NYT: GIMBAL Video of U.S. Navy Jet Encounter with Unknown Object

Ah, that makes sense. It's MidIR, so an InSb (indium-antimonide) array. I've never use one, but, AFAIK, blooming can happen in an InSb focal plane array. Here's a paper about it, with figures, but it's behind a paywall. Maybe someone can find a better source.

Discrimination between electronic and optical blooming in an InSb focal-plane array under high-intensity excitation.
Here's a cheat sheet on page 9 of the PDF file.
https://www.raytheon.com/sites/defa...9/05/Raytheon_TechnologyToday_Issue2_2019.pdf
1625609751630.png
 
The Chilean UFO is not defined.

You can see two distinct heat sources flickering with poorly defined edges. What you would expect looking at the exhaust of a jet engine (airliners have engines wide apart). What you are seeing in the Chilean video is not just "glare". It's simply the hot gases pointing directly towards the camera. That is why they are not a solid shape. They flicker as the gasses diffuse in the atmosphere.

Just like this video shows clearly:

Source: https://twitter.com/DaveFalch/status/1278856646954029057


Gimbal does not flicker. The edges are solid and not undefined. It doesn't look like a jet exhaust.

It could be glare from a solid powerful IR source (e.g. not a flare burning as it would flicker but a hot space capsule reentering? or an IR laser pointing at the camera?).

I think you're correct in so much as the GIMBAL video does not, in my opinion, closely resemble any of the examples of IR glare that have been presented. You can get something of an aproximation with some handwaving but the fact of the matter is that the GIMBAL object appears as far more of a steady and precise image.
 
I think the major problem with the `rotating glare caused by rotating window' hypothesis lies in the ATFLIR optics.

The ATFLIR optics is basically an extreme telephoto lens, constructed with mirrors instead of lenses. The first mirror (12 in the picture) is the entrance area of the lens:
1625737446228.png
(picture was taken from one of the Raytheon patents)

The angle, not the location, of incoming light rays determines at which pixel these rays end up.
In other words: Every pixel is created by the sum of all light rays falling onto the whole entrance mirror area at exactly the angle associated with this pixel.
The range of incoming light ray angles that ultimately land in the image is extremely small because of the small field of view and long viewing distance of the ATFLIR:

1625738863620.png

Smudges or damage on the wind screen will have two effects on the incoming rays:
1. They block them.
2. They scatter them.

Rays that are blocked are not a big problem. As long as enough rays reach the image area to reconstruct the pixels, the image can still be constructed perfectly:
1625738900340.png

Scattered rays can become visible, but they will affect all pixels in the image area since they will be scattered all over the angular FOV of the ATFLIR (which is in the order of one degree). Since the angle of incoming rays determines at which pixel they end up, scattering will cause a fog-like glare over the whole image:
1625737758557.png
This is the fog-like glare that you see rotating with the object.
It is only logical to see it rotating with the object, because the image-wide scattering pattern of the object's incoming rays, caused by dust, insects, etc on the wind screen, will change a little bit when the object rotates.

You can see a demonstration of similar effects with an optical lens in the video below. Note that the telephoto lens setting in this video best represent what happens in the ATFLIR:


According to a comment from Dave Falch, which can be found at one of his Youtube videos, the FLIR optics acts in the same way:
1625738069371.png
 

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I disagree with that logic. You're basically saying "all smudges are small". I cite as a counter-example ... a large smudge smeared across the whole of the front of the optics. Who could possibly have seen that coming?!

