M. Bouhram’s research while affiliated with Max Planck Institute for Physics and other places

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Publications (48)


Gyrotropic guiding-center fluid theory for the turbulent heating of magnetospheric ions in downward Birkeland current regions. II
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November 2006

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53 Reads

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13 Citations

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Mehdi Bouhram

A new fluid theory in the guiding-center and gyrotropic approximation derivable from the ensemble-averaged Vlasov-Maxwell equations that included the effect of wave-particle interactions for weakly turbulent, weakly inhomogeneous, nonuniformly magnetized plasma was recently given by Jasperse, Basu, Lund, and Bouhram [Phys. Plasmas 13, 072903 (2006) ]. In that theory, the particles are transported in one spatial dimension (the distance s along the magnetic field) but the turbulence is two-dimensional. In this paper, which is intended as a sequel, the above theory is used for quasisteady conditions to find: (1) a new formula for the perpendicular ion-heating rate per unit volume i⊥(s), where i⊥(s) decreases for large s by what we call the “finite ion gyroradius effect”; and (2) a new formula for the perpendicular ion temperature at low altitudes, Ti⊥(s). Parametrized calculations for Ti⊥(s) are also given.

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Gyrotropic guiding-center fluid theory for turbulent inhomogeneous magnetized plasma

July 2006

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67 Reads

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14 Citations

In this paper, a new fluid theory is given in the guiding-center and gyrotropic approximation which is derivable from the Vlasov-Maxwell equations. The theory includes the effect of wave-particle interactions for the weakly turbulent, weakly inhomogeneous, nonuniformly magnetized plasma, and it is applicable to a variety of space and laboratory plasmas. It is assumed that the turbulence is random and electrostatic, and that the velocity-space Fokker-Planck operator can be used to calculate the correlation functions that describe the wave-particle interactions. Conservation laws are derived that relate the low-order velocity moments of the particle distributions to the turbulence. The theory is based on the work of Hubbard [Proc. R. Soc. London, Ser. A 260, 114 (1961)] and Ichimaru and Rosenbluth [Phys. Fluids 13, 2778 (1970)] . In the work presented here, the idea is proposed that the fluid equations can be solved (1) by using measurements of the turbulence to specify the electric-field fluctuations; and (2) by using measurements of the low-order velocity moments to specify the initial and boundary conditions.


Fig. 1. Cluster spacecraft 4 data from 20020418. Panel 1 shows spacecraft and instrument mode, panel 2 instrument sensitivity. Panels 3 and 4 show the H + and O + energy spectrograms, particle flux integrated over all directions. A part of the O + spectrogram contaminated by H + is indicated with a red circle. Panels 5 and 6 shows pitch-angle spectrograms of H + and O + respectively. The angles are in the spacecraft reference frame so the apparent pitch angle for the cold O + beam is actually the angle between the parallel velocity and convection velocity. Pitch-angle 0 is along the direction of the magnetic field so that 180 @BULLET is outflow in the northern hemisphere. Panel 7 shows the magnetic field, both total (red line) and GSE components (orange, black and blue for x, y and z respectively).  
Fig. 2. GSE coordinates of all valid data points used in the study (black dots). The points usually forms continuous lines (individual orbits). The projection on the X-Z and Y-Z plane is shown with grey points.  
Fig. 3. Upper panel: Distribution of perpendicular O + temperature [log eV] for each interval of O + bulk velocity [km s −1 ]. Each column is normalized, the sum of all data bins in a column is 100%. Also shown are the line of equal thermal and bulk velocity (white) and the line of 16% thermal to bulk energy ratio (red). Lower panel: number of data points contributing to each column (blue bars, left y-axis), and the number of measurement days contributing to the column (red line, right y-axis).  
Fig. 4. Upper panel: Distribution of parallel bulk velocity ratio of O + over H + for each interval of O + over H + particle density ratio (log scale). Each column is normalized, the sum of all data bins in a column is 100%. White lines indicate the narrowest region around the maximum in each column which contains 50% of all data points. The two similar red lines show the same distribution limits for the case when the H + moments were calculated for upward moving particles only (see text for further details). The vertical red line indicates where the mass density ratio of H + and O + is unity. Lower panel: number of data points contributing to each column (blue bars, left y-axis), and the number of measurement days contributing to the column (red line, right y-axis).  
Fig. 5. Upper panel: Distribution of magnetic field intensity [nT] for each interval of O + parallel velocity [km s −1 ]. Each column is normalized, the sum of all data bins in a column is 100%. White lines indicate the narrowest region around the maximum in each column which contains 50% of all data points. Lower panel: Number of data points contributing to each column (blue bars, left y-scale), and the number of measurement days contributing to the column (red line, right y-scale).  

