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I recently studied about bernoulli's equation/principle.

After the derivation of the said equation , my book gave some applications of the principle, which include torricelli's theorem/law.

In deriving torricelli's law from bernoulli's principle, the pressure at the opening of the tank in which the fluid is contained , is said to be equal to the same pressure which is applied at the the top surface of the applied fluid , namely the pressure of the atmosphere.

But my book also states that the pressure drops (according to bernoullis principle) when the fluid passes through a narrow pipe or opening and its velocity increases.

So why does the pressure remain the same in this situation ? Why doesn't it change? Any help would be much appreciated , THANKS.

Could you please answer in simple and easy to learn terms , Thanks AGAIN.

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Here is a proof on wikipedia if any one else wants to follow along. The proof states that the pressure in the water is zero (I will take atmospheric pressure to be zero) after it has exited the hole. This is because there is no longer fluid on top of it after it goes out the hole. However, the proof does not say that the pressure is zero immediately inside the hole. In fact, the pressure there will be given by $\rho g h$, (where $\rho$ is the fluid mass density, $g$ is the acceleration of gravity, and $h$ is the depth in the water) as you would have expected.

So what happens is as the water moves through the hole it moves to a region of high pressure ($\rho g h$) to a region of zero pressure. This pressure gradient causes the water to accelerate to a speed given by $\dfrac{1}{2} v^2 = gh$.

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I agree with don_Gunner94's answer.

If the fluid come out from the constricted passage to atmosphere,it will experience atmospheric pressure,which is same as the pressure acting at top of the container.

Even according to Bernoulli's principle, Static pressure + Dynamic Pressure = Constant

Therefore, the pressure acting on the fluid when it is inside the container would be static and when it will come out of the passage and open to atmosphere would be dynamic,all together total pressure remains constant.

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I suppose that the best way to answer this question is by using an analogy. Take a glass of water(at room temperature) and place it in a refrigerator. What happens to the water? It cools down. Now you take this glass of cold water and keep it back outside. What happens now? The temperature of the water comes back to the room temperature. Why? Because the water is exposed to room conditions and hence through heat transfer, it's temperature rises up to that of the room temperature. Similarly, your fluid when flowing through a constricted passage(analogous to a refrigerator) experiences a drop in pressure(as your textbook states). But at the exit of the passage, it is once again exposed to atmospheric conditions and hence it's pressure rises back to the atmospheric pressure!

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  • $\begingroup$ A constricted passage means one where there's a reduction in cross section for flow, in case you weren't aware of that $\endgroup$ Commented Jan 21, 2016 at 3:26

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