That would not change much, unless this large smudge manages to keep its diffraction/scattering of the light within much less than one degree.
The FOV of the ATFLIR is about one degree, so for the diffraction/scattering to land in about 10% of the image it should stay within 0,1 degree (order of magnitude) over the entire smudge area. The scattering should be pretty consistent as well, otherwise not enough light will hit the area around the object in the final image (20 in the picture) to be in the saturation range of the imaging electronics. That's a pretty special smudge..
On top of that the smudge diffraction/scattering would affect every pixel, so the clouds should be blurry as well, and this blur around the clouds should rotate with the gimbal, too.
1625746406874.png
 
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Yes. So if a smudge only scatters light a little (I.e., into a small cone) it will create an enhancement around every bright object in the field. The clouds already have fuzzy edges and are not nearly as bright as the main object so you don’t see the enhanced scatter. The main object is bright, probably saturating at the center, so it’s easier to see the impact of the mild scattering. Much the same way that a telescope with a secondary spider will show diffraction spikes around bright stars but not around dimmer, extended objects like planets or nebulae.
 
Yes. So if a smudge only scatters light a little (I.e., into a small cone) it will create an enhancement around every bright object in the field. The clouds already have fuzzy edges and are not nearly as bright as the main object so you don’t see the enhanced scatter. The main object is bright, probably saturating at the center, so it’s easier to see the impact of the mild scattering. Much the same way that a telescope with a secondary spider will show diffraction spikes around bright stars but not around dimmer, extended objects like planets or nebulae.
The scattering must be (1) very consistent and (2) very concentrated to cause a delineated black image saturation spot like that.

Diffraction spikes of a telescope are caused by edge diffraction along the edge of telescope vanes. This type of diffraction is (1) very consistent (it is the same along the entire vane) and (2) not very concentrated (it spreads out, which is why the spikes are spread out while diminishing in intensity along the length of the spikes).
So even a telescope vane, which is very consistent and symmetrical, cannot cause a delineated spot like the gimbal. Let alone an accidental smudge over the ATFLIR window surface.

The video I posted above with the photographic lens damage is also very telling.

As soon as the telescope vanes are curved or less straight at the edges, the diffraction spikes are turned into a veiling glare (though the symmetry of the vanes sometimes causes some vague interference patterns in the glare). This veiling glare is not well delineated and of much less intensity than the star. A smudge on the window cannot cause these kind of effects, it will never be as symmetrical and consistent.
1625758896349.png1625758960662.png
 
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I lost track on the scatter discussion. I used to have a TMA model (Zemax) Well I still have it, but no Zemax anymore (changed jobs). If I would still have it, I could play a bit to see if we can reproduce the images discussed..
 
A smudge on the window cannot cause these kind of effects, it will never be as symmetrical and consistent.

and yet the effect rotates at exactly the moment you might expect the gimbal to rotate and when other artifacts in the scene rotate. It’s definitely suspicious.
 
and yet the effect rotates at exactly the moment you might expect the gimbal to rotate and when other artifacts in the scene rotate. It’s definitely suspicious.
That's only partly the case; the first rotations come a bit earlier.

The background veiling glare that rotates with the object is not that remarkable, you would expect this to happen, too, if a bright object outside rotates. It could simply be veiling glare caused by the normal dirt that accumulates on the ATFLIR front window.

The object does rotate most when the jet is pointing its nose at it. And then there are these strange jolts in the optics that seem to prelude the object's rotation.
I wonder if these jolts could be caused by triggering the laser range designator (LRD). One would expect a small final fine-tuning of the ATFLIR boresight alignment at that moment. The object rotation could be a response to the laser being pointed at it.

As a pilot I would really like to have a range when I'm flying head-on towards an object of unknown size. If the radar did not give me one I would try the LRD. That could explain the fact that most of the object's rotation takes place when the jet is flying straight towards it.
 
That's only partly the case; the first rotations come a bit earlier.

The background veiling glare that rotates with the object is not that remarkable, you would expect this to happen, too, if a bright object outside rotates. It could simply be veiling glare caused by the normal dirt that accumulates on the ATFLIR front window.

The object does rotate most when the jet is pointing its nose at it. And then there are these strange jolts in the optics that seem to prelude the object's rotation.
I wonder if these jolts could be caused by triggering the laser range designator (LRD). One would expect a small final fine-tuning of the ATFLIR boresight alignment at that moment. The object rotation could be a response to the laser being pointed at it.

