Conversation started May 15, 2020 at 10:34.
May 15, 2020 10:34
2
Q: Why don't we include the adhesive and cohesive force while calculating rise in a capillary tube?

GerardThe contact angle of a liquid solid interface is explained by saying that the liquid surface must be perpendicular to the resultant of adhesive cohesive and gravitational forces acting on it, since it cannot sustain shear stresses. However, once the contact angle is determined, the cohesive and...

Do you have an alternate answer for the above question sir?
Particularly, I feel, I'm having the same doubt as the following comment:
I understand your point, the adhesive and cohesive forces play a role in determining the contact angle but surely that is not the end of the story. While writing Newton's Second Law for the fluid column why are we justified in omitting them even though they are at work? In the energy approach you illustrated, there would be some potential energy associated with these forces as well which has seemingly been omitted. Why? — Gerard Oct 23 '15 at 5:33
I'm not sure I understand what Gerard is asking
Did you read the question sir? I think the comment alone is not self understandable.
Or let me explain:
As per Jurin's law,
$$h=\frac{2S\cos\theta}{r\rho g}$$
Why aren't cohesive and adhesive forces involved in the derivation of the above formula?
How can it be self-contained in the contact angle term sir?
They are included. The angle $\theta$ depends on the cohesive and adhesive forces.
Yes sir. I understand. But I don't see why is $S$ involved here. My book states the free surface attracts the tube and this is a consequence of Newton's third law.
Why wouldn't S be involved?
I just don't understand the problem.
May 15, 2020 10:43
Because it's just the force within the fluid molecules. The force between the liquid surface and the tube is adhesive force and not surface tension as per my understanding.
Have you seen the derivation of the contact angle?
Derivation? No sir. I thought it was experimentally determined.
Let me draw a diagram ...
So is the $\cos\theta$ term inversely proportional to $S$ in some way?
May 15, 2020 10:49
@JohnRennie Only thing I know about it is this - the contact angle must be in such a way that the net force (adhesive+cohesive+gravitational) must be perpendicular (normal) to the tangential plane of the free surface of the liquid.
All interfaces have a surface tension because the surface tension is just the interfacial energy in disguise.
So when we look at the point where the liquid, air and solid all meet there are three forces acting as I've drawn. OK so far?
@JohnRennie Ok sir. I think I have a terminology doubt - Isn't the force between solid and liquid and liquid with non-surface liquid molecules called as adhesive and cohesive forces respectively rather than surface tension?
No. The terms adhesive and cohesive forces are rather vague while surface tension is precisely defined.
Or a colloid scientist might also use the term interfacial energy because the interfacial energy and the surface tension are the same thing.
Fine. I didn't know that. This seems new to me.
I can prove it if you want ...
Prove that interfacial energy and the surface tension are the same thing I mean.
May 15, 2020 10:55
@JohnRennie Another doubt before I say ok : Why are the two horizontal forces horizontal? In the explanation of contact angles, the adhesive/cohesive forces weren't normal or parallel to the interface.
Because surface tension always acts in the plane of the interface.
Ok sir. Now I think cohesive/adhesive forces are much different than interfacial energy.
@JohnRennie But aren't they dimensionally inconsistent? One is force per unit length and the other is energy.
Dimensionally inconsistent eh? :-)
Shall we check?
Ok sir. I think I pressed the wrong switch :-)
(interfacial energy is energy per unit area not just energy)
May 15, 2020 10:59
I agree. Surface energy per area is surface tension. Yes it's consistent dimensionally. Misinterpreted energy as pure energy.
Fine sir :-)
If you wish shall we proceed regarding the main question?
6 mins ago, by John Rennie
Prove that interfacial energy and the surface tension are the same thing I mean.
OK, consider a soap film held inside a wire frame. I'll use this as an example because it's the sort of thing we've all played with so it should be intuitive. I'll draw a diagram:
