 16.3 applies in that if we refer the position of the shear center to the web/flange junction 2 (or 3) it is only necessary to obtain the shear flow distribution in the flange 34 (or 12). First, we must calculate the section’s properties. Taking moments of area about the top flange
2(50+50+25) \bar{y}=2 \times 50 \times 25+2 \times 25 \times 50
which gives
\bar{y}=20 mm
Now taking moments of area about the vertical web
2(50+50+25) \bar{x}=2 \times 50 \times 25+2 \times 25 \times 12.5
from which
\bar{x}=12.5 mm
The second moments of area are then calculated using the methods of Section 15.4.5.
I_{x x}=2 \times 50 \times 20^{2}+\left(2 \times 50^{3} / 12\right)+2 \times 50 \times 5^{2}+2 \times 25 \times 30^{2}
i.e.,
I_{x x}=108,333 mm ^{4}
I_{y y}=\left(2 \times 50^{3} / 12\right)+2 \times 50 \times 12.5^{2}+2 \times 50 \times 12.5^{2}+\left(2 \times 25^{3} / 12\right)
i.e.,
I_{y y}=54,689 mm ^{4}
I_{x y}=2 \times 50(+12.5)(+20)+2 \times 50(-12.5)(-5)
i.e.,
I_{x y}=31,250 mm ^{4}
Note that the flange 34 makes no contribution to I_{x y} since its centroid coincides with the y axis of the section. Considering the horizontal position of the shear center we apply a vertical shear load, S_{y}, through the shear center and determine the shear flow distribution in the flange 34. Since S_{x}=0, Eq. (16.14) reduces to
q_{s}=-\left(\frac{S_{x} I_{x x}-S_{y} I_{x y}}{I_{x x} I_{y y}-I_{x y}^{2}}\right) \int_{0}^{s} t x d s-\left(\frac{S_{y} I_{y y}-S_{x} I_{x y}}{I_{x x} I_{y y}-I_{x y}^{2}}\right) \int_{0}^{s} t y ds (16.14)
q_{s}=\left[\left(S_{y} I_{x y}\right) /\left(I_{x x} I_{y y}-I_{x y}^{2}\right)\right] \int_{0}^{s} t x d s-\left[\left(S_{y} I_{y y}\right) /\left(I_{x x} I_{y y}-I_{x y}^{2}\right)\right] \int_{0}^{s} t y d s (i)
Substituting the values of I_{x x} etc. gives
q_{s}=1.26 \times 10^{-5} S_{y} \int_{0}^{s} x d s-2.21 \times 10^{-5} S_{y} \int_{0}^{s} y d s (ii)
On the flange 34, x=12.5-s and y=-30 mm \text {. } Eq. (ii) then becomes
q_{43}=S_{y} \times 10^{-5} \int_{0}^{s}(82.05-1.26 s) d s
Integrating gives
q_{43}=S_{y} \times 10^{-5}\left(82.05 s-0.63 s^{2}\right) (iii)
Now taking moments about the flange/web junction 2
S_{y} \xi_{S}=\int_{0}^{25} q_{43} \times 50 d s
Substituting for q_{43} from Eq. (iii) and integrating gives
\xi_{ S }=11.2 mm
We now apply S_{x} only through the shear center and carry out the same procedure as above. Then
q_{43}=S_{x} \times 10^{-5}\left(2.19 s^{2}-92.55 s\right) (iv)
Taking moments about the web/flange junction 2
S_{x} \eta_{ S }=-\int_{0}^{25} q_{43} \times 50 d s
Note that in this case the moment of the resultant of the internal shear flows is in the opposite sense to that of the applied force. Substituting for q_{43} from Eq. (iv) and carrying out the integration gives
\eta_{ S }=7.2 mm