Tuesday, August 11, 2009

Effects Of Whippets On The Body

The histogram

The histogram of a digital image is a graphical representation of the number of pixels for each value of intensity.

I find it useful to explain this with a simple analogy: imagine that we create an image with the values \u200b\u200bof the coins of our currency: Any currency is a primary portion of the image (typically associated with what we usually call "pixels") and each coin is obviously associated with a value in cents or in Euro (associated to what we usually call ADU (Analog to Digital Unit "is the unit of luminous intensity of a pixel). Clearly the analogy is not perfect, in fact the most valuable coins are not the brightest (maybe this is why I managed to create a recognizable image ...)

Anyway, here on a composition that should give the idea of a composite image of coins.

What is the histogram of this composition? Very simple: just pick up the coins, sort them by value, and rearrange them in a row from lowest to the higher in order to immediately identify which values \u200b\u200bare more in the image.

It is clear that the values \u200b\u200bare more prevalent than those of 1 and 2 cents, while less frequent by 5 cents and 2 euros.

Thus the histogram is nothing but a "frequency distribution" ordered by the smallest value to largest value.

But apart from the mathematical definition of what good practice can be a histogram? For normal photography
land histogram can indicate, for instance if the subject is too "overexposed" or otherwise "underexposed" In the first case you would notice a spike in values in the right histogram, namely that corresponding to the brightest pixels in the second case to the contrary, the peak values \u200b\u200bwe would have left the histogram. The histogram clearly also depends on the subject of the picture, especially in the case of astronomical photographs. Let's look at a few examples compared with a normal photograph "Earth." To simplify the discussion, all samples are in black and white and processed 8 bits (256 levels of gray).

The first picture is a classic popular astronomical object: a comet. Even in the case of other entities such as galaxies or nebulae, however, the histogram does not differ much from that mostrato sulla destra. Abbiamo una forte concentrazione di pixel poco luminosi, ovvero sulla sinistra dell'istogramma seguito da un graduale presenza di pixel via via più luminosi. La prima concentrazione altro non rappresenta che il numero di pixel del fondo cielo: non a caso il picco si attesta attorno ai valori 12-13 ADU, proprio quelli indicati come valore di fondo cielo dell'immagine (vedi il valore B nella barra di stato sotto l'immagine). La seconda parte dell'istogramma rappresentato dalla "coda" di valori via via più luminosi identifica la chioma e la coda della cometa con le stelle comprese nel campo di ripresa. Si noti poi il picco intorno al valore 255 ovvero il valore più luminoso per un'immagine a 8 bit: si tratta di tutti quei pixel concentrati in the more luminous (and often saturated) image as the center of the comet's coma and the saturated star in the upper right.


The second image is a typical extended astronomical object as a planet: Mars. Note now that in this case the sky background image is completely black (B = 0) and that it immediately identifies with the peak vertical histogram at the value 0. The rest of the histogram reflects changes in the gray surface of the planet. The greater the number of pixels around the number 150 and represent the surface of the planet while the lighter brighter focused nell'intorno cap polar and cover a range of values \u200b\u200bfrom 230 to 255.

Finally, as a third example, a typical figure ground: a human face. In a correctly exposed photograph and includes a balanced view of the entire range of gray values \u200b\u200bfrom 0 to 255 with the appearance of the histogram is almost flat.

Sunday, April 26, 2009

Gay Bodybuilders In Nj

The postprocessing 2 - Color Calibration

Our goal is simple yet ambitious: we want to create an image of the planetary nebula in color, which is as close as possible to view "real" object, just as if we were floating in space near of M27.

using any image editing program, we soon realize that the manipolazione dei colori così come della luminosità o del contrasto, ci porta a creare centinaia di modalità di visualizzazioni, a volte molto differenti l'una dall'altra.
Questi potenti strumenti informatici, più che aiutarci, così come avviene nelle fotografie terrestri tradizionali, in questo caso ci disorientano e ci lasciano perplessi: quali sono i veri colori degli oggetti celesti?

