In surface science, the du Noüy ring method is a technique for measuring the surface tension of a liquid. The method involves slowly lifting a ring, often made of platinum, from the surface of a liquid. The force, F, required to raise the ring from the liquid's surface is measured and related to the liquid's surface tension γ:

${\displaystyle F=w_{\text{ring}}+2\pi \cdot (r_{\text{i}}+r_{\text{a}})\cdot \gamma ,}$

where r_i is the radius of the inner ring of the liquid film pulled, and r_a is the radius of the outer ring of the liquid film.^[1] w_ring is the weight of the ring minus the buoyant force due to the part of the ring below the liquid surface.^[2]

When the ring's thickness is much smaller than its diameter, this equation can be simplified to

${\displaystyle F=w_{\text{ring}}+4\pi R\gamma ,}$

where R is the average of the inner and outer radius of the ring, i.e. ${\displaystyle (r_{\text{i}}+r_{\text{a}})/2.}$^[2]

This technique was proposed by the French physicist Pierre Lecomte du Noüy (1883–1947) in a paper published in 1925.^[3]

Close up of the ring drawn out of the liquid

The measurement is performed with a force tensiometer, which typically uses an electrobalance to measure the excess force caused by the liquid being pulled up and automatically calculates and displays the surface tension corresponding to the force. Earlier, torsion wire balances were commonly used. The maximum force is used for the calculations, and empirically determined correction factors are required to remove the effect caused by the finite diameter of the ring:

${\displaystyle F=w_{\text{ring}}+4\pi R\gamma f,}$

with f being the correction factor.

The most common correction factors include those by Zuidema and Waters (for liquids with low interfacial tension), Huh and Mason (which covers a wider range than Zuidema–Waters), and Harkins and Jordan (more precise than Huh–Mason, while still covering the most widely used liquids).^[4]

The surface tension and correction factors are expressed by

${\displaystyle \gamma ={\frac {F}{4\pi R}}f,}$

where γ is surface tension, R is the average diameter of the ring, and f is correction factor.

Zuidema and Waters^[2]

${\displaystyle (f-a)^{2}={\frac {4b}{\pi ^{2}}}{\frac {1}{R^{2}}}{\frac {\gamma _{\text{measured}}}{\rho _{\text{lower}}-\rho _{\text{upper}}}}+C,}$

where

F = maximum pull of rings [dyn/cm],

ρ = density of the lower and upper phases,

${\displaystyle C=0.04534-1.679{\frac {r}{R}},}$

a = 0.7250,

b = 0.0009075 [s²⋅cm⁻¹],

r = Du Noüy wire radius,

R = Du Noüy ring radius.

Huh & Mason^[5][6]

The correction factor is described as a function of ${\displaystyle {\tfrac {R}{r}}}$ and ${\displaystyle {\tfrac {R^{3}}{V}}.}$ See the references.

Harkins and Jordan^[7][8]

The correction factor is tabulated as a function of ${\displaystyle R/r}$ and ${\displaystyle R^{3}/V}$; see the references.

See also

A classical torsion wire-based du Noüy ring tensiometer. The arrow on the left points to the ring itself.

• Sessile drop technique
• Wilhelmy plate

References

External links

Wikimedia Commons has media related to Du Noüy ring method.

• Video showing a classical torsion wire du Noüy tensiometer
• Picture of a classical torsion wire du Noüy tensiometer (National Institutes of Health)