As a pilot I would really like to have a range when I'm flying head-on towards an object of unknown size. If the radar did not give me one I would try the LRD. That could explain the fact that most of the object's rotation takes place when the jet is flying straight towards it.

As far as I know the ATLFIR LASER is not used for ranging aerial targets, if it fires there is an indicator showing it fires.

The LASER is for ground target designation and ranging and has a range limit.
 
As far as I know the ATLFIR LASER is not used for ranging aerial targets, if it fires there is an indicator showing it fires.

The LASER is for ground target designation and ranging and has a range limit.
Googled it:

The Raytheon ATFLIR has plug-and-play performance, and integrates advanced visible-light cameras and infrared sensors with a target laser designator to locate and designate targets day or night at ranges exceeding 40 nautical miles and altitudes surpassing 50,000 feet, Raytheon officials say.
Content from External Source
Source: https://www.militaryaerospace.com/s...79/electrooptical-infrared-targeting-avionics

Maybe one of the flight simulator users here can explain how it is operated, and whether we should see it on the ATFLIR screen if it is engaged?
 
Googled it:

The Raytheon ATFLIR has plug-and-play performance, and integrates advanced visible-light cameras and infrared sensors with a target laser designator to locate and designate targets day or night at ranges exceeding 40 nautical miles and altitudes surpassing 50,000 feet, Raytheon officials say.
Content from External Source
Source: https://www.militaryaerospace.com/s...79/electrooptical-infrared-targeting-avionics

Maybe one of the flight simulator users here can explain how it is operated, and whether we should see it on the ATFLIR screen if it is engaged?

That quote is misleading, the SIM docs which I have read a lot show you how the laser/when is used.

Perhaps you can read them as well if you are interested?

https://forums.vrsimulations.com/su...aser_Target_Designator.2FRanger_.28LTD.2FR.29

Laser Armed - The laser is initially commanded to ARM via the LTD/R ARM switch on the Sensor Control Panel. Full arming can only take place when:
  • Landing gear is up and locked
  • Aircraft in A/G Master Mode
 
Maybe one of the flight simulator users here can explain how it is operated, and whether we should see it on the ATFLIR screen if it is engaged?

This is the page from the manual, LTD/R will be clearly displayed if it is on as the laser is very powerful so it's treated like a weapon itself.
1625835674131.png

As this spot is blank in the video we know that this switch was set in the 'safe' position.

1625835984534.png

The purpose of the LTD/R is to designate a target for laser bombing. You set the ATFLIR on a ground target, then release a bomb, the laser will then fire automatically and that bomb will follow your laser to the target. The point in the range function is so that the bomb knows how far it has to go and can compute a time-to-impact and detonate it's fuse at the right time.

As far as I know the laser is never used in air-to-air modes, and never pointed at something the operator doesn't want to kill. Imagine a soldier pointing the laser on his rifle at civilians in order to find out how far away they are.

The Raytheon ATFLIR has plug-and-play performance, and integrates advanced visible-light cameras and infrared sensors with a target laser designator to locate and designate targets day or night at ranges exceeding 40 nautical miles and altitudes surpassing 50,000 feet, Raytheon officials say.
I would say that this doesn't mean you can designate targets that are 50,000ft high but instead means you can designate ground targets whilst staying 50,000ft in the air above them.
 
As far as I know the laser is never used in air-to-air modes, and never pointed at something the operator doesn't want to kill. Imagine a soldier pointing the laser on his rifle at civilians in order to find out how far away they are.
The 1-micron tactical laser target designator is blinding, but the 1.55 micron training laser is eyesafe. The laser marker is used as a laser pointer to mark a target for other targeting pods to pick up with their laser spot tracker. I'm not aware if ATFLIR uses the eyesafe laser for air-to-air ranging.