Le nostre incertezze sono dovute al fatto che non abbiamo nella nostra memoria visiva un'immagine "reale" di confronto, come può avvenire per gli oggetti terrestri: il rosso "Ferrari" , per fare un esempio, sappiamo com'è e possiamo più o meno avvicinarci ad esso se abbiamo necessità di equilibrare i colori di una foto sportiva fatta ad un Gran Premio. Con tecniche più oggettive, i fotografi professionisti utilizzano la tecnica del "bilanciamento del bianco" che consiste nell'equilibrare i tre canali RGB fondamentali in modo tale che un oggetto bianco o grigio abbia gli stessi valori di pixel nel rosso, nel verde e nel blu.
Ma il rosso delle emissioni H-alfa presente in tante nebulose (compresa questa) come appare nella realtà? Anche con telescopi di grande apertura e sotto cieli incontaminati è difficilissimo cogliere i reali colori di nebulose galassie e comete perchè i nostri occhi lavorano in regime di bassissima illuminazione: siamo in una situazione di visione scotopica : i nostri eyes have difficulty distinguishing differences in chromaticity and everything seems almost "black and white" (and this can be also found in terrestrial normal night vision).

But just as there is a reference to "ground" for white, even in astronomy, we can use a "light blue" reference: our Sun, or rather, the stars, like our Sun, are of a very precise and determined the spectral class : the G2V . Just like the sunlight at noon (well, at the zenith) is considered the standard for white light earth, the stars of the same spectral class G2V may be taken as a reference standard for white in astronomical images.

A list of these reference stars you can find it here , along with the file. Tdf to identify them in the program GUIDE , truly global multi-functional and cost often use to support my observations.

Our set is images of M27 however, was not acquired with the intention of making use of the tri-color "aesthetic," so we have not taken one of these stars using the same instrumental set, we must be content with what we (often the case, unfortunately!)
To continue this short tutorial, but we can make a reasonable approximation: a star search in the field of view spectral type close to that reference.


Let's help once again GUIDE: This program can represent the stars with the color corresponding to the spectral class of membership (see above) and simply click the right button on the star to read the information available: the Class G stars are represented in yellow, and we immediately note that there may be two candidates to the east of the nebula. That lower, very bright, we must immediately discard as it is always overexposed, while a bit 'higher up, just below the variable DQ Vulpeculae, is nearly perfect: it is the HD 345452 and class spettrale G5, un pizzico più "arancione" del nostro Sole. Certamente questa piccola differenza non avrà un effetto tangibile nel nostro processo di calibrazione colore.


Abbiamo un'ulteriore fortuna: al momento della ripresa del set di immagini, M27 era ad oltre 70 gradi sopra all'orizzonte, quindi risulta praticamente nullo ogni effetto di arrossamento dovuto all'assorbimento atmosferico.

Ora che abbiamo tre immagini RGB equivalenti (stesso tempo d'esposizione) dello stesso oggetto ripreso con lo stesso identico set strumentale e per di più nella stessa serata, senza che l'oggetto abbia cambiato significativamente la propria altezza sul cielo, possiamo procedere al calcolo dei coefficients for color correction with the reference star HD 345452. The operation is very simple: for each image R, G and B flows are measured in ADU of the star sample, for example using the zoom window and using the pointer to "crown".


In the above we can see is the measurement of the stars: you choose a range for the pixels in central opening so as to contain most of the stellar flux (usually chooses an aperture equal to 4-5 times the FWHM of the evening). The status bar of the window are three numbers V, S and B: these are: the net flow of the full sky, flow includes the sky background and finally the local value of the background sky. Note the value V for the three images in R, G and B:

VR = 334173 = 211426 VG
ADU ADU ADU
VB = 103364

calculate the weights of the colors than, for example, the red channel we get

R = 334173/334173 = 1.00
G = 334173/211426 = 1.58
B = 334173/103364 = 3.23

Substituting these three coefficients corresponding to those calculated automatically by the dialog Astroart Tri , finally we get the picture with the colors balanced with respect to a star of spectral type similar to our Sun (see below).


If we compare the image above with the balanced automatically by Astroart will notice a difference: in this case, the automatic balancing favored the green and blue channels.

image above, properly balanced with a star of spectral type similar to that of the Sun, most stars appear yellow-orange that used for the calculation of the coefficients appears perfectly white, while investigating further, there are some stars with very special colors, from bright red to blue to blue (see image below).

1 - Variable DQ Vul: it is a giant red, variable type Mira . The white star in the low to his right is our reference star HD 345452, which is used for color balance.

2 - central star of M27 is a white dwarf and is a decided color azzurognolo.

3 - Variable " Goldilocks" is probably a long-period variable of the class "Mira". The feature that distinguishes this star is the curious circumstance that led to his discovery: do you think has been identified for the first time by an amateur astronomer in the Czech Republic comparing ... two magazine covers astronomical !

