Measuring Seeing, The Differential Image Motion Monitor (DIMM) |
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Автор: Marc Sarazin. Чтобы познакомиться с картинкой полного размера, нажмите на её эскиз. Чтобы можно было использовать все картинки для урока английского языка, скачайте бесплатно презентацию «Measuring Seeing, The Differential Image Motion Monitor (DIMM).ppt» со всеми картинками в zip-архиве размером 1577 КБ.
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1 | Measuring Seeing, The Differential | 17 | Automated DIMM Operation. The system |
Image Motion Monitor (DIMM). Marc Sarazin | automatically switches to another star in | ||
(European Southern Observatory). | case of clouds The seeing is independent | ||
2 | List of Themes How to find the ideal | of cloudiness (although sometimes pretty | |
site...and keep it good? Optical | good with high cirrus clouds) Aperture | ||
Propagation through Turbulence Mechanical | photometry alows to monitor the sky | ||
and Thermal Index of Refraction Signature | variability. July 2001. Zanjan, Iran. 17. | ||
on ground based observations Correction | 18 | Automated DIMM Operation. Aperture | |
methods Integral Monitoring Techniques | photometry on ca 5000 DIMM short exposures | ||
Seeing Monitoring Scintillation Monitoring | allows to monitor the flux variability, | ||
Profiling Techniques Microthermal Sensors | equivalent to the extinction variability | ||
Scintillation Ranging Modelling | (June 2000 statistics below). The | ||
Techniques. July 2001. Zanjan, Iran. 2. | threshold for photometric sky is between | ||
3 | Why Differential Image Motion? The | 1% and 2% relative flux rms. July 2001. | |
tracking errors are automatically | Zanjan, Iran. 18. | ||
subtracted The wind has no effect on the | 19 | DIMM Seeing vs. VLT Image Quality. | |
measurements The telescope optical quality | DIMM converts image motion into large | ||
is not important (nevertheless circular | telescope seeing with the assumption of an | ||
images are required, i.e. no coma allowed) | infinite outer scale of the turbulence. UT | ||
Easy to implement with state of the art | images turned out about 10% better than | ||
amateur astronomer detectors The DIMM | predicted by DIMM, confirming the finite | ||
gives two statistical estimates of the | character of the outer scale. Comparison | ||
same variable. July 2001. Zanjan, Iran. 3. | of DIMM seeing (Y axis), with FORS Science | ||
4 | Optical Propagation The Signature of | Verification (SV) Image Quality (X axis) | |
Atmospheric Turbulence. Seeing: (radian, | as processed by the SV team, corrected for | ||
??^-0.2). Fried parameter: ( meter, | zenith and 500nm. July 2001. Zanjan, Iran. | ||
??^6/5). July 2001. Zanjan, Iran. 4. | 19. | ||
5 | DIMM Principle. Two images of the same | 20 | Corrected DIMM Seeing vs. VLT Image |
star are created on a CCD, corresponding | Quality. DIMM converts image motion into | ||
to light having traveled through two | large telescope seeing with the assumption | ||
parallel columns in the atmosphere. July | of an infinite outer scale of the | ||
2001. Zanjan, Iran. 5. | turbulence. UT images turned out about 10% | ||
6 | DIMM Principle. The variance of the | better than predicted by DIMM, confirming | |
image motion through a circular aperture | the finite character of the outer scale. | ||
of diameter D depends on the seeing as: | Correcting for that effect is possible by | ||
The variance of the differential image | removing from the DIMM the share of the | ||
motion through circular apertures of | tilt of an 8m aperture. Comparison of DIMM | ||
diameter D, separated by d is: July 2001. | seeing (Y axis) after correction for outer | ||
Zanjan, Iran. 6. | scale, with FORS Science Verification (SV) | ||
7 | DIMM Principle. The final estimate of | Image Quality (X axis) as processed by the | |
the seeing is the average of both parallel | SV team, corrected for zenith and 500nm. | ||
and perpendicular motions. July 2001. | July 2001. Zanjan, Iran. 20. | ||
Zanjan, Iran. 7. | 21 | Corrected DIMM Seeing vs. VLT Image | |
8 | DIMM Principle. Error Budget for a 10% | Quality. DIMM converts image motion into | |
accuracy goal. The instrumental noise | large telescope seeing with the assumption | ||
(sampling, centroiding) is measured in the | of an infinite outer scale of the | ||
lab on fixed sources. The constant part | turbulence. UT images turned out about 10% | ||
can be subtracted out, the noise is the | better than predicted by DIMM, confirming | ||
remaining variance, about +/- 0.002 | the finite character of the outer scale. | ||
pixel^2, or 5% relative error at 0.2” | Correcting for that effect is possible by | ||
seeing. The plate scale is calibrated on | removing from the DIMM the share of the | ||
double stars of known separation The | tilt of an 8m aperture. Comparison of DIMM | ||
measurement noise might increase if the | seeing (Y axis) after correction for outer | ||
signal to noise ratio is too low: images | scale, with UT1 Science Verification (SV) | ||
with low SNR due to scintillation have to | Image Quality (X axis) as processed by the | ||
be rejected. The statistical noise is | SV team from Test Camera long exposures, | ||
inversely proportional to the square root | corrected for zenith and at 500nm. July | ||