@GuruVishnu there. The light blue area is the soap film.
Ok sir. The blue rod is movable right?
The blue line is a sliding wire that we can pull outwards a distance $dx$ to stretch the film.
May 15, 2020 11:07
Ok sir. I saw this setup to find the surface energy of a soap film.
In that case you've done the calculation!
Yes sir. Now I see interfacial energy you meant is same as the surface energy I referred to. However:
13 mins ago, by John Rennie
Prove that interfacial energy and the surface tension are the same thing I mean.
That's what I'm about to do.
Ok sir :-)
Let's call the length of the wire $\ell$. Calling it $d$ was a poor choice because that's going to get confused with the $dx$.
May 15, 2020 11:10
Ok sir. Just to simplify things - Are we going to obtain $U/A=S$?
If yes, we can definitely skip this step.
So if we pull the wire a distance $dx$ we create a new area of soap film $dA = \ell dx$, and the increase in energy is $EdA = E\ell dx$ where $E$ is the energy per unit area. OK so far?
I was just wondering how could $U$ and $S$ have the same dimensions if the interfacial energy and surface energy meant the same thing.
@JohnRennie Yes sir.
$U$ is the total energy?
i.e. in my notation $U = EA$ ?
Increase in surface energy. I missed a $\Delta$ sir because HCV didn't mention it. I thought it was some kind of convention.
But he uses this interchangeably.
OK. Anyhow the working is trivial. The increase in energy has to come from the work done $E\ell dx = dW = Fdx$
May 15, 2020 11:13
Finally he says: We see that the surface tension of a liquid is equal to the surface energy per unit surface area.
And $F = S\ell$
So we end up with $E=S$
instead of increase in surface energy per unit surface area.
@JohnRennie Ok sir. So is $E=U/A$ or in English: Interfacial energy equal to the surface energy per unit area? I see it's just surface tension then. Just a new term to be stored in memory.
Apart from the forces being along the surface, especially the horizontal ones, I find it's ok to proceed sir:
26 mins ago, by John Rennie
user image
It's trivial from here. The horizontal component of the total force at the junction must be zero because if it wasn't zero the liquid would flow left or right depending on the total force.
So we get:
$$ \gamma_{sa} = \gamma_{ls} + \gamma_{la}\cos\theta $$
Rearrange to get $\cos\theta$
May 15, 2020 11:20
Ok sir. Just for confirmation: Is $\gamma_{sa}$ adhesive, $\gamma_{ls}$ cohesive and $\gamma_{la}$ surface tension sir?
No
$\gamma_{sa}$ is the surface tension of the solid-air interface, which is probably easier to understand as the interfacial energy of the solid-air interface.
This is related to cohesion.
Fine sir. It also solved the mystery why it's parallel to the surface :-)
Imagine taking a block of the solid and splitting it along a plane of area $A$. So where we had a solid-solid interface of area $A$ we now have two solid-air interfaces of area $A$.
So all the $\gamma$ terms are just the surface tensions of appropriate phases on either sides like solid/gas or solid/liquid, and so on.
May 15, 2020 11:24
Ok sir. It seems we're just transforming the components of cohesive and adhesive forces to surface tensions. Similar to expressing 5 m/s of velocity in the first quadrant as 3i +4j. Is this a correct inference sir?
Basically yes
Ok sir. Thank you :-)
But, the following doesn't seem to hold true:
42 mins ago, by Guru Vishnu
So is the $\cos\theta$ term inversely proportional to $S$ in some way?
It needs $\gamma_{ls}=S$ to be satisfied...
@GuruVishnu $S$ is what I've called $\gamma_{la}$. Yes?
So our equation for the contact angle is:
$$ \gamma_{sa} = \gamma_{ls} + S\cos\theta $$
$$ \cos\theta = \frac{\gamma_{sa} - \gamma_{ls}}{S} $$
$\cos\theta$ is indeed inversely proportional to $S$ if the other two surface tensions are constant.
Ok sir. Fine. That was an error from my side when I switched from one set of terminologies to the other. I understood this completely. And the modified Jurin's law is as per my initial expectation, independent of $S$:
$$h=\frac{2(\gamma_{sa}-\gamma_{ls})}{r\rho g}$$
and has the cohesive and adhesive terms hidden inside the surface tension terms.
Thank you very much sir :-)
May 15, 2020 11:43
:-)
 
Conversation ended May 15, 2020 at 11:43.