Double Yield Point
Muhammad Umair Bukhari

     Engr.umair.bukhari@gmail.com

        www.bzuiam.webs.com
             03136050151
Definition:
Stress beyond which a material deforms by a relatively large
   amount for a small increase in stretching force.
Beyond this stress, the material no longer obeys Hook, s law .
                OR
It can be defined as the point where a tensile test piece begins
   to extend permanently. If the load is reduced to zero , the test
   piece will not return to its original length.
 The stress-strain curve for certain low carbon
  steels displays a double yield point.
 The material is expected to plastically deform at
  stress δ1.
 However, small interstitial atoms clustered
  around the dislocations interfere with slip and
  raise the yield point to δ2.
 Only after we apply the higher stress δ2 does the
  dislocation slip.
 After slip begins at δ2 , the dislocations move away
  from cluster of small atoms and continues to move
  very rapidly at the lower stress δ1 .
 We can easily determined the lower yield strengths for
  metals having this type of stress-strain behavior
 We can also see the double yield point phenomenon in
  polythene.
 Under mechanical deformations, three grades of
  polythene which differ mainly in terms of branch
  content exhibit two yield points.
 The first yield point occurs at low applied strains and
  marks the onset of temporary plastic deformation;
 The second yield point occurs at higher strains and
  marks the onset of permanent plastic deformation,
  and is associated with the development of a neck in
  tension
 The present work describes structural measurements
  carried out on these three polythene samples before
  and subsequent to different levels of tensile
  deformation
 X-Ray diffraction, transmission electron microscopy
  and optical microscopy were carried out on the
  isotropic materials and after the first and yield points
  under tensile deformation.

Double yield point

  • 1.
  • 2.
    Muhammad Umair Bukhari Engr.umair.bukhari@gmail.com www.bzuiam.webs.com 03136050151
  • 3.
    Definition: Stress beyond whicha material deforms by a relatively large amount for a small increase in stretching force. Beyond this stress, the material no longer obeys Hook, s law . OR It can be defined as the point where a tensile test piece begins to extend permanently. If the load is reduced to zero , the test piece will not return to its original length.
  • 4.
     The stress-straincurve for certain low carbon steels displays a double yield point.  The material is expected to plastically deform at stress δ1.  However, small interstitial atoms clustered around the dislocations interfere with slip and raise the yield point to δ2.  Only after we apply the higher stress δ2 does the dislocation slip.
  • 5.
     After slipbegins at δ2 , the dislocations move away from cluster of small atoms and continues to move very rapidly at the lower stress δ1 .  We can easily determined the lower yield strengths for metals having this type of stress-strain behavior
  • 6.
     We canalso see the double yield point phenomenon in polythene.  Under mechanical deformations, three grades of polythene which differ mainly in terms of branch content exhibit two yield points.  The first yield point occurs at low applied strains and marks the onset of temporary plastic deformation;  The second yield point occurs at higher strains and marks the onset of permanent plastic deformation, and is associated with the development of a neck in tension
  • 7.
     The presentwork describes structural measurements carried out on these three polythene samples before and subsequent to different levels of tensile deformation  X-Ray diffraction, transmission electron microscopy and optical microscopy were carried out on the isotropic materials and after the first and yield points under tensile deformation.