*****************************
.5k*y^2 = .5k*x^2 + m*g*(x+a/2)
 
This is the "true" elastic PE PLUS the gravitational PE 
measured from x= -a/2 !
*****************************
 
 
  ----- Original Message ----- 
  
  
  Sent: Tuesday, December 04, 2001 9:52 
  PM
  Subject: Re: test problem
  
  To perhaps clarify further aspects of this type 
  problem:
  As before, let x = the mass position as measured (up is 
  positive) from the relaxed spring position.
  Let x=-a (a will be positive) be the equilibrium position 
  for the hanging mass, so that ka=mg.
  Let y = the mass position as measured (up is positive) from 
  this (x=-a) equilibrium position, so that y = x + a.
   
  Then N2 gives for the DE of motion:
   
  mx'' = -k*x - mg  ; Now substitute x = y-a  
  =>
   
  my'' = -k*y + k*a -mg  ; Now use ka = mg  
  =>
   
  my'' = -k*y  => SHM about the point y=0 
  (x=-a)
   
  Note also that the "pseudo" elastic PE of this y oscillation 
  is:
   
  .5 K*y^2 = .5 k*x^2 + .5*k*a^2 + kax ; Now use ka=mg  
  =>
   
  ,5k*y^2 = .5k*x^2 +.5 m*g*(x+a)
   
  This is the "true" elastic PE PLUS the gravitational PE 
  measured from x= -a !
   
  IE: You can use the "pseudo" elastic PE as the TOTAL 
  system PE (Cuz it is so, numerically, if the arbitrary zero of 
  gravitational PE is properly chosen).