Liquid in a vertical pipe open at the lower end and closed at the top

AI Thread Summary
A vertical pipe partially filled with liquid can either retain the liquid or allow it to fall out, depending on the pipe's diameter. In small diameter pipes, surface tension creates a stable meniscus that prevents the liquid from escaping, while in larger pipes, the liquid can fall due to the instability caused by long wavelength capillary waves, known as Rayleigh-Taylor instability. The critical diameter for water in air is approximately 8.5 mm, below which the liquid remains stable. The phenomenon is closely related to the properties of the liquid, including viscosity. For a deeper understanding, the textbook "Physics of Continuous Matter" by B. Lautrup provides comprehensive insights.
anders_r_r
Messages
5
Reaction score
0
Consider a vertical pipe partially filled with liquid. The pipe is open at the lower end and closed at the top. See the attached picture. Will the liquid fall out or not?

In a small diameter pipe a stable meniscus will form due to surface tension and prevent the water from falling out. In a larger diameter pipe the liquid will fall out of the pipe. What is the exact criterion that determines wether or not the water will fall out? Where/how do I find the answer? Can someone point me in the right direction?

/Anders
 

Attachments

Physics news on Phys.org
I suppose it depends on what liquid. Perhaps its viscosity, but maybe also other properties it may have.
 
Thanks for your input, Dr Lots-o'watts.

I suppose that the answer is closely related to the stability of the meniscus. In a large pipe the surface tension may not be strong enough to create a stable meniscus.
 
After a few days of searching I found the answer :-)

In the large diameter tube long wavelength capillary waves on the interface between the gas and liquid causes the interface to be unstable and the liquid will fall out. This phenomena is called the Rayleigh-Taylor instability.

When the diameter of the tube is sufficiently small, the longest possible wavelength of the capillary waves is not long enough to cause instablity, thus the liquid will stay in the tube.

If the gas is air and the liquid is water, the critical diameter of the tube is 8.5 mm.

The theory is very well explained in the textbook: "Physics of continuous matter" by B. Lautrup.
 
Hello! Let's say I have a cavity resonant at 10 GHz with a Q factor of 1000. Given the Lorentzian shape of the cavity, I can also drive the cavity at, say 100 MHz. Of course the response will be very very weak, but non-zero given that the Loretzian shape never really reaches zero. I am trying to understand how are the magnetic and electric field distributions of the field at 100 MHz relative to the ones at 10 GHz? In particular, if inside the cavity I have some structure, such as 2 plates...
Back
Top