Calculate Water Pressure at Points 0-5 in a Siphon

In summary, a siphon is a device used to empty a large vessel of water. To calculate or state the initial (absolute) pressures at points 0, 1, 2, 3, 4, and 5, one must take into account the pressure exerted by the atmosphere (P0), the density and gravity of water, and the height of the water at each point. The pressure at point 3 may seem to contradict the pressure due to the height of water above between points 3 and 4, but this can be explained by the difference between hydrostatic and dynamic pressure. The pressure at point 5 must satisfy the mechanical constraint of P=Patm (atmospheric pressure). In another
  • #1
bruceflea
11
0
A siphon is used to empty a large vessel of water (see picture). Calculate/state the intial (absolute) pressures at points 0, 1, 2, 3, 4 and 5.

http://img499.imageshack.us/img499/8104/siphon1oq.th.jpg

P0 = 1.013 x 10^5 Pa - the pressure exerted on the water by the atmosphere

P1 = Po + density x gravity x height of water

P2 = Po + density x gravity x height of water

The answer for pressure at point 3 is 1.013x10^5 Pa but I'm not sure why that is.

P4 = P3 - density x gravity x height of water

P5 = 1.013 x 10^5 Pa - the minimum pressure required to overcome atmospheric pressure.

Could someone please explain the pressure at point 3 for me?

Thanks
 
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  • #2
Assuming that P3 is at the same elevation as P1, then the pressure P3 = P1, which would seem to contradict the pressure due to the height (2 m) of water above between P4 and P3.

I'll have to get back to this later.
 
  • #3
Astronuc said:
Assuming that P3 is at the same elevation as P1, then the pressure P3 = P1, which would seem to contradict the pressure due to the height (2 m) of water above between P4 and P3.
I'll have to get back to this later.

One knows that Bernoulli problems are tricky if we don't pay attention to the physics underlying. There is no contradiction because pressure at point 1 is different than pressure at point 3 (assuming 1 is far away from the hole). Pressure at point 1 is the Hydrostatic pressure, whereas pressure at point 3 is a Static pressure influenciated by the dynamic fluid motion (the fluid is being accelerated!). Moreover, as Astronuc pointed out, pressure at point 3 must be the same than pressure at point 5 if there is no transversal section variation and 5 and 3 are at the same altitude (apply Bernoulli). Pressure at point 5 must satisfy the mechanical constraint P=Patm, therefore the pressure at 3 must be also Patm. The Static pressure lost from 1 to 3 is due to the transformation of Hydrostatic pressure in Dynamic pressure.
 
  • #4
Calculate/state the intial (absolute) pressures at points 0, 1, 2, 3, 4 and 5.
I was pondering whether the fluid was moving or is the question referring to the moment just prior to movement of the fluid.

There must be a gradient of pressure for the fluid to move.
 
  • #5
Astronuc said:
I was pondering whether the fluid was moving or is the question referring to the moment just prior to movement of the fluid.
There must be a gradient of pressure for the fluid to move.

If there is no motion, then P1=P3=Hydrostatic pressure. Let's think of how the water is put into motion. In order to get the siphon working one must suck at the siphon exit to generate the motion (similarly when trying to take the gas out of the car gas deposit). I mean, the siphon does not start to work spontaneously.
 
  • #6
Clausius2 said:
One knows that Bernoulli problems are tricky if we don't pay attention to the physics underlying. There is no contradiction because pressure at point 1 is different than pressure at point 3 (assuming 1 is far away from the hole). Pressure at point 1 is the Hydrostatic pressure, whereas pressure at point 3 is a Static pressure influenciated by the dynamic fluid motion (the fluid is being accelerated!). Moreover, as Astronuc pointed out, pressure at point 3 must be the same than pressure at point 5 if there is no transversal section variation and 5 and 3 are at the same altitude (apply Bernoulli). Pressure at point 5 must satisfy the mechanical constraint P=Patm, therefore the pressure at 3 must be also Patm. The Static pressure lost from 1 to 3 is due to the transformation of Hydrostatic pressure in Dynamic pressure.

Thanks, makes perfect sense.

Just to make sure I understand this here's another siphon situation.

http://img427.imageshack.us/img427/1121/siphon22ho.th.jpg

The entrance of the siphon is at the bottom of the tank and the exit is below the tank.

For this situation would the pressure at the exit be Patm and so the pressure at the entrance would be Patm - dgh?

Assuming that the exit pressure is Patm, with respect to bernouilli's problems, do fluids always leave (or its reasonable to assume so) pipes/hoses/siphons at atmospheric pressure, whether the exit is up, down or horizontal?
 
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  • #7
The surrounding air is at atmospheric pressure, so the water at the siphons exit has to be atmospheric pressure, and actually is might be slightly higher due to interatomic forces which are responsible for surface tension.
 
  • #8
bruceflea said:
For this situation would the pressure at the exit be Patm and so the pressure at the entrance would be Patm - dgh?
What is "h"?. If h is the difference of altitude between the exit and entrance then you're right.
Assuming that the exit pressure is Patm, with respect to bernouilli's problems, do fluids always leave (or its reasonable to assume so) pipes/hoses/siphons at atmospheric pressure, whether the exit is up, down or horizontal?
About the boundary condition P=Patm for an outflowing jet
The boundary condition P=Patm is usually employed in bernoulli problems as a mechanical constraint at outflowing jets into the atmosphere. This boundary constraint is only valid at high Reynolds number, when [tex]\partial P/\partial r[/tex] is negligible. The assumption underlying is the boundary layer flow. The exiting jet flow would be described by Prandtl boundary layer equations, developing an annular boundary layer due to air viscosity. At high Re, this boundary layer is thin enough to assume the internal pressure in the jet core is the same than the external surrounding pressure (pressure remains constant radially across the layer). The existence of this layer is unavoidable. Because of that one always assume a flow discharge as an irreversible process, because this layer is an entropy generator, and some kinetic energy is ultimately dissipated.
The condition P=Patm would not be longer valid at small Re (Stokes flow), or at very high Mach (in supersonic flow) where the hydrostatic boundary condition is not felt by some fluid particles due to the hyperbolicity of the flow.
 

What is a siphon?

A siphon is a tube used to transfer liquid from a higher point to a lower point by utilizing the force of gravity. It works by creating a vacuum that pulls the liquid up and over the highest point of the siphon and then down to the lower point.

How do you calculate water pressure at points 0-5 in a siphon?

To calculate water pressure at points 0-5 in a siphon, you will need to use the following formula: P = ρgh, where P is the pressure, ρ is the density of water, g is the acceleration due to gravity, and h is the height of the water column at each point. Plugging in the values for each point will give you the water pressure at that specific point in the siphon.

What factors can affect water pressure in a siphon?

The factors that can affect water pressure in a siphon include the height of the water column, the diameter and length of the siphon tube, the density of the liquid being siphoned, and any external forces acting on the system, such as friction or air pressure.

Can water pressure in a siphon be negative?

Yes, it is possible for water pressure in a siphon to be negative. This can occur at the highest point of the siphon, where the water column is at its lowest height. In this case, the pressure will be negative, indicating that the liquid is being pulled up and over the highest point of the siphon.

Is water pressure constant throughout a siphon?

No, water pressure is not constant throughout a siphon. It will vary at each point along the siphon due to changes in height, diameter, and external forces. The pressure will also decrease as the liquid flows down the siphon due to friction and other factors.

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