Introduction to Mechanics of Deformable Solids |
From inside the book
Results 1-3 of 75
Page 37
... Maxwell models . The initial rigidity of the dashpot means that in the Kelvin model the initial strain is zero , whereas in the Maxwell model the initial strain is the elastic stretch of the spring , σ1 / EM . In both models the dashpot ...
... Maxwell models . The initial rigidity of the dashpot means that in the Kelvin model the initial strain is zero , whereas in the Maxwell model the initial strain is the elastic stretch of the spring , σ1 / EM . In both models the dashpot ...
Page 42
... Maxwell component but does not strain the Kelvin component or the Maxwell dashpot imme- diately . A stress of EM1 is imposed . As time goes on , the Maxwell and the Kelvin dashpots move and the Maxwell spring relaxes . The Kelvin spring ...
... Maxwell component but does not strain the Kelvin component or the Maxwell dashpot imme- diately . A stress of EM1 is imposed . As time goes on , the Maxwell and the Kelvin dashpots move and the Maxwell spring relaxes . The Kelvin spring ...
Page 119
... Maxwell assemblage . @ const M = Mee ( EM / CM ) < EM = linearly with time from its elastic value 0 ML / EMI . This rotational creep for a beamlike assemblage is the analog of the axial creep in a Maxwell bar under tension or ...
... Maxwell assemblage . @ const M = Mee ( EM / CM ) < EM = linearly with time from its elastic value 0 ML / EMI . This rotational creep for a beamlike assemblage is the analog of the axial creep in a Maxwell bar under tension or ...
Other editions - View all
Common terms and phrases
applied assemblage axes axial force beam behavior cantilever centroid circumferential column compatibility components of stress constant creep cylinder deflection diameter direction displacement elastic-perfectly plastic elongation equations of equilibrium factor of safety free-body sketch homogeneous idealization increase inelastic initial interior pressure isotropic J₂ Kelvin Kelvin material limit linear Maxwell linear-elastic linear-viscoelastic linear-viscous load maximum Maxwell material modulus Mohr's circle neutral axis nonlinear normal stress outer P₁ P₂ perfectly plastic perpendicular plane plastic-limit principal stresses Prob problem pure bending radial radius ratio rectangular residual stress rigid end plates rotation shaft shear strain shear stress shell shown in Fig simple shear solution statically determinate steel stress and strain stress-strain curve stress-strain relations Suppose surface symmetry T₁ T₂ temperature tensile tensile stress thick-walled time-dependent torque torsion uniform unloading versus viscous yield curve yield stress Young's modulus zero ΕΙ σα σο στ