ORCID Profile
0000-0002-5886-3509
Current Organisation
University College London
Does something not look right? The information on this page has been harvested from data sources that may not be up to date. We continue to work with information providers to improve coverage and quality. To report an issue, use the Feedback Form.
Publisher: American Geophysical Union (AGU)
Date: 12-2012
DOI: 10.1029/2012JA018201
Publisher: Springer Science and Business Media LLC
Date: 02-08-2012
Publisher: Elsevier BV
Date: 05-2012
Publisher: American Geophysical Union (AGU)
Date: 04-2012
DOI: 10.1029/2012GL051312
Publisher: American Geophysical Union (AGU)
Date: 12-05-2007
DOI: 10.1029/2006GL028921
Publisher: Springer Science and Business Media LLC
Date: 13-05-2008
Publisher: American Geophysical Union (AGU)
Date: 02-2020
DOI: 10.1029/2019JA027542
Publisher: Springer Science and Business Media LLC
Date: 06-2009
DOI: 10.1038/NATURE08070
Abstract: The discovery of water vapour and ice particles erupting from Saturn's moon Enceladus fuelled speculation that an internal ocean was the source. Alternatively, the source might be ice warmed, melted or crushed by tectonic motions. Sodium chloride (that is, salt) is expected to be present in a long-lived ocean in contact with a rocky core. Here we report a ground-based spectroscopic search for atomic sodium near Enceladus that places an upper limit on the mixing ratio in the vapour plumes orders of magnitude below the expected ocean salinity. The low sodium content of escaping vapour, together with the small fraction of salt-bearing particles, argues against a situation in which a near-surface geyser is fuelled by a salty ocean through cracks in the crust. The lack of observable sodium in the vapour is consistent with a wide variety of alternative eruption sources, including a deep ocean, a freshwater reservoir, or ice. The existing data may be insufficient to distinguish between these hypotheses.
Publisher: MDPI AG
Date: 20-10-2022
DOI: 10.3390/JMSE10101551
Abstract: A floating oscillating water column (OWC) wave energy converter (WEC) supported by mooring lines can be modelled as an elastically supported OWC. The main objective of this paper is to investigate the effects of the frequency ratio on the performance of floating OWC (oscillating water column) devices that oscillate either vertically or horizontally at two different mass ratios (m = 2 and 3) through two-dimensional computational fluid dynamics simulations. The frequency ratio is the ratio of the natural frequency of the system to the wave frequency. Simulations are conducted for nine frequency ratios in the range between 1 and 10. The hydrodynamic efficiency achieves its maximum at the smallest frequency ratio of 1 if the OWC oscillates horizontally and at the largest frequency ratio of 10 if the OWC oscillates vertically. The frequency ratio affects the hydraulic efficiency of the vertical oscillating OWC significantly stronger than that of the horizontal oscillating OWC, especially when it is small. The air pressure and the volume oscillation in OWC is not affected much by the horizontal motion of the OWC but is significantly affected by the vertical motion, especially at small frequency ratios.
Publisher: American Geophysical Union (AGU)
Date: 08-2015
DOI: 10.1002/2015JA021319
Publisher: AIP
Date: 2005
DOI: 10.1063/1.2032682
Publisher: Oxford University Press (OUP)
Date: 02-2010
Publisher: American Astronomical Society
Date: 08-01-2008
DOI: 10.1086/527545
Publisher: Springer Science and Business Media LLC
Date: 12-2021
DOI: 10.1007/S10686-021-09810-Z
Abstract: Some of the major discoveries of the recent Cassini-Huygens mission have put Titan and Enceladus firmly on the Solar System map. The mission has revolutionised our view of Solar System satellites, arguably matching their scientific importance with that of their host planet. While Cassini-Huygens has made big surprises in revealing Titan’s organically rich environment and Enceladus’ cryovolcanism, the mission’s success naturally leads us to further probe these findings. We advocate the acknowledgement of Titan and Enceladus science as highly relevant to ESA’s long-term roadmap, as logical follow-on to Cassini-Huygens . In this White Paper, we will outline important science questions regarding these satellites and identify the science themes we recommend ESA cover during the Voyage 2050 planning cycle. Addressing these science themes would make major advancements to the present knowledge we have about the Solar System, its formation, evolution, and likelihood that other habitable environments exist outside the Earth’s biosphere.
Publisher: American Geophysical Union (AGU)
Date: 11-2008
DOI: 10.1029/2008JA013592
Publisher: Elsevier BV
Date: 06-1997
Publisher: American Geophysical Union (AGU)
Date: 2012
DOI: 10.1029/2011JA017222
Publisher: American Geophysical Union (AGU)
Date: 31-12-2008
DOI: 10.1029/2007RG000238
Publisher: American Geophysical Union (AGU)
Date: 09-2015
DOI: 10.1002/2015JA021290
Publisher: Copernicus GmbH
Date: 15-05-2023
DOI: 10.5194/EGUSPHERE-EGU23-15246
Abstract: The Jovian magnetosphere can undergo significant changes in its size due to varying external (e.g. solar activity) or internal (e.g. hot plasma pressure) conditions. Simulations have shown that the difference in the dayside stand-off distance between a compressed and an expanded state can be around 30 Jovian radii.In this work, we study the compressibility of the Jovian magnetosphere using a large ensemble of axisymmetric models, obtained from the recently updated UCL/AGA magnetodisc code. Each model is defined by its size (via the stand-off distance) and hot plasma content (via the hot plasma index). Using these models as virtual magnetopause crossings we estimate the compressibility index, calculated via changes in the dayside stand-off distance as a function of the external pressure, which characterises the overall response of the magnetosphere.We find that the system size plays an important role in the Jovian case, as we observe a change in the compressibility index as a function of the stand-off distance. This has also been noted in existing studies on Saturn, using a linear relation between changes in the stand-off distance and the external pressure.As a complementary study, we also estimate the compressibility index using magnetopause crossings from recently published catalogues based on JUNO data.
