Question #82306

Find the expression for the volume of liquid passing per second, V, through a pipe when the flow is steady. Assume the V proportional to (i) the coefficient of viscosity η of the liquid (ii) the radius r of the pipe and (iii) the pressure gradient, (ρ/l), causing the flow, where ρ is the pressure difference between the ends of the pipe and l is the length.

Expert's answer

Answer on Question #82306 - Physics - Mechanics - Relativity

Find the expression for the volume of liquid passing per second, VV, through a pipe when the flow is steady. Assume the VV proportional to (i) the coefficient of viscosity η\eta of the liquid (ii) the radius rr of the pipe and (iii) the pressure gradient, (ρ/l)(\rho / l), causing the flow, where ρ\rho is the pressure difference between the ends of the pipe and ll is the length.

Solution

According to what is given, take a small piece of a tube of length dx\mathrm{d}x. On the sides of the tube the force dF\mathrm{d}F acts:


dF=η2πrldvdrdx.\mathrm{d}F = \eta \cdot 2\pi r \cdot l \cdot \frac{\mathrm{d}v}{\mathrm{d}r} \cdot \mathrm{d}x.


On the sides of the tube the force ff acts:


df=πr2(p1p2)=πr2dpdxdx.\mathrm{d}f = \pi r^2 (p_1 - p_2) = \pi r^2 \cdot \frac{\mathrm{d}p}{\mathrm{d}x} \cdot \mathrm{d}x.


If the flow is steady, the sum of these forces is 0 (remember that dp=ρ\mathrm{d}p = \rho):


2ηldvdr=rρ.2\eta l \cdot \frac{\mathrm{d}v}{\mathrm{d}r} = r \cdot \rho.


Since it's steady, v=const,dv/dr=const,dp/dx=constv = \mathrm{const}, \mathrm{d}v / \mathrm{d}r = \mathrm{const}, \Rightarrow \mathrm{d}p / \mathrm{d}x = \mathrm{const}.

Thus,


dvdr=ρ2ηlr,\frac{\mathrm{d}v}{\mathrm{d}r} = \frac{\rho}{2\eta l} r,


Integrate it:


v=ρ4ηlr2.v = \frac{\rho}{4\eta l} r^2.


Per every 1 second volume dVdV passes through the pipe's cross-section of inner rr and outer r+drr + dr radii:


dV=2πrdrv,\mathrm{d}V = 2\pi r \mathrm{d}r \cdot v,V=πρ2ηl0rr2rdr=πρ2ηlr44=π8ρr4ηl.V = \pi \frac{\rho}{2\eta l} \int_{0}^{r} r^2 \cdot r \cdot \mathrm{d}r = \pi \frac{\rho}{2\eta l} \cdot \frac{r^4}{4} = \frac{\pi}{8} \cdot \frac{\rho r^4}{\eta l}.


This is Poiseuille's law. However he got the expression by dimensional analysis.

Answer:

V=π8ρr4ηl.V = \frac{\pi}{8} \cdot \frac{\rho r^4}{\eta l}.


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