I would say that this doesn't mean you can designate targets that are 50,000ft high but instead means you can designate ground targets whilst staying 50,000ft in the air above them.
That's how I interpreted it. A fighter jet can designate ground targets from its maximum altitude.
 
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The 1-micron tactical laser target designator is blinding, but the 1.55 micron training laser is eyesafe. The laser marker is used as a laser pointer to mark a target for other targeting pods to pick up with their laser spot tracker. I'm not aware if ATFLIR uses the eyesafe laser for air-to-air ranging.
I always assumed the range in the Gofast video was measured with a laser. But maybe that's a radar range then?
 
Thanks. Lots of speculation but unfortunately no real answers. Flight simulators will only get you so far (otherwise it would be fairly easy for others to find the weak spots in US air defence), and the rest remains guesswork.
According to Raytheon's website,
Raytheon's Advanced Targeting Forward Looking Infrared pod delivers pinpoint accuracy and reliability for air-to-air and air-to-ground mission support.
Content from External Source
From an engineering viewpoint, it would be very hard to align a nose-mounted radar and a wing-mounted, detachable ATFLIR to one degree accuracy. It would be even harder if you want to be able to mount an ATFLIR under different jets.

To reliably get the range to the ATFLIR's boxed target specifically, radar and ATFLIR need to be aligned to 0,1 degree accuracy (the ATFLIR FOV is about 1 degree and a target covers about 10% of the FOV). So given these considerations I guess the LRD is the only device that can reliably tell you the distance to a boxed target since the LRD is fully integrated in the ATFLIR pod with advanced boresight alignment.
 
Thanks. Lots of speculation but unfortunately no real answers. Flight simulators will only get you so far (otherwise it would be fairly easy for others to find the weak spots in US air defence), and the rest remains guesswork.
According to Raytheon's website,
Raytheon's Advanced Targeting Forward Looking Infrared pod delivers pinpoint accuracy and reliability for air-to-air and air-to-ground mission support.
Content from External Source
From an engineering viewpoint, it would be very hard to align a nose-mounted radar and a wing-mounted, detachable ATFLIR to one degree accuracy. It would be even harder if you want to be able to mount an ATFLIR under different jets.

To reliably get the range to the ATFLIR's boxed target specifically, radar and ATFLIR need to be aligned to 0,1 degree accuracy (the ATFLIR FOV is about 1 degree and a target covers about 10% of the FOV). So given these considerations I guess the LRD is the only device that can reliably tell you the distance to a boxed target since the LRD is fully integrated in the ATFLIR pod with advanced boresight alignment.

Um no, RADAR can scan targets in a large area. The sources all say the laser is not used for ranging in air to air, this much is clear, you seem to be disregarding the evidence here.
 
Um no, RADAR can scan targets in a large area. The sources all say the laser is not used for ranging in air to air, this much is clear, you seem to be disregarding the evidence here.
What evidence? The manual of a flight simulator? Apart from that I haven't seen much evidence.

The Raytheon site says:
The streamlined ATFLIR integrates laser tracking and infrared targeting functions on F/A-18 aircraft into a single compact pod, freeing an air-to-air weapon station for other mission requirements.
Content from External Source
Meaning: you don't need two air-to-air weapon stations anymore (one for laser tracking and the other for infrared targeting) because we have integrated them both in a single pod.

Concerning the radar you seem to have misunderstood me. I was not talking about scan area but about the required accuracy and the required alignment accuracy between radar and ATFLIR as a logical result of that.
 
The background veiling glare that rotates with the object is not that remarkable, you would expect this to happen, too, if a bright object outside rotates. It could simply be veiling glare caused by the normal dirt that accumulates on the ATFLIR front window.

How would that work?

You seem to be positing that the saucer shape is the shape of the object, a hot object, but not hot enough to create a surrounding glare, but somehow hot enough to create a veiling glare?

This makes no sense.
 
How would that work?