Publisher: American Geophysical Union (AGU)
Date: 20-07-2018
DOI: 10.1029/2018GL078141
Publisher: American Geophysical Union (AGU)
Date: 09-2017
DOI: 10.1002/2017JA024595
Publisher: Oxford University Press (OUP)
Date: 21-09-2009
Publisher: Copernicus GmbH
Date: 08-10-2020
Abstract: & & & strong& Background: & /strong& The magnetopause (MP) boundary is formed by the solar wind plasma flow interacting with a planetary magnetic field. Magnetic reconnection is an important process at this boundary as it energises plasma via release of magnetic energy. Reconnection of the IMF and internal magnetic field of the planet produces an & #8220 open& #8221 magnetosphere allowing solar wind and magnetosheath particles to directly enter the magnetosphere. At Saturn, the nature of MP reconnection remains unclear. Masters et al. (2012) hypothesised that viable reconnection under a large difference in plasma & #946 across the MP also requires a high magnetic shear (i.e. magnetic fields either side of the boundary close to anti-parallel).& & & & & strong& Objective: & /strong& The current study uses bulk electron heating at MP crossings (& #8216 events& #8217 ) as a reconnection signature to test the following hypotheses, suggested by the study of Masters et al. (2012). 1) Events where the boundary is locally closed would have essentially no observed temperature change, whereas most events with locally open boundary should have observed change close to the theoretical prediction. 2) Events with evidence of plasma energization should be in the & #8216 reconnection possible& #8217 regime, whereas those without such evidence should be in the & #8216 reconnection suppressed& #8217 regime.& & & & & strong& Methods: & /strong& We analysed 70 MP crossings made by the Cassini spacecraft from April 2005 to July 2007, previously reported by Masters et al. (2012). These 70 events have a determined plasma & #946 on both sides of the MP. Magnetic field and particle data were used to characterize the crossings. The bulk temperature was determined using three different methods, related to properties of the observed energy distribution (including methods from Lewis et al. 2008). We compared the observed heating of magnetosheath electrons with the prediction based on reconnection, using the semi-empirical relationship proposed by Phan et al. (2013) which relates the degree of bulk electron heating to the inflow Alfven speed.& & & & & strong& Results:& /strong& Plots of observed versus predicted electron temperature change for all 70 crossings showed that there is positive correlation between the two when the 1d moment method (Lewis et al. 2008) was used to calculate heating (Figure 1). We do see a tendency of better agreement with prediction for the locally & #8216 open& #8217 boundary cases based on the threshold & Bn/B & = 0.1 for the minimum variance component of the magnetic field. For the case of locally & #8216 closed& #8217 boundary (Bn/B & 0.1), we observe a cluster of points near dT=0, but also numerous cases of significant heating. We find five cases where the observed heating exceeds prediction significantly (& eV). These results suggest that although a large portion of events fit our hypothesis 1 within uncertainty, there are some which do not. Based on the magnetic shear measured locally by the spacecraft either side of the MP, we find 81% of events with no energisation were situated in the & #8216 reconnection suppressed& #8217 regime, and 43% of events with energization lay in the & #8216 reconnection possible& #8217 regime (Figure 2). These results support hypothesis 2 to some extent.& & & & & strong& Conclusion:& /strong& & & & & A statistical study of observed and theoretical electron bulk heating was performed at the magnetopause based on 70 magnetopause crossings detected by the Cassini spacecraft. Our results support both hypotheses 1 and 2 to some extent. One reason why some events do not fit our hypotheses is because we are assuming local conditions to be indicative of the putative reconnection site. However, the spacecraft could be quite distant from this site, and still magnetically connected to it. Another reason is temporal variability in the near-magnetopause environment. We plan to analyse the dataset further in future work, by taking these aspects into account.& & & & & img src=& quot data:image/jpeg base64, 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 qhYaeLgTGS4uDsmdB+9PQYx/OgDp8ijIrI/seP8A5+Lj/v6aP7Hj/wCfi4/7+mgDXyKjSOKLd5aqu47m2gDJPc+9Zn9jx/8APxcf9/TR/Y8f/Pxcf9/TQBr5FJkViTaUiQyOLi4yqkj96ewqO00tZbaOR7i4LMoJ/enrQB0GRRkVkf2PH/z8XH/f00f2PH/z8XH/AH9NAGvkUZFZH9jx/wDPxcf9/TSf2RH/AM/Fx/39NAGxkUVzcttHCILm1upnBmVT+93qQTyPSukoAKKKKACjIrL1beYI41dk8yZFJQ4ODnvTP7Hj/wCfi4/7+mgDXyKMisj+x4/+fi4/7+ms/wDs8f2l9m+0XGzyt2PNPXOKAOnyKMisj+x4/wDn4uP+ o/seP/AJ+Lj/v6aANfIqIwwGUTlFMoXaHwNwXrjPXFZv8AY8f/AD8XH/f00f2PH/z8XH/f00Aa+RSZFZP9jx/8/Fx/39NUrfThJdXMTXFxtjZAv7091BP60AdJkUZFZH9jx/8APxcf9/TR/Y8f/Pxcf9/TQBr5FGRWR/Y8f/Pxcf8Af00f2PH/AM/Fx/39NAGvkUVhHTbfc8Qupy6ruKiY7gDnBx6cVd0mR5dOt3kYsxjXJPU8UAaFFFFABRkUhrnNPsPtlnHczXFxvkBLYkIGcntQB0mRRkVkf2PH/wA/Fx/39NZ+paf9mtfNiuLgNvQf609CwBoA6fIoyKyP7Hj/AOfi4/7+mj+x4/8An4uP+ oA1simSxQzxtFMiyIwwysAQR7g1mf2PH/AM/Fx/39NH9jx/8APxcf9/TQBrDAGB0pcisj+x4/+fi4/wC 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 P/iqRv8AkLp/1wb/ANCFalAGZ/ZFl6S/9 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 