M. D. Desch’s research while affiliated with Johnson Space Center and other places

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Publications (191)


Lightning storms on Saturn observed by Cassini ISS and RPWS during 2004–2006
  • Article

October 2007

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73 Reads

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90 Citations

Icarus

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Shawn P. Ewald

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[...]

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Joseph Ferrier

We report on Cassini Imaging Science Subsystem (ISS) data correlated with Radio and Plasma Wave Science (RPWS) observations, which indicate lightning on Saturn. A rare bright cloud erupt at ∼35° South planetocentric latitude when radio emissions (Saturn Electrostatic Discharges, or SEDs) occur. The cloud consisting of few consecutive eruptions typically lasts for several weeks, and then both the cloud and the SEDs disappear. They may reappear again after several months or may stay inactive for a year. Possibly, all the clouds are produced by the same atmospheric disturbance which drifts West at 0.45 °/day. As of March 2007, four such correlated visible and radio storms have been observed since Cassini Saturn Orbit Insertion (July 2004). In all four cases the SEDs are periodic with roughly Saturn's rotation rate (h10m39), and show correlated phase relative to the times when the clouds are seen on the spacecraft-facing side of the planet, as had been shown for the 2004 storms in [Porco, C.C., and 34 colleagues, 2005. Science 307, 1243–1247]. The 2000-km-scale storm clouds erupt to unusually high altitudes and then slowly fade at high altitudes and spread at low altitudes. The onset time of individual eruptions is less than a day during which time the SEDs reach their maximum rates. This suggests vigorous atmospheric updrafts accompanied by strong precipitation and lightning. Unlike lightning on Earth and Jupiter, where considerable lightning activity is known to exist, only one latitude on Saturn has produced lightning strong enough to be detected during the two and a half years of Cassini observations. This may partly be a detection issue.


Figure 2. An illustration of the model showing the cyclostrophic winds in the X/Y plane and vertical winds along z.  
Figure 3. The grain X/Y positions after (a) 10 time steps, (b) 300 time steps, and (c) 499 time steps. Charged positive, negative, and neutral grains are indicated by pluses, minuses, and dots, respectively.
Figure 4. A three-dimensional perspective of the grains in the cyclostrophic/vertical winds at (a) 10 time steps, (b) 300 time steps, and (c) 499 time steps.  
Figure 6. The magnetic field as a function of simulation time for DF = À1.6 V.
Figure 7. The magnetic field as a function of simulation time for DF = À0.16 V.

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A model of the ULF magnetic and electric field generated from a dust devil
  • Article
  • Full-text available

November 2006

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168 Reads

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18 Citations

Journal of Geophysical Research Atmospheres

It has been demonstrated that terrestrial dust devils emit ULF magnetic radiation. On Mars, dust devils may also generate such magnetic emissions, which might be used as a hazard alert for manned missions. Specifically, grains in dust devils become charged via contact electrification, and it has been proposed that the cyclonic motion of these charged grains in the vortex wind fields accounts for the magnetic emission. To test this hypothesis in general and the possible Mars application, a computer simulation of the contact electrification/wind blowing phenomena was created, with the charge distribution and resulting magnetic fields monitored as a function of time. The results indicate that indeed a fluctuating charge distribution in a vortex wind can account for the ULF magnetic fields measured from a dust devil. The contact electrification process is a function of composition, and we demonstrate that the various compositions will give rise to different magnetic field responses from the dust devil. We also demonstrate that this system of swirling charged grains develops vertical currents and associated electric fields, as suggested in preceding works.

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Figure 1. 
Figure 2. Modeled ratios of the autocorrelations assuming waves from Saturn (solid line) and Jupiter (dashed line) as a function of frequency during episode A1 of the SED storm A (first 1.5 hours, DOY 195, 02:30-04:00 SCET, 2004). The measured ratios are plotted as asterisks with error bars.
Figure 3. Modeled ratios of the autocorrelations assuming waves from Saturn (solid line) and Jupiter (dashed line) as a function of frequency during the event on DOY 203, 2003, around 20:30 SCET. The ratios of the autocorrelations measured by the w-antenna and the dipole are plotted as asterisks with error bars. The numbers denote the intensity of the respective single burst in dB above the background as measured by the dipole.
Discrimination between Jovian radio emissions and Saturn electrostatic discharges

November 2006

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81 Reads

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6 Citations

1] Short vertical streaks in the dynamic spectrum of the Cassini/RPWS (Radio and Plasma Wave Science) receiver in the frequency range of a few MHz can be due to Jovian radio emissions or SEDs (Saturn electrostatic discharges). Although Jupiter is increasingly far from Cassini, the peaks of decametric Jovian arcs can still be detected a few dB above the galactic background, and in some cases they look very similar to the SEDs caused by lightning in Saturn's atmosphere. We show a method for discriminating between these two phenomena by using the ratio of the measured autocorrelations in case the receiver uses at least two antennas. We analyze the special event from July 22, 2003, which was interpreted as the first indication of SEDs at a time when the spacecraft was still at a distance of 1.08 AU from Saturn, and find that it originated from Jupiter.


