4. Load acting parallel to the member axis
Load acting perpendicular to the member axis
Load acting in-plane of the member
Shift the load to the CG
of member geometry
Find the effect of the
load on the member
Show the state of the
stress at critical point
Develop the design equation
Analysis of Eccentrically Loaded Member
5. ๐น๐
๐ถ๐ต
๐น
๐ = ๐น๐ ๐ถ๐ต
๐น
๐น
๐ต
๐น๐
๐ถ
What would be the effect of load at
a point along the axis of the load?
What would be the effect of load at a
point away from the axis of the load?
๐น and ๐
๐ in the plane of cross section
๐ in a plane perpendicular to
the plane of cross section
Twisting
Bending
Axial deformation
Load Transfer and Effect of Load
6. Effect of forces and moments at point A
๏ง Force along x-axis is transverse load and cause in-plane/transverse
shear.
๏ง Force along y-axis is also transverse load and cause in-
plane/transverse shear.
๏ง Force along z-axis is axial load and causes elongation.
๏ง Couple ( ๐ ๐ฅโ๐ฆ ) in the plane of cross-section and hence induces
twisting.
๏ง Couple (๐ ๐ฆโ๐ง) in the plane perpendicular to cross-section and hence
causes bending in y-z plane.
๏ง Couple (๐๐งโ๐ฅ) in the plane perpendicular to cross-section and hence
causes bending in z-x plane.
Member under General Loading
7. Net effect of all forces at point A
๐ญ ๐ = ๐๐๐ N (+x)
๐ญ ๐ = ๐๐๐ + ๐๐๐ + ๐๐๐ + ๐๐๐ = ๐๐๐๐ N (-y)
๐ญ ๐ = ๐๐๐ N (+z)
๐ด ๐โ๐ = โ๐๐๐๐ + ๐๐๐๐ + ๐๐๐๐ = ๐๐๐๐ N-m, (cw)
๐ด ๐โ๐ = โ๐๐๐๐๐ + ๐๐๐๐ โ ๐๐๐๐ โ ๐๐๐๐ โ ๐๐๐๐ = ๐๐๐๐๐ N-m (acw)
๐ด ๐โ๐ = ๐๐๐๐ โ ๐๐๐๐ = ๐๐๐๐ N-m (acw)
Solution
8. Effect of Load and Corresponding Induced Stresses
Elongation Tensile stressAxial tensile Load
Compression Axial compressive Load Compressive/bearing stress
Bending Moment acting in transverse plane Compressive and tensile stress
Twisting Moment acting in plane of cross-section Torsional shear stress
Sliding In-plane load In-plane shear stress
๐ =
๐น
๐ด
๐ =
๐น
๐ด
๐ =
๐น๐
๐ผ
๐ฆ
๐ =
๐น
๐ด
๐ =
๐น๐
๐ฝ
๐