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So, if we have a large pipe which is constricted in the middle, the fluid in the middle section will move faster. Why is it so? What dictates that liquid that an X amount of it must pass on the other side regardless of the size of the encasement?

The only reason I could think about is because that the initial pressure which causes the movement somehow is being transferred to a smaller area, but that makes no sense...

Thank you very much!

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Seems to me that the "meat" of your question is not about Bernoulli's principle, but rather a related concept called "conservation of mass" . I'll address that first, and get to Bernoulli's principle later.

Conservation of mass

The idea you are looking for is Conservation of Mass. If you assume the fluid doesn't have any "gaps" or spaces (and real fluids don't) and isn't compressible (which is true for liquids and often close enough for gasses) then the flow rate must be the same everywhere in the pipe.

Consider some section of the pipe, for instance the part of the pipe between cross-sectional areas A1 and A2 in the diagram above. Fluid flows into it at some rate, say x liters/minute. It has to go somewhere, and if it can't compress and you don't allow empty spaces then the only place for it to go is out the other end. For every fluid molecule that passes through A1, one must exit at A2, otherwise the fluid would pile up in that section of the pipe. So, fluid must exit the segment at the same rate of x liters/minute. Since we chose our segment endpoints arbitrarily, the rate of flow must be the same everywhere.

Now, if the pipe gets thinner, say half the diameter, the flow has to speed up to twice the speed to maintain the constant x liters/minute flow.

Bernoulli's principle then says that the pressure in this narrow section of pipe decreases, but I don't think the main gist of your post was about Bernoulli's principle. But since that's the title of the post, here goes:

Bernoulli's Principle

To address "Why does Bernoulli's principle work?", there's two ways to look at it:

  1. conservation of energy
  2. acceleration due to pressure differences

conservation of energy

Bernoulli's equation is often derived using conservation of energy. We've seen from conservation of mass that the fluid molecules in the pipe above have to speed up when they pass through the narrow part of the pipe. That means their kinetic energy has to increase since KE = mv^2 /2. Where does this energy come from? It comes from a decrease in pressure.

Usually, one thinks of pressure in terms of force per unit area (i.e. pounds per square inch) but pressure can also be thought of as energy per unit volume. So, less pressure means less energy. Essentially, Bernoulli's equation expresses the trade-off between kinetic energy of the moving fluid and the "potential" energy contained in the pressure. (often the equation includes a term for gravitational potential energy too.)

The nice thing about deriving Bernoulli's principle from conservation of energy is that the derivation can be done using only algebra - no calculus needed. That's why you see this treatment in high school texts. The thing is, the concept of energy wasn't around in 1738 when Bernoulli derived his formula. The term "energy" was first used by Thomas Young in 1807, and it would be another thirty years or so before the law of conservation of energy was clearly established. So, Bernoulli was about a century too early to use conservation of energy.

acceleration due to pressure differences

Bernoulli actually derived the equation from first principles (i.e. Newton's laws of motion) and if you examine this derivation it becomes clearer why Bernoulli's principle works. Basically, you look at a small volume of fluid and the forces on that volume. If the pressure is decreasing along the direction of travel then there is more pressure behind than in front. This makes a net force on the volume, and according to F=ma the fluid accelerates. On the other hand, if the pressure is increasing, then there's more pressure in front than behind and the fluid slows down.

Bernoulli simply took the intuitive idea of "more pressure behind than in front means the fluid will accelerate", quantified the pressure and speed using Newton's second law (F= ma) to get an intermediate equation, and then and used calculus to integrate that equation to get the equation we're familiar with today.

Thinking about Bernoulli's principle this way makes it intuitively clear why it happens - of course the fluid will accelerate if there's more pressure behind than in front. Unfortunately, to derive the equation this way means you need to know calculus so it's rarely taught this way in high school science classes. That's a shame, because the physics is fairly simple if you think about it this way.

Many students struggle to find an intuitive reason why faster moving fluid has lower pressure - why should the pressure drop just because it's moving faster? And if you express Bernoulli's principle as "faster moving fluid has lower pressure" it's mysterious why this should be so.

But if you think of it as "pressure differences cause the fluid to accelerate and gain speed" it's obvious why it works. From an intuitive perspective, the usual statement of Bernoulli's principle ("faster moving air causes lower pressure") gets it exactly backwards - the change in speed is a ''result'' of pressure differences, not the ''cause''. Or as Klaus Weltner put it in the American Journal of Physics

Textbooks stating that the higher streaming velocity is the reason for the low pressure are wrong. It is the other way round. The low pressure is the reason for the higher velocity of the streaming air.

-from "A comparison of explanations of the aerodynamic lifting force" Klaus Weltner Am. J. Phys. 55, 50 (1987); http://dx.doi.org/10.1119/1.14960

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  • $\begingroup$ What is the intuitive reason that the constricted part has lower pressure to begin with? $\endgroup$ – afuna Nov 26 '18 at 18:17
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It sounds like you are not asking about Bernoulli's principle, which describes energy conservation in a fluid, but about why fluids move faster in the thin section of a pipe. This is not Bernoulli's principle, it is just something someone might have mentioned when talking about Bernoulli's principle.

Suppose the liquid moves the same speed everywhere in the pipe.

In a fat section, you might have 100 liters/minute passing through. Then in a thin section with one tenth the cross-sectional area, you would have 10 liters/minute passing through. If you watched the fluid for an entire year, more than 50 million liters would pass through the fat part, but only 5 million liters through the thin part. But they're connected, so everything that flows through the fat part flows through the thin part. Where did the missing 45 million liters go? The answer is that the liquid goes ten times faster in the thin part so that 50 million liters pass through there in a year, too.

If the fluid is compressible it is a bit different, because the conserved quantity is mass, not volume, but the idea is basically the same.

The physical cause of the fluid speeding up is that there is a pressure gradient in the fluid. The pressure gradient comes from a combination of the fluid properties and the boundary conditions of the situation.

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  • $\begingroup$ Thank you for the answer. Hee is the thing though, you said that the fat section has 100 liters passing through it (in contrast to the thin section with 10 litres), and I don't understand why. It seems to me like the fat section should have the MAXIMUM capacity of transferring 100 litres but it should be dependant on the exit hole (like a bucket which will loose water faster the bigger the hole in it). $\endgroup$ – dactylo May 4 '15 at 9:02
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The Bernoilli Effect is one of the most poorly explained phenomenons there is. I have never seen it explained simply. I think Mark was referring to two different sized pipes under the same pressure, then one pipe with a thin section. This picture should explain it all.

enter image description here

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