 
  
  
  
  
In electron microscopy (Frank (1992)) one is faced with the case
  
 
for some   where
  where   .
 .   does not satisfy Orlov's condition, and (3.9) cannot be
satisfied since
  does not satisfy Orlov's condition, and (3.9) cannot be
satisfied since   for some
  for some   . In that case we put
 . In that case we put
  
 
With this choice of v, (3.8) is the minimal norm solution of Pf = g. A proper discretization along the lines of section 2.1 leads to the weighted backprojection algorithm of electron microscopy, see Frank (1992).