Capillary Action: Physically Possible Forms

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Homework Help Overview

The discussion revolves around the physical possibilities of three forms of capillaries in relation to capillary action. The original poster presents a scenario where the height of fluid in different capillary shapes is analyzed, emphasizing that the contact angle is zero, indicating perfect wetting.

Discussion Character

  • Exploratory, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to analyze each case of capillary forms, suggesting that case a is possible based on the relationship between fluid height and capillary radius. They express uncertainty regarding cases b and c, questioning the implications of the Young-Laplace equation and whether all cases can indeed be possible.

Discussion Status

The discussion is ongoing, with the original poster seeking clarification on the physical feasibility of the capillary forms. Some participants have engaged by addressing the posting etiquette, but there has been no resolution or consensus on the capillary cases themselves.

Contextual Notes

There is a lack of specific data such as densities or dimensions, which may affect the analysis of the capillary forms. The original poster also notes the relevance of the fluid's contact angle in their reasoning.

khuysent
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Homework Statement



(see figure) Three forms of capillaries are given, and the question is simple : which of these are physically possible?

There are no data given (such as densities or dimensions of the capillaries), so it is just the form that is of importance here. The three cases stand on their own, so the fact that the height of the fluid in case c is higher than in the other cases is irrelevant. The fluid has a contact angle of 0 (perfect wetting)

Homework Equations



*The equation for the height of the fluid in a simple, straight capillary with perfect wetting (contact angle = 0) :
h = (2.sigma) / ( (Rhl - Rha) . g . Rcap)

sigma = surface tension
Rhl = density of liquid
Rha = density of air
g = 9.81 N/kg
Rcap = radius of capillary

*The Young-Laplace equiation
Pi - Po = sigma (1/R1 + 1/R2)

Pi = pressure inside
Po = pressure outside
sigma = surface tension
R1 and R2 are the principal radii of curvature at the interface
(see also wikipedia : young-laplace equation)

The Attempt at a Solution



Case a : is possible, I think. One can imagine a fluid for which the height in a capillary with the thickest radius would be higher than the point where the radius gets smaller. In this case, the fluid would keep rising in the smaller radius (because smaller radius means higher fluid) with the result as given in the figure.
I think the height in this case would be
h = (2.sigma) / ( (Rhl - Rha) . g . Rcap) with Rcap the smallest of the two radii, because the pressure at a point in the fluid is (Rhl - Rha) . g . h with h the distance to the surface, and the pressure difference given by young-laplace is (2.sigma) / Rcap

Case b and c : I'm not sure about these ones, I would say they are possible too, with the same explanation as above, but then I don't really get the point of the question, if they are all possible. Or am I missing something? I was thinking about a situation where laplace-young would predict the pressure to rise when you go up the capillary, which would be impossible?

Can someone please help with this one? I am thinking about it for quite some time now...

Thanks,

Kristof
 

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Do not multiple-post questions across forums. I'm leaving this post here in Advanced Physics for now, and I deleted the duplicate post in Intro Physics.
 
ok, that's fine, I didn't really now where to put it
 
anyone to help, please?
 

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