# 5.4 Curvature Effect: Kelvin Effect

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- 3379

Let’s look at curvature effect first (see figure below). Consider the forces that are holding a water drop together for a flat and a curved surface. The forces on the hydrogen bonding in the liquid give a net inward attractive force to the molecules on the boundary between the liquid and the vapor. The net inward force, divided by the distance along the surface, is called ** surface tension, σ**. Its units are N/m or J/m

^{2}.

Sketches of the curvature effect. Left is a flat surface of pure water; right is a curved surface of pure water.

Credit: W. Brune

If the surface is curved, then the amount of bonding that can go on between any one water molecule on the surface and its neighbors is reduced. As a result, there is a greater probability that any one water molecule can escape from the liquid and enter the vapor phase. Thus, the evaporation rate increases. The greater the curvature, the greater the chance that the surface water molecules can escape. Thus, it takes less energy to remove a molecule from a curved surface than it does from a flat surface.

When we work through the math, we arrive at the ** Kelvin Equation**:

\[e_{s c}(T)=e_{s}(T) \cdot \exp \left(\frac{2_{\sigma}}{n_{L} \cdot R \cdot T \cdot r_{d}}\right)\]

where* e_{sc} *is the equilibrium vapor pressure over

*curved surface of pure water,*

*a**is the equilibrium vapor pressure over a flat surface of pure water, both of which are functions of temperature, although*

*e*_{s}*is also a function of the drop radius,*

*e*_{sc}*is the number of moles per volume of water (55.5 moles L*

*n*_{L}^{-1}).

*is the molar gas constant,*

*R***is the water surface tension, and*

*σ**is the radius of the drop.*

*r*\[\left(\frac{2 \sigma}{n_{L} \cdot R^{*}}\right)=3.3 \times 10^{-7} \mathrm{m} K^{-1}\]

Since the evaporation is much, much greater over a curved surface, the condensation must also be much, much greater in order to keep condensation = evaporation, which is required for saturation (i.e., equilibrium). Thus, the saturation vapor pressure over a curved surface is much greater than the saturation vapor pressure over a flat surface of pure water.

When we plot this equation, we get the following figure:

Dependence of ratio of the saturation vapor pressure over a curved surface to saturation vapor pressure over a flat surface on the drop radius.

Credit: W. Brune

Note the rapid increase in equilibrium vapor pressure for particles that have radii less than 10 nm. Of course, all small clusters of water vapor and CCN start out at this small size and grow by adding water.

The Kelvin Equation can be approximated by expanding the exponential into a series:

\[e_{s c}(T)=e_{s}(T) \cdot\left(1+\frac{2 \sigma}{n_{L} \cdot R^{*} \cdot T \cdot r_{d}}\right)=e_{s}(T) \cdot\left(1+\frac{a_{K}}{r_{d}}\right), \quad\) where \(a_{K}=\frac{2 \sigma}{n_{L} \cdot R^{*} \cdot T}\]

### Summary

Cloud drops start as very small spherical drops, but the vapor pressure required for them to form is much greater than * e_{s}* until they get closer to 10

^{-2}μm in size. The Kelvin effect is important only for tiny drops; it is important because all drops start out as tiny drops and must go through that stage. As drops gets bigger, their radius increases and

*approaches*

*e*_{sc}*.*

*e*_{s}So, is it possible to form a cloud drop out of pure water? This process is called * homogeneous nucleation.* The only way for this to happen is for two molecules to stick together, then add another, then another, etc. But the radius of the nucleating drop is so small that the vapor pressure must be very large. It turns out that drops probably can nucleate at a reasonable rate when the relative humidity is about 440%. Have you ever heard of such a high relative humidity?

So, the lesson here is that homogeneous nucleation is very unlikely because of the Kelvin effect.