[ASK] Integral - Draining a Pipe

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SUMMARY

The discussion focuses on calculating the time to drain a pipeline using the orifice equation \(Q=CA_{o}\sqrt{2gh}\), where \(C\) is the coefficient of discharge, \(A_{o}\) is the orifice area, \(g\) is gravity, and \(h\) is the fluid head. The integration of this equation leads to the formula \(t=\frac{2 A_{p}}{slope} \frac{1}{CA_{o}\sqrt{2g}}(h_{1}^{1/2}-h_{0}^{1/2})\) for determining drainage time. Additionally, the discussion addresses the scenario with a constant flow, modifying the equation to include \(K\). A user also provides a method for evaluating the integral \(\int \frac{dh}{\sqrt h + B}\) using substitution.

PREREQUISITES
  • Understanding of fluid dynamics principles, specifically orifice flow.
  • Familiarity with calculus, particularly integration techniques.
  • Knowledge of the orifice equation and its components.
  • Basic understanding of hydraulic systems and flow rates.
NEXT STEPS
  • Study the derivation and applications of the orifice equation in fluid mechanics.
  • Learn advanced integration techniques, including substitution and integration by parts.
  • Explore the impact of varying coefficients of discharge on drainage calculations.
  • Investigate the effects of slope and cross-sectional area on flow rates in pipelines.
USEFUL FOR

Engineers, fluid mechanics students, and professionals involved in hydraulic design and analysis will benefit from this discussion, particularly those focused on drainage systems and flow calculations.

bleedpurple
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My first post, and first use of Latex. Here goes.

The engineering problem of calculating the time to drain a pipeline, tank, or vessel through an orifice is fairly straightforward using the orifice equation.\(Q=CA_{o}\sqrt{2gh}\)

With C being the coefficient of discharge for the orifice, Ao being the area of the orifice, g is the acceleration of gravity, and h the energy 'head' or elevation of the fluid above the orifice all in feet.
This equation can then be integrated by expressing Q as the change in volume over time.

\(Q=\frac{dv}{dt}\)

And expressing V as a function of head, h.
For a pipeline with constant gradient or slope the volume equals the cross sectional area of the pipe, Ap x length, and the length is the elevation change or head, h divided by the slope.

Therefore:

\(\frac{dv}{dt}=\frac{A_{p}}{slope} \frac{d_h}{dt} =C\,A_{o}\sqrt{2gh}\)and

\(\int{h^{-1/2}}dh=C\,A_{o}\sqrt{2gh} \frac{slope}{A_{p}} \int{dt}\)

or

\(\int{dt} = \frac{A_{p}}{slope} \frac{1}{CA_{o}\sqrt{2g}}\int{h^{-1/2}}dh\)

from this the result is

\(t=\frac{2 A_{p}}{slope} \frac{1}{CA_{o}\sqrt{2g}}(h_{1}^{1/2}-h_{0}^{1/2})\)

Now the case where there is also a constant flow in addition to the orifice flow.

\(Q=CA_{o}\sqrt{2gh}+K\)

resolves to the integral

\(\int{dt} = \frac{A_{p}}{slope CA_{o}\sqrt{2g}} \int\frac{1}{h^{1/2}+\frac{K}{CA_{o}\sqrt{2g}}}dh\)

from this the result is ?
 
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Hi bleedpurple, welcome to MHB! (Wave)

Good job with the $\LaTeX$!

I take it you're wondering how to evaluate $\int \frac{dh}{\sqrt h + B}$?
If so, let's substitute $u=\sqrt h + B\Rightarrow h=(u-B)^2 \Rightarrow dh=2(u-B)du$:
$$\int \frac{dh}{\sqrt h + B} = \int \frac{2(u-B)\,du}{u} = 2\int (1-\frac Bu)\,du
= 2(u-B\ln u) = 2\Big(\sqrt h + B - B\ln(\sqrt h + B)\Big)
$$
 

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