4 - A mysterious star that is characterized by the strong blue color.

In the chart above, a collection of spectra of stars of different spectral class: each spectrum has been separated in the scale of the relative brightness to avoid duplication (data taken from Pickles 1998).
As you can see the stars emit light across the visible spectrum band: the color (ie surface temperature) is determined by the position of peak brightness.

planetary nebulae, however, as well as supernova remnants or areas of star formation in galaxies, emit radiation bands much more isolated and restricted: it is said that have a range of "issue" characterized by rows of bright generated by ionized elements, especially hydrogen and oxygen. The color of such objects is therefore strongly influenced by these "gaps" in the emission of radiation and especially from our "vision system" or by the telescope, the CCD camera, and especially by the filters used for recovery.
To realize this mechanism is more convenient to construct a chart: 100 made a hypothetical emission intensity of the spectral line, or transmission of a filter or quantum efficiency of our CCD camera, we can draw respectively

lines most important issue of our planetary nebula (Hbeta to 486.1 nm, OIII to 495.9 and 500.7 nm and 656.3 nm in Halfa) represented by the continuous vertical lines;
the transmission curves of the filters B, V and R represented by the dotted lines;
of CCD quantum efficiency (QE) represented by a continuous curve of fuchsia.


The emission line two times ionized oxygen on OIII 500.7 nm is by far the most intense and therefore the one that dominates the brightness and color of the nebula. The second most important line is the intensity as the transition to hydrogen H alpha 656.3 nm. We note that the latter falls almost exclusively in the area of \u200b\u200bthe red filter, as it should happen as it is at a wavelength of the light spectrum decidedly in the red.
different and more delicate is the situation for the row of 'OIII about 500.7 nm: note that falls in the area of \u200b\u200binterference of the two filters B and V: in fact, there is also shown in color scale in the x-axis, 500 nm almost exactly the area seem to separate from the blue green color spectrum. Unfortunately, this dichotomy is not perfect just as well represented by the filters used: in fact the line of 'OIII filter V is intercepted by around 50% of its relative intensity. The same line but was intercepted by B filter only 7% of its intensity on! This is why the nebula appears to us so green!
To bring a little 'things we must give the same weight of the green to blue filter, ie, a simple ratio B = 0.5 / 0.07 = 7.14.

Back then 3 images in our RV and B of the nebula and with the command Tricromia Astroart apply to the following factors:


R = 1.00 G = 1.00 B = 7.14


The result? Here it is below.


If the two images side by side centered on the nebula, we can better appreciate the differences.

So, in summary, we have attempted an initial color calibration using the technique of spectral type star sample similar to our Sun which is a G2V star. The stars appear with colors consistent with their spectral classes but maintained a strong nebulous light green: so in real life? Probably not. In fact we have seen that these nebulae, unlike stars, they emit primarily on well-defined lines of the electromagnetic spectrum. In particular, M27 has a strong emission line three times ionized oxygen [OIII] which has the distinction of emitting around 500 nm, ie in the middle of the transition from blue to green spectrum.
Everything depends on how they act out the filters B and V (= G) used .
In particular, the V filter used for this set of shooting, trapping at least 50% of the issue, unlike the B filter that records only 7% (for the same course of time of exposure). To balance the colors (ie for 50% the contribution of the blue filter), we then multiplied by the coefficient of the color blue filter for an appropriate correction factor (in our case B = 0.5 / 0.07 = 7.14 while keeping R = 1 and V = 1). As
each filter is different (even the same filters of the same manufacturer are slight differences) should be compared to determine the influence of these OIE and redefine the line ratios of the RGB color.
so doing, however, we return to unbalance the colors of the stars.
It follows that, with only three RGB images, we could never make an image with stars and nebula simultaneously balanced colors.
Actually, you may correct the image of the heavy editing (though this is not our goal), or, even more complex and expensive, can be corrected using a fourth image, made with a narrow-band filter on the 500, 7 nm, or to be added in the band in blue or green band, after the color calibration of the method G2V star. We

Monday, March 9, 2009

Joe Jonas And Cerebral Palsy

The postprocessing 1 - Composition RGB

how to get a visa SCIENCE FRAME on a specific photometric band: the band Johnson V system. We do not have the time to make any specific analysis or calibration of the image. We just captured image by selecting the electromagnetic waves that correspond roughly to the green color of the electromagnetic spectrum. Since we have two other Johnson filter system, the filter B (λ 0 = 440 nm, FWHM = 100 nm) and the filter R (λ 0 = 700 nm, FWHM = 210 nm) we can simulate the composition of the tri-color RGB type , when in fact you are using il filtro V al posto del classico G (Green = verde).

