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Finite Element Analysis perturbation files for Rubin Observatory Simonyi Survey Telescope and LSST Camera

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Zenodo2023-09-27 更新2026-05-26 收录
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## Notes on FEA files <br> # M1M3 Bending modes M1M3_1um_156_grid.fits.gz - source = IM/data/M1M3/M1M3_1um_156_grid.txt - shape = (5256, 159) - Each row is one of 5256 FEA nodes. - 0th column is M1M3 disambiguator - 1st and 2nd columns are FEA node x and y in M1M3 CS - Last 156 columns are bending modes; the z-displacement of each node for each mode. M1M3_1um_156_force.fits.gz - source = IM/data/M1M3/M1M3_1um_156_force.txt - shape = (156, 159) - Each row is one of 156 bending modes. - 0th column is actuator ID - 1st and 2nd columns are actuator x and y in M1M3 CS - Last 156 columns are forces in Newtons for each mode. <br> # M1M3 print through M1M3_dxdydz_zenith.fits.gz - source = IM/data/M1M3/M1M3_dxdydz_zenith.npy - shape = (5256, 3) - Each row is one of 5256 FEA nodes. - Columns are dx, dy, dz in M1M3 CS. - This is the gravitational "print through" when mirror is zenith pointing M1M3_dxdydz_horizon.fits.gz - source = IM/data/M1M3/M1M3_dxdydz_horizon.npy - shape = (5256, 3) - Each row is one of 5256 FEA nodes. - Columns are dx, dy, dz in M1M3 CS. - This is the gravitational "print through" when mirror is horizon pointing M1M3_force_zenith.fits.gz - source = IM/data/M1M3/M1M3_force_zenith.npy - shape = (256,) - Each row is one of 256 actuators. (So we consider the x and y actuators here too.) - Columns are forces in Newtons. - These are the mirror support forces when the mirror is zenith pointing. (Is this after optimization? Include LUT or not?) M1M3_force_horizon.fits.gz - source = IM/data/M1M3/M1M3_force_horizon.npy - shape = (256,) - Each row is one of 256 actuators. (So we consider the x and y actuators here too.) - Columns are forces in Newtons. - These are the mirror support forces when the mirror is horizon pointing. (Is this after optimization? Include LUT or not?) <br> # M1M3 Thermal M1M3_thermal_FEA.fits.gz - source = IM/data/M1M3/M1M3_thermal_FEA.npy - shape = (5244, 7) - Each row is one of 5244 FEA nodes. (Why aren't these the same as above? I don't know.) - Columns are: - 0: Unit-Normalized FEA x - 1: Unit-Normalized FEA y - 2: Bulk temperature dz coefficient - 3: x temperature gradient dz coefficient - 3: y temperature gradient dz coefficient - 3: z temperature gradient dz coefficient - 3: r temperature gradient dz coefficient <br> # M1M3 Miscellany M1M3_influence_256.fits.gz - source = IM/data/M1M3/M1M3_influence_256.npy - shape = (5256, 256) - Each row is one of 5256 FEA nodes. - Each column is one of 256 actuators. - Values are dz/dF for each actuator/node. M1M3_LUT.fits.gz - source = IM/data/M1M3/M1M3_LUT.txt - shape = (257, 91) - First column is index in degrees (0-90 inclusive). Last 256 columns are forces in Newtons. - Each column is LUT for one value of the elevation index. M1M3_1000N_UL_shape_156.fits.gz - source = IM/data/M1M3/M1M3_1000N_UL_shape_156.npy - shape = (5256, 156) - Rows must be FEA nodes, columns must be bending modes. - Not sure what the purpose is of this one. <br> # M2 Bending modes M2_1um_grid.fits.gz - source = IM/data/M2/M2_1um_grid.DAT - shape = (15984, 75) - Each row is one of 15984 FEA nodes. - 0th column is node index ? - 1st and 2nd columns are FEA node x and y in M2 CS - Last 72 columns are bending modes; the z-displacement of each node for each mode. M2_1um_force.fits.gz - source = IM/data/M2/M2_1um_force.DAT - shape = (72, 75) - Each row is one of 72 bending modes. - 0th column is actuator ID - 1st and 2nd columns are actuator x and y in M2 CS - Last 72 columns are forces in Newtons for each mode. # M2 print through / thermal M2_GT_FEA.fits.gz - source = IM/data/M2/M2_GT_FEA.txt - shape = (9084, 6) - Each row is one of 9084 FEA nodes. (Why aren't these the same as above? I don't know.) - Columns are: - 0: Unit-Normalized FEA x - 1: Unit-Normalized FEA y - 2: Zenith print through dz coefficient - 3: Horizon print through dz coefficient - 4: z temperature gradient dz coefficient - 5: r temperature gradient dz coefficient <br>

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2023-09-27
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