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Lesson 4 of 4

Surface tension and capillarity.

About 20 minutes · 6 practice questions

A liquid that climbs a thin tube with no pump: surface tension and the glass's pull, why a tube half as wide holds a column twice as tall, Jurin's law, mercury that sinks, and why capillary action alone can't lift water to the top of a tree.

Step 1 of 6 · A liquid that climbs

Step 1 of 6

A liquid that climbs

Stand a thin glass tube in a glass of water and the water inside rises above the water outside. No pump, no suction: the liquid simply climbs and stops. This is capillary action, and it is why a paper towel soaks up a spill and a sugar cube drinks coffee from the bottom up. The Scene has a wide vessel joined at the bottom to three thin tubes, each twice as wide as the one before.

Try it: choose Molecules under Zoom to the molecules. The molecule inside the liquid is pulled equally every way; the one at the surface is not pulled upward, so its pulls add up to one arrow pointing in.

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Step 2 of 6

The tube’s width

The surface’s pull along the rim grows with the tube’s circumference, 2πr2\pi r⁠. The water it has to lift grows with the area of the section, πr2\pi r^2⁠. The Liquid is fixed now: Water.

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Step 3 of 6

Jurin’s law

The column stops where the pull along the rim holds up exactly the weight of the raised water. That is Jurin’s law:

h=2γcos⁡θρgrh = \frac{2\gamma\cos\theta}{\rho g r}⁠

γ\gamma⁠ is the surface tension, the force along each metre of the surface’s edge, in N/m. θ\theta⁠ is the contact angle, the angle at which the liquid’s surface meets the glass; ρ\rho⁠ is the liquid’s density and rr⁠ the tube’s inner radius. Water’s surface tension is unusually high, which is why a carefully placed paper clip can rest on water without sinking. Both Parameters are fixed now.

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Step 4 of 6

Forty millimetres

Now you can change the Narrowest tube.

Try it: after answering, choose Soapy water under Liquid. The soap gathers at the surface and weakens its pull, and the columns climb less than half as high.

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Step 5 of 6

Mercury

Not every liquid climbs. What decides is which pulls harder: the glass on the liquid’s molecules, or the liquid on itself. Glass pulls water nearly as hard as water pulls itself, so water wets glass. Mercury is a liquid metal, and its atoms pull on each other very hard.

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Step 6 of 6

Trees

Capillary action carries ink along the fibres of paper, lifts melted wax up a candle’s wick, and draws water through the gaps in soil. But trees grow tens of metres tall.

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Still of the Surface tension and capillarity 3D scene
Interactive scene

Loading the interactive version…

Each step sets up the Scene for you, and a control marked “fixed” stays put for that step.

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Practice · Choose

The water climbs the thin tubes above the level in the wide vessel, with no pump. What lifts it?

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Practice · Predict, then look

Narrowest tube is 1 mm. It is changed to 0.5 mm. Predict: what will happen to the height of its column?

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Practice · Calculate

Use Jurin’s law to work out how high Water climbs in a tube 1 mm across inside. Water’s surface tension is 0.0728 N/m, its density 998 kg/m³, and it wets glass completely, θ=0°\theta = 0^\circ⁠. Take g = 9.81 m/s².

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Practice · Reach the target

Change the Narrowest tube until the water climbs 40 mm above the level in it.

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Practice · Predict, then look

The Liquid is changed to Mercury. Predict: what will happen in the tubes?

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Practice · Choose

The water-carrying vessels in a tree are about 0.04 mm wide. Can capillary action alone lift water to the top of a 30 m tree?