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Basic Pressure / Flow question. My Brain hurts. 1

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FBW

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Nov 29, 2012
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Hi All, I'm wondering if someone can help me understand some pressure/flow concepts im having a hard time wrapping my head around. What started with me trying to figure out a theoretical flow of gas through an orifice has turned into 2 nights of google searches and now i give up.

Can someone please explain to me how it's possible to have fluid flow (liquid or gas) from a low pressure area to a high pressure area. I've done some study on Bernoulli principal and its all fine and nice until you realize you don't understand why the fluid is moving in the first place. If the sum of all static and dynamic pressures in the system has to be zero, then how do i have flow at all. I know there's a reason, but i cant grasp it.

And in my mind, it also suggests that i can build a piece of pipe with progressively larger diameter, and increase the pressure inside it infinitely by continuing to make the diameter larger (and hence the flowrate less), regardless of the pressure source. I can actually build a system with 1 psi going "in" and a million coming "out" by changing flow rates. I know that cant be right. I'm missing some piece of the puzzle here.

Im also struggling with a "chicken-or-the-egg" type of confusion when i think about pressure and flow. Does pressure cause flow? Or does the resistance to flow cause pressure? Round and round I go.

Sorry about the novice question. Hope someone can help me get it straight? Thanks.
 
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When using the Bernoulli equation on incompressible fluids one must consider mechanical energy, not just static pressures, velocities or elevations and, of course, the friction losses along the fluid path. By using the search engine on Bernoulli you'll probably find hundreds of useful posts.
 
FBW- Bernouilli is a simple energy balance- forget for the moment about momentum which just confuses matters in my opinion. As you accelerate the fluid by increasing its velocity (reducing diameter), the extra kinetic energy of the fluid you accelerated (1/2 m v^2) has to come from somewhere. It comes from a reduction in potential energy, or more properly the fraction of the mechanical work done by the thing that pushed the fluid into the tube that is available as static pressure. Ignoring elevation head for the moment, that work is proportional to P*V where V is volume rather than velocity, which shows up as P/rho (density) in the Bernoulli equation, i.e. P/m*V, since the kinetic energy term in Bernouilli has similarly been divided by m). When you decelerate again, you get some of that kinetic energy back as increased P*V. In reality, you lose energy all along the way as a result of friction with the walls and within the fluid itself.

So: sure, assuming some perfect incompressible and inviscid fluid, if you had done some incredible amount of external work on the fluid to force it to flow in a pipe at some extraordinarily high velocity and only 1 psi of static pressure, you could, by decelerating it in increasing diameters, trade that enormous velocity for a high static pressure. But in reality there are limits due to friction, and with gases due to sonic flow, so perhaps that's why it offends your commonsense. Yes, I know it's peculiar to think of a fluid flowing from an area of low static pressure to one of higher static pressure, but that's because that notion is a simplified model of how fluids flow- easy to understand, and predictive in many circumstances, but inaccurate when velocity is changing (i.e. when flowing through an orifice, venturi etc.)
 
In addition to moltenmetal's excellent explanation, I'd only add that the Bernoulli's energy ebalance quation for frictionless incompressible, irrotational, flow per unit mass, between points 1 and 2, is:

p[sub]1[/sub]/d + v[sub]1[/sub][sup]2[/sup]/2 + z[sub]1[/sub]g = p[sub]2[/sub]/d + v[sub]2[/sub][sup]2[/sup]/2 + z[sub]2[/sub]g​
where:

p, is static pressure, d is density, v is speed, z is elevation, g is acceleration of gravity and:

p/d is the flow work when the fluid is displaced through a volumetric space 1/d against the restraint of pressure
v[sup]2[/sup]/2 is the kinetic energy per unit mass
zg is the potential energy per unit mass with the horizontal reference level 0-0.

Dividing all members of the equation by g, one gets the dimensions of length or height, in which the first term is called pressure head, and the second velocity head.
p[sub]1[/sub]/gd + v[sub]1[/sub][sup]2[/sup]/2g + z[sub]1[/sub] = p[sub]2[/sub]/gd + v[sub]2[/sub][sup]2[/sup]/2g + z[sub]2[/sub]​
 
You start with a total head, T[sub]H[/sub], = datum + pressure head + velocity head.
Then, mathematically, you can decrease V[sub]H[/sub], say by some given amount, then you are mathematically permitted to increase pressure until you run out of T[sub]H[/sub], or vice versa. You can't increase pressure indefinitely, because you soon run out of TH.



you must get smarter than the software you're using.
 
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