Capillary length

The pressure of a static fluid does not depend on the shape, total mass or surface area of the fluid. It is directly proportional to the fluid's specific weight—the force exerted by gravity over a specific volume, and its vertical height. However, a fluid also experiences pressure that is induced by surface tension, commonly referred to as the Young–Laplace pressure. Surface tension originates from cohesive forces between molecules, and in the bulk of the fluid, molecules experience attractive forces from all directions. The surface of a fluid is curved because exposed molecules on the surface have fewer neighboring interactions, resulting in a net force that contracts the surface. There exists a pressure difference either side of this curvature, and when this balances out the pressure due to gravity, one can rearrange to find the capillary length.

In the case of a fluid–fluid interface, for example a drop of water immersed in another liquid, the capillary length denoted ${\displaystyle {\lambda }_{\mathrm{c}}}$ or ${\displaystyle l_{\mathrm{c}}}$ is most commonly given by the formula,

${\displaystyle {\lambda }_{\mathrm{c}}=\sqrt{\frac{\gamma }{\mathrm{\Delta }\rho g}}}$,

where ${\displaystyle \gamma }$ is the surface tension of the fluid interface, ${\displaystyle g}$ is the gravitational acceleration and ${\displaystyle \mathrm{\Delta }\rho }$ is the mass density difference of the fluids. The capillary length is sometimes denoted ${\displaystyle {\kappa }^{-1}}$ in relation to the mathematical notation for curvature. The term capillary constant is somewhat misleading, because it is important to recognize that ${\displaystyle {\lambda }_{\mathrm{c}}}$ is a composition of variable quantities, for example the value of surface tension will vary with temperature and the density difference will change depending on the fluids involved at an interface interaction. However if these conditions are known, the capillary length can be considered a constant for any given liquid, and be used in numerous fluid mechanical problems to scale the derived equations such that they are valid for any fluid. For molecular fluids, the interfacial tensions and density differences are typically of the order of ${\displaystyle 10-100}$ mN m⁻¹ and ${\displaystyle 0.1-1}$g mL⁻¹ respectively resulting in a capillary length of ${\displaystyle \sim 3}$mm for water and air at room temperature on earth. On the other hand, the capillary length would be ${\displaystyle \lambda c=6.68}$mm for water-air on the moon. For a soap bubble, the surface tension must be divided by the mean thickness, resulting in a capillary length of about ${\displaystyle 3}$ meters in air! The equation for ${\displaystyle {\lambda }_{\mathrm{c}}}$ can also be found with an extra ${\displaystyle \sqrt{2}}$ term, most often used when normalising the capillary height.

Origin

Theoretical

One way to theoretically derive the capillary length, is to imagine a liquid droplet at the point where surface tension balances gravity.

Let there be a spherical droplet with radius ${\displaystyle {\lambda }_c}$,

The characteristic Laplace pressure ${\displaystyle P_{\gamma }}$, due to surface tension, is equal to

${\displaystyle P_{\gamma }=2\frac{\gamma }{{\lambda }_{\mathrm{c}}}}$,

where ${\displaystyle \gamma }$ is the surface tension. The pressure due to gravity (hydrostatic pressure) ${\displaystyle P_{\mathrm{h}}}$ of a column of liquid is given by

${\displaystyle P_{\mathrm{h}}=\rho gh=2\rho g{\lambda }_{\mathrm{c}}}$,

where ${\displaystyle \rho }$ is the droplet density, ${\displaystyle g}$ the gravitational acceleration, and ${\displaystyle h=2{\lambda }_{\mathrm{c}}}$ is the height of the droplet.

At the point where the Laplace pressure balances out the pressure due to gravity ${\displaystyle P_{\mathrm{h}}=P_{\gamma }}$,

${\displaystyle {\lambda }_{\mathrm{c}}=\sqrt{\frac{\gamma }{\rho g}}}$.

Relationship with the Eötvös number

The above derivation can be used when dealing with the Eötvös number, a dimensionless quantity that represents the ratio between the gravitational forces and surface tension of the liquid. Despite being introduced by Loránd Eötvös in 1886, he has since become fairly dissociated with it, being replaced with Wilfrid Noel Bond such that it is now referred to as the Bond number in recent literature.

The Bond number can be written such that it includes a characteristic length- normally the radius of curvature of a liquid, and the capillary length

${\displaystyle \mathrm{B}\mathrm{o}=\frac{\mathrm{\Delta }\rho g{L}^2}{\gamma }}$,

with parameters defined above, and ${\displaystyle L}$ the radius of curvature.

Therefore the bond number can be written as

${\displaystyle \mathrm{B}\mathrm{o}={\left(\frac{L}{{\lambda }_{\mathrm{c}}}\right)}^2}$,

with ${\displaystyle {\lambda }_{\mathrm{c}}}$ the capillary length.

If the bond number is set to 1, then the characteristic length is the capillary length.

Experimental

The capillary length can also be found through the manipulation of many different physical phenomenon. One method is to focus on capillary action, which is the attraction of a liquids surface to a surrounding solid.

Association with Jurin's law

Jurin's law is a quantitative law that shows that the maximum height that can be achieved by a liquid in a capillary tube is inversely proportional to the diameter of the tube. The law can be illustrated mathematically during capillary uplift, which is a traditional experiment measuring the height of a liquid in a capillary tube. When a capillary tube is inserted into a liquid, the liquid will rise or fall in the tube, due to an imbalance in pressure. The characteristic height is the distance from the bottom of the meniscus to the base, and exists when the Laplace pressure and the pressure due to gravity are balanced. One can reorganize to show the capillary length as a function of surface tension and gravity.

${\displaystyle {\lambda }_{\mathrm{c}}^2=\frac{hr}{2\cos \theta }}$,

with ${\displaystyle h}$ the height of the liquid, ${\displaystyle r}$ the radius of the capillary tube, and ${\displaystyle \theta }$ the contact angle.

The contact angle is defined as the angle formed by the intersection of the liquid-solid interface and the liquid–vapour interface. The size of the angle quantifies the wettability of liquid, i.e., the interaction between the liquid and solid surface. A contact angle of ${\displaystyle \theta =0}$ can be considered, perfect wetting.

${\displaystyle {\lambda }_{\mathrm{c}}^2=\frac{hr}{2}}$.

Thus the ${\displaystyle {\lambda }_{\mathrm{c}}^2}$ forms a cyclical 3 factor equation with ${\displaystyle r,h}$.

This property is usually used by physicists to estimate the height a liquid will rise in a particular capillary tube, radius known, without the need for an experiment. When the characteristic height of the liquid is sufficiently less than the capillary length, then the effect of hydrostatic pressure due to gravity can be neglected.

Using the same premises of capillary rise, one can find the capillary length as a function of the volume increase, and wetting perimeter of the capillary walls.

Association with a sessile droplet

Another way to find the capillary length is using different pressure points inside a sessile droplet, with each point having a radius of curvature, and equate them to the Laplace pressure equation. This time the equation is solved for the height of the meniscus level which again can be used to give the capillary length.

The shape of a sessile droplet is directly proportional to whether the radius is greater than or less than the capillary length. Microdrops are droplets with radius smaller than the capillary length, and their shape is governed solely by surface tension, forming a spherical cap shape. If a droplet has a radius larger than the capillary length, they are known as macrodrops and the gravitational forces will dominate. Macrodrops will be 'flattened' by gravity and the height of the droplet will be reduced.