flat_iv wrote:Someone talk me out of this madness.
M. Poiseuille (1797 - 1869) can.
Poiseuille was interested in the flow of a fluid, actually blood, in narrow tubes, and found that the flow rate Q was related to the pressure difference Δp by Q = ( pi*r4/8Lμ ) Δp. Here, r is the radius of the tube, and L its length and μ is the absolute viscosity of the liquid in poise. pi is itself.
This is hard to reproduce on this forum, but that "r4" above is actually r raised to the power 4. Thus, for a given flow rate, we can conclude that e.g. pressure drop is proportional to the length of the tube - which makes perfect sense. We can also conclude that pressure drop is inversely proportional to the fourth power of tube radius (or diameter) for a given flow rate. This means that, for a given flow rate, halving the radius (or diameter) of a tube will increase the pressure drop by a factor of 16! (or , to look at it in the way the equation was presented, the flow rate achievable for a given pressure drop will fall be a factor of 16).
Now, Poiseuille's law only holds true for laminar flow in relatively small tubes, and for high speed flow and larger tubes life becomes more complex, but flow rates through cooling water systems are generally quite low, and the imprecision of partly turbulent flow doesn't let you escape from the generalities of M. P's law: small pipes suck.
On motorcycles the "L" part of the equation is tiny, and the designers are very concerned about weight and aerodynamics, so they are probably using relatively high pressure pumps to keep tube diameters down for low aero drag and low weight.
hth
[ Edited on 16-1-06 by modulus ]