P/iq065oeMfDDeJ28GLqVudbSD7SbLePOEXHzbfxH4EUm0ty4UpzvyK9tX6dzS/siy9Jf+/0n/xVH9kWXpL/AN 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 /yT/4mgC7c/wDHtL/uN/KorD/jyh/3BXBeN/ETeDNN/tG8TUb21wxuJbf7OqQRjqzmQr+AXJJrE8D+P9N8ZXS6bp39qWQe0F5avdJCBcW27ZvXbkrhuCGANAHsdFZn2C5/5 /yT/4mj7Bc/8AP9P+Sf8AxNAGnRWZ9guf+f6f8k/+Jo+wXP8Az/T/AJJ/8TQAap/q4P8Ar4jrTrKOmSO6NNdzSKjhwp2AEj1wua1aACiiigDM1T7kH/XdP615v4s+GL+N/HWia/4j1H7RoHh4C6s9DEWI5NTydt1O+7955S48pNuFbLHJxj1G8tVu4hGXaMqwdWTGQR9QRVb7Bc/8/wBP+Sf/ABNAGnWT/wAxn/tgP5077Bc/8/0/5J/8TXly+PNKfxt/wjIbUvN+0nTftu2H7ObpYhOYsff4Q53YxnigD2Wisz7Bc/8AP9P+Sf8AxNH2C5/5 /yT/4mgDTorM+wXP8Az/T/AJJ/8TR9guf+f6f8k/8AiaANOs20/wCP69/30/8AQBVHUUu9PsZ71Jr27aGNnEFusbSyFRnagYKCx6DJArxDTvjVoF1q01gLfWYJ4buCz1JmW3aOzmnmNrDuZSQ4aVQpKZ25Ge+AD6PorL+wXP8Az/T/AJJ/8TS/YLn/AJ /wAk/wDiaANOisz7Bc/8/wBP+Sf/ABNH2C5/5 /yT/4mgDQk+4fof5Vn6N/yDLb/rmv8qQ6fcng30/5J/8AE1dtrdLW3jt4ySsahQW6nHrQBPRRRQAh6fiK828U+HvEPiz4ez+HPDOtN4evNQRYG1KOLzpoIHfExhG5Qsxj3KjnIRiGwcYr0qsiLSpIEEUN5OiLnauEOB6fdoAqeE/CuieCPDeneE/DluLXTdLt0treMEsQiDGWY5ZmbqzEksSSTk1c1r/jx/7aR/8AoQp/2C5/5 /yT/4muC8eeI7bwlbWUd62oahNqM0iW9vaiEOxt4nuJGJfaoCRxs3qcYHWgD1Ciuc0qRda0211aw1Cd7e8hSeJiEBKSKGXI28HBrQ+wXP/P8AT/kn/wATQBp0VmfYLn/n+n/JP/iaPsFz/wA/0/5J/wDE0AadZepf62w/6+h/6Lel+wXP/P8AT/kn/wATXi/in4o6b4d8U2/hTVLXWWv55lXTdi2+y7lZliBX5spHmQ4eQANsfHK8gHvdFcN4Q1u38aaBbeINLvLyKK48xWinSNZYpYZHiljcAEbo5EZTgkZHBxXTfYLn/n+n/JP/AImgDTorM+wXP/P9P+Sf/E0fYLn/AJ 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& quot alt=& quot & quot /& & & & & & img src=& quot data:image/jpeg base64, 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 /8AiaoeJtLu9a0G90uwuTZ3FzE0cdwM5iY9HG0g5XqOetQ+E9Hv9B0C10rU719SuoN4ku5M75izlt7ZJ+Yg844z0AGBS9jT9h7Xn969uWzva299vLuTd81raGr5uof88I/+ 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 9aANSiqP9nxf89J/+/z/AONH9nxf89J/+/z/AONAF6s+X/kJwf8AXKT+a07+z4v+ek//AH+f/Gqq2yQanCVaRsxSffdn7r6k0AbFFFFAH//W/fyiiigAqjZ/6+8/67j/ANFpV0kAZJwK5eTxL4c0m+u7XVdVsrKcyq4juLiOJypjTB2swODjrQB1NFee6n8Wvhdo1xaWmqeLtEtZ7+UQWsUmoQB5pDj5UXfljyOnrXHP+0L8OpoLO80u8W5s7q6ktnvJ5YdPt7bytuZJTeSQSeWd/wAhRHLkHAOKAPc68x8Z+L7nN74R8HRx3niQ2YuU+0JL9gtUMoiD3EyLjOd7LEGDyeWwyo+YeEw/HjRPFf2KWfxILtPPurafSfB0UmoQ3jSKFihOpyRRIHRWJIieJixU5AHJbfEC9i0O18M+A7XR/BujC6/sqF5H/tzUUuCQ7I1pYGSGGXLF2aedwCSzr1oA9yuLvwb8ItLvdZ1q7b7Zrd61xM2ZLi81G+kUKsNtDl5HIVVSKFMhEAHABNYuh+HNd8Z6zbeP/iVANPttNZp9D8Pu6ulicEfbLxgSkl5tJ2gExwKSFLMWc854R0Y2eqp4g0nw/q3iLXXvmsL3XvFEq2s0VspBkktU2PshJJCRQxRIzDJwPmPott4K1rWZrW/8e6sb2Wyu5riCz03zbKw2OFWNJovNc3HlhSf3jFSzE7RwAAZ15rl98SYn0fwTdS22gXtq5k8U2E8ed6T+U8FmCrlnZUkBn+VUyrRl25X0KSTRPCmjTXVzJBp2m2MbzzzSsI4o15eSSR2wOTlmY9TkmtO3t7e0gjtbWNIYYlCJGihVVRwAAOABVfVNMsda0270fVIVuLO+gkt7iFxlZIpVKupHoVJBrSlyc8fa35b623t1t5jVr6mL4e8Q6F4pJ1rw1qFtqmnzQosd1aSrNC5SSRWAdCQcMCDz1qOy8D+FtP8AGOpePrPT4ote1e0trG8vAP3ksFqXMantxv5I5IC5ztGKPgTwX4f+Hej2PgnwrbC10rSLCC3tos5IUPISWJ5ZmYlmJ5JJNd1XXXrxo1q0MBOXspXSvo5QvdKSWnRNrVXXkXJpSapvT9PMKKKK4DMRvun6VT03/kHWv/XFP/QRVxvun6VT03/kHWv/AFxT/wBBFAF2iiigAqhc/wDH7af70n/oJq/VC5/4/bT/AHpP/QTTQF+iiikAUUUUAUNO/wBTJ/12l/8AQzV+qGnf6mT/AK7S/wDoZq/QAUUUUAUNQ/1cP/XxD/6EKv1j61d2llaLd3k8dvBDPE0ksrhEQbhyzMQB+NZFx8QfANpE0914l0eGNfvPJfwIoz6kvigDr6K8Yuv2gvhLH9pTTtft9Xms7pLOeLTSLlkmfPBK/IAMHc27C9yK4LxD+0h4ft7m50+21zQNFltb1ISbm6XV7mWA53Olpp0jtGzHAQSPznleMEA+jdY13SdBhSbVLmODznEUCO6iSeVvuxxKSC7t0Cjk15ro2naj42vz4l8WQNY6OixzW2g30MJeOeN96XVw+Xw4VVKICPLyd2Tjb4+PiToFhLPrOnadd63eQXLTJrHjC7h023sDc/KiQo4a4iUggKkdspfuSTmk1G11Dx8msWvjm41jxGsPkq+geHLKbTtMc3Crt3XFy0X2zaGDNmby8cmPtTVr6kybSbSuz0/VfGWsfEe6m8LfC6YxaejGHU/EygNbwAcPDZE8T3HYuMxx9yWG2unin8L/AAv0rS/B+hW0sk9zJ5Fpawo80ssz5Z5riQBioJy8ksh9TyeKwPD/AIQ8bWmgx+E9NmtvCej2It0tJLHZdX0kQ+aUOJIvIhJJ2jYJMdQ3SvSNA8J6D4Ze8m0i1WKfUZzc3c7EvNPKeNzuxLHA4AzhRwABTmoqTUXdCpSk4JzVn1W9vmYfhXwteQ3v/CX+LBBL4mubYW0zWzSG2t4d5cRQLIxx23uApkKgkDgDsdS/48pP+A/+hCr1UdS/48pP+A/+hCpLLw6Vm6tpNlrdhLpmop5kEwww+nPFaPQZrF0fxDpWutcppkrSG0k8qXKMm1x2+YDNaQU1+8h069jnryou1Cq1711Z9e+nXTc1oIIraCO3hULHEoRQOwHAqWiuV0HRtY07UdSudS1KW8guJc2sTtkQx+n1z+lOMVJSlKWq/EJzlCUIQhdPS/Raf0tDbT/kIyf9c1/nV+qCf8hGT/rmv86v1kdAUVDHcQTMyRSo7L94KwJH1x0qam01uBWvP+POf/rm/wDI0+2/494v9xf5Uy8/485/+ub/AMjT7b/j3i/3F/lSAmooooAKz5f+QnB/1yk/mtaFZ8v/ACE4P+uUn81oA0KKKKAP/9f9/KKKKAPF/jfHdTeH9Hgt7QXqz61a20kEjbIGF0ktuhmPJ2JLKknyqx3IOB1HCaLJ4T8V+HjqN/4dOrappml2jtd3lnb3ck0TWqvbzY+eU+cBny1JYNkHHWvobX/DWj+JoLe21qAzx2txHdRKHdNs0J3I3yEZKtyM96ZoHhbQPC8U0Gg2Udmlw4kkCDqVUKo56KqgBVHCgYAAoA4PRfhb4FvtIsb2/wDDOk291LBHLJEthbkRyOoLAboQ3B45Ga2ofhZ4Ct5Y57fQ9OjkicOjpY2ysrqchgRFwQRwa9CooA4mL4eeEYFijh0yzjWG4N3GEtIFCXBx+9XEfD8D5hzwK861v4geH/DE2raQdOv0/su5kEyQrbxiSGK0+3TXKYI+VY88HDs3GMHNe91wd98MvBGp3t7qGoaYlxPqEyT3LSO7B3RDEOC2ADGShA4K/KQRxQAkGralP4istL8u7is7u0up/OdQSHheER/MitGqyLI5AYh/k6V132KX/n7n/Nf/AImrwAAwO1LQBQ+xS/8AP3P+a/8AxNRTW08UMkqz3MpRSwRNm5iBnAyAMnoMkCtSop4UuIZIJM7JFKNglThhg4IwQfcc0AfPJ+L0N5bWd3oljqT3OpwWaoZQjrFNdRSXSxSJFl3MdvHLIxjBB2hQcnj2zSFvr7SrK9vXuLW4uLeKWWAlcxSOoZkPy/wk4/CsbRPhx4L8O3Fnd6RpkcE2nxeTbPuZzGgDqMbieVV2VT1CsVHBIp138RfB2n6jBpV9qCwXV1qw0SGN0fMl+YVnEYIUgDy3X5jhdxC53EAgHT/Ypf8An7n/ADX/AOJo+xS/8/c/5r/8TXP33jzwppviBPC97feVqMnkARmKUoGuS4hVpQhiVpDGwUMwJI4p58eeCFmWA6 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& quot alt=& quot & quot /& & & & & & strong& Figure 1 (Left): & /strong& Observed against predicted bulk electron temperature change for all 70 crossings. & strong& First column& /strong& : Heating based on 3d moment method for full energy distribution. & strong& Second column& /strong& : Heating based on 3d moment method for the cold energy distribution. & strong& Third column& /strong& : Heating based on 1d moment method for the peak of the energy distribution. & strong& Top panels& /strong& : locally & #8216 closed& #8217 boundary based on threshold Bn/B & 0.1. & strong& Bottom panels& /strong& : locally & #8216 open& #8217 boundary based on threshold Bn/B & 0.1. & strong& Red markers& /strong& : Steady transitions with field rotation. & strong& Green markers& /strong& : Turbulent transitions with field rotation. & strong& Blue markers& /strong& : Transitions without field rotation.