Nano Carbon-metal hybrids

Nucleation

Polymers

2D Materials

Metallic       glass

 Ferroic materials

Diffusion

project:

«Phase transitions and nucleation»

​

Here you will find the proposed materials framed in a  coloured box . The code next to it identifies each item (foto, video, etc.) individually. You will need this code to fill in the form. Additionally, you can have an overview of the materials from all research groups at matter.soundsof.net/materials.

​

We know from everyday experience that can substances can suddenly change their properties depending on external conditions such as pressure and temperature. Such a sudden change is called a phase transition. Water for instance, is liquid at ambient conditions, but when the temperature is decreased below the freezing point, water turns into ice. However, often such a phases transition does not occur immediately. For instance, water can remain liquid for long times even below zero degrees Celsius and diamonds are stable practically indefinitely even if graphite is the preferred form of carbon.

This behavior can be understood by considering how a system transforms from one phase to another. It does so by forming nucleus of the stable phase growing in the original phase, a process called nucleation. An example is a small crystal of ice forming in the undercooled liquid as shown in the figure below.

At conditions of practical importance critical nuclei are microscopically small such cannot be directly observed in an experiment. Since computer simulations allow us to observe such transitions with atomic resolution, they are a particularly useful tool to elucidate the mechanism of the transition under these circumstances

This movie shows the freezing process of an initially fluid gold nanocluster upon cooling together with a graph indicating crystallinity. Within a very short moment the gold atoms form the precursor (the so-called critical nucleus) of a completely ordered structure which then quickly grows to form a solid cluster with an icosahedral shape. Other shapes are also possible and it is an interesting question which parameters (i.e. number of atoms) favour which forms. Computer simulations like this accompanied by free energy calculations and advanced techniques such as transition path sampling allow us to extract important properties in such rare event situations, e.g. the melting temperature or the rate constant.

For instance, in engineering applications where strong water propulsion is desired, for instance at the trailing edge of an underwater propeller (see picture above) or in turbines, cavitation is an undesirable yet hardly avoidable phenomenon, in the course of which bubbles grow to a limited size and collapse afterwards. This collapse of vapor bubbles is a violent process during which high temperatures, pressure waves, and explosive water jets occur that frequently result in significant damage to propellers.

The following movie shows the formation of a bubble in water under tension. Water under tension is a common occurrence in nature, most notably in trees that rely on pulling water from the soil up towards the leaves through narrow pores in the trunk. Under tension, water vapor is the thermodynamically favorable phase and the system undergoes the phase transition from the liquid to the vapor through nucleation of a vapor bubble. Here, water is depicted in red (oxygen) and white (hydrogen) and the yellow spheres indicate the largest bubble in the system. Over the course of the trajectory, this bubble grows until the system abruptly transitions to the vapor.​

Using such simulations we were able to compute the rates of bubble formation under tension which allowed us to investigate a long-standing discrepancy between different types of cavitation experiments. Furthermore, our results show that the dynamics of bubble growth are essentially determined by the viscosity of the surrounding liquid, indicating that this macroscopic principle holds even for bubbles which are only a few atom diameters in size.

Research team

Principal Investigator: Prof. Christoph Dellago

- P. Geiger

- G. Menzl

- A. Singraber

- C. Karner

- C. Cardelli