Non ci resta quindi che riprendere altre due sequenze di immagini (e di FLAT FIELD ) esattamente come abbiamo fatto per il filtro V . Se il tutto avviene nella stessa serata e la nostra camera CCD è correttamente termostatata (mantiene la temperatura stabile sul punto di lavoro impostato ad esempio a -30 °C +/- 1°C) e se utilizziamo gli stessi tempi d'esposizione, possiamo anche evitare di riprendere i DARK FRAME ed utilizzare quelli già ripresi durante la sequenza in filtro V.

Alla fine del processo di pretrattamento di tutte e tre le sequenze di immagini, ci troveremo un desktop come quello illustrato sopra. Notate come lo stesso oggetto, ripreso con i 3 filtri, appare sostanzialmente differente, non solo nella intensità luminosa (particolarmente accentuata con il filtro V, nell'immagine al centro), ma anche nei particolari, come nell'immagine in R posta in primo piano.

La realizzazione di una composizione RGB utilizzando Astroart è estremamente semplice: mantenendo aperte sul desktop le 3 immagini, con il comando Colore > Tricromia si aprirà la seguente finestra di controllo:


I tre pulsanti in alto permettono di selezionare l'immagine corrispondente ad ognuna delle tre bande colore mentre il triangolino nero in basso on the right expands the window with a preview image. If this is how we activate it appears:

image, somewhat psychedelic, is due to the fact that the three frames are not yet aligned with each other: Astroart can do it on the fly without exiting the dialog Tri: just click on the small button just to the right with the two squares superimposed Astroart use its powerful algorithms for automatic alignment to display the correct alignment of the frame:

ignored for the moment and the other small buttons we click the plus sign check green to get the final image:

The background sky is dark and the stars correctly, apart from the lack of blooming is particularly accentuated in the red channel, seem to have a different color as one would expect for stars of different spectral and therefore different temperature. But the nebula? It seems very "green" with red-violet edges. It 's so that would appear to us if we had the power to bring us closer to a sci-fi spaceship "bastions of M27"? Probably not
: Astroart helps with his balance algorithm, to give a "rough" to the color calibration of the image but there are actually more correct tools to get a color calibration that better approaches the true vision of the human eye. And most importantly for this particular celestial objects, you must make some considerations, and then the corrections on their emission characteristics in the range of the visible spectrum.

In the next post we will see what these considerations. For the moment let's enjoy the video of this first step of postprocessing to create a tri-color with Astroart 4.0

Saturday, February 14, 2009

2010 Dolls By Jan Maclean

The preprocessing: 2 - "SCIENCE FRAME"

In previous arguments we have identified a number of digital elements that are normally used for astrophotography: the LIGHT FRAME and FLAT FIELD , with their dark frame, bias frame and . These four types of digital elements, they are actually arrays of numbers which, when combined, will produce the final image is correct (which we call SCIENCE FRAME). The term "correct" does not mean of course only from the aesthetic point of view but also from the photometric point of view (which is what most interests us).

photometrically corrected image is necessarily "better" because "pure", but the opposite is true: on the Net you see thousands of stunning astronomical images, but the vast majority of "impure", ie an end in themselves, generate ( often damaged) after hours of violence by various image-editing program. We amateur astronomers have the dangerous presumption to be able to overcome our shortcomings and technical equipment with a heavy and massive intervention of "image processing". To do what? Photo galleries of boring to be published with pride on our personal Web page. After all this is the ultimate goal of so many amateurs in the best case, however, after taking dozens of times throughout the Messier catalog along with more exotic and spectacular NGC, surely "get tired" and here, the amateur astronomer becomes a virtuoso "amateur astronomer" to search for the "photon lost."

It's time to do as the preprocessing classico di una serie di immagini riprese su una singola banda fotometrica: la banda V (visual) . Per le nostre riprese infatti utilizzeremo un filtro centrato all'incirca sulla banda V del sistema fotometrico di Johnson -Cousins: l'argomento filtri fotometrici è abbastanza complesso ma importante e merita una riflessione più dettagliata che faremo in futuro. Per il momento ci basti sapere che il nostro filtro V seleziona una banda di lunghezze d'onda centrate sui 522 nm e con un'ampiezza a metà altezza ( FWHM ) di 90 nm. In pratica stiamo selezionando una banda dello spettro elettromagnetico centrata sul colore verde della luce visibile.

