Use contact geometry to predict capillary rise or depression
Cohesion refers to attraction between molecules of the same material; adhesion refers to attraction across different materials. Surface tension γ is force per length, with units N/m. It describes the tendency of an interface to reduce area. It is not the same quantity as pressure, although a curved interface can sustain a pressure difference.
Learning outcome: Compare contact angles 0°, 90° and 120° at two radii. Retain signed height and signed vertical surface force, and explain why using the absolute value of cosine would destroy the physical distinction.
Starting recap
Declare density, pressure reference, flow regime and admissible force constraints. Convert area and volume units before balancing forces, mass or energy.
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At radius 0.5 mm and contact angle 0°, the capillary rise is 0.024 m. At the same radius and 120° the depression is −0.012 m.
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For the stated angle convention, a contact angle above 90° predicts:
Experiment
Compare contact angles 0°, 90° and 120° at two radii. Retain signed height and signed vertical surface force, and explain why using the absolute value of cosine would destroy the physical distinction.
Resolve the sign and geometry of capillary displacement
Worked teaching model · synthetic values · Ideal static cylindrical capillary, surface tension .06 N/m, liquid density 1000 kg/m³, g=10. Contact angle is measured through liquid. Signed height relative to a broad reservoir; ignore meniscus volume and molecular-scale corrections. Virtual only.
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Rise or depression versus contact angle
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: ideal capillary balance (solid). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Rise or depression versus contact angle
ideal capillary balance
| contact angle (degrees) | signed height (m) |
|---|---|
| 0 | 0.012 |
| 3 | 0.0119836 |
| 6 | 0.0119343 |
| 9 | 0.0118523 |
| 12 | 0.0117378 |
| 15 | 0.0115911 |
| 18 | 0.0114127 |
| 21 | 0.011203 |
| 24 | 0.0109625 |
| 27 | 0.0106921 |
| 30 | 0.0103923 |
| 33 | 0.010064 |
| 36 | 0.0097082 |
| 39 | 0.00932575 |
| 42 | 0.00891774 |
| 45 | 0.00848528 |
| 48 | 0.00802957 |
| 51 | 0.00755184 |
| 54 | 0.00705342 |
| 57 | 0.00653567 |
| 60 | 0.006 |
| 63 | 0.00544789 |
| 66 | 0.00488084 |
| 69 | 0.00430042 |
| 72 | 0.0037082 |
| 75 | 0.00310583 |
| 78 | 0.00249494 |
| 81 | 0.00187721 |
| 84 | 0.00125434 |
| 87 | 0.000628031 |
| 90 | 0 |
| 93 | -0.000628031 |
| 96 | -0.00125434 |
| 99 | -0.00187721 |
| 102 | -0.00249494 |
| 105 | -0.00310583 |
| 108 | -0.0037082 |
| 111 | -0.00430042 |
| 114 | -0.00488084 |
| 117 | -0.00544789 |
| 120 | -0.006 |
At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.
| Quantity | Value | Unit |
|---|---|---|
| Signed capillary height | 0.006 | m |
| Vertical surface-tension resultant | 0.000188496 | N |
| Signed hydrostatic column force | 0.000188496 | N |
| Contact-angle cosine | 0.5 | ratio |
Wetting geometry sets the sign; the narrower tube magnifies the signed capillary displacement.
Balance 2 pi r gamma cos(theta)=rho g pi r² h. Contact angle below 90 degrees gives rise, above it gives depression. Cohesion describes attraction within a liquid and adhesion across different materials. Surface tension has units N/m, not pressure; meniscus curvature can nevertheless produce a pressure difference.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
Wetting geometry sets the sign; the narrower tube magnifies the signed capillary displacement.
Balance 2 pi r gamma cos(theta)=rho g pi r² h. Contact angle below 90 degrees gives rise, above it gives depression. Cohesion describes attraction within a liquid and adhesion across different materials. Surface tension has units N/m, not pressure; meniscus curvature can nevertheless produce a pressure difference.
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Why does an attraction-based microscopic explanation still require a specified macroscopic contact angle?
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