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Characteristics of high altitude oxygen ion energization and outflow as observed by Cluster: A statistical study

May 2006

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101 Reads

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71 Citations

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M. Waara

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The results of a statistical study of oxygen ion outflow using Cluster data obtained at high altitude above the polar cap is reported. Moment data for both hydrogen ions (H+) and oxygen ions (O+) from 3 years (2001-2003) of spring orbits (January to May) have been used. The altitudes covered were mainly in the range 5–12 RE geocentric distance. It was found that O+ is significantly transversely energized at high altitudes, indicated both by high perpendicular temperatures for low magnetic field values as well as by a tendency towards higher perpendicular than parallel temperature distributions for the highest observed temperatures. The O+ parallel bulk velocity increases with altitude in particular for the lowest observed altitude intervals. O+ parallel bulk velocities in excess of 60 km s-1 were found mainly at higher altitudes corresponding to magnetic field strengths of less than 100 nT. For the highest observed parallel bulk velocities of O+ the thermal velocity exceeds the bulk velocity, indicating that the beam-like character of the distribution is lost. The parallel bulk velocity of the H+ and O+ was found to typically be close to the same throughout the observation interval when the H+ bulk velocity was calculated for all pitch-angles. When the H+ bulk velocity was calculated for upward moving particles only the H+ parallel bulk velocity was typically higher than that of O+. The parallel bulk velocity is close to the same for a wide range of relative abundance of the two ion species, including when the O+ ions dominates. The thermal velocity of O+ was always well below that of H+. Thus perpendicular energization that is more effective for O+ takes place, but this is not enough to explain the close to similar parallel velocities. Further parallel acceleration must occur. The results presented constrain the models of perpendicular heating and parallel acceleration. In particular centrifugal acceleration of the outflowing ions, which may provide the same parallel velocity increase to the two ion species and a two-stream interaction are discussed in the context of the measurements.


Figure 1. Drawing that shows the simulation domain and the trajectory of the Cassini orbiter during Saturn's orbit insertion (SOI) on July 1, 2004. The dipole field lines are indicated. The vertical axis gives z and the horizontal axis gives the radial distance along the magnetic equator.
A test-particle model of the atmosphere/ionosphere system of Saturn's main rings

March 2006

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59 Reads

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30 Citations

1] The first pass of the Cassini orbiter near the A and B rings of Saturn, formed mainly by H 2 O ice particles, revealed the presence of an ionosphere composed of O + and O 2 + ions. Such a result suggests the existence of an atmospheric halo made up of molecular oxygen surrounding the rings. It is produced by solar UV radiation-induced decomposition of ice releasing molecular oxygen which does not stick on the surface at the relevant temperatures. A Monte Carlo model of the atmosphere/ionosphere ring system that uses test-particles and incorporates chemical processes and transport of both neutrals and plasma ions is developed. Published ion data from the ion mass spectrometer (IMS) experiment were used as constraint and the model provides a very satisfactory fit between simulated O + and O 2 + ion densities and those measured along Cassini trajectory., A test-particle model of the atmosphere/ionosphere system of Saturn's main rings, Geophys. Res. Lett., 33, L05106, doi:10.1029/2005GL025011.


Le halo ionosphérique autour des anneaux de Saturne

March 2006

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15 Reads

Comptes Rendus Physique

During its insertion on an orbit around Saturn, the Cassini orbiter flew above the A and B rings and observations have revealed the presence of an ionosphere composed of O+ and O2+ ions. These observations can be explained by the presence around the rings of an atmospheric halo made up of molecular oxygen produced by the photolytic decomposition of the ice which constitutes the grains. At the temperature of the ring particles, oxygen molecules do not stick on the ice and thus are not lost during collisions with grains. A model of the formation of the ionospheric halo is presented based on a test-particle approach to describe the transport and the physical and chemical mechanisms that play an essential role. This model provides a very satisfactory fit with the data. To cite this article: M. Bouhram et al., C. R. Physique 7 (2006).


