Surface Tension and force required to pull a thin ring

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Discussion Overview

The discussion revolves around the force required to pull a circular glass plate from the surface of water and how this scenario changes when the plate is instead in mercury. Participants explore the implications of surface tension, adhesion, and cohesion in these contexts, questioning the assumptions made in a numerical example problem related to surface tension.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • One participant suggests that the force required to remove a glass plate from water is high due to strong adhesive forces between water molecules and glass, while in mercury, the lack of adhesion would result in less force needed.
  • Another participant questions whether the original problem adequately considered the adhesion between water and the plate, implying that it may have oversimplified the situation by focusing solely on cohesive effects.
  • A different participant points out that without seeing the complete problem, it is unclear where misunderstandings may lie, noting that using a circular ring to measure interfacial energy is a common practice.
  • One participant emphasizes that the problem is poorly posed, making several assumptions, and highlights the complexities involved in separating the disc from the fluid, including the movement of the contact line and the pressure jump across the air-fluid interface.
  • Concerns are raised about the neglect of the pressure jump that occurs when the disc is pulled, suggesting that the initial force required may be much greater than indicated by the problem.

Areas of Agreement / Disagreement

Participants express differing views on the assumptions made in the numerical example problem, with some agreeing that it oversimplifies the situation while others seek clarification on specific aspects. No consensus is reached regarding the implications of adhesion and cohesion in the context of the problem.

Contextual Notes

Participants note that the problem lacks explicit assumptions regarding adhesive forces and does not account for the complexities of contact line motion and pressure changes, which may significantly affect the required force.

Ahsan Khan
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Hi everyone,

While studying surface tension I came across a(numerical example) problem which asks to find the force required to pull a circular glass plate of some given radius from the surface of water(assume plane of plate on water surface). Value of surface tension of water is also given in problem. The solution was done by simply multiplying surface tension of water with length of circumference. And it ends.

Now what I am thinking is that what would be the solution if instead of water the circular plate were in mercury which do not stick on glass. Since mercury does not stick(wet) on glass (as cohesive force of mercury molecules is much greater than adhesive force between mercury and glass) therefore no or very little force should be required to remove plate from mercury than that required for glass. The force required to remove glass plate from water would be high because molecules of water strongly holding the glass and will not leave it so force is required to break cohesive force of water that is surface tension of water. But in case of mercury, mercury molecules do not hold glass so tightly therefore while trying to remove plate from mercury, the mercury molecules leave the plate even when the applied force is less than that required to break the cohesive force between mercury molecules.

This is what I suppose. Is my understanding true?

Regards!
Thanks a bunch.
 
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You seem to be wondering if the example problem was perhaps being a little simplistic - did they neglect the adhesion between water and the plate, considering only cohesive effects? In Mercury, the surface tension would be higher because of the cohesion is higher, but adhesion to the plate would be lower.

You should look at the rest of the passage before the example to see what assumptions they used in the problem, and see if you can investigate how surface tension relates to adhesion.
 
ovais said:
Hi everyone,

While studying surface tension I came across a(numerical example) problem which asks to find the force required to pull a circular glass plate of some given radius from the surface of water(assume plane of plate on water surface). Value of surface tension of water is also given in problem. The solution was done by simply multiplying surface tension of water with length of circumference. And it ends.

Without seeing the problem it's unclear where the misunderstanding is. For example, using a circular *ring* to measure interfacial energy is common (https://en.wikipedia.org/wiki/Du_Noüy_ring_method) as is using a rectangular plate (https://en.wikipedia.org/wiki/Wilhelmy_plate), neither of which seems to correspond to your problem.
 
Simon Bridge said:
You seem to be wondering if the example problem was perhaps being a little simplistic - did they neglect the adhesion between water and the plate, considering only cohesive effects?

Exactly.

Simon Bridge said:
You should look at the rest of the passage before the example to see what assumptions they used in the problem, and see if you can investigate how surface tension relates to adhesion.

The problem is, the complete passage of question is not mentioning any assumption but just solved ignoring how (less)adhesive force can affect the answer.

Below is the example problem with its solution:

Regards
 

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ovais said:
Exactly.



The problem is, the complete passage of question is not mentioning any assumption but just solved ignoring how (less)adhesive force can affect the answer.

Below is the example problem with its solution:

Regards

Thanks for posting the actual question: this is a poorly-posed problem that makes several badly-conceived assumptions. For example, as the disc is pulled up two things can happen. If the disc is non-wetting, the contact line must move across the face of the disc (dewetting) in order to separate the disc from fluid. If the disc is wetting, there will be some mass of fluid that remains attached to the disc (pendant drop). While drop necking/rupture process is mostly understood, contact line motion is not. Neither process can be ignored.

Even if the question is restricted to an initial raising force, the calculation neglects the pressure jump that occurs across the curved air-fluid interface.- the pressure jump will be very high initially, resulting in a force much greater than your question indicates. For some reason I think this type of measurement has been performed and published, it's related to capillary pressure and applied to multiphase flow problems.
 

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