#################### PYOTE 5.1.0 session started: Sun Nov 3 16:07:25 2024 #################### filename: E:\ASTRONOMIA\1-Immagini CCD\Occultazioni\2024_11_02_(501) Urhixidur\Capture 2024-11-02T19_25_53Z\501_con pyote.csv If the csv file came from PyMovie - columns with prefix: signal will be read. ==================== file header lines ==================== # PyMovie Version 4.0.5 # source: E:\ASTRONOMIA\1-Immagini CCD\Occultazioni\2024_11_02_(501) Urhixidur\Capture 2024-11-02T19_25_53Z.adv # # Aperture photometry was used to extract the lightcurves # # lunar background: False # yellow mask = default: False # # aperture name: target # ____ aperture size: 31 # ____ x,y: (217, 129) at frame 1219 # ____ threshold: 1729 # ____ def mask radius: 3.2 # ____ color: green # ____ joggable: False # ____ auto textOut: False # ____ thumbnail source: False # ____ csv output order: 0 # # aperture name: reference # ____ aperture size: 31 # ____ x,y: (310, 130) at frame 1219 # ____ threshold: 1614 # ____ def mask radius: 3.2 # ____ color: yellow # ____ joggable: True # ____ auto textOut: False # ____ thumbnail source: False # ____ csv output order: 1 # # date at frame 0: 2024-11-02 #ADV-VERSION: 2 #ADVLIB-VERSION: 2.0 #ALTITUDE: 0 #BINNING-X: 2 #BINNING-Y: 2 #BITPIX: 16 #CAMERA-MODEL: QHY174M #CAMERA-SENSOR-INFO: ADC bit depth : 12 #EFFECTIVE-PIXEL-SIZE-X: 11.720000267028809 #EFFECTIVE-PIXEL-SIZE-Y: 11.720000267028809 #FSTF-TYPE: ADV #HEIGHT: 300 #LATITUDE: 46.23141783333333 #LONGITUDE: 9.024031666666666 #POSITION-REFERENCE: WGS84 #RECORDER-SOFTWARE: SharpCap #RECORDER-SOFTWARE-VERSION: 4.1.12196.0 #WIDTH: 480 #TIME-SOURCE: Camera GPS # # Aperture photometry was used to extract the lightcurves ==================== end header lines ==================== No time step irregularities found. timeDelta: 0.500141 seconds per reading timestamp error rate: 0.00% Home directory: C:\Users\stefa\AppData\Local\Packages\PythonSoftwareFoundation.Python.3.10_qbz5n2kfra8p0\LocalCache\local-packages\Python310\site-packages\pyoteapp We found C:\Users\stefa\Documents\model-examples already present. Adding any new examples ... Use min/max event to locate a "D and R" event has been selected minEvent: 5 maxEvent: 50 Number of candidate solutions: 54809 (using event min/max entries) New solver results... Integer (non-subframe) solution... sigB:14777.60 sigA:11971.85 B:164168.89 A:127225.65 in entryNum units: D: 580 R: 600 noise corr coefs: [1.00, 0.0599] (based on 1200 points) sigmaB: 14712.75 Subframe adjusted solution... sigB:14712.75 sigA:11873.76 B:164168.89 A:127225.65 in entryNum units: D: 580 R: 600 D(subframe): 580.0000 R(subframe): 600.0000 in frameNum units: D: 580 R: 600 D(subframe): 580.0000 R(subframe): 600.0000 ... end New solver results Error bar report based on 100,000 simulations (units are readings)... loDbar @ .68 ci: -0.4385 hiDbar @ .68 ci: 0.4638 loDbar @ .95 ci: -1.4822 hiDbar @ .95 ci: 1.3334 loDbar @ .9973 ci: -3.9235 hiDbar @ .9973 ci: 3.7950 loDurBar @ .68 ci: -0.7463 hiDurBar @ .68 ci: 0.7232 loDurBar @ .95 ci: -2.0414 hiDurBar @ .95 ci: 2.1404 loDurBar @ .9973 ci: -4.7657 hiDurBar @ .9973 ci: 4.6716 Timestamp validity check ... From timestamps at D and R, calculated 20 reading blocks. From reading blocks, calculated 20 blocks. Timestamps appear valid @ D and R ================= 0.68 containment interval report ================= B: 164168.89 {+/- 424.90} sigmaB: 14712.75 A: 127225.65 {+/- 2724.03} sigmaA: 11873.76 magDrop report: percentDrop: 22.5 magDrop: 0.277 +/- 0.023 (0.68 ci) snr: 2.51 D: 580.00 {+0.45,-0.45} (frame number) D: [19:30:42.9276] {+0.2256,-0.2256} seconds R: 600.00 {+0.45,-0.45} (frame number) R: [19:30:52.9305] {+0.2256,-0.2256} seconds Duration (R - D): 20.0000 {+0.7347,-0.7347} readings Duration (R - D): 10.0029 {+0.3675,-0.3675} seconds =============== end 0.68 containment