** GOES-16 data posted on this page are preliminary, non-operational data and are undergoing testing **
Clear Air Turbulence (CAT) is defined as the erratic movement of air masses in the absence of visual clues, such as clouds. In this short exercise, you will see GOES-16 Visible (0.64 um) imagery, GOES-16 Clean Window Infrared Imagery (10.3 um) and Water Vapor Imagery, both lower (6.2 um) and upper (7.3 um) channels:
**Click to play** The GOES-16 Visible Animation shows units of Reflectance -- how much sunlight is reflected off of the clouds? (That is, the albedo). Where are the in-flight turbulence risks? Why do you answer that way?
**Click to play** The GOES-16 Clean Window measures radiation that has been emitted from the Earth (in clear skies) or from cloud tops (over thick clouds). It is called "Clean" because very little absorption of energy occurs at this wavelength; absorption, when it happens, results in cooler brightness temperatures because the absorbed energy is then re-emitted from a higher, usually colder, part of the atmosphere
**Click to play** The Upper Level Water Vapor channel on GOES-16 (6.2 um) is affected strongly by the absorption of atmospheric energy at that wavelength by water vapor. If there is water vapor between the emitting surface (the Earth, or a thick cloud), water vapor will quickly absorb the emitted energy, and then re-emit it from a higher (usually cooler) level. Structures in water vapor imagery -- transverse bands (that is, bands that are perpendicular to the flow) -- have been related to turbulence using legacy GOES Imagery.
**Click to play**"Mid-Level" Water Vapor is, as the name suggests, in between the Upper Level Water Vapor (above) and the low-level water vapor (below). That is, the information represented in the animation at the link is between the other levels. Whether or not a feature is visible in 1, 2 or all 3 water vapor animations is evidence of that feature's depth.
**Click to play**"Low-Level" Water Vapor is detected using a wavelength at which absorption of atmosperic energy is not greatly sensitive to water vapor. (It is, however, a region that is sensitive to absorption by sulfur dioxide -- so be careful using this if volcanism is active) Because water vapor is not quite so effective at absorbing energy at this wavelength (7.3 um, compared to 6.9 and 6.2 um), energy emitted at a particular level has a better chance of escaping to space where the satellite can detect it. Another way of saying that is that the computer can see farther down into the (clear) atmosphere with this wavelength than with the upper- and mid-level water vapor channels.
**Click to play** The GOES-16 Low-Level Water vapor animation at this link is overlain by pilot reports of turbulence.
| VISIBLE | Clean IR | Upper-Level Water Vapor | Mid-Level Water Vapor | Lower-Level Water Vapor | Lower-Level Water Vapor with PIREPs |
|---|---|---|---|---|---|
| 1802 | 1802 | 1802 | 1802 | 1802 | 1802 |
| 1807 | 1807 | 1807 | 1807 | 1807 | 1807 |
| 1812 | 1812 | 1812 | 1812 | 1812 | 1812 |
| 1817 | 1817 | 1817 | 1817 | 1817 | 1817 |
| 1822 | 1822 | 1822 | 1822 | 1822 | 1822 |
| 1827 | 1827 | 1827 | 1827 | 1827 | 1827 |
| 1832 | 1832 | 1832 | 1832 | 1832 | 1832 |
| 1837 | 1837 | 1837 | 1837 | 1837 | 1837 |
| 1842 | 1842 | 1842 | 1842 | 1842 | 1842 |
| 1847 | 1847 | 1847 | 1847 | 1847 | 1847 |
| 1852 | 1852 | 1852 | 1852 | 1852 | 1852 |
| 1857 | 1857 | 1857 | 1857 | 1857 | 1857 |
| 1902 | 1902 | 1902 | 1902 | 1902 | 1902 |
| 1907 | 1907 | 1907 | 1907 | 1907 | 1907 |
| 1912 | 1912 | 1912 | 1912 | 1912 | 1912 |
| 1917 | 1917 | 1917 | 1917 | 1917 | 1917 |
| 1922 | 1922 | 1922 | 1922 | 1922 | 1922 |
| 1927 | 1927 | 1927 | 1927 | 1927 | 1927 |
| 1932 | 1932 | 1932 | 1932 | 1932 | 1932 |
| 1937 | 1937 | 1937 | 1937 | 1937 | 1937 |
| 1942 | 1942 | 1942 | 1942 | 1942 | 1942 |
| 1947 | 1947 | 1947 | 1947 | 1947 | 1947 |
| 1952 | 1952 | 1952 | 1952 | 1952 | 1952 |
| 1957 | 1957 | 1957 | 1957 | 1957 | 1957 |