of the number of samples in the time | 2001. Zanjan, Iran. 21. | ||
series. The relative error on the seeing | 22 | DIMM Seeing vs. Large Telescope Image | |
is about 6% for 200 exposures. The | Quality. DIMM converts image motion into | ||
temporal under sampling due to too long | large telescope seeing with the assumption | ||
exposure time: no way to correct for it | of an infinite outer scale of the | ||
because the velocity of the tilt is | turbulence. Assuming that the outer scale | ||
unknown. Interlacing two exposure times is | larger than the telescope aperture, a | ||
the best way to control. The very bad | first order correction is obtained by | ||
seeing (>2”) is over estimated because | removing the one axis image jitter | ||
the stellar image breaks into speckles. | (Gradient tilt) variance from the long | ||
July 2001. Zanjan, Iran. 8. | exposure FWHM: Outer scale correction | ||
9 | DIMM Precursor. A visual DIMM was used | coefficient to apply to the DIMM estimates | |
in the 60’s for site selection purposes in | of the image quality of a 8m telescope | ||
Chile and in Uzbekistan (photo: Maidanak | limited by the atmosphere, for 0 and 60 | ||
Observatory). See: J. Stock and G. Keller, | degree zenith angle, as a function of the | ||
1960, in Stars and Stellar System, Vol. 1, | observing wavelength (the following | ||
Chicago University Press. July 2001. | central wavelength of the bands [U, B, V, | ||
Zanjan, Iran. 9. | R, I, J, H, K, L, M, N] corresponding to | ||
10 | Portable DIMM Operation. Preparing for | [0.36, 0.44, 0.55, 0.64, 0.79, 1.25, 1.65, | |
nighttime measurements on the high chilean | 2.2, 3.4, 5.0, 10] in mm). July 2001. | ||
sites (5200m) in the vicinity of the ALMA | Zanjan, Iran. 22. | ||
project Source: Cornell Atacama project | 23 | Monitoring Turbulence Height with the | |
http://astrosun.tn.cornell.edu/atacama. | DIMM. Scintillation through DIMM apertures | ||
July 2001. Zanjan, Iran. 10. | of 10-12cm diameter can be related to the | ||
11 | Portable DIMM Operation. Alignment of | isoplanatic angle (Loos & Hogge, Appl. | |
C11 telescope mount on a high chilean site | Opt. 18, 15; 1979) and then to the | ||
(5200m) in the vicinity of the ALMA | normalized 5/3rd moment of the turbulence | ||
project Pixel size=0.7” Pupil Diameter=9cm | height (Hbar). The atmospheric seeing | ||
Pupil Separation=12cm Exposure | (black lower curve, in arcsec) is the | ||
Time=10/20ms 50 frames/mn Photo credit: P. | cumulative effect of several turbulent | ||
Recabarren, Observatory of Cordoba, | layers at various altitudes: monitoring | ||
Argentina. July 2001. Zanjan, Iran. 11. | the characteristic altitude of the | ||
12 | Portable DIMM Operation. 1m high | turbulence (red upper curve, in km) is | |
platform and daytime protection of the | necessary for planning adaptive optics | ||
portable DIMM on the high chilean sites | instrumentation. In this example, the bad | ||
(5200m) in the vicinity of the ALMA | seeing is located at low altitude while | ||
project Source: Cornell Atacama project | good conditions are produced by a few | ||
http://astrosun.tn.cornell.edu/atacama. | layers at high altitude. July 2001. | ||
July 2001. Zanjan, Iran. 12. | Zanjan, Iran. 23. | ||
13 | Portable DIMM Operation. 5m high tower | 24 | Local Seeing: Ground Layer Turbulence |
and daytime protection of the portable | at Paranal. Measurement of the | ||
DIMM at the observatory of Maidanak, | microthermal activity and Seeing at | ||
Uzbekistan. The telescope stands in free | Paranal (GSM Campaign, Nice University) | ||
air circulation to prevent build-up of | during a night presenting variable | ||
local thermal pockets. July 2001. Zanjan, | conditions (F. Martin, R. Conan, A. | ||
Iran. 13. | Tokovinin, A. Ziad, H. Trinquet, J. | ||
14 | Automated DIMM Operation. Daytime | Borgnino, A. Agabi and M. Sarazin; Optical | |
protection of the automated DIMM at the | parameter relevant for high angular | ||
VLT Observatory The enclosure control is | resolution at Paranal from GSM instrument | ||
linked to the meteorological station | and surface layer contribution; Astron. | ||
(closes when wind>18m/s, Rh>80%). | Astrophys. Supplement, v.144, p.39-44; | ||
July 2001. Zanjan, Iran. 14. | June 2000). July 2001. Zanjan, Iran. 24. | ||
15 | Automated DIMM Operation. 35cm | 25 | Local Seeing: Seeing Impact of Ground |
Telescope for the automated DIMM at the | Layer. Measurement of the microthermal | ||
VLT Observatory Pixel size=0.7” Pupil | activity and Seeing at Paranal (GSM | ||
Diameter=11cm Pupil Separation=20cm | Campaign, Nice University): The | ||
Exposure Time=5ms 600 frames/mn. July | contribution of the layer 7-21m above | ||
2001. Zanjan, Iran. 15. | ground is marginal both during good and | ||
16 | Automated DIMM Operation. The seeing | bad seeing conditions . July 2001. Zanjan, | |
is updated every minute for zenith | Iran. 25. | ||
observation at 0.5 micron wavelength The | 26 | Conclusion. Intercalibration of the | |
accuracy is better than 10% above 0.2” The | site monitoring instruments is | ||
natural atmospheric noise is about 10% of | recommended. July 2001. Zanjan, Iran. 26. | ||
the seeing. July 2001. Zanjan, Iran. 16. | |||
Measuring Seeing, The Differential Image Motion Monitor (DIMM).ppt |
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