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![[DIR]](/icons/back.gif) | Parent Directory | | - | |
![[IMG]](/icons/image2.gif) | rcs_MUSA_20170227_173242_1064lt.png | 17-Jan-2018 12:14 | 121K | |
![[IMG]](/icons/image2.gif) | rcs_MUSA_20170227_121602_1064lt.png | 17-Jan-2018 12:14 | 66K | |
![[IMG]](/icons/image2.gif) | rcs_MUSA_20170220_124458_1064lt.png | 17-Jan-2018 12:14 | 76K | |
![[IMG]](/icons/image2.gif) | rcs_MUSA_20170216_180603_1064lt.png | 17-Jan-2018 12:14 | 97K | |
![[IMG]](/icons/image2.gif) | 201702_potenza_measurements.png | 17-Jan-2018 12:14 | 22K | |
![[IMG]](/icons/image2.gif) | 201702_potenza_lwc-scaled-adiabatic.png | 17-Jan-2018 12:14 | 7.2K | |
![[IMG]](/icons/image2.gif) | 201702_potenza_iwc-Z-T-method.png | 17-Jan-2018 12:14 | 7.5K | |
![[IMG]](/icons/image2.gif) | 201702_potenza_classification.png | 17-Jan-2018 12:14 | 8.5K | |
![[IMG]](/icons/image2.gif) | 201702_palaiseau_measurements.png | 17-Jan-2018 12:14 | 74K | |
![[IMG]](/icons/image2.gif) | 201702_palaiseau_lwc-scaled-adiabatic.png | 17-Jan-2018 12:14 | 9.3K | |
![[IMG]](/icons/image2.gif) | 201702_palaiseau_iwc-Z-T-method.png | 17-Jan-2018 12:14 | 25K | |
![[IMG]](/icons/image2.gif) | 201702_palaiseau_classification.png | 17-Jan-2018 12:14 | 18K | |
![[IMG]](/icons/image2.gif) | 201702_mace-head_measurements.png | 17-Jan-2018 12:14 | 159K | |
![[IMG]](/icons/image2.gif) | 201702_mace-head_lwc-scaled-adiabatic.png | 17-Jan-2018 12:14 | 29K | |
![[IMG]](/icons/image2.gif) | 201702_mace-head_iwc-Z-T-method.png | 17-Jan-2018 12:14 | 44K | |
![[IMG]](/icons/image2.gif) | 201702_mace-head_classification.png | 17-Jan-2018 12:14 | 22K | |
![[IMG]](/icons/image2.gif) | 201702_lindenberg_measurements.png | 17-Jan-2018 12:14 | 106K | |
![[IMG]](/icons/image2.gif) | 201702_lindenberg_lwc-scaled-adiabatic.png | 17-Jan-2018 12:14 | 15K | |
![[IMG]](/icons/image2.gif) | 201702_lindenberg_iwc-Z-T-method.png | 17-Jan-2018 12:14 | 28K | |
![[IMG]](/icons/image2.gif) | 201702_lindenberg_classification.png | 17-Jan-2018 12:14 | 17K | |
![[IMG]](/icons/image2.gif) | 201702_chilbolton_measurements.png | 17-Jan-2018 12:14 | 132K | |
![[IMG]](/icons/image2.gif) | 201702_chilbolton_lwc-scaled-adiabatic.png | 17-Jan-2018 12:14 | 16K | |
![[IMG]](/icons/image2.gif) | 201702_chilbolton_iwc-Z-T-method.png | 17-Jan-2018 12:14 | 34K | |
![[IMG]](/icons/image2.gif) | 201702_chilbolton_classification.png | 17-Jan-2018 12:14 | 19K | |
![[IMG]](/icons/image2.gif) | 201701_potenza_measurements.png | 17-Jan-2018 12:14 | 74K | |
![[IMG]](/icons/image2.gif) | 201701_potenza_lwc-scaled-adiabatic.png | 17-Jan-2018 12:14 | 21K | |
![[IMG]](/icons/image2.gif) | 201701_potenza_iwc-Z-T-method.png | 17-Jan-2018 12:14 | 23K | |
![[IMG]](/icons/image2.gif) | 201701_potenza_classification.png | 17-Jan-2018 12:14 | 14K | |
![[IMG]](/icons/image2.gif) | 201701_palaiseau_measurements.png | 17-Jan-2018 12:14 | 62K | |
![[IMG]](/icons/image2.gif) | 201701_palaiseau_lwc-scaled-adiabatic.png | 17-Jan-2018 12:14 | 8.7K | |
![[IMG]](/icons/image2.gif) | 201701_palaiseau_iwc-Z-T-method.png | 17-Jan-2018 12:14 | 22K | |
![[IMG]](/icons/image2.gif) | 201701_palaiseau_classification.png | 17-Jan-2018 12:14 | 17K | |
![[IMG]](/icons/image2.gif) | 201701_mace-head_measurements.png | 17-Jan-2018 12:14 | 64K | |
![[IMG]](/icons/image2.gif) | 201701_mace-head_lwc-scaled-adiabatic.png | 17-Jan-2018 12:14 | 15K | |
![[IMG]](/icons/image2.gif) | 201701_mace-head_iwc-Z-T-method.png | 17-Jan-2018 12:14 | 18K | |
![[IMG]](/icons/image2.gif) | 201701_mace-head_classification.png | 17-Jan-2018 12:14 | 12K | |
![[IMG]](/icons/image2.gif) | 201701_lindenberg_measurements.png | 17-Jan-2018 12:14 | 91K | |
![[IMG]](/icons/image2.gif) | 201701_lindenberg_lwc-scaled-adiabatic.png | 17-Jan-2018 12:14 | 14K | |
![[IMG]](/icons/image2.gif) | 201701_lindenberg_iwc-Z-T-method.png | 17-Jan-2018 12:14 | 24K | |
![[IMG]](/icons/image2.gif) | 201701_lindenberg_classification.png | 17-Jan-2018 12:14 | 16K | |
![[IMG]](/icons/image2.gif) | 201701_juelich_measurements.png | 17-Jan-2018 12:14 | 34K | |
![[IMG]](/icons/image2.gif) | 201701_juelich_lwc-scaled-adiabatic.png | 17-Jan-2018 12:14 | 6.0K | |
![[IMG]](/icons/image2.gif) | 201701_juelich_iwc-Z-T-method.png | 17-Jan-2018 12:14 | 9.2K | |
![[IMG]](/icons/image2.gif) | 201701_juelich_classification.png | 17-Jan-2018 12:14 | 9.0K | |
![[IMG]](/icons/image2.gif) | 201701_chilbolton_measurements.png | 17-Jan-2018 12:14 | 115K | |
![[IMG]](/icons/image2.gif) | 201701_chilbolton_lwc-scaled-adiabatic.png | 17-Jan-2018 12:14 | 17K | |
![[IMG]](/icons/image2.gif) | 201701_chilbolton_iwc-Z-T-method.png | 17-Jan-2018 12:14 | 29K | |
![[IMG]](/icons/image2.gif) | 201701_chilbolton_classification.png | 17-Jan-2018 12:14 | 17K | |
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