Page 15 - Pressure Vessel Design Manual
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2    Pressure Vessel Design Manual

         effects  long  or  short  term?  Do  they  apply  to  a  localized   In  any  pressure  vessel  subjected  to  internal  or  external
         portion of the vessel or are they uniform  throughout?   pressure,  stresses  are set up in  the  shell wall. The state  of
           How these  stresses  are  interpreted  and  combined,  what   stress is triaxial and the three principal  stresses are:
         significance they have to the overall safety of the vessel, and
         what  allowable stresses  are  applied will  be  determined  by   ox = 1ongitudmaVmeridional stress
         three things:                                           04  = circumferentialAatitudina1 stress
                                                                 or = radial stress
           1. The strengtwfailure theory utilized.
           2. The types and categories of loadings.              In addition, there may be bending and shear stresses. The
           3. The hazard the stress represents  to the vessel.   radial stress is a direct stress, which is a result of the pressure
                                                               acting directly on the wall, and causes a compressive stress
                                                               equal to the pressure. In thin-walled vessels this stress is so
                                                               small compared  to  the  other  “principal”  stresses  that  it  is
                   Membrane Stress Analysis                    generally ignored. Thus we assume for purposes of analysis
                                                               that the state of  stress is biaxial. This greatly simplifies the
           Pressure  vessels  commonly  have  the  form  of  spheres,   method of combining stresses in comparison to triaxial stress
         cylinders,  cones,  ellipsoids,  tori,  or  composites  of  these.   states. For thickwalled vessels  (RJt  <  lo), the radial stress
         When the thickness is small in comparison with other &men-   cannot  be  ignored  and  formulas  are  quite  different  from
         sions (RJt  > lo), vessels are referred to as membranes and   those used in finding “membrane stresses” in thin shells.
         the associated stresses resulting from the contained pressure   Since ASME Code, Section VIII, Division 1, is basically for
         are called membrane stresses. These membrane stresses are   design by rules, a higher factor of safety is used to allow for
         average tension  or compression  stresses. They are assumed   the  “unknown”  stresses  in  the  vessel.  This  higher  safety
         to be uniform across the vessel wall and act tangentially to its   factor, which allows for these unknown stresses, can impose
         surface. The membrane or wall is assumed to offer no resis-   a  penalty  on  design  but  requires  much  less  analysis. The
         tance  to bending. When the wall offers resistance  to bend-   design  techniques  outlined  in  this  text  are  a  compro-
         ing, bending stresses occur in addtion to membrane stresses.   mise  between  finding  all  stresses  and  utilizing  minimum
           In  a  vessel  of  complicated  shape  subjected  to  internal   code formulas. This additional knowledge of stresses warrants
         pressure,  the simple membrane-stress  concepts  do not  suf-   the use of higher allowable stresses in some cases, while meet-
         fice to give an adequate idea of the true stress situation. The   ing the requirements  that all loadings be considered.
         types  of heads  closing the vessel, effects of  supports, varia-   In conclusion, “membrane stress analysis’’ is not completely
         tions  in  thickness  and  cross  section,  nozzles,  external  at-   accurate  but  allows  certain  simplifymg assumptions  to  be
         tachments,  and  overall  bending  due  to  weight,  wind,  and   made while maintaining a fair degree of accuracy. The main
         seismic activity all cause varying stress distributions  in  the   simplifying assumptions are that the stress is biaxial and that
         vessel. Deviations from a true membrane shape set up bend-   the stresses are uniform across the shell wall. For thin-walled
         ing in  the  vessel wall  and cause  the  direct  loading to vary   vessels  these  assumptions  have  proven  themselves  to  be
         from point to point. The direct loading is diverted from the   reliable.  No  vessel  meets  the  criteria  of  being  a  true
         more  flexible to the  more  rigid portions  of  the vessel. This   membrane,  but  we  can  use  this  tool  with  a  reasonable
         effect is called “stress redistribution.”             degree of accuracy.




                                       STRESS/FAILURE THEORIES


           As  stated previously, stresses  are meaningless  until  com-   They are the “maximum stress  theory” and the “maximum
         pared  to  some  stresdfailure  theory.  The  significance  of  a   shear stress theory.”
         given  stress  must  be  related  to  its  location  in  the  vessel
         and  its  bearing  on  the  ultimate  failure  of  that  vessel.
         Historically, various  ‘‘theories” have been  derived  to  com-   Maximum Stress Theory
         bine  and  measure  stresses  against  the  potential  failure
         mode.  A  number  of  stress  theories,  also  called  “yield cri-   This theory is the oldest, most widely used and simplest to
         teria,” are available for  describing the  effects  of  combined   apply.  Both  ASME  Code,  Section  VIII,  Division  1,  and
         stresses. For purposes  of this book, as these  failure theories   Section  I  use  the  maximum  stress  theory  as  a  basis  for
         apply to pressure vessels, only two theories will be discussed.   design.  This  theory  simply  asserts  that  the  breakdown  of
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