You seem to be positing that the saucer shape is the shape of the object, a hot object, but not hot enough to create a surrounding glare, but somehow hot enough to create a veiling glare?

This makes no sense.
It seems he is imagining a scenario in which the dirt causes a primarily diffuse scatter, filling all field angles with some fraction of the primary light source, rather than a primarily forward scattering function, which would cause localized glares around bright objects in the field.

on my current project I contracted an optics company to do a scattered light analysis of my instrument’a optical system and they showed me scattering functions as related to cleanliness level, defined as a certain density of small particulates on optical surfaces, and all of the functions were greatly peaked around 0 degrees of scattering deviation.

I’m sure I could be wrong but I still believe that with dust or smudges you would see local glares around the brights objects and possibly additionally some broader scattered light across the field. But if I only saw the broad scattered light without the point glares I would think it’s from some kind of stray light source outside the field of view.

but it could be different with large dust particles or smudges than with the small amounts of contaminants my analysis was concerned with.
 
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It seems he is imagining a scenario in which the dirt causes a primarily diffuse scatter, filling all field angles with some fraction of the primary light source, rather than a primarily forward scattering function, which would cause localized glares around bright objects in the field.

on my current project I contracted an optics company to do a scattered light analysis of my instrument’a optical system and they showed me scattering functions as related to cleanliness level, defined as a certain density of small particulates on optical surfaces, and all of the functions were greatly peaked around 0 degrees of scattering deviation.

I’m sure I could be wrong but I still believe that with dust or smudges you would see local glares around the brights objects and possibly additionally some broader scattered light across the field. But if I only saw the broad scattered light without the point glares I would think it’s from some kind of stray light source outside the field of view.

but it could be different with large dust particles or smudges than with the small amounts of contaminants my analysis was concerned with.
These are the scatter functions of 1 micron (top figure) and 2,5 micron (bottom figure) dust particles for different wavelengths:
Screenshot_2021-07-11-09-45-52-026~2.jpeg
Screenshot_2021-07-11-09-32-59-490~2.jpeg

Source
For a scattering angle from 0 to 1 degree, the FOV of the ATFLIR, the scattering intensity is almost uniform. This means the scattering glare will be evenly distributed over the entire image, not localized around the object.

1 to 2,5 microns is a typical dust article size:
Screenshot_2021-07-11-09-43-59-245~2.jpeg
Source
 
@Itsme , The graphs you show are related to mie scattering (volume scattering).
I was always using BRDF to look into stray light of optics. (https://en.wikipedia.org/wiki/Bidirectional_reflectance_distribution_function)
With BRDF you can model/predict straylight inside an optical system, as it relates to surfaces (of optics).

If you look below, you see that the "glossy" component (uniform roughness of optics) is distributed more wider, angularly, as opposed to the "specular" distribution (dirt/particles/smudges).

1-s2.0-S0263224118303725-gr2.jpg
source
 
You're still assuming isotropy. Smears are highly anisotropic. Highly correlated with the direction of the last wipe of the cloth that cleaned them.

Also, dust clouds are irrelevant here - this is an extremely thin layer, not an extensive diffusive medium.
 
@Itsme , The graphs you show are related to mie scattering (volume scattering).
I was always using BRDF to look into stray light of optics. (https://en.wikipedia.org/wiki/Bidirectional_reflectance_distribution_function)
With BRDF you can model/predict straylight inside an optical system, as it relates to surfaces (of optics).

If you look below, you see that the "glossy" component (uniform roughness of optics) is distributed more wider, angularly, as opposed to the "specular" distribution (dirt/particles/smudges).

1-s2.0-S0263224118303725-gr2.jpg
source

The 'R' in BRDF stands for Reflection. We're talking about transmission here, transmission through the ATFLIR windscreen:
Screenshot_2021-07-11-17-31-10-168~2.jpeg

I think mie scattering is a good approximation for dust particles caught on/in the windscreen. The additional transition in refractive index (air to window) will probably only make the scattering function even wider.
 