& & & & & strong& Figure 2 (Right):& /strong& & Assessment of diamagnetic suppression of reconnection using the 70 MP crossings. Colour represents observed heating using 1d moment method. The solid curve corresponds to a current sheet thickness L = 1 d& sub& i& /sub& & sub& ,& /sub& and the dashed curves on the left and right of it correspond to L = 0.5 d& sub& i& & /sub& and L = 2 d& sub& i& /sub& , respectively. & strong& & #8216 x& #8217 & /strong& & strong& markers& /strong& : Steady transitions with field rotation. & strong& & #8216 o& #8217 markers& /strong& : Turbulent transitions with field rotation. & strong& & #8216 v& #8217 markers& /strong& : Transitions without field rotation.& & & & & & &
Publisher: Elsevier BV
Date: 11-2002
Publisher: Wiley
Date: 04-12-2020
Publisher: American Geophysical Union (AGU)
Date: 02-2021
DOI: 10.1029/2020JE006578
Abstract: The Cassini spacecraft completed 22 orbits around Saturn known as the “Grand Finale” over a 5 months interval, during which time the spacecraft traversed the previously unexplored region between Saturn and its equatorial rings near periapsis. The magnetic field observations reveal the presence of temporally variable low‐latitude field‐aligned currents which are thought to be driven by velocity shears in the neutral zonal winds at magnetically conjugate thermospheric latitudes. We consider atmospheric waves as a plausible driver of temporal variability in the low‐latitude thermosphere, and empirically constrain the region in which they perturb the zonal flows to be between ±25° latitude. By investigating an extensive range of hypothetical wind profiles, we present and analyze a timeseries of the modeled velocity shears in thermospheric zonal flows, with direct comparisons to empirically inferred angular velocity shears from the B ϕ observations. We determine the maximum temporal variability in the peak neutral zonal winds over the Grand Finale interval to be ∼350 m/s assuming steady‐state ionospheric Pedersen conductances. We further show that the ionospheric currents measured must be in steady‐state on ∼10 min timescales, and axisymmetric over ∼2 h of local time in the near‐equatorial ionosphere. Our study illustrates the potential to use of magnetospheric datasets to constrain atmospheric variability in the thermosphere region.
Publisher: American Geophysical Union (AGU)
Date: 2020
DOI: 10.1029/2019JA026792
Abstract: Jupiter's upper atmosphere is ∼700 K hotter than predicted based on solar extreme ultraviolet heating alone. The reason for this still remains a mystery and is known as the “energy crisis.” It is thought that the interaction between Jupiter and its dynamic magnetosphere plays a vital role in heating its atmosphere to the observed temperatures. Here, we present a new model of Jupiter's magnetosphere‐ionosphere‐thermosphere‐coupled system where we couple a three‐dimensional atmospheric general circulation model to an axisymmetric magnetosphere model. We find that the model temperatures are on average ∼60 K, with a maximum of ∼200 K, hotter than the model's two‐dimensional predecessor making our high‐latitude temperatures comparable to the lower limit of observations. Stronger meridional winds now transport more heat from the auroral region to the equator increasing the equatorial temperatures. However, despite this increase, the modeled equatorial temperatures are still hundreds of kelvins colder than observed. We use this model as an intermediate step toward a three‐dimensional atmospheric model coupled to a realistic magnetosphere model with zonal and radial variation.
Publisher: American Geophysical Union (AGU)
Date: 10-2018
DOI: 10.1029/2018JA025764
Publisher: Springer Science and Business Media LLC
Date: 06-2008
DOI: 10.1038/NATURE07077
Abstract: Planetary aurorae are formed by energetic charged particles streaming along the planet's magnetic field lines into the upper atmosphere from the surrounding space environment. Earth's main auroral oval is formed through interactions with the solar wind, whereas that at Jupiter is formed through interactions with plasma from the moon Io inside its magnetic field (although other processes form aurorae at both planets). At Saturn, only the main auroral oval has previously been observed and there remains much debate over its origin. Here we report the discovery of a secondary oval at Saturn that is approximately 25 per cent as bright as the main oval, and we show this to be caused by interaction with the middle magnetosphere around the planet. This is a weak equivalent of Jupiter's main oval, its relative dimness being due to the lack of as large a source of ions as Jupiter's volcanic moon Io. This result suggests that differences seen in the auroral emissions from Saturn and Jupiter are due to scaling differences in the conditions at each of these two planets, whereas the underlying formation processes are the same.
