chapter 8 surface phenomena and dispersion system 8.1 surface tension

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Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

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Page 1: Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

Chapter 8

Surface phenomena and dispersion system

8.1 Surface tension

Page 2: Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

Liquid

vapor

Interface

Supercritical fluid

Capillary action

Page 3: Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

Surface: The boundary between non-gaseous phases and

vacuum. The boundary between liquid or solid phase and

their vapors can be approximated as Surface.

In other cases, the boundary is interface.

Two important concepts

Surface and Interface

So far, we have only considered bulk properties of

materials. In this section, the surface / interface properties of

pure liquid/vapor, solution surface and solid / gas interface

will be treated.

Page 4: Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

1. Some surface phenomena

Nickel-floating on Shuyu Spring, Jinan

1) Nickel-floating

Page 5: Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

A nickel floating on water surface

Once immersed in water, the nickel would sink at once.

?

Buoyancy

Gravity

Page 6: Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

Why do the bubbles formed due to turbulence/torrent disappear immediately?

Page 7: Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

2. Micro-mechanism of surface tension: Unbalanced force and surface tension

A net attractive force exists for molecules at the surface.

Page 8: Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

The energy of a molecule at the surface is higher

than that in the interior

Surface area enlargement

To move molecules toward the surface, i.e., enlarge the surface area, energy must be expended.

dAW '

dAW '

Page 9: Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

3. Theoretical definition of the surface tension

dAW ' dAW '

For reversible process:

,' T pW dG ,T p

G

A

is the excess energy per m2 possessed by the surface. specific surface energy.

Its unit is J m-2 = N m-1, which can be taken as the force exerted on unit length. surface tension

Page 10: Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

dAdG

The energy of the surface increases with the enlargement of the surface area.

B

BBdndAVdPSdTdG

At constant temperature and pressure:

-W = dA is another kind of useful energy.

Page 11: Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

Why are free water droplets always in ball shape.

Page 12: Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

1. capillary rise

2. maximum bubble pressure

3. ring method

4. drop weight method

5. Wilhelmy slide method

6. the shape of drops or bubbles

7. flow method

8. capillary waves method, etc.

5 Measurement of surface tension:

Page 13: Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

Wilhelmy slide method

Slide l

Soap film

ldxA 2

ldxAW 2

FdxW

l

F

2

Page 14: Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

maximum bubble pressure

Page 15: Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

6 Influential Factors on surface tension

0,,

BnPAT

Surface tension decreases with the increase of temperature.

1) temperature

temperature dependence of surface tension

T / oC H2O C6H6 CH3OH C2H5OH

0 75.64 31.6 29.5 24.0

25 71.94 28.2 27.1 21.8

50 67.91 25.0 24.6 19.8

70 63.5 21.9 22.0

Page 16: Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

Surface tension decreases with increasing temperature.

At critical temperature (Tc), surface tension equals 0.

The empirical equation proposed by Eotvos and modified by Ramsay and Shields :

)0.6(3/2 TTkV cm

Vm is the molar volume of the liquid, k is a proportional fact

or, for non-polar liquid, equals 2.2 10-7 J K-1.

Page 17: Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

B

BBdndAVdPSdTdG

BB nPAnPT TA

S

,,,,

BB nPAnPT TT

A

ST

,,,,

0,,

BnPTA

ST is the heat adsorbed by unit area enlargement.

Adiabatic expansion of surface area will result in temperature decrease.

0,,

BnPA

TT

0

,,

BnPAT

As temperature increases, surface tension decreases.

Page 18: Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

2) co-existing phase dependence of surface tension

Surface tension of water at 20 oC contacting with different liquids.

vapor iso-pentane benzene butanol

72.8 49.6 32.6 6.8

Antonow law

'' 212,1 '', BWBW

Saturated with benzene

Saturated with water

Page 19: Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

Because the intermolecular interaction between liq

uid molecules is small, the interface tension is usually

less than 80 mN m-1.

Substances Substance

Hg / 20 oC 486.5 NaCl 400

Fe / m. p. 1880 MgO 1200

NaNO3/308 116.6 mica 2400-5400

3) nature

Page 20: Chapter 8 Surface phenomena and dispersion system 8.1 Surface tension

discussion

1) Can you compare the surface tension of two liquids

by examination of drop / bubble shape?

2) For the charged surface, will the surface tension

increase or decrease?