双语化学辞典Chem Lexicon
概念 · 表面化学 · 界面现象 Surface chemistry · Interfacial phenomena

表面张力Surface tension

拼音Pinyin biǎo miàn zhāng lì 别名Also 表面自由能;界面张力;surface free energy; interfacial tension

定义Definition

表面张力是液体表面层中沿表面作用、使表面积趋于最小的收缩力,数值上等于增加单位表面积所需做的可逆功(表面自由能),单位为 N/m 或 J/m²,常用 mN/m。25 °C 时水的表面张力约为 72 mN/m。

Surface tension is the contracting force acting along a liquid surface that tends to minimise its area; numerically it equals the reversible work needed to create unit area of new surface (the surface free energy), in N/m or J/m², usually quoted in mN/m. Water's surface tension is about 72 mN/m at 25 °C.

原理Principle

液体内部的分子受到周围分子各方向的吸引,合力为零;表面分子只受到内侧和侧面分子的吸引,合力指向液体内部,因此表面分子能量更高。液体总是倾向于减小表面积,所以小液滴呈球形。分子间作用力越强,表面张力越大:汞(约 485 mN/m)>水(72)>乙醇(22)。温度升高,表面张力降低,到临界温度时为零。

A molecule inside a liquid is pulled equally in all directions, but one at the surface is pulled only inward and sideways, so surface molecules have higher energy. A liquid therefore minimises its surface, which is why small drops are spherical. Stronger intermolecular forces mean higher surface tension: mercury (about 485 mN/m) > water (72) > ethanol (22). Surface tension falls with temperature and vanishes at the critical point.

相关方程Key equations

杨-拉普拉斯方程 Δp = 2γ/r 给出弯曲液面内外的压力差,解释了小气泡内压更大和毛细现象(毛细上升高度 h = 2γcosθ/(ρgr))。杨氏方程 γ_SG = γ_SL + γ_LG·cosθ 描述接触角与润湿:θ < 90° 为润湿,θ > 90° 为不润湿,荷叶表面 θ > 150° 为超疏水。开尔文方程说明小液滴的蒸气压比平面液体高,这是过饱和与奥斯特瓦尔德熟化的原因。吉布斯吸附方程把溶质的表面吸附量与表面张力随浓度的变化联系起来。

The Young–Laplace equation Δp = 2γ/r gives the pressure difference across a curved surface, explaining why small bubbles have higher internal pressure and capillary rise, h = 2γcosθ/(ρgr). Young's equation γ_SG = γ_SL + γ_LG·cosθ links contact angle to wetting: below 90° a liquid wets, above 90° it does not, and lotus leaves exceed 150°, superhydrophobic. The Kelvin equation shows small drops have higher vapour pressure than flat liquid, the cause of supersaturation and Ostwald ripening. The Gibbs adsorption equation relates a solute's surface excess to how surface tension changes with concentration.

历史与应用History and applications

1805 年杨和拉普拉斯分别建立了毛细现象的理论;1878 年吉布斯建立了界面热力学;1891 年波克尔斯在家中厨房发明了测量表面张力的槽法,为朗缪尔膜天平奠定基础。表面张力现象应用于洗涤、喷墨打印、泡沫和乳液稳定、矿物浮选、微流控和防水涂层,水黾能在水面行走也依靠它。

Young and Laplace independently developed the theory of capillarity in 1805, and Gibbs founded interfacial thermodynamics in 1878. In 1891 Agnes Pockels, working in her kitchen, invented the trough method for measuring surface tension, the forerunner of the Langmuir film balance. Surface tension matters in washing, inkjet printing, stabilising foams and emulsions, mineral flotation, microfluidics and water-repellent coatings, and it lets pond skaters walk on water.

反应Reactions

Δp = 2γ/r杨-拉普拉斯方程h = 2γcosθ/(ρgr)毛细上升Δp = 2γ/r(-); h = 2γcosθ/(ρgr)

r 为曲率半径或毛细管半径。

r is the radius of curvature or of the capillary.

水,r = 1 μm 气泡:Δp = 2×0.072/10−6 ≈ 1.44×105 Pawater, r = 1 μm : Δp = 2×0.072/10−6 ≈ 1.44×105 Pa

微小气泡内压约 1.4 个大气压

A micrometre bubble carries about 1.4 atm of extra pressure

年表Timeline

  • 1805

    杨和拉普拉斯建立毛细理论

    Young and Laplace develop the theory of capillarity

  • 1878

    吉布斯界面热力学

    Gibbs's interfacial thermodynamics

  • 1891

    波克尔斯发明表面张力槽

    Pockels invents the surface-tension trough

  • 1997

    巴特洛特解释荷叶效应

    Barthlott explains the lotus effect

相关公式Formulas

杨–拉普拉斯方程 Young–Laplace equation→
\[\Delta p = \gamma\left(\frac{1}{R_1} + \frac{1}{R_2}\right) \xrightarrow{\text{球面}} \frac{2\gamma}{r},\qquad h = \frac{2\gamma\cos\theta}{\rho g r}\]\[\Delta p = \gamma\left(\frac{1}{R_1} + \frac{1}{R_2}\right) \xrightarrow{\text{sphere}} \frac{2\gamma}{r},\qquad h = \frac{2\gamma\cos\theta}{\rho g r}\]
例题Worked example

25 °C 水(γ = 0.072 N/m)中半径 1 μm 的气泡:Δp = 2×0.072/10⁻⁶ = 1.44×10⁵ Pa ≈ 1.4 atm。半径 0.1 mm 玻璃毛细管中水上升约 15 cm。

A 1 μm bubble in water has Δp ≈ 1.4 atm; water rises ~15 cm in a 0.1 mm radius capillary.

杨氏方程(接触角) Young's equation (contact angle)→
\[\gamma_{sg} = \gamma_{sl} + \gamma_{lg}\cos\theta,\qquad W_a = \gamma_{lg}(1 + \cos\theta)\]
吉布斯吸附等温式 Gibbs adsorption isotherm→
\[\Gamma_2 = -\frac{1}{RT}\left(\frac{\partial\gamma}{\partial\ln a_2}\right)_T \approx -\frac{c}{RT}\frac{d\gamma}{dc}\]
例题Worked example

十二烷基硫酸钠在 CMC(8 mmol/L)以下 γ–lg c 斜率给出 Γ ≈ 3×10⁻⁶ mol/m²,即每个分子约占 0.5 nm²。

SDS below its CMC gives Γ ≈ 3×10⁻⁶ mol m⁻² (~0.5 nm² per molecule).