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Section 2.2  Tension


                      1200 L                             304 Stainless steel

                                                     70-30 Brass, as received
                      1000 -  8650 Steel
                                         1112 Steel,
                                         C0|d roned   70-30 Brass, annealed
                    E5 80° `                              1020 Steel
                    §                                     4130 Steel

                    CD
                    g 600                                 Copper, annealed
                    gg                                    2024-T36 AI
                    I: 400                                2024-O Al
                                                 ,        1100-O AI  4
                                 6061-O Al
                       200
                                      1100-H14 Al
                         O
                          0   0.2  0.4  0.6  0.8  1.0  1.2  1.4  1.6  1.8  2.0
                                             True strain (S)


              FIGURE 2.6  True stress-true strain curves in tension at room temperature for various
              metals. The curves start at a finite level of stress: The elastic regions have too steep a slope to
              be shown in this figure; thus, each curve starts at the yield stress, Y, of the material.
              2.2.5 Strain at Necking in a Tension Test

              As noted earlier, the onset of necking in a tension-test specimen corresponds to the
              ultimate tensile strength of the material. Note that the slope of the load-elongation
              curve at this point is zero, and it is there that the specimen begins to neck. The speci-
              men cannot support the load because the cross-sectional area of the neck is becoming
              smaller at a rate that is higher than the rate at which the material becomes stronger
              (strain-hardens).
                   The true strain at the onset of necking is numerically equal to the strain-
              hardening exponent, n, of the material. Thus, the higher the value of n, the higher
              the strain that a piece of material can experience before it begins to neck. This
              observation is important, particularly in regard to sheet-metal-forming operations
              that involve the stretching of the workpiece material (Chapter 16). It can be seen in
              Table 2.3 that annealed copper, brass, and stainless steel have high n values; this
              means that they can be stretched uniformly to a greater extent than can the other
              metals listed.



               EXAMPLE 2.| Calculation of Ultimate Tensile Strength
               This example shows that the UTS of a material can be  Solution Because the necking strain corresponds to
               calculated from its K and  71 values. Assume that a  the maximum load, the necking strain for this mate
               material has a true stress-true strain curve given by  rial is

                                                                                 6 = n = 0.5
                               0' = 69005 psi.                                              ’
                                           _
                                                                the true ultimate tensile strength is
                                  _        _
               Calculate the true ultimate tensile strength and the
                                                                                          ' = 488 MPa.
               engineering UTS of this material.                       O' = KH” = 69O(O.5)  0 5
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