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T-80 B e c a u s e  t h e  t h e o r y  a n d equations  of  these  methods  are  so complicated,  they  are  beyond  the scope of this treatment.  Usually, all stock worm gears are produced with crowning. 9.4  Self-Locking Of Worm Mesh Self-locking  is  a  unique  characteristic  of  worm  meshes  that  can  be  put  to  advantage. It  is  the  feature  that  a  worm  cannot  be  driven  by  the  worm  gear.    It  is  very  useful  in  the design  of  some  equipment,  such  as  lifting,  in  that  the  drive  can  stop  at  any  position without concern that it can slip in reverse.  However, in some situations it can be detrimental if the system requires reverse sensitivity, such as a servomechanism. Self-locking does not occur in all worm meshes, since it requires special conditions as outlined  here.    In  this  analysis,  only  the  driving  force  acting  upon  the  tooth  surfaces  is considered  without  any  regard  to  losses  due  to  bearing  friction,  lubricant  agitation,  etc. The governing conditions are as follows: Let Fu1 = tangential driving force of worm Then, Fu1 = Fn (cosan singm cos)     (9-6) where: a=  normal pressure angle g =  lead angle of worm m =  coefficient of friction Fn  =  normal driving force of worm If Fu1 > 0 then there is no self-locking effect  at  all.  Therefore,  Fu1  £  0  is  the critical limit of self-locking. Let an  in  Equation  (9-6)  be  20°,  then the condition: Fu1 £ 0   will become: (cos20° singmcosg) £ 0 Figure  9-11  shows  the  critical  limit  of  self-locking  for  lead  angle  and  coefficient  of friction m.    Practically,  it  is  very  hard  to  assess  the  exact  value  of  coefficient  of  friction m. Further, the bearing loss, lubricant agitation loss, etc. can add many side effects.  Therefore, it  is  not  easy  to  establish  precise  self-locking  conditions.    However,  it  is  true  that  the smaller the lead angle g, the more likely the self-locking condition will occur. 0.20 0.15 0.10 0.05 0 0 3° 6° 9° 12° Lead angle g Fig. 9-11 The Critical Limit of Self-locking of Lead Angle g  and Coefficient of Friction m Fig. 9-10 The Value of Factor (k ) 14° 15° 16° 17° 18° 19° 20° 21° 22° 23° Axial Pressure Angle  ax 0.6 0.55 0.5 0.45 0.4 0.35 k