Production, ionization and redistribution of O2 in Saturn's ring atmosphere

February 2006

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55 Reads

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115 Citations

Icarus

Molecular oxygen produced by the decomposition of icy surfaces is ubiquitous in Saturn's magnetosphere. A model is described for the toroidal O2 atmosphere indicated by the detection of and O+ over the main rings. The O2 ring atmosphere is produced primarily by UV photon-induced decomposition of ice on the sunlit side of the ring. Because O2 has a long lifetime and interacts frequently with the ring particles, equivalent columns of O2 exist above and below the ring plane with the scale height determined by the local ring temperature. Energetic particles also decompose ice, but estimates of their contribution over the main rings appear to be very low. In steady state, the O2 column density over the rings also depends on the relative efficiency of hydrogen to oxygen loss from the ring/atmosphere system with oxygen being recycled on the grain surfaces. Unlike the neutral density, the ion densities can differ on the sunlit and shaded sides due to differences in the ionization rate, the quenching of ions by the interaction with the ring particles, and the northward shift of the magnetic equator relative to the ring plane. Although O+ is produced with a significant excess energy, is not. Therefore, should mirror well below those altitudes at which ions were detected. However, scattering by ion–molecule collisions results in much larger mirror altitudes, in ion temperatures that go through a minimum over the B-ring, and in the redistribution of both molecular hydrogen and oxygen throughout the magnetosphere. The proposed model is used to describe the measured oxygen ion densities in Saturn's toroidal ring atmosphere and its hydrogen content. The oxygen ion densities over the B-ring appear to require either significant levels of UV light scattering or ion transmission through the ring plane.


Ion composition measurements on field lines connected to the Enceladus torus

January 2006

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7 Reads

The first pass of the Cassini probe in the vicinity of Saturn, above the E-ring, put in evidence a plasma consisting of water group ions with a small nitrogen bearing ion component (3%). Using a simple model for the transport of ions along Saturn's magnetospheric field lines, we show that these ions can be traced back to the Enceladus torus. Such a result can be explained by the existence in this icy satellite, which was observed to be geologically active during a close fly-by, of volatile components such as ammonia NH3, or by the previous implantation of Nitrogen of external origin on its surface.


A model of the neutral and plasma tori around Saturn's A and B rings

January 2006

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15 Reads

Plasma measurements during Cassini's orbit insertion on July 1, 2004 revealed the + presence of an ionosphere above the A and B rings with O2 and O+ as major ions, suggesting the existence of a toroidal atmosphere made up of molecular oxygen. It is likely produced by radiation-induced decomposition of ice releasing both H2 and O2 molecules which do not stick on the surface at the relevant temperatures (80-100 K). Here, we present results of a study based on a hybrid model of the neutral and plasma tori that uses a test-particle approach for ions and neutrals. The model makes use of Monte Carlo techniques and takes into account chemical processes that lead to plasma creation such as photo-ionization and charge exchange. Key features of the plasma transport along Saturn's corotating magnetic field lines include the impact/transmission probability for plasma particles to pass through the rings, taking into account the electrostatic charging of ring particles, and the ambipolar electric field, which preserves electric neutrality above the ring plane. We will account for escape of oxygen and hydrogen from the ring system and chemical recombination of the ring particle surfaces. Published plasma data from CAPS are used as constraints or inputs to the model.


Verifying closure relations for a multimoment fluid model of the long-range potential in downward auroral current regions

January 2006

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11 Reads

Recently we have developed a fluid theory in the guiding center and gyrotropic approximation that includes the effect of wave-particle interactions for the turbulent weakly inhomogeneous non-uniformly magnetized plasma and is applicable to the field-aligned Birkeland current system of the earth s magnetosphere We assume that the turbulence is random and electrostatic and that we can calculate the correlation functions that describe the wave-particle interactions from the velocity-space Fokker-Planck operator From FAST satellite data of the electric field fluctuations we can determine the momentum and energy transfer rates in the fluid equations due to the plasma turbulence This model also uses satellite data as a boundary condition we solve the fluid equations downward to the estimated double layer altitude and upward into the magnetosphere The results of this calculation depend to a significant extent on how the system of equations is closed We seek to verify the closure relations in our model by comparing the high-altitude predictions of a run based on FAST data at sim 4000 km with measurements from Polar at sim 8 R E on nearly the same flux tube We can run our model with different possible closures in order to see which one best predicts the high-altitude observations


