Cr–La system

16 accepted literature values from 2 paper(s) (experimental 7, model 9); 2 calculated phase diagram(s). 18 further extracted value(s) not accepted by the reader-agreement checks are only in the JSON/CSV.

Data: JSON · CSV · interactive explorer · interactive phase diagram · phases (5) · papers (bibliography) · Markdown

Accepted values by evidence class
Evidence classValues
experimental7
model9
Accepted values by property group
Property groupValues
invariant reaction11
phase transition4
other property1

Calculated phase diagrams

Binary phase diagrams calculated with pycalphad 0.11.2 from the SGTE binary collection (Hallstedt 2025, CC BY 4.0). Evidence class: model.

Assessments with a calculated phase diagram
TDB fileAssessmentSHA-256Links
CrLa-09Cha.tdbW. Chan, C. Gao, O.N. Dogan, P. King, A.D. Rollett, J. Phase Equilib. Diffus., 30, 578-86(2009). doi:10.1007/s11669-009-9581-37eae47ddc2ae31cacba91eb581a06d8c4a493fafda31e53de4e901b25a137d70viewer · TDB · JSON
CrLa-09Pov.tdbE. Povoden, M. Chen, A.N. Grundy, T. Ivas, L.J. Gauckler, J. Phase Equilib. Diffus., 30, 12-27(2009). doi:10.1007/s11669-008-9463-0af1685101b0145ad083258c09bda4e082c1a4e1a0e44f11a98444c43ca655fbaviewer · TDB · JSON
Calculated three-phase invariants (model, mole fraction of the second component)
TDB fileT (K)Phases at the invariant
CrLa-09Cha.tdb2101.7BCC_A2 (x(La) 0.02155) + LIQUID#2 (x(La) 0.07873) + LIQUID (x(La) 0.73847)
CrLa-09Cha.tdb1142.91LIQUID (x(La) 0.97333) + FCC_A1 (x(La) 0.9963) + BCC_A2 (x(La) 0.99909)
CrLa-09Cha.tdb1138.03BCC_A2 (x(La) 0.00108) + LIQUID (x(La) 0.96903) + FCC_A1 (x(La) 0.99553)
CrLa-09Cha.tdb549.93BCC_A2 (x(La) 0) + FCC_A1 (x(La) 0.99999) + DHCP (x(La) 1)
CrLa-09Pov.tdb2142.42BCC_A2 (x(La) 0.00263) + LIQUID#2 (x(La) 0.02661) + LIQUID (x(La) 0.83326)
CrLa-09Pov.tdb1133.96LIQUID (x(La) 0.97187) + BCC_A2 (x(La) 0.99998) + FCC_A1 (x(La) 0.99999)
CrLa-09Pov.tdb1126.03BCC_A2 (x(La) 2.000e-5) + LIQUID (x(La) 0.96675) + FCC_A1 (x(La) 0.99999)
CrLa-09Pov.tdb1126.03BCC_A2 (x(La) 2.000e-5) + LIQUID (x(La) 0.96675) + FCC_A1 (x(La) 0.99999)
CrLa-09Pov.tdb550BCC_A2 (x(La) 0) + FCC_A1 (x(La) 1) + DHCP (x(La) 1)

Convex hulls: Materials Project DFT hull · OQMD DFT hull · CALPHAD hull CrLa-09Pov

Invariant reactions (literature)

Invariant reactions reported in the literature for the Cr–La system (11)
T (K)Reaction / phasesCompositions (mole fraction)ClassSourceLocationQuote
2108.25monotectic: L1 -> L2 + CrL1: La 0.024; L2: La 0.976model[1] Chan 2009
cites Ray 2009
Table 3, p. 7, row 3
report
2103.15monotectic: L1 -> L2 + CrL1: La 0.009; L2: La 0.82; Cr: La 0experimental[1] Chan 2009
cites Massalski 1990
Table 3, p. 7, row 2
report
2102.15monotectic: L1 -> L2 + CrL1: La 0.0787; L2: La 0.739; Cr: La 0.0215model[1] Chan 2009Table 3, p. 7, row 4
report
1983.15monotectic: L1 -> L2 + CrL1: La 0.0399; Cr: La 0.0246experimental[1] Chan 2009
cites Savitskii 1960
Table 3, p. 7, row 1
report
1190.45eutectic: L2 -> Cr + βLaL2: La 0.9997model[1] Chan 2009
cites Ray 2009
Table 3, p. 7, row 9
report
1143.15L2 + γLa -> βLaL2: La 0.973; γLa: La 0.999; βLa: La 0.996model[1] Chan 2009Table 3, p. 7, row 5
report
1140.75eutectic: L2 -> Cr + βLaL2: La 0.97026model[1] Chan 2009
cites Terekhova 1990
Table 3, p. 7, row 8
report
1138.15eutectic: L2 -> Cr + βLaexperimental[1] Chan 2009
cites Savitskii 1960
Table 3, p. 7, row 6
report
1138.15eutectic: L2 -> Cr + βLaL2: La 0.966; Cr: La 0; βLa: La 1experimental[1] Chan 2009
cites Massalski 1990
Table 3, p. 7, row 7
report
1138.15eutectic: L2 -> Cr + βLaL2: La 0.969; Cr: La 0.0011; βLa: La 0.996model[1] Chan 2009Table 3, p. 7, row 10
report
550.15βLa -> Cr + αLaβLa: La 1; Cr: La 0; αLa: La 1model[1] Chan 2009Table 3, p. 7, row 11
report

Other properties

Phase transition (4)

Phase transition, Cr–La system
PropertyValueT (K)Phases / compositionClassSourceLocationQuote
Phase transition540 K540o-prv -> r-prvmodel[2] Povoden 2009p. 11
report
The calculated transition temperature of 540 K is shown by the broken line in Fig. 6.
Phase transition545 K545o-prv -> r-prvexperimental[2] Povoden 2009p. 11
report
The experimentally determined Cp-peak around 545 K caused by the first-order transition o-prv M r-prv is in fact a discontinuity which cannot be implemented in the model.
Phase transition2130 K2130Cr + liquidexperimental[2] Povoden 2009
cites Savitskii 1960
p. 8
report
Considerable deviations of the calculated liquidus from experiments at the Cr-rich side of the system can be ascribed to the problem of two different melting temperatures for Cr cited in the literature, which are 2180 and 2130 K. The higher value was favored by Dinsdale[10] and is adopted in this study, whereas the lower melting temperature was chosen by Savitskii et al.[12] and Svechnikov et al.…
Phase transition2180 K2180Cr + liquidmodel[2] Povoden 2009
cites Dinsdale 1991 doi
p. 8
report
Considerable deviations of the calculated liquidus from experiments at the Cr-rich side of the system can be ascribed to the problem of two different melting temperatures for Cr cited in the literature, which are 2180 and 2130 K. The higher value was favored by Dinsdale[10] and is adopted in this study, whereas the lower melting temperature was chosen by Savitskii et al.[12] and Svechnikov et al.…

Other property (1)

Other property, Cr–La system
PropertyValueT (K)Phases / compositionClassSourceLocationQuote
Other
printed: enthalpy change
231 unspecified960experimental[2] Povoden 2009
cites Yu 2005
p. 2
report
An enthalpy change of 231 kJ mol-1 was determined for this reaction at the average temperature of 960 K.[30]

Sources

Reporting papers the values were read from (a value cited from another work names that work in its row).

  1. Wren Chan, Michael C. Gao, Ömer N. Doğan, Paul King, Anthony D. Rollett, Thermodynamic Assessment of Cr-Rare Earth Systems, J. Phase Equilib. Diffus. 30, 578-586 (2009). doi:10.1007/s11669-009-9581-3
  2. E. Povoden, M. Chen, A.N. Grundy, T. Ivas, L.J. Gauckler, Thermodynamic Assessment of the La-Cr-O System, J. Phase Equilib. Diffus. 30, 12-27 (2009). doi:10.1007/s11669-008-9463-0