# Difference between revisions of "Spinodal"

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Figure 1 shows the free energy of mixing as a function of composition for one portion of the two-phase region. Let's look at composition <math>\phi_a</math> with free energy <math>F_a</math>. Small fluctuation in composition create a higher energy state <math>F_{a'}</math>, and this compostion is therefore considered metastable. On the other hand, composition <math>\phi_b</math> is unstable since small fluctuations in composition create a lower energy state. A quick way to visualize stability can be seen in Figure 2. Point (1) is metastable because small fluctuations lead to higher energy states, but if it gets enough energy to make it over the barrier, it can move to a lower energy state. Point (2) is unstable because any fluctuations will cause it to move to a lower energy state. Point (3) is stable. | Figure 1 shows the free energy of mixing as a function of composition for one portion of the two-phase region. Let's look at composition <math>\phi_a</math> with free energy <math>F_a</math>. Small fluctuation in composition create a higher energy state <math>F_{a'}</math>, and this compostion is therefore considered metastable. On the other hand, composition <math>\phi_b</math> is unstable since small fluctuations in composition create a lower energy state. A quick way to visualize stability can be seen in Figure 2. Point (1) is metastable because small fluctuations lead to higher energy states, but if it gets enough energy to make it over the barrier, it can move to a lower energy state. Point (2) is unstable because any fluctuations will cause it to move to a lower energy state. Point (3) is stable. | ||

− | For every free energy curve, we can find two compositions in the 2-phase region corresponding to the transition from the metastable compositions to unstable compositions -- that is to say, the inflection points on the free energy versus composition curves. Let's consider what the spinodal looks like for the [[regular solution]] model. | + | For every free energy curve, we can find two compositions in the 2-phase region corresponding to the transition from the metastable compositions to unstable compositions -- that is to say, the inflection points on the free energy versus composition curves. Let's consider what the spinodal looks like for the [[regular solution]] model. We can find the spinodal line by looking at |

+ | <center><math>{{\partial^2 G_{mix}} \over \partial {x_A}^2} = 0</math></center> | ||

+ | By taking this derivative and solving for <math>T_{s}</math> (below which the homogeneous mixture passes from a unstable to metastable state), we will define a [[phase boundary]] on our temperature versus composition [[phase diagram]] (Figure 3). | ||

+ | <center> <math>T_{s} = {{2 \epsilon x_A} \over R} (1-x_A)</math></center> | ||

## Revision as of 04:00, 10 December 2011

Entry by Emily Redston, AP 225, Fall 2011

Please see phase separation for an introduction to the regular solution model phase diagram we will be focusing on.

Figure 1 shows the free energy of mixing as a function of composition for one portion of the two-phase region. Let's look at composition <math>\phi_a</math> with free energy <math>F_a</math>. Small fluctuation in composition create a higher energy state <math>F_{a'}</math>, and this compostion is therefore considered metastable. On the other hand, composition <math>\phi_b</math> is unstable since small fluctuations in composition create a lower energy state. A quick way to visualize stability can be seen in Figure 2. Point (1) is metastable because small fluctuations lead to higher energy states, but if it gets enough energy to make it over the barrier, it can move to a lower energy state. Point (2) is unstable because any fluctuations will cause it to move to a lower energy state. Point (3) is stable.

For every free energy curve, we can find two compositions in the 2-phase region corresponding to the transition from the metastable compositions to unstable compositions -- that is to say, the inflection points on the free energy versus composition curves. Let's consider what the spinodal looks like for the regular solution model. We can find the spinodal line by looking at

By taking this derivative and solving for <math>T_{s}</math> (below which the homogeneous mixture passes from a unstable to metastable state), we will define a phase boundary on our temperature versus composition phase diagram (Figure 3).

The curve on the right above is magnified and replotted here. This is the phase diagram of a two-component liquid system whose free energy of mixing is described by the regular solution model. When the <math>\chi </math> parameter is greater than two, the system phase separates. The outer curve is the phase boundary. The inner curve is the spinodal - the energy vs concentration relation where the homogeneous mixture passes from a unstable to metastable state.

As a brief aside, the name spinodal, which means "thorn" in Latin, refers to their shape in one-component systems [1].