Fig. 1. Exemple de spectre en temps de vol obtenu le 30 Juin 2004 vers 20:30 TU.
Fig. 2. Trajectoire de Cassini du 30 juin 2004 à 18h00 au 1 juillet 2004 à 12h00 TU projetée dans les plans X-Z (haut) et X-Y (bas). L'axe Z est parallèle au pôle nord de Saturne et l'axe Y perpendiculaire à l'axe Saturne-Soleil qui est inclinée d'environ 23 • par rapport au plan X-Y . Dans le plan X-Y , les cercles en pointillés indiquent les orbites des principaux satellites de glace : Mimas (M), Encelade (E), Téthys (T), Dione (D) et Rhéa (R).
Fig. 3. Cartes dans le plan des anneaux montrant la position de la source des ions N + sur des intervalles de 3 heures, obtenus à partir du modèle de transport. Les niveaux de gris correspondent aux flux d'ions observés suivant une échelle logarithmique et sont normalisés par rapport à la valeur maximum mesurée.
Le satellite Encelade source d'ions N + dans la magnétosphère de Saturne

December 2005

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75 Reads

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5 Citations

Comptes Rendus Physique

The first pass of the Cassini probe in the vicinity of Saturn, above the E-ring, demonstrated a plasma consisting of water group ions (H+, O+, OH+, H2O+) with a small N+ ion component (3%). Using a simple model for the transport of magnetospheric ions, we show that the N+ ions can be traced back to the Enceladus satellite. Such a result can be explained by the existence in this icy satellite, supposed to be still geologically active, of volatile components such as ammonia NH3, or by the previous implantation of N+ ions of external origin on its surface. To cite this article: M. Bouhram et al., C. R. Physique 6 (2005).


Citations (19)


... Despite the absence of supporting observations, there was strong agreement between the Monte Carlo simulations and the estimates of the mean particle theory. Bouhram et al. [2002Bouhram et al. [ , 2003aBouhram et al. [ , 2003bBouhram et al. [ , 2004] developed a two-dimensional, Monte Carlo model for ion outflow from 50 the dayside cusp/cleft, which is associated with transverse ion heating, they examined the cusp cleft region's transverse heating and ion outflow. They used their model to interpret the Cluster observations, i.e. saturation of transverse energization rate, in terms of finite perpendicular wavelength effects in the wave-particle interactions. ...

Reference:

Comparing Monte Carlo simulations, mean particle theory estimates, and observations of H + and O + outflows at high altitudes and latitudes
On the altitude dependence of tranversely heated oxygen ion distributions.

... These signatures were also well-correlated with observed solar wind pressure enhancements, leading the authors to conclude that in this instance, the magnetopause reconnection rate was modulated by the upstream pressure and/or variations in the IMF clock angle, rather than being inherently self-varying. In a further study into the same event, Cerisier et al. (2005) showed that following each reconnection burst as observed by Cluster and IMAGE, channels of fast ionospheric convection were observed by SuperDARN on the poleward side of the auroral intensifications. The ionospheric convection bursts started shortly after the auroral intensifications, and their duration was longer (∼10 min, cf. ...

Ionospheric Signatures of Plasma Injections in the Cusp Triggered by Solar Wind Pressure Pulses

Journal of Geophysical Research Atmospheres

... Moreover, when harmonic LHWs are strongly excited, the background ions are also strongly accelerated. This result reveals the possibility that harmonic LHWs are involved in ion acceleration phenomena commonly observed in the polar region, such as ion outflow, 36,37 which has been a long-standing unresolved problem. ...

