Page 399 - Marks Calculation for Machine Design
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P1: Naresh
                                      15:28
                          January 4, 2005
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                 Brown˙C09
                       TABLE 9.1
                                Summary of Additional Coils for Compression Springs
                                        Total  MACHINE ENERGY                Free  381
                                                   Solid
                           Type         coils     length      Pitch (p)    length (L o )
                       Plain             N a     (N a + 1)d  (L o − d)/N a  pN a + d
                       Squared          N a + 2  (N a + 3)d  (L o − 3d)/N a  pN a + 3d
                       Plain & Ground   N a + 1  (N a + 1)d  L o /(N a + 1)  p(N a + 1)
                       Squared & Ground  N a + 2  (N a + 2)d  (L o − 2d)/N a  pN a + 2d
                       Source: Design Handbook, Associated Spring—Barnes Group, Bristol, Conn., 1981.
                    Stability.  In Chap. 6 column buckling was discussed where if the compressive stress
                    (σ axial ) became greater than a critical stress (σ cr ), depending on the slenderness ratio of the
                    column, the design would be unsafe. Similarly, as the length of a cylindrical helical spring
                    increases, buckling can occur at a critical deflection (y cr ) given by Eq. (9.37) as
                                                              
                                                          2    1/2
                                                         λ eff
                                        y cr = L o C 1 1 − 1 −                 (9.37)
                                                
                                                         C 2
                    where (λ eff ) is the effective slenderness ratio and given by Eq. (9.38) as
                                                     αL o
                                                λ eff =                         (9.38)
                                                      D
                    and (α) is an end-condition constant.
                      Values for four typical end conditions for helical springs are given in Table 9.2. Notice
                    the similarity with the coefficient (C ends ) for slender columns given in Chap. 6.

                               TABLE 9.2  Summary of the End-Condition Constant (α)
                               α                   End condition
                               0.5      Both ends supported on flat parallel surfaces
                               0.7      One end supported on flat surface, other end hinged
                               1        Both ends hinged
                               2        One end support on flat surface, other end free


                      The constants (C 1 ) and (C 2 ) in Eq. (9.37) are called elastic constants and are given by
                    the following relationships:
                                                     E
                                             C 1 =                              (9.39)
                                                  2(E − G)
                                                    2
                                                  2π (E − G)
                                             C 2 =                              (9.40)
                                                    2G + E
                                                                               2
                      To avoid taking the square root of a negative number in Eq. (9.37), the ratio (λ /C 2 )
                                                                               eff
                    must be less than or equal to 1. This means the free length (L o ) must be less than or equal
                    to the quantity on the right-hand side of Eq. (9.41).
                                                            1/2


                                               π D  2(E − G)
                                          L o ≤                                 (9.41)
                                                α   2G + E
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