Bernoulli's principal and pressure difference due to altitude

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Discussion Overview

The discussion revolves around Bernoulli's principle and its implications regarding pressure differences due to altitude in fluid dynamics. Participants explore the relationship between fluid velocity, pressure, and gravitational effects, particularly in the context of a pipe extending from sea level to a high altitude.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions whether the reverse of Bernoulli's principle can occur, suggesting that high velocity at altitude may contradict intuitive understanding.
  • Another participant clarifies that Bernoulli's principle applies under specific conditions, emphasizing that pressure differences due to altitude are primarily influenced by gravity rather than fluid speed.
  • A different participant notes that the Bernoulli equation is an energy balance equation and suggests that potential energy must be included, mentioning that temperature changes can affect the results for larger altitude variations.
  • A follow-up question is posed regarding the final pressure in a sealed pipe extending from sea level to a high altitude, prompting discussion about pressure gradients within the pipe.
  • One participant asserts that the pressure inside the pipe will follow the atmospheric gradient, indicating that pressure will vary from P1 at the top to P2 at the bottom.
  • Another participant presents a hypothetical scenario involving a bicycle air pump at high altitude, questioning whether the pressure at the top would be ambient or sea level pressure.
  • A response indicates that, accounting for weather phenomena, the pressure at 3000 feet would be ambient pressure.

Areas of Agreement / Disagreement

Participants express differing views on the implications of Bernoulli's principle and the effects of altitude on pressure. There is no consensus on the interpretations of pressure changes in the discussed scenarios.

Contextual Notes

Participants highlight the importance of considering external factors such as temperature changes and atmospheric conditions, which may influence the application of Bernoulli's principle and pressure calculations.

swaise
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Bernoulli's principal states that as velocity of a fluid increases, the static pressure decreases. I wonder if the reverse order can also happen. For example, if there is a pipe laid on the side of a mountain that is 3000 ft high. The bottom end of the pipe would be exposed to pressure at sea level, while the top would be exposed to a pressure much lower than sea level.

If we apply Bernoulli's equation, the indicated velocity is quite high. Yet intuitively, I can't believe this could be true.

How should I look at this concept?
 
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swaise said:
Bernoulli's principal states that as velocity of a fluid increases, the static pressure decreases.
That's only true when there is no external work done during the transition when the fluid accelerates or declerates. The typical example is fluid in a pipe of varying diameters, with the assumption that the pipe does not perform any work on the fluid.

The pressure difference related to altitude is due to gravity, not speed. There's a third term in the Bernoulli equation, density x (gravitational acceleration) x height. Wiki article:

http://en.wikipedia.org/wiki/Bernoulli's_principle
 
Bernoulli equation is an energy balance equation, so yes, potential energy must be included. You can get a rough estimate by considering velocity you get from simple Bernoulli equation as what you need to get to the altitude in the v²=2gh sense, but this ignores the temperature changes, so it will only work for small altitude changes. In a more general form Bernoulli equation for atmosphere will include temperature gradients and gravitational potential.
 
Thank you for the replies. I have a second question.

See the attached picture for details. Let's assume we have a pipe that extends from sea level to 3000 meters. Let's also assume the the whole pipe is filled with air at sea level pressures and the bottom is open to the atmosphere while the top is sealed, as show in step 1 - left column.

If then, we go through the cycles of sealing and unsealing the segments as show in the picture. What would the final pressure be? At the location where the "?" is placed. Would it be P2 or something lower than P2 since gravity is lower at this level?
 

Attachments

  • pump cycle.jpg
    pump cycle.jpg
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The air inside the pipe will have same gradient as atmosphere. If you close it at the top and leave it open at the bottom, the pressure will be P2 at the bottom and P1 at the top, with everything in between in the middle.
 
Really? I am so disappointed in nature...

Just to solidify my understanding of this concept. Imagine a bicycle air pump. That has a really good seal and is 3000 ft high. If we pull the pump up while the air is drawn from the bottom at sea level, would the pressure at the top of the cylinder at 3000 feet be ambient pressure or sea level pressure?
 
Give or take some corrections for weather phenomena, it will be ambient pressure at 3k feet.
 

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