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Astronomical seeing

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Astronomical seeing refers to the degradation of images of celestial objects due to turbulence in Earth's atmosphere.

Atmos struct imaging
Atmos struct imaging

This phenomenon causes astronomical objects to appear blurred, twinkling, or distorted. The core cause is the rapidly changing variations in the optical refractive index along the light path. As light travels from a distant star toward a detector, it passes through layers of air with different temperatures and wind speeds. These variations act like moving, rotating cells of air that perturb the incoming light waves. Because of this, seeing acts as a major limitation to the angular resolution of ground-based telescopes. Without the atmosphere, a telescope's resolution would be limited only by diffraction, which depends on the size of the telescope aperture.

To understand the mechanism, we must look at how light waves interact with the air. In classical theory, light is treated as an oscillation in a field. When these wavefronts pass through the atmosphere, they are perturbed by refractive index variations. This means the phase and amplitude of the light waves change as they move through turbulent layers.

Atmos struct imaging
Atmos struct imaging

In a short-exposure image, a single point source like a star does not appear as a steady Airy pattern. Instead, it breaks up into a rapidly changing pattern of many tiny dots called speckles. These speckles move around very quickly, often more than 100 times every second. When a telescope takes a long-exposure image, these shifting speckles average out into a single, fuzzy, filled disc. This shape is known as a seeing disc.

Astronomers use several specific parameters to describe and measure seeing conditions. The first is the full width at half maximum (FWHM) of the seeing disc. This measurement describes the diameter of the blurred blob seen in long exposures. The second is the Fried parameter, denoted as r0. Named after David L. Fried, r0 describes the size of a typical "lump" of uniform air within the turbulent atmosphere. At the best observatories, r0 is typically between 10 and 20 centimeters at visible wavelengths. The third measure is the atmospheric time constant, known as the Greenwood time constant (t0). This parameter describes the time-scale over which the turbulence changes significantly.

These parameters are essential for designing modern technology like adaptive optics systems. The Fried parameter, r0, determines the required spacing for the actuators in an adaptive optics system. Meanwhile, the Greenwood time constant, t0, determines the correction speed needed to compensate for atmospheric effects.

ast seeing 7r0
ast seeing 7r0

These values are not constant; they vary based on the wavelength of light being used. For large telescopes, the resolution of long-exposure images is generally slightly higher at longer wavelengths. This is because the timescale of the changing speckle patterns is substantially lower at those wavelengths.

Different environments and locations offer vastly different seeing qualities. Seeing is a variable quantity that changes by location, by night, and even within minutes. Excellent seeing is often defined as a seeing disc smaller than 0.4 arcseconds or a Fried parameter larger than 30 centimeters. A value of 1.0 arcsecond is considered good for an average astronomical site. However, urban environments usually have much worse seeing. The best conditions are found at high-altitude observatories on small islands, such as Mauna Kea or La Palma. At these mountaintops, the wind often brings in stable air that has not been in contact with the ground.

Historically, the effects of seeing led to significant scientific misunderstandings. In the past, atmospheric seeing was indirectly responsible for the belief that there were canals on Mars. When viewing a bright object like Mars, a still patch of air might occasionally drift in front of the planet. This creates a brief moment of clarity. Before the invention of charge-coupled devices, observers had to rely on their memories to record these moments.

Jupiter with Lucky Imaging
Jupiter with Lucky Imaging

Because they drew what they remembered from these brief clearings, they incorrectly believed Mars had linear features. This shows how the atmosphere can trick the human eye and mind.

Seeing also manifests as scintillation, which is the technical term for the twinkling of stars.

This happens because the brightness of the star appears to fluctuate as the light is distorted. In an astronomical interferometer, seeing causes the fringes to move rapidly. Understanding these complex movements allows astronomers to use techniques like speckle imaging to process short-exposure images. By studying the math behind the wavefront perturbations, scientists can continue to push the limits of what ground-based telescopes can see.

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🖼️ Images & Media (10)
File:Atmos struct imaging.svg
Atmos struct imaging.svg
File:Zeta bootis short exposure.png
Zeta bootis short exposure.png
Szintillation.Sirius.480.webm
File:ast seeing 2r0.png
ast seeing 2r0.png
File:ast seeing 7r0.png
ast seeing 7r0.png
File:ast seeing 20r0.png
ast seeing 20r0.png
File:Not telescope sunset 2001.jpg
Not telescope sunset 2001.jpg
File:Seeing Moon.gif
Seeing Moon.gif
File:A Mix of Colours and Wonder.jpg
A Mix of Colours and Wonder.jpg
File:Jupiter_with_Lucky_Imaging.jpg
Jupiter_with_Lucky_Imaging.jpg
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