Publisher: Elsevier BV
Date: 12-2009
Publisher: MDPI AG
Date: 02-08-2021
DOI: 10.3390/APP11157131
Abstract: Integral bridges are a class of bridges with integral or semi-integral abutments, designed without expansion joints in the bridge deck of the superstructure. The significance of an integral bridge design is that it avoids durability and recurring maintenance issues with bridge joints, and maybe bearings, which are prevalent in traditional bridges. Integral bridges are less costly to construct. They require less maintenance and therefore cause less traffic disruptions that incur socio-economic costs. As a consequence, integral bridges are becoming the first choice of bridge design for short-to-medium length bridges in many countries, including the UK, USA, Europe, Australia, New Zealand and many other Asian countries. However, integral bridge designs are not without challenges: issues that concern concrete creep, shrinkage, temperature effects, bridge skew, structural constraints, as well as soil–structure interactions are lified in integral bridges. The increased cyclic soil–structure interactions between the bridge structure and soil will lead to adverse soil ratcheting and settlement bump at the bridge approach. If movements from bridge superstructures were also transferred to pile-supported substructures, there is a risk that the pile–soil interactions may lead to pile fatigue failure. These issues complicate the geotechnical aspects of integral bridges. The aim of this paper is to present a comprehensive review of current geotechnical design practices and the amelioration of soil–structure interactions of integral bridges.
Publisher: American Geophysical Union (AGU)
Date: 2004
DOI: 10.1029/2004JA010614
Publisher: Elsevier BV
Date: 12-2014
Publisher: Elsevier BV
Date: 12-2014
Publisher: American Geophysical Union (AGU)
Date: 03-0001
DOI: 10.1029/2007JA012540
Publisher: Elsevier BV
Date: 11-2007
Publisher: Wiley
Date: 18-12-2019
Publisher: Elsevier BV
Date: 03-1997
Publisher: Springer Science and Business Media LLC
Date: 02-10-2014
Publisher: Copernicus GmbH
Date: 15-05-2023
DOI: 10.5194/EGUSPHERE-EGU23-16080
Abstract: Mirror modes are large litude, non-propagating compressive structures often observed in the magnetosheath. They appear in the form of quasi-sinusoidal oscillations in the magnetic field, with clear magnetic dropouts (& #8216 dips& #8217 ) or enhancements (& #8216 eaks& #8217 ). Mirror modes are usually accompanied by a corresponding, anticorrelated signature in plasma density. Typically, the growth of mirror mode fluctuations is triggered when magnetized plasma traverses the bow shock (BS) or draping of the magnetic field around the magnetopause (MP), producing anisotropic ion distribution functions in a high plasma & #946 environment.In this work, nine years of in-situ Cassini data and the latest published catalogue of BS and MP crossings at Saturn were used to perform a detailed statistical analysis of magnetic fluctuations associated with mirror mode structures in Saturn& #8217 s magnetosheath. 182 single traversals through the magnetosheath between the bow shock and the magnetopause were used to study the evolution of mirror mode structures across Saturn& #8217 s outer and inner magnetosheath and to assess the effects of magnetic shear at the MP on the mirror mode structures near the MP. Violante et al. (1995) analysed two MP crossings at Saturn by Voyagers 1 and 2 and found that in the high magnetic shear MP, mirror waves appear with increasing litude and decreasing frequency until the MP, whilst in the other low magnetic shear case, the mirror waves ceased to grow in the presence of a plasma depletion layer but are still present, albeit with smaller litude.The litude and frequency of mirror waves near the magnetopause are also examined against signs of magnetic reconnection. Tsurutani et al. (1982) suggested that the litude of mirror wave structures could impact magnetic reconnection at the MP boundary as alternating high and low regions and the plasma temperature anisotropies may lead to patchy and sporadic reconnection.
Publisher: American Astronomical Society
Date: 16-09-2010
Publisher: Elsevier BV
Date: 09-2021
Publisher: American Geophysical Union (AGU)
Date: 10-2010
DOI: 10.1029/2010GL045159
Publisher: Springer Science and Business Media LLC
Date: 10-09-2011
Publisher: American Geophysical Union (AGU)
Date: 11-2010
DOI: 10.1029/2010GL044622
Publisher: Copernicus GmbH
Date: 08-10-2020
DOI: 10.5194/EPSC2020-851
Abstract: & & The trapping of charged particles in planetary magnetic fields is a process which underpins many important aspects of planetary magnetospheres, such as ring current evolution, particle acceleration, and the flow of current through the system, both free and bound. As part of our effort for the Europlanet project, the UCL group have developed codes which accurately model the trajectories of charged particles in magnetic field models appropriate for the magnetospheres of Jupiter and Saturn. These will form the basis of a service for the SPIDER task. In this presentation, we show ex les of ion trajectories at both planets for representative 'start values' of equatorial distance, pitch angle, and values of particle energy. The simulations provide an indication of how particle orbits become less adiabatic as one approaches energies where gyroradii become comparable to magnetic field curvature radius. The disk-like fields of the gas giants are particularly effective at 'scattering' adequately high-energy particle trajectories as they cross the equator, where the field lines are most 'pinched' and have the smallest length scales.& &
Publisher: Elsevier BV
Date: 12-2009
Publisher: Elsevier BV
Date: 07-2007
Publisher: Cambridge University Press (CUP)
Date: 10-2010
DOI: 10.1017/S1743921311020448
Abstract: The science of extra-solar planets is one of the most rapidly changing areas of astrophysics and since 1995 the number of planets known has increased by almost two orders of magnitude. A combination of ground-based surveys and dedicated space missions has resulted in 560-plus planets being detected, and over 1200 that await confirmation. NASA's Kepler mission has opened up the possibility of discovering Earth-like planets in the habitable zone around some of the 100,000 stars it is surveying during its 3 to 4-year lifetime. The new ESA's Gaia mission is expected to discover thousands of new planets around stars within 200 parsecs of the Sun. The key challenge now is moving on from discovery, important though that remains, to characterisation: what are these planets actually like, and why are they as they are? In the past ten years, we have learned how to obtain the first spectra of exoplanets using transit transmission and emission spectroscopy. With the high stability of Spitzer, Hubble, and large ground-based telescopes the spectra of bright close-in massive planets can be obtained and species like water vapour, methane, carbon monoxide and dioxide have been detected. With transit science came the first tangible remote sensing of these planetary bodies and so one can start to extrapolate from what has been learnt from Solar System probes to what one might plan to learn about their faraway siblings. As we learn more about the atmospheres, surfaces and near-surfaces of these remote bodies, we will begin to build up a clearer picture of their construction, history and suitability for life. The Exoplanet Characterisation Observatory, EChO, will be the first dedicated mission to investigate the physics and chemistry of Exoplanetary Atmospheres. By characterising spectroscopically more bodies in different environments we will take detailed planetology out of the Solar System and into the Galaxy as a whole. EChO has now been selected by the European Space Agency to be assessed as one of four M3 mission candidates.
Publisher: American Astronomical Society
Date: 03-1998
DOI: 10.1086/305259
Publisher: Springer Science and Business Media LLC
Date: 06-01-2015
Publisher: IOP Publishing
Date: 30-11-2001
Publisher: American Geophysical Union (AGU)
Date: 14-05-2020
DOI: 10.1029/2019GL086438
Abstract: We use magnetopause crossings of the Cassini spacecraft to study the response of Saturn's magnetosphere to changes in external and internal drivers. We explain how solar wind pressure can be corrected to account for the local variability in internal plasma particle pressure. The physics‐based method is applied to perform the most robust estimation of magnetopause compressibility at Saturn to date, using 7 years' worth of magnetometer data from the Cassini mission and accounting for variable internal drivers—particle pressure and azimuthal ring current. The concept of magnetopause compressibility is generalized to quantitatively account for its detailed variation with respect to the position of the magnetopause. An analytical fit is provided to map the compressibility index to values of the stand‐off distance. In particular, the procedure shows that the Kronian system appears to behave similarly to that of Jupiter when expanded outwards and more like the Earth's magnetopause when compressed.
