Eu3W-1 base conditions 600 °C: 153 A, 0.8T, 6.5 SLM
Emissivity
measurements
## [1] "Sandblasted emissivity"
| 694 |
0.41 |
| 731 |
0.42 |
| 770 |
0.43 |
| 866 |
0.44 |
| 1338 |
0.51 |
| 1175 |
0.49 |
## [1] "LASAG damaged emissivity"
| 600 |
0.16 |
| 656 |
0.20 |
| 727 |
0.23 |
| 800 |
0.25 |
| 922 |
0.27 |
| 1030 |
0.30 |
| 1150 |
0.32 |
| 1302 |
0.33 |
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