Saturn lightning recorded by Cassini/RPWS in 2004

July 2006

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57 Reads

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67 Citations

Icarus

During 2004 the Cassini/RPWS (Radio and Plasma Wave Science) instrument recorded about 5400 SEDs (Saturn Electrostatic Discharges), which were organized in 4 storm systems and 95 episodes. A computer algorithm with different intensity thresholds was applied to extract the SEDs from the RPWS data, and a statistical analysis on the main characteristics of these SEDs is performed. Compared to the SEDs recorded by the Voyagers in the early 1980s, some characteristics like SED rate, intensity, signal duration, or power spectrum are similar, but there are also remarkable differences with regard to time occurrence and frequency range: The first appearance of SEDs (storm 0) was recorded by RPWS from a distance of more than 300 Saturn radii at the end of May 2004, followed by storm A in mid-July, storm B at the beginning of August, and the most prominent storm C throughout most of September. There were also significant intervals of time with no detectable SED activity, e.g., SEDs were practically absent from October 2004 until June 2005. No clear indication for SEDs below a frequency of 1.3 MHz could be found. We suggest that the SED storms A, B, C, and possibly also storm 0 originate from the same storm system residing at a latitude of 35 • South, which lasted for several months, waxed and waned in strength, and rotated with the Voyager radio period of Saturn. The SED source might be located in the updrafting water clouds beneath the visible cloud features detected in the Cassini images.


Figure 2. General Atomics' Altus uninhabited aerial vehicle during an Altus Cumulus Electrification Study (ACES) flight. The Poynting vector system is located in the bulb at the end of the nose-extending boom.
Figure 3. (top) Peak VHF electric field in 5 min intervals along with the figure eight flight path of the Altus (blue) over (bottom left) a south Florida storm and (bottom right) the storm located northwest of Key West.
Figure 4. Discharge-related (a) electric field, (b) Poynting flux, and (c) radiation impedance as a function of frequency, for lightning events in the vicinity of the Altus during 1830– 1930 UT on 10 August 2002. The events identified with ‘‘n’’ originate from the storm nearby and were overflown by the Altus, and those labeled ‘‘se’’ originate from a storm located about 35 km to the southeast of the Altus. Note that the events become nicely ordered when considering radiation impedance. 
Figure 5. Elevation and azimuth of the lightning radiation between 7 and 14 kHz at 1837:13 UT in the Altus’ frame of reference. The aircraft nose is pointed toward the origin (0, 0). Note that the emission originates from a source located $ 45 ° from the nose. 
Radiation impedance over a thunderstorm

June 2006

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280 Reads

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5 Citations

In the summer of 2002 the Altus Cumulus Electrification Study obtained radiated Poynting flux measurements in the near vicinity of lightning discharge events. These measurements not only allow a determination of radiated power but also allow a calculation of the radiation impedance above a thunderstorm when the thunderstorm was acting as an antenna. This impedance is significant since it defines the level of displacement currents propagating into the middle atmosphere and, as applications demonstrate, is a critical quantity in understanding the relationship between power and displacement current in the near vicinity of a thunderstorm. We find that the radiation impedance of the thunderstorm is surprisingly low in the VLF and varies inversely with frequency consistent with a capacitive-like coupling from the thunderstorm to middle atmosphere.


Changing electrical nature of Saturn's rings: Implications for spoke formation

April 2006

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22 Reads

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9 Citations

During Cassini's orbit insertion at Saturn, the trajectory took the spacecraft overtop the planet's famed ring system. At this time, the Cassini Radio and Plasma Wave Science (RPWS) instrument obtained unprecedented observations of electron density in the vicinity of the rings. Using this information and a model of photoemission anticipated from the rings, we demonstrate that the ring surface potential undergoes a seasonal change in electrical configuration, being primarily unipolar (of one charge polarity/potential) during the Voyager era and now bipolar (two separate polarities/potentials) during the Cassini era. We calculate the approximate ring/sun opening angle required for the transition from unipolar to bipolar configuration. Using electron density profiles, we explicitly examine the conditions for current balance on the B ring and show which regions are most likely to charge to positive potentials and those that may remain negative as a function of ring opening angle relative to the sun. Finally, we demonstrate that the current body of observations of Saturn ring spokes is consistent with their formation only on negatively-charged surfaces, and suggest future times and locations to look for spoke activity based upon the model.






Citations (76)


... The geometric model of the UKR sources with properties relevant for passive sounding is shown in Figure 2. The UKR sources are located around the northern and southern magnetic poles, which are not aligned with the spin axis of Uranus and the radio emission is beamed along the edge of a hollow-cone (Desch et al., 1991;Farrell, 1992;Zarka, 1998). Note that the northern magnetic pole resides in the southern planetographic hemisphere and vice-versa. ...