interval report =============== ================= 0.95 containment interval report ================= B: 164168.89 {+/- 849.80} sigmaB: 14712.75 A: 127225.65 {+/- 5448.06} sigmaA: 11873.76 magDrop report: percentDrop: 22.5 magDrop: 0.277 +/- 0.047 (0.95 ci) snr: 2.51 D: 580.00 {+1.41,-1.41} (frame number) D: [19:30:42.9276] {+0.7041,-0.7041} seconds R: 600.00 {+1.41,-1.41} (frame number) R: [19:30:52.9305] {+0.7041,-0.7041} seconds Duration (R - D): 20.0000 {+2.0909,-2.0909} readings Duration (R - D): 10.0029 {+1.0458,-1.0458} seconds =============== end 0.95 containment interval report =============== ================= 0.9973 containment interval report =============== B: 164168.89 {+/- 1274.69} sigmaB: 14712.75 A: 127225.65 {+/- 8172.08} sigmaA: 11873.76 magDrop report: percentDrop: 22.5 magDrop: 0.277 +/- 0.070 (0.9973 ci) snr: 2.51 D: 580.00 {+3.86,-3.86} (frame number) D: [19:30:42.9276] {+1.9302,-1.9302} seconds R: 600.00 {+3.86,-3.86} (frame number) R: [19:30:52.9305] {+1.9302,-1.9302} seconds Duration (R - D): 20.0000 {+4.7187,-4.7187} readings Duration (R - D): 10.0029 {+2.3600,-2.3600} seconds =============== end 0.9973 containment interval report ============= D frame number: 580.00 D: 0.6800 containment intervals: {+/- 0.46} (readings) D: 0.9500 containment intervals: {+/- 1.48} (readings) D: 0.9973 containment intervals: {+/- 3.92} (readings) R frame number: 600.00 R: 0.6800 containment intervals: {+/- 0.46} (readings) R: 0.9500 containment intervals: {+/- 1.48} (readings) R: 0.9973 containment intervals: {+/- 3.92} (readings) Duration (R - D): 20.0000 readings Duration: 0.6800 containment intervals: {+/- 0.7347} (readings) Duration: 0.9500 containment intervals: {+/- 2.0909} (readings) Duration: 0.9973 containment intervals: {+/- 4.7187} (readings) =============== Summary report for Excel file ===================== This light curve has not been block integrated. This 'drop' has a zero probability of being an artifact of noise. >>>> probability > 0.0000 indicates the 'drop' may be spurious (a noise artifact). Consult with an IOTA Regional Coordinator. >>>> probability = 0.0000 indicates the 'drop' is unlikely to be a noise artifact, but does not prove that the 'drop' is due to an occultation >>>> Consider 'drop' shape, timing, mag drop, duration and other positive observer chords before reporting the 'drop' as a positive. All times are calculated/reported based on the assumption that timestamps are start-of-exposure times. It is critical that you make appropriate time adjustments when timestamps are NOT start-of-exposure times. If you use the North American Excel Spreadsheet report, all times will be properly corrected for camera delay and reported start-of-exposure times. For other users worldwide, use the appropriate corrections documented in the North American Spreadsheet report form - use the documentation shown on the Corrections Tables tab. magDrop report: percentDrop: 22.5 magDrop: 0.277 +/- 0.047 (0.95 ci) snr: 2.51 D time: [19:30:42.9276] D: 0.6800 containment intervals: {+/- 0.2256} seconds D: 0.9500 containment intervals: {+/- 0.7041} seconds D: 0.9973 containment intervals: {+/- 1.9302} seconds R time: [19:30:52.9305] R: 0.6800 containment intervals: {+/- 0.2256} seconds R: 0.9500 containment intervals: {+/- 0.7041} seconds R: 0.9973 containment intervals: {+/- 1.9302} seconds Duration (R - D): 10.0029 seconds Duration: 0.6800 containment intervals: {+/- 0.3675} seconds Duration: 0.9500 containment intervals: {+/- 1.0458} seconds Duration: 0.9973 containment intervals: {+/- 2.3600} seconds Enter D and R error bars for each containment interval in Excel spreadsheet without + or - sign (assumed to be +/-) =========== end Summary report for Excel file ===================== Solution 'envelope' in the main plot drawn using 0.95 containment interval error bars