VIDEO LECTURE
MAIN CONCEPTS
Simply application of drawing a streamline and applying Bernoulli's equation, paying careful attention of points which are atmospheric pressure and points which are not. Get the Printer Friendly Version COMMENTS
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LESSON
A siphon is shown in the figuare below. Assuming that fluid viscosity can be neglected, we seek to estimate the velocity of water leaving C as a free jet. In addition, we later find the pressure of water in the tube at B and at A’. We assume that the flow is steady and the water is incompressible.
We draw a streamline as labeled by the red dotted line from the free surface at point A to the free jet at point C. Applying Bernoulli’s equation between these two points, we have
First we noticed that at both points, the water is exposed to the atmosphere and thus the pressure at each point is equal. We have taken the reference level to be at point C as shown Since the flow rate of water is through a small tube from a large container, we can say that Our equation now becomes
We do the same of drawing a streamline and applying Bernoulli’s equation, this time from A’ inside the tube to point C. Again, we take C as the reference level.
Beware that the pressure at point A’ is NOT atmospheric pressure simply because the water is moving with a certain velocity in the tube, unlike the water at point A. From the principle of continuity,
This is the difference between the pressure at A’ and the atmosphere. We can simply use a given value for atmospheric pressure to find Lastly, doing the same for points B and C
Again, from the principle of continuity,
The term All information presentated, less questions and exercises, is original content of Donny, with slight references to various books.
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