u-system accounts - lever-rulestefanb/files/thermodynamics/lever... · 2014. 3. 2. · let us take...

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Lever-Rule Stefan Bringuier March 2, 2014 The essence of the lever-rule is that the fraction of each phase at a given composition is the ratio of the differences in composition weight percent (or atomic). Let us take for example a complete solubility system such as Si-Ge with two phases α and L, shown in Fig. 1. The total number of moles is given by: n T = n L + n α (1) Let us now select a composition corresponding to the weight fraction at X o Ge , the total number of moles of Ge at this composition is: X o Ge n T (2) So that the that the number of moles of Ge is the sum of the number of moles in the α and L phases. X o Ge n T = X L Ge n L + X α Ge n α (3) Normalizing Eq. 3 with respect to the total number of moles, yields Eq. 4a which allows us to determine the fraction of each phase anywhere on the phase diagram. Lets look at the Si-Ge phase diagram again, specifically at the compo- sition with weight fraction X Si =0.3 at 1100 C (note the axis goes from Si to Ge). Notice how this point falls in the two phase region, we thus can invoke the lever-rule (Eq. 4a). n T n T = n L + n α n T 1= Z L + Z α X o Ge = X L Ge Z L + X α Ge Z α (4a) 1

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Page 1: U-System Accounts - Lever-Rulestefanb/Files/Thermodynamics/lever... · 2014. 3. 2. · Let us take for example a complete solubility system such as Si-Ge with two phases and L, shown

Lever-Rule

Stefan Bringuier

March 2, 2014

The essence of the lever-rule is that the fraction of each phase at a givencomposition is the ratio of the differences in composition weight percent (oratomic). Let us take for example a complete solubility system such as Si-Gewith two phases α and L, shown in Fig. 1. The total number of moles isgiven by:

nT = nL + nα (1)

Let us now select a composition corresponding to the weight fraction atXoGe, the total number of moles of Ge at this composition is:

XoGenT (2)

So that the that the number of moles of Ge is the sum of the number ofmoles in the α and L phases.

XoGenT = XL

GenL +XαGenα (3)

Normalizing Eq. 3 with respect to the total number of moles, yieldsEq. 4a which allows us to determine the fraction of each phase anywhere onthe phase diagram.

Lets look at the Si-Ge phase diagram again, specifically at the compo-sition with weight fraction XSi = 0.3 at 1100 ◦C (note the axis goes fromSi to Ge). Notice how this point falls in the two phase region, we thus caninvoke the lever-rule (Eq. 4a).

nTnT

=nL + nαnT

1 = ZL + Zα

XoGe = XL

GeZL +XαGeZα (4a)

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Page 2: U-System Accounts - Lever-Rulestefanb/Files/Thermodynamics/lever... · 2014. 3. 2. · Let us take for example a complete solubility system such as Si-Ge with two phases and L, shown

Figure 1: Si-Ge phase diagram1.

Before getting the values for the composition of the L and α from thephase diagram, let us rearrange Eq. 4a using Si weight fraction, to solve forZα:

ZL = 1 − Zα

XoSi = XL

Si (1 − Zα) +XαSiZα

Zα =XoSi −XL

Si

XαSi −XL

Si

(5a)

On the phase diagram we use the tie-line construction method to measurethe composition of the two phases. The tie-lines correspond to the composi-tion at which the the free energies are a minimum and satisfy the conditionsfor thermodynamic equilibrium. The tie-lines are always constructed be-tween phase-boundaries. This is shown by the red line, the tie-line willdepend on initial starting overall composition. For a value of Xo

Si = 0.3 thecorresponding XL

Si and XαSi are 0.18 and 0.49, respectively. Plugging these

numbers into Eq. 5a gives:

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Page 3: U-System Accounts - Lever-Rulestefanb/Files/Thermodynamics/lever... · 2014. 3. 2. · Let us take for example a complete solubility system such as Si-Ge with two phases and L, shown

Zα = 0.2926

The reader who is not familiar with the lever-rule will quickly notice thatthe fraction of α is not the same as the composition of Si. It maybe the casethat by incorrectly understanding the derivation of the lever-rule one mightinitially mistake or guess that then fraction of α is equal to composition ofSi.

References

[1] R.W. Olesinski and G.J. Abbaschian. The gesi (germanium-silicon) sys-tem. Bulletin of Alloy Phase Diagrams, 5(2):180–183, 1984.

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