I'm well aware that the problem is one of convection not conduction as are the references on heat exchangers I've been reading.
Out of 60 or so scenarios that are listed, the one that seems to be of closest relevance is turbulent flow of a cold gas over a "warm wall". In this case the Prandtl and Grashof numbers can be disregarded and the coefficient is a function of the Reynolds number:-
P= 0.055k/l R^0.75 (Imperial Units) and R= vL/n where
k= thermal conductivity
l= length of pipe
n= kinematic viscosity
v= velocity
L: "for lengths greater than 2 feet use L=2"
This begs a whole host of questions:-
What exactly does a "warm wall" consist of?
Should I read "length of wall" for length of pipe?
Why are we dividing by l when the transmitted power is already per unit of surface area anyway?
What is the relevant dimension for irregular objects?
Is l the same as L, and if not is "lengths greater than 2 feet" referring to l or L?
Why is R apparently being calculated from a longitudinal rather than a lateral dimension?