Latest results from the KEOPS Campaign - 03/02/2015 - 12/02/2015
Ian McWhirter (electro-optical engineer), Anasuya Aruliah (Principal Investigator) and Amy Ronksley (finishing PhD student) travelled to the ESRANGE Rocket Range near Kiruna, Sweden to undertake maintenance and calibration of the two Fabry-Perot Interferometers. This is in preparation for a tristatic optical and radar experiment, using FPIs, EISCAT radars and the KAIRA radar around new moon on the 18th Feb 2015.The experiment is part of an investigation into what mechanism can cause extreme upward winds in the upper atmosphere. There was a lot of work to do on the instruments since it has been 5 years since the last visit. Both etalons required re-parallelising, the motor driving one of the viewing mirrors needed to be fixed, a filter wheel needed to be un-stuck, the broken all-sky camera needed replacement; the new cloud sensor needed to be fixed to the outside wall and its software installedi; general cleaning of instrument; laser scans; checking temperature control; update software and windows operating system to Win7.
The campaign has been funded by the EOARD grant from the US Air Force.
Latest results from C-REX mission - 24/11/2014
The rocket was launched successfully from Andoya rocket range at 08:05UT 24th November 2014. Images captured from our UCL all-sky camera at 08:15UT show bright green patches where the gas has been released to the right of the image (left image), and then at 08:17UT when the gas has accelerated away along the E-field lines and faded (right image).
Successive images captured by the UCL all-sky camera at 08:15UT and 08:17UT. The canisters of gas released can be seen by the bright green patches to the right of the left image.Here the right image at 08:16UT is from another ASC operated by the Kjell Henriksen Observatory, and shows more canisters have released the gas indicated again by the bright green patches to the right of the image. The faint line across the middle of the image is aurora. The twilight sun can be seen to the south, but these are CCD cameras, so it would be dark to our eyes as Svalbard has 24 hours night from Nov-Jan.
The Atmospheric Physics LaboratoryThe Atmospheric Physics Laboratory has conducted ground-based observations of the arctic auroral regions for the past 30 years, most noted for the spectacular Northern Lights as seen in Figure 1. We have had a network of Fabry-Perot Interferometers (FPIs) situated at Kiruna, Sodankylä and Svalbard since the early 1980s, illustrated in Figures 2 and 3.
These state-of-the-art optical instruments provide continual monitoring of the upper atmosphere through the winter months of September to March. We are able to obtain high temporal and spatial resolution observations of aurora and airglow emissions, giving measurements of winds, temperatures, and gravity waves.
We are also able to study the coupling mechanisms between the dynamics of the ionosphere and thermosphere, under control of the magnetosphere.
The FPIs will be employed in a forthcoming NASA rocket experiment called C-REX, led by Dr Mark Conde at the University of Alaska, and involves scientists from the USA and UK. The all-sky Scanning Doppler Imager (SCANDI) will provide measurements of neutral winds and neutral temperatures over a region that is 1000km in diameter, while the narrow field FPI will measure the vertical wind component at a high time resolution.
The C-REX mission aims to probe the Earth’s geomagnetic cusp region and is focused on the thermosphere (altitude region 90km to 500km). In-situ observations by the CHAMP satellite have shown that the neutral mass density can increase by as much as 100% over a horizontal extent of only a few hundred kilometres. The increased density is due to the upwelling of denser air from below. This rapid changing of the thermosphere is a key area of interest due to its impact on high inclination orbits, affecting both industry and science satellites, as well as its potential to deliver a more cohesive analysis of the space environment. The mechanism/s driving this remains a mystery to the scientific community because the high viscosity of the thermosphere should result in slowly varying and spatially vast fluctuations. Several proposed explanations will be tested, including Joule or particle heating forcing neutral gas upwelling, and collisional drag from fast upwelling ions. As single mechanism models fail to reproduce satellite data, it follows that the anomaly is most likely an amalgamation of these processes. To establish this a system comprising of ground, rocket and satellite observations is needed, ultimately providing a 3-D view of the ion and neutral velocity fields. The aim is to reveal the significance of each mechanism when compared with a coupled thermosphere-ionosphere model such as APL’s CMAT2.
Figure 6: Two images recorded by SCANDI on the 22 January 2012. Left: 06:05:15 UT, faint aurora are beginning to appear to the north. Right: 07:26:15 UT, strong aurora observed, which fills the northern half of the field of view. Note that both the red and green emissions are from forbidden electron transitions between energy levels for atomic oxygen. The intensity of the red emission over the SCANDI field of view is plotted in the red row in Figure 4.
Current developments in this field include the findings of the APL Scandinavian FPIs and the EISCAT Svalbard Radar (ESR) in a previous cusp upwelling experiment; this focused on a solar coronal mass ejection (CME) event on 22 January 2012, leading to increased geomagnetic activity (magnetic reconnection) at the Earth. Here, strong vertical winds (see Figures 4 and 5) were observed under cusp conditions connected to the rapid transport of ions. Figure 5 shows the SCANDI horizontal neutral wind vectors in geomagnetic coordinates, in which significant activity can be seen 30-40 minutes after the CME arrived. The observations indicated a strong agreement with previous CMAT2 model simulations. The hypothesis being tested is that frictional drag heating, together with soft particle precipitation (from the CME in our case study), will deposit energy at high altitudes (around 150-200km). This can result in significant upwelling because only a short column of rarefied air lies above the heating source. Consequently a dramatic increase in neutral mass density can be seen by a satellite at 400km altitude. These rapid and small spatial scale fluctuations in the thermosphere are shown in Figure 4 by the changes in temperature and line-of-sight wind components. For example, a dramatic drop in temperature of around 500K (green row) can be observed in the south of the SCANDI field of view between the images at 06:05UT and 07:26UT. Figure 5 shows the corresponding wind speeds, which start small and then grow to fast winds, but only in the northern half of the field of view. This can be interpreted by referring to the corresponding all-sky camera images in Figure 6 which highlights the appearance of strong red aurora in the northern half of the field of view.
A comparison of the EISCAT radar measurements of the ionosphere while the FPI measures the neutral thermosphere is shown in Figure 7. There is a clear correspondence between the large increase in the EISCAT ion temperature and the large upwelling observed by the FPI. The ion temperature is proportional to the size of the ion velocities. Figure 8 confirms the presence of large ion velocities by showing Super Dual Auroral Radar Network (SuperDARN) radar measurements of bursts of fast plasma flow of several hundred m/s. Both the EISCAT and SuperDARN radars independently support frictional drag acting in the altitude region of 150-200km as the likely source of heating.