Ion outflow and associated perpendicular heating in the cusp observed by Interball Auroral Probe and Fast Auroral Snapshot

Journal of Geophysical Research Atmospheres

... The ELS measures energetic electrons, providing the electron distribution at energies from 0.6 eV to 28 keV at a spectral resolution of 17% and an angular resolution of 20°. Correction for the spacecraft potential as determined from CAPS ion species iden- tification [Crary et al., 2006] has been applied to the electron distributions. Among other parameters, the LP measures the characteristics of thermal electrons, including the electron density and temperature [Wahlund et al., 2005]. ...

Dynamics and composition of plasma at Titan
  • Citing Article
  • January 2005

... Moore, Lundin, et al., 1999;, and references therein). For example, Bouhram et al. (2004) studied the moments of O+ conics including the velocity, temperature, and energy in the cusp/cleft below 6 Re and showed that these quantities increase with altitude monotonically. Many waves or structures are proposed to energize ions, for example, lower hybrid waves (Chang & Coppi, 1981), ion cyclotron waves (Chang et al., 1986), broadband extremely low-frequency waves (Hultqvist, 1996), Alfven waves (Hull et al., 2019), and quasi-static potential drops (Lundin & Hultqvist, 1989). ...

On the altitude dependence of transversely heated O distributions in the cusp/cleft

... The ring current maximum energy density is usually at the dusk-side magnetosphere (e.g., Fu et al., 2001;Kistler et al., 2016;Zeng et al., 2020). Bouhram et al. (2005) reported that energetic O + ion density in the mid-latitude dayside magnetopause boundary layer presented a significant dawn-dusk asymmetry with high density on the dusk side and lower density on the dawn side. Zeng et al. (2020) investigated the statistical characteristics of the dayside spatial distribution of O + ion density from MMS data. ...

Survey of energetic O+ ions near the dayside mid-latitude magnetopause with Cluster

... Ionospheric outflow in the cusp -subject to intense magnetosheath inflow and strong wave activity -is the dominant source of O + in the magnetosphere (Dubouloz et al., 2001), with typical total fluxes of 2 × 10 25 s −1 (Pollock et al., 1990). Recent studies show that a majority of this outflow will escape, either directly from the cusp (Slapak et al., 2013) or in the distant tail via the plasma mantle (Nilsson, 2011;Nilsson et al., 2012). ...

Spatial structure of the cusp/cleft ion fountain: A case study using a magnetic conjugacy between Interball AP and a pair of SuperDARN radars

Journal of Geophysical Research Atmospheres

... The multipoint measurements provided by the Cluster mission enable an assessment of the ion outflow response to changes in the plasma and wave inputs within the cusp at mid-to high-altitudes. Past multipoint Cluster observational studies have made significant advances in our knowledge of the dayside cusp region, such as in cusp structure, location, and dynamics, and the spatial and temporal evolution of cusp plasma in relation to reconnection processes and solar wind variations (e.g., Bouhram et al., 2004;Cargill et al., 2005;Dunlop et al., 2005;Escoubet et al., 2006Escoubet et al., , 2013Pitout & Bogdanova, 2021;Pitout et al., 2006;Trattner et al., 2005Trattner et al., , 2008Zong et al., 2008, and references therein). However, the distribution and temporal evolution of the plasma and electromagnetic energy input and consequences to ion outflow are not fully understood. ...

Multipoint analysis of the spatio-temporal coherence of dayside O+ outflows with Cluster

... The plasma remains trapped on the field line through the process of reconnection and remains with the field line as it continues through the Dungey cycle. Su et al. 2001, found evidence of plasmasphere material on open field lines with magnetosheath material during periods of K p ≥ 4 using both the Interball Auroral Probe and Polar satellites [3]. Su did not find as many instances of plasmasphere material on open field lines as they thought they would and among other causes, speculated that plasmaspheric material heating could make it indistinguishable from magnetosheath plasma using their method. ...

Plasmaspheric material on high-latitude open field lines

Journal of Geophysical Research Atmospheres

... Using the observed turbulent fluctuations, it will be possible to calculate the global energization and acceleration of charged particles and their phase space distributions using kinetic and/or fluid equations selfconsistently within the auroral range (Chang et al., 2004;Jasperse et al, 2006aJasperse et al, , 2006b. Such calculations are, however, too detailed and complicated for inclusion in this brief chapter. ...

Gyrotropic guiding-center fluid theory for turbulent inhomogeneous magnetized plasma