You're still assuming isotropy. Smears are highly anisotropic. Highly correlated with the direction of the last wipe of the cloth that cleaned them.

Also, dust clouds are irrelevant here - this is an extremely thin layer, not an extensive diffusive medium.
Dust is very relevant here, see ATFLIR windscreen picture above.
I'm only assuming near isotropy in the first degree of scattering, because that's the only scattered light that will travel to the imaging electronics via the optics. The (an)isotropy of the rest of the scattered light is irrelevant.
 
And please keep in mind that the ATFLIR does not in any way image the front window, see post above. Basically that's why it is so insensitive to dust and smudges on that window. But it's a hard concept to get into your head, it's tempting to imagine the ATFLIR 'looking through the window'.
 
These are the scatter functions of 1 micron (top figure) and 2,5 micron (bottom figure) dust particles for different wavelengths:
Screenshot_2021-07-11-09-45-52-026~2.jpeg
Screenshot_2021-07-11-09-32-59-490~2.jpeg

Source
For a scattering angle from 0 to 1 degree, the FOV of the ATFLIR, the scattering intensity is almost uniform. This means the scattering glare will be evenly distributed over the entire image, not localized around the object.

1 to 2,5 microns is a typical dust article size:
Screenshot_2021-07-11-09-43-59-245~2.jpeg
Source
I’ve attached an image of a series of BSDFs I received from an optical engineer doing a scattered light analysis of an instrument I am working on. There are a few different ones but focus on the higher set, which correspond to what’s called CL400, a specific cleanliness level that correlates to a certain particle size distribution (i don’t have that at hand). The lower set is from surface roughness of the optics and is negligible in comparison.

You’ll notice a couple of things. These scattering functions are highly specular, especially compared to the functions you posted above. For example, for the blue curve in the middle, angle of incidence is zero degrees, by ten degrees out it is at least an order of magnitude lower than your curves.

I admit that perhaps these curves are not appropriate for this situation but we’d have to figure out what really is. I don’t believe that your plots, and even mine, are definitive answers. But I do know the plots I’ve seen are specifically for examining the impacts of light scattering from optics. It seems your source is for laser scattering through air with particulates, like for measuring pollution.

If my optics had a really bad smudge we’d have to have them cleaned and wouldn’t fly with that. We even expect that the CL400 is too high for us, given that most of the optics will be assembled in a clean room.
 

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The 'R' in BRDF stands for Reflection. We're talking about transmission here, transmission through the ATFLIR windscreen:

BSDF and BTDF are the equivalent of the reflection version, and are the same function. But I stand corrected.
 
Dust is very relevant here, see ATFLIR windscreen picture above.
I'm only assuming near isotropy in the first degree of scattering, because that's the only scattered light that will travel to the imaging electronics via the optics. The (an)isotropy of the rest of the scattered light is irrelevant.
I just realized I can make this statement a bit stronger: I only assume there is NO anisotropy in scattered light over the angular size of the object in the Gimbal video. I guess that's in the order of 0,1 degree.
 
Dust is very relevant here, see ATFLIR windscreen picture above.
I'm only assuming near isotropy in the first degree of scattering, because that's the only scattered light that will travel to the imaging electronics via the optics. The (an)isotropy of the rest of the scattered light is irrelevant.

Wow. Way to misquote. You can't go from "dust clouds are irrelevant - this is an extremely thin layer, not an extensive diffusive medium." to "Dust is very relevant" unless you're literally prepared to just throw away they entire argument of your interlocutor. In which case, goodbye.
 
I’ve attached an image of a series of BSDFs I received from an optical engineer doing a scattered light analysis of an instrument I am working on. There are a few different ones but focus on the higher set, which correspond to what’s called CL400, a specific cleanliness level that correlates to a certain particle size distribution (i don’t have that at hand). The lower set is from surface roughness of the optics and is negligible in comparison.

