Hello!
In a first order, flow resistance is inverse proportional to fourth power of tube diameter.
We are maybe not talking about the same thing. I say that
for a given flow
(in liters per second), the resistance is inverse proportional to the
fifth power
of the tube diameter. Here is the proof:
It's generally admitted that fluide flow in a tube can be described with the
following relation:
dP/dL = l * r * V^2 / 2D (Equation A)
where:
dP is the difference of pressure between both ends of the tube
dL is the length of a piece of the tube for the current experiment
-> But let's leave this under the forem dP/dL which will be linear
pressure loss of our tube.
l is a general factor of pressure loss (a constant in standard units)
r is the volumic mass
V is the speed of the fluid
D is the diameter of the tube
As r and l are both constants, we can call the product K, and then we get:
dP/dL = K V^2/2D (Equation B)
Now we are talking about a constant flow (let's call it Q for quantity, let's remind
that it's a quantity per second and that it's a constant, 1l/s in my example above),
and we want to know the difference of pressure between both ends as a function of
the diameter.
As Q is constant we can express V from Q and D.
As V is the speed of the fluid, it is the length per second. It is therefore Q/S,
S being the surface.
S = pi D^2/4
Therefore V = Q/S = 4Q / pi D^2
When squared, this yields:
V^2 = 16 Q^2 / pi^2 D^4
And therefore, replacing this in Eqiation B:
dP/dL = K * 16 Q^2 / (pi^2 D^4) * (2D)
And we get finally:
dP/dL = 8 K Q^2 / pi^2 D^5
That's about it.
Dora.