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L02 - Load and stress analysis
302315 L02 - Load and stress analysis
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Identify critical cross sections Principle stress determination
Load analysis Assume materials to be homogeneous and isotropic Determine all applied loads (forces, moments, torques) and present where those appear on the part’s geometry using FBD Load termination Based on the load distribution, determine what cross sections of the part are most heavily loaded. Identify critical cross sections (SFD, BMD) Determine the stress distribution over the cross section of interest. Locate the highest of applied and combine stresses Stress determination identify state of stress at a points of interest Stress element Calculate the principal stresses and maximum shear stress Principle stress determination Calculate the critical deflection of the part Critical Deflection Failure criteria
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Crimping tool-static loading
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FBD Link3 Link4 Link2
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15 varibles; 13 equations 1) F12x + F32x = 0 2) Fh + F12y + F32y = 0 3) RhFh + (R12xF12y - R12yF12x) + (R32xF32y – R32yF32x) = 0 4) F23x + F43x = 0 5) F23y + F43y = 0 6) (R23xF23y – R23yF23x) + (R43xF43y – R43yF43x) = 0 7) Fc4x + F34x + F14x = 0 8) Fc4y + F34y + F14y = 0 9) (Rc4xFc4y – Rc4yFc4x) + (R34xF34y – R34yF34x) + (R14xF14y – R14yF14x) = 0 Link2 Link3 Link4 10) F32x - F23x = 0 Given 11) F32y - F23y = 0 12) F43x - F34x = 0 13 varibles; 13 equations 13) F43y - F34y = 0
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Cross product Mz= (RxFy-RyFx) Moment = R x F (+) i (-) j (+) k Rx Ry
Rz Fx Fy Fz M = Mxi + Myj + Mzk i j k Rx Ry Rz Fx Fy Fz i j k Rx Ry Rz Fx Fy Fz i j k Rx Ry Rz Fx Fy Fz Mxi = (RyFz-RzFy)i Myj = - (RxFz-RzFx)j Mzk = (RxFy-RyFx) k In 2 - D (+) i (-) j (+) k Rx Ry Fx Fy Mx= 0 Mz= (RxFy-RyFx) My = 0
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Assignment AS01
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Solving system of linear equations
Inverse matrix Cramer’s rule Gaussian elimination
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solution Force geometric data 1 Fh 0.236 kN Rh -111.76 mm 2 F12x 6.732
R12x 35.56 3 F12y -1.695 R12y 1.27 4 F32x -6.732 R32x 55.88 5 F32y 1.459 R32y 2.032 6 F23x R23x -15.24 7 F23y -1.459 R23y 3.302 8 F43x R43x 15.24 9 F43y R43y -3.302 10 F34x R34x 4.064 11 F34y R34y 19.304 12 F14x 1.969 R14x -4.064 13 F14y -0.390 R14y 14 Fc4x -8.701 Rc4x 11.43 15 Fc4y 1.849 Rc4y 8.636 16 Fc1x 8.701 Rc1x 17 Fc1y -1.849 Rc1y 18 F21x R21x 19 F21y 1.695 R21y 20 F41x -1.969 R41x 21 F41y 0.390 R41y solution
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matrix
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Link 3 – compression load
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Link 4 – bending load
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Combine load
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Load Static load dynamic load Impact load Vibration Beam load Type
Load termination Determine all applied loads (forces, moments, torques) and present where those appear on the part’s geometry using FBD dynamic load Impact load Vibration Beam load Type location direction Time-variation Magnitude concentrate force duration distribute continuation torque uniform moment non-uniform
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Stress analysis Column and Beam
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Identify critical cross sections Principle stress determination
Stress analysis Assume materials to be homogeneous and isotropic Determine all applied loads (forces, moments, torques) and present where those appear on the part’s geometry using FBD Load termination Based on the load distribution, determine what cross sections of the part are most heavily loaded. Identify critical cross sections (SFD, BMD) Determine the stress distribution over the cross section of interest. Locate the highest of applied and combine stresses Stress determination identify state of stress at a points of interest Stress element Calculate the principal stresses and maximum shear stress Principle stress determination Calculate the critical deflection of the part Critical Deflection Failure criteria Calculate Von Mises effective stress at each selected point based on the principal stresses Trial on a material Compute safety factor based on tensile yield strength of that material DUCTILE MATERIALS Calculate Coulomb-Mohr effective stress at each selected stress element based on its principal stresses Compute safety factor based on ultimate tensile strength of that material BRITTLE MATERIALS
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Stress component sxx txy txz tyx syy tyz tzx tzy szz sxx txy tyx syy
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transformation stress
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Normal stress The plane at which zigma is max, shear stress is zero
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SHEER STRESS The plane at which shear stress is max,
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Principal stress
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Mohr’s circle 2-D https://youtu.be/WOCFY4gnTyk
3-D
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Assignment Dynamic load Stress in Beam
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Dynamic loading Fx = max Fy = may Mz = Izz dynamic analysis
Fz = maz Mx = Ixx – (Iy-Iz)yz My = Iyy – (Iz-Ix)zx Mz = Izz – (Ix-Iy)xy 2-D in x-y plane Fx = max Fy = may Mz = Izz
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caSE : Link 4 STRESS IN BEAM
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Shear stress SFD – Sheer force diagramj
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Stress due to bending BMD – Bending moment diagramj
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