Page 184 - Mechanical Behavior of Materials
P. 184

Problems and Questions                                                     185


                   (b) Determine true stresses and strains, and plot the true stress–strain curve, showing
                      both raw and corrected values of true stress. Also evaluate the true fracture stress and
                      strain.
                   (c) Calculate true plastic strains for the data beyond yielding to fracture. Then fit Eq. 4.24
                      to these values and the corresponding corrected stresses, determining H and n.

                                     Table P4.22
                                     Engr. Stress  Engr. Strain  Diameter
                                       σ, MPa         ε          d,mm
                                          0         0            6.32
                                        125         0.0006        —
                                        257         0.0012        —
                                        359         0.0017        —
                                        317         0.0035        —
                                        333         0.0070        —
                                        357         0.0100        —
                                        397         0.0170        —
                                        458         0.0300        —
                                        507         0.0500        —
                                        541         0.0790       5.99
                                        576           —          5.72
                                        558           —          5.33
                                        531           —          5.08
                                        476           —          4.45
                                        379           —          3.50
                                     (Final point is fracture.)

            4.23 Several values of the strength coefficient H are missing from Table 4.6. Estimate these values.
            4.24 Assume that a material is quite ductile, so that elastic strains are small compared with plastic
                 strains over most of the stress–strain curve. Plastic and total strains can then be taken as
                                                          n
                 equivalent, ˜ε p ≈˜ε, and Eq. 4.23 becomes ˜σ = H ˜ε .
                   (a) Show that the strain hardening exponent n is then expected to be equal to the true
                      strain ˜ε u at the engineering ultimate strength point—that is, n ≈˜ε u . (Suggestion: Start
                                                     n
                      by making substitutions into ˜σ = H ˜ε from Sections 4.5.1 and 4.5.2, to obtain an
                      equation σ = f (˜ε, H, n) that gives engineering stress.)
                   (b) How closely is this expectation realized for the tension test on AISI 1020 steel of
                      Ex. 4.1, 4.2, and 4.3? (See Table E4.1 and Fig. 4.21.)
                   (c) From your derivation for (a), write an equation for estimating the ultimate tensile
                      strength σ u from H and n. How well does this estimate work for the AISI 1020 steel
                      of Ex. 4.1, 4.2, and 4.3?
            4.25 On the basis of the data in Tables 4.2 and 4.6 for 2024-T4 aluminum, draw the entire
                 engineering stress–strain curve up to the point of fracture on linear graph paper. Accurately
                 plot the initial elastic slope and the points corresponding to yield, ultimate, and fracture, and
   179   180   181   182   183   184   185   186   187   188   189