Reference:

Feasibility of Passive Sounding of Uranian Moons Using Uranian Kilometric Radiation
URANUS AS A RADIO SOURCE
  • Citing Chapter
  • September 1991

... But note however that we did not observe series of bands as regularly organized as523 in. towards high latitudes has been attributed to propagation effects from high 531 latitude sources(MacDowall et al., 1993;Desch, 1994; Hospodarsky et al., 2004). We find 532 here (9) that the occurrence of QP reaches extremely high values (> 80%) at high lat-533 itudes, and that it seems better organized in magnetic latitude, revealing a very active 534 auroral-related process.535The ...

Jupiter Radio Bursts and Particle Acceleration
  • Citing Article
  • January 1994

International Astronomical Union Colloquium

... Other notable projects such as the Altus Cumulus Electrification Study (ACES; Blakeslee et al. 2002;Mach et al. 2005) and the Western States Fire Mission (Ambrosia et al. 2004;Mach et al. 2005;Wegener et al. 2008) have also used large, high-altitude, longendurance UA. The versatility of small UA (<25 kg takeoff weight) has been embraced by a number of investigators who require flexibility in launch and landing, rapid deployability, and reduced cost of operation, maintenance, and replacement compared to the large class of UA. ...

The Altus Cumulus Electrification Study (ACES): A UAV-Based Science Demonstration
  • Citing Conference Paper
  • May 2002

... Derived from works of Jester and Falcke (2009); Cecconi et al. (2012); Zarka et al. (2012); Klein Wolt et al. (2012); Boudjada et al. (2013); Zarka et al. (2018); Jácome et al. (2022); Desch and Rucker (1983); Kurth et al. (2005); Zarka et al. (1996);Kaiser et al. (1996); R.Manning and Dulk (2001);Novaco and Brown (1978); G. A.Dulk et al. (2001);Zarka et al. (2004); A.Vecchio et al. (2021);Meyer-Vernet (1979). ...

WIND/WAVES observations of man-made radio transmissions
  • Citing Article
  • May 1996

... Unfortunately, only a small number of ionospheric pump facilities exist in the world, and so it is not easy to quantify this effect properly. However, sprites and their parent lightning discharges are known to produce powerful radio waves over a broad spectrum (e.g., Füllekrug et al. 2011b;Siingh et al. 2008;Farrell and Desch 1992), including the HF band. This means that the upper-hybrid resonance can be stimulated for a wide altitude range in the F-region. ...

Cloud-to-stratosphere lightning discharges: A radio emission model
  • Citing Article
  • April 1992

... Furthermore, several episodes have been found when periodic non-Io DAM was observed simultaneously with so-called "bullseyes", U-shaped narrowband emissions in the low frequency 20-50 kHz band (Kaiser and MacDowall, 1998), observed by Ulysses/URAP spacecraft. Farrell et al. (2004) explained the "bullseyes" emission as Jovian narrowband kilometric emissions (nKOM) generated in the radially extended plasma fingers developed in the course of the interchange instability in the Io torus. These latitudinal extended fingers may be a plasma source which supplies the cyclotron maser in the auroral region. ...

Remote sensing of possible plasma density bubbles in the inner Jovian dayside magnetosphere
  • Citing Article
  • September 2004

Journal of Geophysical Research Atmospheres

... This process is often referred to as the Dungey cycle [22], and interaction of the high energy electrons with the atmosphere produces the aurora australis and borealis on Earth. Interestingly, the observed auroral radio power from the magnetised Solar System planets is seen to directly scale with the power of the incident solar wind, both kinetically and magnetically [23,50,51,52] -with the kinetic relation often referred to as the radiometric Bode's law, and the magnetic relation as the radio-magnetic scaling law. ...

On the possibility of coherent cyclotron emission from extrasolar planets
  • Citing Article
  • June 1999

Journal of Geophysical Research Atmospheres

... During magnetotail reconnection, whistler waves are associated with perpendicular heating of few to tens of keV electrons leading to a temperature anisotropy that promotes wave growth 9 . Farrell et al. 10,11 reported waves around electron plasma frequency during magnetotail reconnection. Whistler waves are often related to the dayside magnetic reconnection [12][13][14][15][16][17] . ...

The role of upper hybrid waves in magnetic reconnection
  • Citing Article
  • December 2003

... This radio emission is known as Saturn Kilometric Radiation, or SKR. Observations from the Ulysses (Lecacheux et al., 1997) and later Cassini (Gurnett et al., 2005) missions revealed that the SKR period was actually drifting over time, and thus could not be associated with the core rotation rate. A reanalysis of magnetometer data from the Voyager and Pioneer missions then showed a similar periodic behaviour in the magnetic field (Espinosa and Dougherty, 2000). ...

Cassini Radio and Plasma Wave Observations at Saturn
  • Citing Article
  • March 2005

... During magnetotail reconnection, whistler waves are associated with perpendicular heating of few to tens of keV electrons leading to a temperature anisotropy that promotes wave growth 9 . Farrell et al. 10,11 reported waves around electron plasma frequency during magnetotail reconnection. Whistler waves are often related to the dayside magnetic reconnection [12][13][14][15][16][17] . ...

The dominance of electron plasma waves near a reconnection X-line region
  • Citing Article
  • October 2002