Set foot on Titan with OPTIS!

How it's made! Discover how OPTIS created the first physically realistic insights of Titan!

September 21st, 2017 | Innovation

Titan and Saturn

The simulations you are about to discover are physics-based renderings of the surface of Titan, with a plausible terrain geometry. The sky diffusion, the sun direct illuminance, the dark surface spectrum and reflectance, and the haze properties come from the data collected by the Huygens probe of ESA's Cassini mission, during its descent and landing on January 14, 2005*.

 

The 3D environment features a terrain with the reflectance function and the spectrum of the dark areas of Titan, where Huygens landed. The sky corresponds to the configuration at the landing of Huygens with the sun at about 34-degree-polar angle. The data was taken from a radiative transfer simulation: it is dark near the horizon because no data was available below 89.3 degrees of polar angle. We included a 3D model of Huygens, with a measured reflectance function and spectrum of raw aluminum. We also have placed some pebbles randomly; they are rendered using a reflectance function corresponding to the bright areas of the surface, but still with the dark area spectrum. The haze features all major absorption and scattering sources: methane, Rayleigh and of course the Titan aerosol, defined with the single-scattering albedo and absorption and scattering coefficients. In some images, two LED spots have been placed to simulate what would be the effect of artificial lighting. They have a nearly conical intensity diagram and a 6500K LED spectrum: each has 100W of luminous power canted 45 degrees between nadir and horizon. The size of the total scene is 300m x 300m. The haze can barely be seen at these scales, the visibility near the surface is about 30km.

 

All data are spectral. The sky and sunlight sources range from 477 to 740nm because the DISR visible spectrometer starts at 477nm and the violet photometer was not included in this simulation. Radiance in wavelengths below 477nm is very low so this is still a good approximation. The surface spectrum ranges from 400 to 740nm and all atmospheric effects have been extrapolated down to 350nm to allow artificial light sources to interact fully with it. Colours in the images are computed from spectra using the CIE 1931 color matching functions that reproduce the human eye response.

 

The brightest point of images is defined to some value in candela per square meter (cd/m²), the adaptation value, given for each image. This unit has been chosen because of its relation to human vision, but W/m².sr values are also available in the simulation results if one is interested. In this case of fixed adaptation, the rest of luminance data in images is linear below this value. In some other cases where it is mentioned, images have been processed with the OPTIS human vision tool that applies a non-linear luminance mapping that uses the small dynamic range of 8-bit images in a way that looks similar to what the human eye would see, and the contrast of these images can be taken as what a 30-year-old human would see.

 

Before starting with the actual Titan simulations, to better understand the luminance levels at the surface of Titan, here is a rendering of the surface lit by a cloudless earth sky, 10 minutes after sunset (latitude 48 degrees N on April 27), which makes the sun about 2 degrees below the horizon. The light of the two LED projectors can be seen on the surface. The vertical field of view is 90 degrees, which is very wide, causing Huygens to appear distorted. Adaptation is 1000 cd/m². The black and white dots above the horizon are the points of emission of the LED projectors, back view and facing.

 

Keeping the same camera settings and adaptation, here is the same scene with Titan's sky instead of the Earth's. The sun can be seen in the upper part of the halo as a white pixel, the position mismatch is due to the fact that the grid of the sky diffuse data is not well aligned with the actual sun position, also meaning that the halo should be a bit brighter than that. The sun can still be easily seen through the atmosphere, but it is too faint compared to the sky to contribute to the illumination of the scene.

 

So Titan during the day is darker than Earth before sunrise or after sunset. Now we can return to a light level where we can see with a better contrast. Contrast is limited on Titan due to the very diffuse illumination of the sky, but with the sun and the LED in the field of view, here is what the contrast would be for a human. A glare effect has been integrated into the human vision rendering to simulate a large exceeding of the dynamic range.

The picture below is what Titan's surface would look like in Huygens natural landing conditions (no LED). Adaptation is 200 cd/m². Except for Huygens, most of the image is below 42 cd/m²; to understand how dark this is, consider that the daylight vision starts at about 10 cd/m² for the human eye. The small brightness variation in the image does make the human vision rendering useless.

Another scene with a 3km terrain was made, and this view compares, on a linear luminance scaling with an adaptation of 100 cd/m², a simulation including the atmospheric effects (haze) on the left with the same simulation without it on the right.

To help the brain do the white balance, garden plastic chairs have been placed in the following scenes. There are also two LED projectors, 200W of luminous power, 20 meters above ground pointing toward Huygens and the chairs. We can see that the chairs take Titan's global color when not illuminated by the LED (first image), and are almost white even when illuminated by them from 20 meters (second image). These images have human vision contrasts.

Finally, with the 3km terrain as well, here is another shot at a wide angle view, without LED projectors, in human vision contrast mode, with a higher-definition sky. There is a slight problem with the sun appearing darker than the halo in this human vision image, while it is more than 100 times brighter in the data, but otherwise, it should be correct. We can see that the shadow of Huygens appears on the ground.

 

Other images, settings, or measurements, can be made on demand, to info@optis-world.com.

 

* Data have been provided by Lyn Doose and Erich Karkoschka from the Lunar and Planetary Laboratory of the University of Arizona and transformed by Vincent Hourdin from OPTIS, for use in OPTIS softwarethe SPEOS radiometric simulation.

 

To go further

Discover the white paper about the Titan adventure