Publisher: Elsevier BV
Date: 2005
Publisher: American Geophysical Union (AGU)
Date: 09-2007
DOI: 10.1029/2006JA012098
Publisher: American Geophysical Union (AGU)
Date: 03-2015
DOI: 10.1002/2014JA020256
Publisher: Copernicus GmbH
Date: 19-07-2011
DOI: 10.5194/ANGEO-29-1253-2011
Abstract: Abstract. The atmosphere of Saturn's largest moon Titan is driven by photochemistry, charged particle precipitation from Saturn's upstream magnetosphere, and presumably by the diffusion of the magnetospheric field into the outer ionosphere, amongst other processes. Ion pickup, controlled by the upstream convection electric field, plays a role in the loss of this atmosphere. The interaction of Titan with Saturn's magnetosphere results in the formation of a flow-induced magnetosphere. The upstream magnetoplasma environment of Titan is a complex and highly variable system and significant quasi-periodic modulations of the plasma in this region of Saturn's magnetosphere have been reported. In this paper we quantitatively investigate the effect of these quasi-periodic modulations on the convection electric field at Titan. We show that the electric field can be significantly perturbed away from the nominal radial orientation inferred from Voyager 1 observations, and demonstrate that upstream categorisation schemes must be used with care when undertaking quantitative studies of Titan's magnetospheric interaction, particularly where assumptions regarding the orientation of the convection electric field are made.
Publisher: American Geophysical Union (AGU)
Date: 11-2008
DOI: 10.1029/2008JA013265
Publisher: American Geophysical Union (AGU)
Date: 2005
DOI: 10.1029/2005GL022835
Publisher: Elsevier BV
Date: 2005
Publisher: Elsevier BV
Date: 07-2013
Publisher: American Geophysical Union (AGU)
Date: 06-2014
DOI: 10.1002/2014JA019941
Publisher: American Geophysical Union (AGU)
Date: 2004
DOI: 10.1029/2003JA010258
Publisher: American Geophysical Union (AGU)
Date: 06-2020
DOI: 10.1029/2019JA027219
Abstract: The 2007–2009 solar minimum was the longest of the space age. We present the first of two companion papers on Chandra and XMM‐Newton X‐ray c aigns of Jupiter through February–March 2007. We find that low solar X‐ray flux during solar minimum causes Jupiter's equatorial regions to be exceptionally X‐ray dim (0.21 GW at minimum 0.76 GW at maximum). While the Jovian equatorial emission varies with solar cycle, the aurorae have comparably bright intervals at solar minimum and maximum. We apply atomic charge exchange models to auroral spectra and find that iogenic plasma of sulphur and oxygen ions provides excellent fits for XMM‐Newton observations. The fitted spectral S:O ratios of 0.4–1.3 are in good agreement with in situ magnetospheric S:O measurements of 0.3–1.5, suggesting that the ions that produce Jupiter's X‐ray aurora predominantly originate inside the magnetosphere. The aurorae were particularly bright on 24–25 February and 8–9 March, but these two observations exhibit very different spatial, spectral, and temporal behavior 24–25 February was the only observation in this c aign with significant hard X‐ray bremsstrahlung from precipitating electrons, suggesting this may be rare. For 8–9 March, a bremsstrahlung component was absent, but bright oxygen O 6+ lines and best‐fit models containing carbon, point to contributions from solar wind ions. This contribution is absent in the other observations. Comparing simultaneous Chandra ACIS and XMM‐Newton EPIC spectra showed that ACIS systematically underreported 0.45‐ to 0.6‐keV Jovian emission, suggesting quenching may be less important for Jupiter's atmosphere than previously thought. We therefore recommend XMM‐Newton for spectral analyses and quantifying opacity/quenching effects.
Publisher: Elsevier BV
Date: 11-1997
Publisher: American Geophysical Union (AGU)
Date: 08-2008
DOI: 10.1029/2007JA012963
Publisher: American Geophysical Union (AGU)
Date: 10-2008
DOI: 10.1029/2008JA013276
Publisher: American Geophysical Union (AGU)
Date: 03-09-2015
DOI: 10.1002/2015GL065477
Publisher: American Geophysical Union (AGU)
Date: 2005
DOI: 10.1029/2005GL022569
Publisher: American Geophysical Union (AGU)
Date: 02-2011
DOI: 10.1029/2010GL046193
Publisher: Elsevier BV
Date: 10-2000
Publisher: American Geophysical Union (AGU)
Date: 05-2014
DOI: 10.1002/2013JA019411
Publisher: American Geophysical Union (AGU)
Date: 02-2021
DOI: 10.1029/2020JA028264
Abstract: Energetic particles ( ∼25 keV) have been observed routinely in the terrestrial magnetosheath, but have not been well studied at the magnetosheaths of the outer planets. Here we analyze energetic electrons and ions (mostly protons) in the vicinity (±1 R S ) of Saturn's magnetopause, using particle data acquired with the low‐energy magnetosphere measurements system, one of the three sensors of the magnetosphere imaging instrument on board the Cassini spacecraft, during a period of ∼14 years (2004–2017). It is found that energetic particles, especially ions, are also common in Saturn's magnetosheath. A clear inward (toward Saturn) gradient in the electron differential flux is identified, suggestive of magnetospheric sources. Such an inward gradient does not appear in some of the ion channels. We conclude that Saturn's magnetopause acts as a porous barrier for energetic electrons and, to a lesser extent, for energetic ions. A dawn‐dusk asymmetry in the gradient of particle flux across the magnetopause is also identified, with a gradual decrease at the dawn and a sharp decrease at the dusk magnetopause. It is also found that magnetic reconnection enhanced flux levels just outside of the magnetopause, with evidence suggesting that these particles are from magnetospheric sources. These findings strongly suggest that Saturn's magnetosphere is most likely the main source of energetic particles in Saturn's magnetosheath and magnetosphere leakage is an important process responsible for the presence of the energetic particles in Saturn's magnetosheath.
Publisher: American Geophysical Union (AGU)
Date: 28-12-2014
DOI: 10.1002/2014GL061747
Publisher: American Geophysical Union (AGU)
Date: 04-2011
DOI: 10.1029/2010JA016045
Publisher: Wiley
Date: 18-10-2020
Publisher: American Geophysical Union (AGU)
Date: 07-2010
DOI: 10.1029/2010JA015351
Publisher: American Geophysical Union (AGU)
Date: 08-2019
DOI: 10.1029/2019JA026751
Abstract: We describe a new method of constructing an equilibrium magnetopause surface based on the pressure balance between external and internal pressure sources. Details are given for every step of the procedure, including the initial pressure balance condition (which determines magnetopause morphology), the related underlying assumptions, and the final optimized magnetopause surface. Our method produces a final equilibrium magnetopause surface that satisfies the local balance between the solar wind dynamic pressure and planetary magnetic pressure with an error no greater than 1 % . We also discuss the contribution of hot plasma pressure and equatorial ring currents and their effects on magnetopause morphology. For each optimized magnetopause boundary, we give coefficients for fitted polynomial approximations to allow simple and accurate reproductions for practical applications. We specifically discuss the potential application to the modeling of Saturn's magnetopause and describe how the equilibrium magnetopause model can be used to estimate the compressibility of the boundary.
