text: can be expressed as follows:
  where:
  , so that .
  The vector Laplacian of a vector of the type  reads:
  It can thus be calculated that:
  Therefore:
  Thus the vorticity is:
  where we have used the vanishing of the divergence of  to relate the vector laplacian and a double curl.
  The equation of motion's left hand side is the curl of the following:
  We calculate the derivative separately for each term in .
  Note that:
  And also:
  We thus have:
  Combining all the terms we have:
  Taking the curl, we find an expression that is equal to  times the gradient of the following function, which is the pressure:
  where  is the pressure at infinity, .is the polar angle originated from the opposite side of the front stagnation point ( where is the front stagnation point).
  Also, the velocity is derived by taking the curl of :
  These p and u satisfy the equation of motion and thus constitute the solution to Oseen's approximation.