L'oggetto astronomico al centro of our times is a famous planetary nebula: M27.
When point after the object and accurate focus can take a series of light frame as the one shown in the figure below.


The number of LIGHT FRAME is to shoot at their own discretion for the time we need to know that the greater the number of LIGHT FRAME and less "grainy" will be the final image (ie the better the signal-to- Final noise). The argument "signal to noise ratio is very important and will be addressed soon. In our case, were taken 5 LIGHT FRAME with an exposure time of 240 seconds each. Also for the exposure time there is no fixed rule adaptable to all situations: the only sure thing is that even in this case, the longer the exposure, the greater the signal to noise ratio of single LIGHT FRAME. Rather, the upper limit of exposure time may be dictated by the presence or absence of stars easily saturable just as you can see in the image above: The two brightest stars, one to the left and bottom right of M27 have an early blooming, clear signal that you have exceeded the limit of linearity CCD sensor (for aesthetic purists will see that you can correct this type of defect). Immediately after the
LIGHT FRAME will be the turn of the dark frames and bias frame: these are not strictly necessary unless, as in our case, the CCD camera has no problems with temperature stability during shooting of the different frames. The presence of bias frame in the window of the preprocessing of Astroart automatically instruct the program to make an optimization of several dark frames before creating the master dark frame to subtract the LIGHT FRAME.
Finally, it should return the flat field, taking care to maintain the optical train (same filter and same fire V) used during the resumption of LIGHT FRAME. In our case we used the technique of Master Sky Flat then we have ready for use FLAT MASTER FRAME.

Once you have all of our frames, we can finally fill in the file File window Pretreatment of Astroart: selezionamo the file folder and drag the same with a simple drag & drop in the corresponding boxes as indicated in the figure below:


At this point we have to tell the program how we want to do pre-processing: This stage is set in the Options folder window Pretreatment .

First we show that we want to "mediate" the 5 5 BIAS and DARK FRAME FRAME to create the MASTER DARK FRAME. Successivamente vogliamo allineare i 5 LIGHT FRAME (scegliendo l'opzione " Auto allineamento " con il metodo " Tutte le stelle ") per poi sommarli insieme ed ottenere l'immagine finale. La cartella Opzioni apparirà come nella figura qui sotto:


Ora possiamo lanciare il pretrattamento facendo click sul pulsante OK: in pochi secondi avremo sul nostro desktop la finestra con l'immagine finale aperta (SCIENCE FRAME) e 3 immagini ridotte ad icona in basso a sinistra: BIAS00.FIT, DARK00.FIT e FLAT00.FIT che sono rispettivamente i nostri MASTER BIAS FRAME, MASTER DARK FRAME e MASTER FLAT FIELD utilizzati nel processo: se desideriamo possiamo salvarli per utilizzarli in altri processi (il MASTER FLAT FIELD non ha comunque subito alcuna processo in quanto è lo stesso file salvato che avevamo trascinato nella finestra "Flat Fields" di prima ).

Tutto questo può sembrare un po' complicato descritto solo a parole: qui sotto tutti i passaggi sono mostrati in un breve video.



Abbiamo così creato il nostro primo SCIENCE FRAME dell'oggetto M27 in banda V: si tratta della somma di 5 esposizioni di 240 secondi, dunque l'integrazione totale equivale a 5 x 240 = 1200 secondi = 20 minuti. Se nella cartella Opzioni della finestra Pretrattamento avessimo scelto una option of combining different images, or " Media" or "Median " or " Sigma," the total integration time of the final image would always be equivalent to that of a single exposure, or 240 seconds .

Saturday, January 3, 2009

Planes Used In Movie Commando

The preprocessing: 1 - Sky-Master Flat

One of the most delicate and mysterious in a way that approaches for the beginner to astronomy is the construction of digital MASTER FLAT FIELD. In a previous post we have seen that there are basically two types of flat field: the Flat-Dome, made from an artificial light source is near the telescope, and the Sky-Flat , obtained by illumination the sky background during the hours of dawn or dusk. The latter type of flat field has the advantage of not requiring special equipment for recovery but requires some dexterity and speed of recovery of the frames during the short period of time, and some more attention in the processing of frames to create properly MASTER SKY FLAT.