Publisher: American Geophysical Union (AGU)
Date: 06-2012
DOI: 10.1029/2011JA017472
Publisher: American Geophysical Union (AGU)
Date: 07-2020
DOI: 10.1029/2020JA027827
Publisher: Elsevier BV
Date: 02-2012
Publisher: Springer Science and Business Media LLC
Date: 05-08-2008
Publisher: American Geophysical Union (AGU)
Date: 10-2011
DOI: 10.1029/2011JA016941
Publisher: American Geophysical Union (AGU)
Date: 07-2014
DOI: 10.1002/2013JA019388
Publisher: American Geophysical Union (AGU)
Date: 25-03-2021
DOI: 10.1029/2020GL091796
Abstract: A sustained quasi‐dipolar magnetic field between the current sheet outer edge and the magnetopause, known as a cushion region, has previously been observed at Jupiter, but not yet at Saturn. Using the complete Cassini magnetometer data, the first evidence of a cushion region forming at Saturn is shown. Only five ex les of a sustained cushion are found, revealing this phenomenon to be rare. Four of the cushion regions are identified at dusk and one pre‐noon. It is suggested that greater heating of plasma post‐noon coupled with the expansion of the field through the afternoon sector makes the disc more unstable in this region. These results highlight a key difference between the Saturn and Jupiter systems.
Publisher: American Geophysical Union (AGU)
Date: 09-2019
DOI: 10.1029/2018JA026363
Publisher: American Geophysical Union (AGU)
Date: 14-06-2007
DOI: 10.1029/2007GL029764
Publisher: American Association for the Advancement of Science (AAAS)
Date: 25-02-2005
Abstract: Cassini's successful orbit insertion has provided the first examination of Saturn's magnetosphere in 23 years, revealing a dynamic plasma and magnetic environment on short and long time scales. There has been no noticeable change in the internal magnetic field, either in its strength or its near-alignment with the rotation axis. However, the external magnetic field is different compared with past spacecraft observations. The current sheet within the magnetosphere is thinner and more extended, and we observed small diamagnetic cavities and ion cyclotron waves of types that were not reported before.
Publisher: American Geophysical Union (AGU)
Date: 19-10-2006
DOI: 10.1029/2006JA011676
Publisher: MDPI AG
Date: 07-05-2023
DOI: 10.3390/JMSE11050996
Abstract: Since concrete is cheaper and more resistant to corrosion than steel, the wide-shallow concrete bucket foundation is being used extensively in ocean engineering. By adding the inner bucket and cruciform skirts, both the bearing capacity and rigidity of the wide-shallow concrete bucket foundation increase significantly. When compared to the hollow steel bucket foundation, the inclusion of thicker skirts, as well as the addition of inner bucket and cruciform skirts, would cause changes to the soil flow mechanism, resulting in soil heave within each compartment and changes in soil strength evolution and penetration resistance during installation in clay. In order to study the influence of the addition of the inner bucket and cruciform skirts on the soil heaving inside each compartment, soil softening and penetration resistance, three-dimensional large deformation finite element (LDFE) models for the bucket foundation with and without inner bucket, and cruciform skirts considering soil remolding were established using the Coupled Eulerian–Lagrangian (CEL) approach. It was found that the inner bucket significantly changes the soil flow and softening of the soil during penetration of the bucket foundation. According to the theoretical analysis and numerical results, the diameter of the optimal inner bucket is equal to 5/8 of the outer diameter. The adhesion coefficient observed in this study falls within the range of 0.5 to 0.8, which is higher than the theoretical value of 0.25 that assumes the soil is fully remolded. The reason for this discrepancy is that the soil is only partially remolded during the actual installation of the bucket foundation. The neglect of the softening of the soil or considering the soil as completely softened will result in significant variation in the predicted penetration resistance hence, partial softening of the soil should be taken into account.
Publisher: American Association for the Advancement of Science (AAAS)
Date: 13-05-2005
Abstract: The magnetic field signature obtained by Cassini during its first close encounter with Titan on 26 October 2004 is presented and explained in terms of an advanced model. Titan was inside the saturnian magnetosphere. A magnetic field minimum before closest approach marked Cassini's entry into the magnetic ionopause layer. Cassini then left the northern and entered the southern magnetic tail lobe. The magnetic field before and after the encounter was approximately constant for ∼20 Titan radii, but the field orientation changed exactly at the location of Titan's orbit. No evidence of an internal magnetic field at Titan was detected.
Publisher: Springer Science and Business Media LLC
Date: 11-2008
DOI: 10.1038/NATURE07440
Abstract: The majority of planetary aurorae are produced by electrical currents flowing between the ionosphere and the magnetosphere which accelerate energetic charged particles that hit the upper atmosphere. At Saturn, these processes collisionally excite hydrogen, causing ultraviolet emission, and ionize the hydrogen, leading to H(3)(+) infrared emission. Although the morphology of these aurorae is affected by changes in the solar wind, the source of the currents which produce them is a matter of debate. Recent models predict only weak emission away from the main auroral oval. Here we report images that show emission both poleward and equatorward of the main oval (separated by a region of low emission). The extensive polar emission is highly variable with time, and disappears when the main oval has a spiral morphology this suggests that although the polar emission may be associated with minor increases in the dynamic pressure from the solar wind, it is not directly linked to strong magnetospheric compressions. This aurora appears to be unique to Saturn and cannot be explained using our current understanding of Saturn's magnetosphere. The equatorward arc of emission exists only on the nightside of the planet, and arises from internal magnetospheric processes that are currently unknown.
Publisher: American Geophysical Union (AGU)
Date: 04-2017
DOI: 10.1002/2017JA023918
Publisher: MDPI AG
Date: 27-06-2022
DOI: 10.3390/JMSE10070885
Abstract: This paper proposes the penetration displacement solutions of large-diameter open-ended steel pipe piles (LOSPs) with the diameter exceeding 2 m subjected to hammering load. The ultimate forcing equilibrium relationships between LOSP and soil are analyzed, and the calculated formula for self-sinking depth is derived. Next, a partial differential equation of pile hammering by single blow in soft soil is developed based on wave equation incorporating the kinematic method. A dynamic coefficient of frictional resistance (DCFR) is implemented in the process of derivation, and then the displacement Fourier analytical expression of LOSP under hammering load is presented. The parameters sensitivity of the analytical solution is investigated, and the displacement curve is compared with the numerical result. The new method presented in this paper could be used to assess the penetration development of driven piles under impact loading to predict the punching through or hammer refusal during penetration.
