Strength of materials - Chapter 10: Combined loadings - Nguyễn Sỹ Lâm
10.1 UNSYMMETRIC BENDING
Analysis of pure bending has been limited
to members subjected to bending couples
acting in a plane of symmetry.
• Will now consider situations in which the
bending couples do not act in a plane of
symmetry.
• In general, the neutral axis of the section will
not coincide with the axis of the couple.
• Cannot assume that the member will bend
in the plane of the couples.
• The neutral axis of the cross section
coincides with the axis of the couple
• Members remain symmetric and bend in
the plane of symmetry
Analysis of pure bending has been limited
to members subjected to bending couples
acting in a plane of symmetry.
• Will now consider situations in which the
bending couples do not act in a plane of
symmetry.
• In general, the neutral axis of the section will
not coincide with the axis of the couple.
• Cannot assume that the member will bend
in the plane of the couples.
• The neutral axis of the cross section
coincides with the axis of the couple
• Members remain symmetric and bend in
the plane of symmetry
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- CHAPTER 10: COMBINED LOADINGS 10.1 Unsymmetric Bending 10.2 Eccentric Axial Loadings 10.3 Torsion and Bending 10.4 General Combined Loadings
- 10.1 UNSYMMETRIC BENDING UNSYMMETRIC BENDING y • 0 Fx xdA m dA c or 0 y dA neutral axis passes through centroid y • M M z y m dA Wish to determine the conditions under c which the neutral axis of a cross section σ I or M m I I moment of inertia of arbitrary shape coincides with the c z axis of the couple as shown. defines stress distribution • The resultant force and moment from the distribution of y • 0 M y z xdA z m dA elementary forces in the section c must satisfy or 0 yzdA I yz product of inertia Fx 0 M y M z M applied couple couple vector must be directed along a principal centroidal axis
- 10.1 UNSYMMETRIC BENDING UNSYMMETRIC BENDING M z y M y z x I z I y • Along the neutral axis, M z y M y z M cos y M sin z x 0 I z I y I z I y y I tan z tan z I y • Equation of Neutral Axis M y I M y I y z z y z z M z I y M z I y
- 10.1 UNSYMMETRIC BENDING UNSYMMETRIC BENDING – SUMMARY - - min h x Compression + + stress y max b Mx x - + z h x M M y y - + u Tension stress M y I x y • Equation of Neutral Axis y x M I b (N.A.) x y M M x y (Diagram of Equation : y = ax) z y x I x I y
- 10.1 UNSYMMETRIC BENDING EXAMPLE 10.01 • Resolve the couple vector into components and calculate the corresponding maximum stresses. M z 1600lb in cos30 1386lb in M y 1600lb in sin 30 800lb in I 1 1.5in 3.5in 3 5.359in 4 z 12 I 1 3.5in 1.5in 3 0.9844in 4 y 12 The largest tensile stress due to M z occurs along AB M y 1386lb in 1.75in z 452.6psi 1 4 Iz 5.359in The largest tensile stress due to M z occurs along AD M y z 800lb in 0.75in 609.5psi 2 4 I y 0.9844in • The largest tensile stress due to the combined loading occurs at A. max 1 2 452.6 609.5 max 1062psi
- 10.2 ECCENTRIC AXIAL LOADINGS ECCENTRIC AXIAL LOADING IN A PLANE OF SYMMETRY • Stress due to eccentric loading found by superposing the uniform stress due to a centric load and linear stress distribution due a pure bending moment x x centric x bending P M y A I • Eccentric loading • Validity requires stresses below proportional F P limit, deformations have negligible effect on geometry, and stresses not evaluated near points M Pd of load application.
- 10.2 ECCENTRIC AXIAL LOADINGS EXAMPLE 10.02 • Normal stress due to a centric load A c2 0.25in 2 0.1963in 2 P 160lb 0 A 0.1963in 2 815psi • Equivalent centric load • Normal stress due to and bending moment bending moment P 160lb I 1 c4 1 0.25 4 4 4 M Pd 160lb 0.6in 3.068 10 3 in 4 104lb in Mc 104lb in 0.25in m I .068 10 3 in 4 8475psi
- 10.2 ECCENTRIC AXIAL LOADINGS EXAMPLE 10.03 The largest allowable stresses for the cast iron link are 30 MPa in tension and 120 MPa in compression. Determine the largest force P which can be applied to the link. SOLUTION: • Determine an equivalent centric load and bending moment. • Superpose the stress due to a centric load and the stress due to bending. • Evaluate the critical loads for the allowable Given: tensile and compressive stresses. 3 2 A 3 10 m • The largest allowable load is the smallest Y 0.038m of the two critical loads. I 868 10 9 m4
- 10.2 ECCENTRIC AXIAL LOADINGS GENERAL CASE OF ECCENTRIC AXIAL LOADING • Consider a straight member subject to equal and opposite eccentric forces. • The eccentric force is equivalent to the system of a centric force and two couples. P centric force M y Pa M z Pb • By the principle of superposition, the combined stress distribution is P M z y M y z x A Iz I y • If the neutral axis lies on the section, it may be found from M M P z y y z Iz I y A
- 10.2 ECCENTRIC AXIAL LOADINGS 2 2 SUMMARY M u M x M y M x M y N z z y x M M y - - x y x I x I y A z I I h x x y Mx + + y min b x Compression stress - + h x Mu y - + max x y My b z N z M N + + u y Tension stress z z A h x M y I N I + + Equation of Neutral Axis (N.A.): y x x z x M x I y A M x y (Diagram of Equation : y = ax +b)
- 10.3 TORSION AND BENDING CIRCULAR SHAFTS Mz = M0 max max 2 2 max 4 max Mu z or 2 2 max 3 max u min v 2 2 min 4 max or 2 2 min 3 max
- 10.3 TORSION AND BENDING RECTANGULAR SECTIONS 2 2 S y 4 TB3 1 1 2 2n OR 2 2 S y TB4 1 3 1 3 3n
- 10.4 GENERAL COMBINED LOADINGS RECTANGULAR SECTIONS 2 2 S y 4 TB3 1 1 2 2n OR 2 2 S y TB4 1 3 1 3 3n