For each phase transition, energy has to be put in to change the "hold" to something less strong.

But there is a third regime a phase transition away.

This is well known from the theory of phase transitions.

In contemporary science, this process is known as a phase transition.

James is widely known for his research in phase transitions.

Any addition of thermal energy results in a phase transition.

Therefore they would not have phase transitions as one sees in the states of matter.

A state of matter is also characterized by phase transitions.

This is a great improvement in the study of first order phase transitions.

Below the lower critical dimension there is no phase transition.

After a phase transition, a liquid can turn into a crystal.

He further considered questions of phase transitions in what later became known as Stefan problems.

With further addition of heat, the temperature remains constant while the phase transition takes place.

An example of such behavior is the 3-dimensional ferromagnetic phase transition.

Critical phenomena take place in second order phase transition, although not exclusively.

Its actual value depends on the type of phase transition we are considering.

Instead, they separate oil, and the dropping point as a phase transition does not apply.

The temperature of the phase transition is believed to be quite close to the melting point.

The most physically attractive alternative was a first order phase transition.

These are similar to phase transitions in physical systems.

Later work has also cast doubt on whether there could be a phase transition in the very early universe of the kind required.

Increasing the temperature increases the pressure of these phase transitions.

This work lead to the study of phase transitions.

The model of an ideal gas, however, does not describe or allow phase transitions.

This is a phase transition from the isolated peaks regime.