You’ll notice a couple of things. These scattering functions are highly specular, especially compared to the functions you posted above. For example, for the blue curve in the middle, angle of incidence is zero degrees, by ten degrees out it is at least an order of magnitude lower than your curves.

I admit that perhaps these curves are not appropriate for this situation but we’d have to figure out what really is. I don’t believe that your plots, and even mine, are definitive answers. But I do know the plots I’ve seen are specifically for examining the impacts of light scattering from optics. It seems your source is for laser scattering through air with particulates, like for measuring pollution.

If my optics had a really bad smudge we’d have to have them cleaned and wouldn’t fly with that. We even expect that the CL400 is too high for us, given that most of the optics will be assembled in a clean room.

By the way, the plots you show (1 um and 2.5um dust particles) are limited to 850nm. As you can see the curves broaden when going to longer wavelengths. This is what I mentioned before: IR is more prone to straylight and diffraction effects. So you cannot claim anything using the plots provided. BR(S/T)DF has to be used to observe the effect caused by optics+particulates.
 
By the way, the plots you show (1 um and 2.5um dust particles) are limited to 850nm. As you can see the curves broaden when going to longer wavelengths. This is what I mentioned before: IR is more prone to straylight and diffraction effects. So you cannot claim anything using the plots provided. BR(S/T)DF has to be used to observe the effect caused by optics+particulates.
Of course I can. If the curves broaden with growing wavelength, the part between 0 and 1 degree will be even more homogeneous in mid IR, which only strengthens my arguments.
 
Of course I can. If the curves broaden with growing wavelength, the part between 0 and 1 degree will be even more homogeneous in mid IR, which only strengthens my arguments.
You overlook/ignore my next sentence: "So you cannot claim anything using the plots provided. BR(S/T)DF has to be used to observe the effect caused by optics+particulates.
 
Wow. Way to misquote. You can't go from "dust clouds are irrelevant - this is an extremely thin layer, not an extensive diffusive medium." to "Dust is very relevant" unless you're literally prepared to just throw away they entire argument of your interlocutor. In which case, goodbye.
So, you seem to think you can fly a jet from an aircraft carrier with a big smudge of non-evaporating (i.e. fatty) fluid on the ATFLIR wind screen without it collecting dust?

I appreciate the efforts to evade the logical conclusion from this discussion, but in the end it's unavoidable: Something else must be responsible for the rotating black blob on the ATFLIR imaging electronics. It cannot be something on the ATFLIR wind screen because:
1. The ATFLIR optics shows this would require something on that screen with a mid IR scattering pattern that is highly concentrated in just 0,1 degrees, and consistently so over a large area of the wind screen surface, see post #764 above.
2. Every natural cause of mid IR scattering has a much broader scattering curve than this, see discussion above.
 
You overlook/ignore my next sentence: "So you cannot claim anything using the plots provided. BR(S/T)DF has to be used to observe the effect caused by optics+particulates.
"So you cannot claim anything using the plots provided.": Yes I can, see my previous answer.
"BR(S/T)DF has to be used to observe the effect caused by optics+particulates.": Why? It only takes surface structure into account, not surface contamination.

And what does this image tell exactly?
1626086929590.png

That specular reflected light bends back into itself?

It's just an illustration, not measured data.

IF you would like to use BRDF, you should use the directional diffuse component, defined as:
It arises from diffraction and scattering by the surface roughness.
Content from External Source
Source: http://www.graphics.cornell.edu/~westin/multimedia-paper/node7.html

It is illustrated in the picture below (again, just an illustration).


1626088321574.png

The specular component does not model diffraction or scattering, but sharp mirror-like reflection, see http://www.graphics.cornell.edu/~westin/multimedia-paper/node6.html
 
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So, you seem to think you can fly a jet from an aircraft carrier with a big smudge of non-evaporating (i.e. fatty) fluid on the ATFLIR wind screen without it collecting dust?
No. Show me which sentence gave you that impression.
 
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