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HAL Id: hal-02419618

https://hal.archives-ouvertes.fr/hal-02419618

Submitted on 20 Feb 2020

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Thermodynamic study of iron-fluorine system

S. Chatain, M. Achour, Jl. Fleche, L. Martinelli

To cite this version:

S. Chatain, M. Achour, Jl. Fleche, L. Martinelli. Thermodynamic study of iron-fluorine system.

Colloque Francais de Chimie du Fluor 2017 (CFCF 2017), May 2017, Murol, France. 2017.

�hal-02419618�

(2)

Context and goals

CALPHAD (CALculation of PHAse Diagram) Method

Literature review

First principle calculations

Optimisation results

Further work

References

Thermodynamic study of iron-fluorine system

Sylvie Chatain

1

, Mickaël Achour

2

, Jean-Louis Flèche

1

, Laure Martinelli

1

1

Den-Service de la Corrosion et du Comportement des Matériaux dans leur Environnement (SCCME) – CEA, Université Paris-Saclay, F-91919, Gif-sur-Yvette, France

2

Hall de Recherche de Pierrelatte (HRP) – Division Chimie et Enrichissement, F-26701, Pierrelatte, France

Phase diagram

Thermodynamic properties

Solid Compounds

∆ ∆∆ ∆H°f ,298 K

(kJ/mol) Experimental method Reference

FeF2

-710.12 -715.5±0.5

Equilibrium pressure (2ndlaw) Equilibrium pressure (3rdlaw) [81Sch] -705.8±41.8 Equilibrium pressure [28Jel]

FeF3

-989.6±2.2 Calometric bomb [81Joh] -1037.6±4.5 F.e.m (3rdlaw) [81Sch]

-1056 -1043

Equilibrium pressure (3rdlaw) Equilibrium pressure (2ndlaw) [28Jel] -993 Equilibrium pressure (2ndlaw) [37Dom] -990.8±2.1 Calometric bomb [79Fer]

Computational method for calculating

multicomponent phase diagrams

Phase diagram = graphical representation of thermodynamic properties

Combination of

thermodynamics (Gibbs energies)

and

phase diagrams

data

Thermodynamic equilibrium at T, p, N

i

is calculated by

minimizing the total Gibbs

energy G of the system

600 800 1000 1200 1400 0.67 0.69 0.71 0.73 0.75 Te m p e ra tu re ( °C ) XF Exp [73Tsi] FeF2 FeF3 liquid FeF2+FeF3 liq+FeF3 liq+FeF2

Lithium ion batteries (LIBs)

- FeF

3

as electrode material, especially cathode

- effect of the nanostructure on

f

⇒ nano CALPHAD

Iron corrosion in liquid UF

6

(cf M. Achour poster)

- FeF

2

and FeF

3

as corrosion products

- improve the Fe-F thermodynamic description

- Fe-F database built using CALPHAD method

Only one experimental phase diagram determined by

Differential Thermal Analysis between FeF

2

and FeF

3

[73Tsi]

Discrepancies on the FeF

2

melting temperature (950 °C [73Tsi],

975 °C [89Joh] or 1100 °C [98Cha])

No FeF

3

fusion: sublimation without melting

-650 -640 -630 -620 -610 -600 -590 -580 -570 -560 500 600 700 800 900 1000 1100 1200 ∆ G °f ( Fe F2 , s ) (k J/ m o l) Temperature (K) [87Aza] [75Cha] [81Sch]

Good agreement for

f, 298 K

(FeF

2

, s) and

f, T

(FeF

2

, s)

f, 298 K

(FeF

3

, s) data scaterred

No thermodynamic properties for gaseous molecule Fe

2

F

6

and only

estimations for FeF

3

Calculations on gaseous molecules performed using Density Functional Theory

implemented in DMol3 software

Generalized gradient approximation for exchange and correlation energy (GGA)

Spin of iron atoms taken into account

M : molecular weight

σ: symmetry number

IA, IBand IC, moment of inertia about principal axis

PV ) T ( E (T) E ) T ( E ) r ( E ) T (

H =coh i+ vib +rot +trans + r

(

)

(

)

[

]

RT PV 2 3 kT h exp 1 kT h exp h k R h 2 1 k R ) r ( E ) T ( H i i i i i i i coh + + ν − − ν − ν + ν + = r

(

)

(

)

[

(

)

]

31482 . 2 P ln R M ln R 2 3 T ln R 2 5 Srot kT h exp 1 ln R kT h exp 1 kT h exp kT h R ) T ( S i i i i i i − − + + + ν − − − ν − − ν − ν =

R 2 3 hc kT h cI 8 h cI 8 h cI 8 ln 2 R ) linear non ( S 3 C 2 B 2 A 2 rot +               π π π σ π =

(

)

(

)

(

)

[

]

R 2 5 R 2 3 kT h exp 1 kT h exp kT h R Cp i 2 i i 2 i + + ν − ν − ν =

Molecules ∆∆∆∆H°f, 298 K (kJ/mol) Reference FeF2 -387.9 This work -389.5 [98Cha] FeF3 -660.8 This work -820.9 [98Cha] Fe2F6 -1472.5 This work

DTA experiments to check the phase diagram between FeF

2

and FeF

3

and between

Fe and FeF

2

FeF

2

fusion temperature measurement

Optimisation of the Fe-F system taken into account the new experimental data

Effect of the nanostructure of FeF

2

and FeF

3

on the phase diagram and

thermodynamic properties

Enlarge the study to Fe-O-F ternary system

[28Jel] K. Jellinek, A. Rudat, Z. Anorg. Allg. Chem. 175 (1928) p. 281-320 [37Dom] L. Domange, Ann. Chim. 7 (1937) p. 225

[73Tsi] T.G. Tsiklauri, E.G. Ippolitov, B.M. Zhigarnovskii, and S.V. Petrov, Soobshch Akad. Nauk. Gruz. SSR, 69 (1973) p. 593-596 [75Cha] G. Chattopadhyay, M.D. Karkhanavala, and S. Chandrasekharaiah, J. Electrochem. Soc. 122 (1975) p.325-327 [79Fer] G. Férey, A.M. Leclerc, R. de Pape, Solid State Communications 29 (1979) p. 477-480

[81Joh] G.K. Johnson, J. Chem. Thermodynamics 13 (1981) p. 465-469 [81Sch] S.C. Schaefer and N.A. Gokcen, High Temp. Science 14 (1981) p. 153-159 [89Joh] H.G. Johansen, A. Sterten and J. Thonstad, Acta Chem. Scand. 43 (1989) p. 417-420 [98Cha] M.W. Chase, NIST-JANAF Thermochemical Tables, (1998)

F e F3 F e F2 FeF2+liq FeF3+FeF2 FeF3+liq

500

600

700

800

900

1000

1100

1200

1300

1400

1500

Te

m

p

e

ra

tu

re

C

)

0.66

0.68

0.70

0.72

0.74

Mole fraction F

liquidus invariants

Acknowledgment: Financial support of Areva

f,298 K

(FeF

2

,s)=-713 kJ/mol

f,298 K

(FeF

3

,s)=-990 kJ/mol

500

600

700

800

900

1000

1100

1200

1300

1400

1500

Te

m

p

e

ra

tu

re

C

)

0

0.2

0.4

0.6

0.8

1.0

Mole fraction F

liquidus invariants Fe F3 Fe F2 F e F3 + F e F2 FeF2+Fe Fe-bcc+liquid Fe-fcc+liquid Fe-bcc+liquid

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