Publisher: American Geophysical Union (AGU)
Date: 11-2018
DOI: 10.1029/2018JA025828
Publisher: Springer Science and Business Media LLC
Date: 05-1999
DOI: 10.1038/20121
Publisher: American Geophysical Union (AGU)
Date: 05-2021
DOI: 10.1029/2020JA028800
Abstract: Magnetic reconnection at the magnetopause (MP) energizes ambient plasma via the release of magnetic energy and produces an “open” magnetosphere allowing solar wind particles to directly enter the system. At Saturn, the nature of MP reconnection remains unclear. The current study examines electron bulk heating at MP crossings, in order to probe the relationship between observed and predicted reconnection heating proposed by Phan et al. (2013, 0.1002/grl.50917 ) under open and closed MP, and how this may pertain to the position of the crossings in the Δ β ‐magnetic shear parameter space. The electron heating for 70 MP crossings made by the Cassini spacecraft from April 2005 to July 2007 was found using 1d and 3d moment methods. Minimum variance analysis was used on the magnetic field data to help indicate whether the MP is open or closed. We found better agreement between observed and predicted heating for events suggestive of locally “open” MP. For events suggestive of locally “closed” MP, we observed a cluster of points consistent with no electron heating, but also numerous cases with significant heating. Examining the events in the Δ β ‐magnetic shear parameter space, we find 83% of events without evidence of energization were situated in the “reconnection suppressed” regime, whilst between 43% to 68% of events with energization lie in the “reconnection possible” regime depending on the threshold used. The discrepancies could be explained by a combination of spatial and temporal variability which makes it possible to observe heated electrons with different conditions from the putative reconnection site.
Publisher: Copernicus GmbH
Date: 08-10-2020
DOI: 10.5194/EPSC2020-256
Abstract: & & The H2020 Europlanet-2020 programme, which ended on Aug 31& sup& st& /sup& , 2019, included an activity called PSWS (Planetary Space Weather Services), which provided 12 services distributed over four different domains (A. Prediction, B. Detection, C. Modelling, D. Alerts) and accessed through the PSWS portal (planetaryspaceweather-europlanet.irap.omp.eu/):& & & & A1. 1D MHD Solar Wind Prediction Tool & #8211 HELIOPROPA,& & & & A2. Propagation Tool,& & & & A3. Meteor showers,& & & & A4. Cometary tail crossings & #8211 TAILCATCHER,& & & & B1. Lunar impacts & #8211 ALFIE,& & & & B2. Giant planet fireballs & #8211 DeTeCt3.1,& & & & B3. Cometary tails & #8211 WINDSOCKS,& & & & C1. Earth, Mars, Venus, Jupiter coupling- TRANSPLANET,& & & & C2. Mars radiation environment & #8211 RADMAREE,& & & & C3. Giant planet magnetodiscs & #8211 MAGNETODISC,& & & & C4. Jupiter& #8217 s thermosphere, D. Alerts.& & & & In the framework of the starting Europlanet-2024 programme, SPIDER will extend PSWS domains (A. Prediction, C. Modelling, E. Databases) services and give the European planetary scientists, space agencies and industries access to 6 unique, publicly available and sophisticated services in order to model planetary environments and solar wind interactions through the deployment of a dedicated run on request infrastructure and associated databases.& & & & C5. A service for runs on request of models of Jupiter& #8217 s moon exospheres as well as the exosphere of Mercury,& & & & C6. A service to connect the open-source Spacecraft-Plasma Interaction Software (SPIS) software with models of space environments in order to compute the effect of spacecraft potential on scientific instruments onboard space missions. Pre-configured simulations will be made for Bepi-Colombo and JUICE missions,& & & & C7. A service for runs on request of particle tracing models in planetary magnetospheres,& & & & E1. A database of the high-energy particle flux proxy at Mars, Venus and comet 67P using background counts observed in the data obtained by the plasma instruments onboard Mars Express (operational from 2003), Venus Express (2006& #8211 ), and Rosetta (2014& #8211 ) & & & & E2. A simulation database for Mercury and Jupiter& #8217 s moons magnetospheres and link them with prediction of the solar wind parameters from Europlanet-RI H2020 PSWS services.& & & & A1. An extension of the Europlanet-RI H2020 PSWS Heliopropa service in order to ingest new observations from Solar missions like the ESA Solar Orbiter or NASA Solar Parker Probe missions and use them as input parameters for solar wind prediction & & & & These developments will be discussed in the presentation.& & & & The Europlanet 2020 Research Infrastructure project has received funding from the European Union's Horizon 2020 research and innovation programme under grant agreement No 654208.& & & & The Europlanet 2024 Research Infrastructure project has received funding from the European Union's Horizon 2020 research and innovation programme under grant agreement No 871149.& &
Publisher: American Association for the Advancement of Science (AAAS)
Date: 12-09-2008
Abstract: After 3 years and 31 close flybys of Titan by the Cassini Orbiter, Titan was finally observed in the shocked solar wind, outside of Saturn's magnetosphere. These observations revealed that Titan's flow-induced magnetosphere was populated by “fossil” fields originating from Saturn, to which the satellite was exposed before its excursion through the magnetopause. In addition, strong magnetic shear observed at the edge of Titan's induced magnetosphere suggests that reconnection may have been involved in the replacement of the fossil fields by the interplanetary magnetic field.
Publisher: American Geophysical Union (AGU)
Date: 09-2020
DOI: 10.1029/2020JA028247
Abstract: We calculate the magnetospheric drag torques on Saturn's northern and southern polar thermospheres during late southern summer in 2008 and northern spring in 2012–2013 using previously derived profiles of ionospheric meridional coupling currents determined from high‐latitude Cassini magnetic field data. We show that the drag torques in the “winter” and “summer” auroral regions are near equal at ~2.3 × 10 16 N m, contrary to the recent discussion of Brooks et al. (2019, 0.1002/2019JA026870 ) who suggest that significant seasonal differences should occur in these regions. Instead, seasonally dependent torques occur in the adjacent polar open field regions, where the “winter” and “summer” torques are ~0.3 × 10 16 and ~1.8 × 10 16 N m, respectively. We derive a simple rotating disc model of the polar thermosphere and estimate the speed of the poleward flow from midlatitudes required to balance these torques in steady state, finding values of tens of m s −1 consistent with previous numerical modeling. Comparison of the calculated torques with concurrent periods of the northern and southern planetary period oscillations (PPOs) does not suggest a direct connection between these quantities as proposed by Brooks et al., 2019, showing at the least that significant additional factors must be involved. We further note some issues with their scenario for dual modulation of radio emissions, previous observations having shown that the principal oscillatory PPO field‐aligned currents that modulate the emissions rotate in the auroral region with periods ~10.7 ± 0.1 hr, propagating through the more slowly rotating ~15–20 hr period outer magnetospheric plasma, with implications for the proposed “atmospheric flywheel” picture.
Publisher: American Geophysical Union (AGU)
Date: 2006
DOI: 10.1029/2005JA011297
Publisher: American Geophysical Union (AGU)
Date: 23-11-2006
DOI: 10.1029/2005JA011574
Publisher: American Geophysical Union (AGU)
Date: 13-08-2008
DOI: 10.1029/2008GL034132
Publisher: Oxford University Press (OUP)
Date: 19-03-2012
Publisher: American Geophysical Union (AGU)
Date: 04-2014
DOI: 10.1002/2014JA019774
Publisher: Elsevier BV
Date: 02-2014
Publisher: American Geophysical Union (AGU)
Date: 2005
DOI: 10.1029/2005JA011054
Publisher: American Geophysical Union (AGU)
Date: 02-2017
DOI: 10.1002/2016JA023544
Location: United Kingdom of Great Britain and Northern Ireland
No related grants have been discovered for Nicholas Achilleos.