Let us see what are the main steps to follow.

Before the shooting sequence of the flat frame, always remember:

1) use the exact same optical configuration used for the resumption of "raw" image: the same fire and the same filter.
2) Check the temperature of the CCD camera is stabilized and / or the fixed point set in the case of thermoelectric temperature control of the CCD.
3) to avoid gradients in the flat frame point the telescope at the zenith and hold off the chase

The first step is then to experiment to determine the correct exposure time based on the brightness of the sky: the goal is to shoot as many frames as possible in the flat short time before the complete darkness of the sky (if you are working during the sunset) and possibly a signal large enough: if we use a 16-bit CCD camera can impose, for example, an average value of the flat frame at least more than half of the range of linearity the CCD camera. In our case, having determined the linearity limit at 60000 ADU, just the flat frame are between 30000 and 60000 ADU. If you think about it is not a simple thing: we need evidence and a bit 'of experience to make the most of the time available (usually only a few tens of minutes). Of course, As the sky darkens and the average signal decreases may be necessary to increase the exposure time, in which case you must take note and remember to take a series of dark frames for the exposure time is longer.

We finally have a series of sky-flat frame like the one shown below:

Here's what a typical sky-flat frame: there are strips of some stars and even the passage of a weak satellite. Note in the status bar below the average backgroud (B = 31,456) in ADU.

As you can see there is no need to keep on tracking telescope on the contrary, keeping it off we make sure that there will be no overlap between a star and the other frame and we can effectively employ the combined median frames.

Note: still not uncommon to read that the number of flat frames or dark frames should be composed of an odd number of images to be combined mode median. This is really a thing of the past when the first astronomical image processing software algorithms implementavono limited and incomplete. The complete algorithm as implemented in modern software Astroart , but also considers the case of an even number of frames. In particular, it establishes that, to calculate the median of n data:
1. n you sort data in ascending or descending order;

2. if the number of data is odd the median is the middle value, whichever is occupying the position (n + 1) / 2.
3. if the number of data n is even, the median is estimated using two values occupying the position (n / 2) and (n / 2 + 1) (generally choose their arithmetic mean). The combination


median is essential for the success of SKY MASTER FLAT: it is the only combination that eliminates the streaks of stars or satellites or other steps "defects" at random and different on each sky -flat frame. To function, however, requires a fundamental requirement: All frames must have approximately the same average value, is said to be "normalized .
If we had taken the flat frame under a constant light source (as in the case of Flat-Dome) this requirement would undoubtedly have been reached without any further steps and we could obtain the master flat field immediately using the appropriate options in the dialog Pretreatment of Astroart. Unfortunately, in our case, the brightness of the background sky changes rapidly during the minutes of twilight and the consequence is that all the sky-flat frame has a mean value different from each other: it is therefore necessary to normalize the same average value of reference.

To proceed with the normalization we have to perform two additional steps.
First subtract each sky-flat frame MASTER DARK FRAME corresponding individually and save the sky-flat frame as correct.

The first page "File" box Pretreatment of Astroart take a look something like this:

In our example we have 10 sky-flat frame (taken with the red filter) and 10 dark frames . Note that in order to save individual sky-flat frame, these should be included in the "Images" rather than in that of the "Flat Field".

While the second page "Options" should be configured as follows:

you click on "OK" we get in our 10 new workbook file with the same file name of the sky-flat frame a suffix " _P" file to indicate that they are "processed" means the program will automatically calculate the MASTER DARK FRAME, it will be removed from the individual sky-flat frame, and saved the resulting files on your hard disk by affixing the suffix indicated.

We can now normalize these 10 rows processed. We need to create a macro and apply it (as shown in the windows below) to the group of files with the suffix "_P".

Use the online help to create and apply macros Astroart.

The "Normalize background" as used in macro takes one argument, a frame of reference from which obtain the normalization constant: just before running the macro, open one of the sky-flat frame processed Astroart desktop and select it when prompted during the launch of the macro.

Always following the setting of our example, we have now in 10 new workbook file named "NormFlatRxxx" where xxx is a sequential number. They are now our standard flat-sky that can be included in the "Flat Fields" box Pretreatment of Astroart (always remembering to select the "median" of the flat field on the "Options" in the same window):



The end result: the MASTER SKY-FLAT perfettamente corretto senza alcun residuo di stelle: