DAMASK_EICMD/examples/config/phase/thermal/Cu.yaml

references:
  - J.G. Hust and A.B. Lankford,
    Thermal Conductivity of Aluminum, Copper, Iron, and Tungsten from 1K to the Melting Point,
    US Department of Commerce, Boulder, Colorado, 1984,
    fit to Tab. 2.4.1 (RRR=300, T_min=150K, T_max=1000K)
  - https://www.mit.edu/~6.777/matprops/copper.htm

output: [T]

K_11: 4.005e+2
K_11,T: -1.075e-1
K_11,T^2: 3.293e-4
K_11,T^3: -7.533e-7
K_11,T^4: 5.223e-10

T_ref: 293.15

C_p: 385.0
data for thermal expansion 2021-05-24 13:32:28 +05:30			`references:`
temperature-dependent thermal conductivity 2022-02-12 20:41:09 +05:30			`- J.G. Hust and A.B. Lankford,`
			`Thermal Conductivity of Aluminum, Copper, Iron, and Tungsten from 1K to the Melting Point,`
			`US Department of Commerce, Boulder, Colorado, 1984,`
re-fit using higher order polynomial where appropriate. Code for fitting in "parameters" repository 2023-01-08 18:24:39 +05:30			`fit to Tab. 2.4.1 (RRR=300, T_min=150K, T_max=1000K)`
reference can now include comments! 2021-07-14 00:16:50 +05:30			`- https://www.mit.edu/~6.777/matprops/copper.htm`
polishing 2022-02-12 23:11:59 +05:30
guide the user 2022-02-20 03:40:05 +05:30			`output: [T]`

re-fit using higher order polynomial where appropriate. Code for fitting in "parameters" repository 2023-01-08 18:24:39 +05:30			`K_11: 4.005e+2`
			`K_11,T: -1.075e-1`
			`K_11,T^2: 3.293e-4`
			`K_11,T^3: -7.533e-7`
			`K_11,T^4: 5.223e-10`
polishing 2022-02-12 23:11:59 +05:30
temperature-dependent thermal conductivity 2022-02-12 20:41:09 +05:30			`T_ref: 293.15`
polishing 2022-02-12 23:11:59 +05:30
fixed symmetry handling - ort not tested, no examples, no documentation => removed - aP is the opposite of isotropic => removed isostropic materials can be easily specified as cI or cF, using C_44 = 1/2 * (C_11 - C_12). Acceptable extra effort for special use case orthorhombic can be easily implemented if needed, but needs test, documentation, and examples 2021-05-24 17:47:04 +05:30			`C_p: 385.0`