Introduction to mechanics of deformable solids |
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Page 59
If the shear-stress vs shear-strain curves are simple T versus <p curves with a
change of scale, the shear strain as computed will be tan y automatically. For
small y there is, as mentioned previously, no important difference between tan 7
and 7 ...
If the shear-stress vs shear-strain curves are simple T versus <p curves with a
change of scale, the shear strain as computed will be tan y automatically. For
small y there is, as mentioned previously, no important difference between tan 7
and 7 ...
Page 61
Changes in length now represent shear strains; forces represent shear stresses.
With this understanding, then ... Elastic and inelastic materials do exist which
show small extension or contraction under simple shear. Correspondingly, they
may ...
Changes in length now represent shear strains; forces represent shear stresses.
With this understanding, then ... Elastic and inelastic materials do exist which
show small extension or contraction under simple shear. Correspondingly, they
may ...
Page 63
Strain The picture of simple shearing strain similarly may be thought of as
extension in some directions and contraction in others. Figure 4.18 shows how a
small rectangular element, of dimensions a X b (see also Fig. 4.9), is distorted Fig
.
Strain The picture of simple shearing strain similarly may be thought of as
extension in some directions and contraction in others. Figure 4.18 shows how a
small rectangular element, of dimensions a X b (see also Fig. 4.9), is distorted Fig
.
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applied assemblage axial force beam behavior centroid circumferential column compatibility components of stress conditions of deformation constant creep cross section cylinder deflection diameter direction displacement elastic-perfectly plastic elongation equations of equilibrium factor of safety free-body sketch fully plastic homogeneous idealization increase inelastic initial interior pressure isotropic Kelvin Kelvin material limit linear Maxwell linear-elastic response linear-viscoelastic linear-viscous load maximum Maxwell material modulus Mohr's circle neutral axis nonlinear normal stress outer perfectly plastic perpendicular plane plastic deformation plastic-limit Poisson's ratio principal stresses Prob problem pure bending radial radius ratio rectangular residual stress rotation shaft shear strain shear stress shell shown in Fig simple shear solution statically statically determinate steel stress and strain stress-strain curve stress-strain relations Suppose surface symmetry temperature tensile stress thick-walled sphere thickness time-dependent tion torque torsion uniform unloading versus viscous yield curve yield stress zero