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  • American Geophysical Union (AGU)  (4)
  • 1990-1994  (4)
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  • American Geophysical Union (AGU)  (4)
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  • 1990-1994  (4)
Year
  • 1
    Online Resource
    Online Resource
    American Geophysical Union (AGU) ; 1994
    In:  Journal of Geophysical Research: Space Physics Vol. 99, No. A4 ( 1994-04), p. 5745-5759
    In: Journal of Geophysical Research: Space Physics, American Geophysical Union (AGU), Vol. 99, No. A4 ( 1994-04), p. 5745-5759
    Abstract: We use results of guiding‐center simulations of ion transport to map phase space densities of the stormtime proton ring current. We model a storm as a sequence of substorm‐associated enhancements in the convection electric field. Our pre‐storm phase space distribution is an analytical solution to a steady‐state transport model in which quiet‐time radial diffusion balances charge exchange. This pre‐storm phase space spectra at L ∼2‐4 reproduce many of the features found in observed quiet‐time spectra. Using results from simulations of ion transport during model storms having main phases of 3, 6, and 12 hr, we map phase space distributions from the pre‐storm distribution in accordance with Liouville's theorem. We find stormtime enhancements in the phase space densities at energies E ∼30‐160 keV for L ∼2.5‐4. These enhancements agree well with the observed stormtime ring current. For storms with shorter main phases (∼3 hr), the enhancements are caused mainly by the trapping of ions injected from open night side trajectories, and diffusive transport of higher‐energy (≳ 160 keV) ions contributes little to the stormtime ring current. However, the stormtime ring current is augmented also by the diffusive transport of higher‐energy ions ( E ≳ 160 keV) during storms having longer main phases (≳ 6 hr). In order to account for the increase in Dst associated with the formation of the stormtime ring current, we estimate the enhancement in particle‐energy content that results from stormtime ion transport in the equatorial magnetosphere. We find that transport alone cannot account for the entire increase in | Dst | typical of a major storm. However, we can account for the entire increase in |D st | by realistically increasing the stormtime outer boundary value of the phase space density relative to the quiet‐time value. We compute the magnetic field produced by the ring current itself and find that radial profiles of the magnetic field depression resemble those obtained from observational data.
    Type of Medium: Online Resource
    ISSN: 0148-0227
    Language: English
    Publisher: American Geophysical Union (AGU)
    Publication Date: 1994
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    SSG: 16,13
    Library Location Call Number Volume/Issue/Year Availability
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  • 2
    Online Resource
    Online Resource
    American Geophysical Union (AGU) ; 1993
    In:  Journal of Geophysical Research: Space Physics Vol. 98, No. A3 ( 1993-03), p. 3835-3849
    In: Journal of Geophysical Research: Space Physics, American Geophysical Union (AGU), Vol. 98, No. A3 ( 1993-03), p. 3835-3849
    Abstract: This is an investigation of stormtime particle transport that leads to formation of the ring current. Our method is to trace the guiding‐center motion of representative ions (having selected first adiabatic invariants µ) in response to model substorm‐associated impulses in the convection electric field. We compare our simulation results qualitatively with existing analytically tractable idealizations of particle transport (direct convective access and radial diffusion) in order to assess the limits of validity of these approximations. For µ ≲ 10 MeV/G ( E ≲ 110 keV at L ≈ 3) the ion drift period on the final (ring‐current) drift shell of interest ( L ≈ 3) exceeds the duration of the main phase of our model storm, and we find that the transport of ions to this drift shell is appropriately idealized as direct convective access, typically from open drift paths. Ion transport to a final closed drift path from an open (plasma‐sheet) drift trajectory is possible for those portions of that drift path that lie outside the mean stormtime separatrix between closed and open drift trajectories. For µ ∼ 10‐25 MeV/G (110 keV ≲ E ≲ 280 keV at L ≈ 3) the drift period at L ≈ 3 is comparable to the postulated 3‐hr duration of the storm, and the mode of transport is transitional between direct convective access and transport that resembles radial diffusion. (This particle population is transitional between the ring current and radiation belt). For µ ≳ 25 MeV/G (radiation‐belt ions having E ≳ 280 keV at L ≈ 3) the ion drift period is considerably shorter than the main phase of a typical storm, and ions gain access to the ring‐current region essentially via radial diffusion. By computing the mean and mean‐square cumulative changes in 1/ L among (in this case) 12 representative ions equally spaced in drift time around the steady‐state drift shell of interest ( L ≈ 3), we have estimated (from both our forward and our time‐reversed simulations) the time‐integrated radial‐diffusion coefficients D LL sim for particles having selected values of µ ≳ 15 MeV/G. The results agree surprisingly well with the predictions ( D LL ql ) of quasilinear radial‐diffusion theory, despite the rather brief duration (≈ 3 hr) of our model storm and despite the extreme variability (with frequency) of the spectral‐density function that characterizes the applied electric field during our model storm. As expected, the values of D LL sim deduced (respectively) from our forward and time‐reversed simulations agree even better with each other and with D LL sim when the impulse amplitudes which characterize the individual substorms of our model storm are systematically reduced.
    Type of Medium: Online Resource
    ISSN: 0148-0227
    Language: English
    Publisher: American Geophysical Union (AGU)
    Publication Date: 1993
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    detail.hit.zdb_id: 3094181-7
    detail.hit.zdb_id: 3094219-6
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    SSG: 16,13
    Library Location Call Number Volume/Issue/Year Availability
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  • 3
    Online Resource
    Online Resource
    American Geophysical Union (AGU) ; 1992
    In:  Geophysical Research Letters Vol. 19, No. 6 ( 1992-03-20), p. 621-624
    In: Geophysical Research Letters, American Geophysical Union (AGU), Vol. 19, No. 6 ( 1992-03-20), p. 621-624
    Abstract: Guiding‐center simulations of stormtime transport of ring‐current and radiation‐belt ions having first adiabatic invariants μ ≳ 15 MeV/G (E ≳ 165 keV at L ∼ 3) are surprisingly well described (typically within a factor of ≲ 4) by the quasilinear theory of radial diffusion. This holds even for the case of an individual model storm characterized by substorm‐associated impulses in the convection electric field, provided that the actual spectrum of the electric field is incorporated in the quasilinear theory. Correction of the quasilinear diffusion coefficient for drift‐resonance broadening (so as to define ) reduced the typical discrepancy with the diffusion coefficients deduced from guiding‐center simulations of representative‐particle trajectories to a factor ∼3. The typical discrepancy was reduced to a factor ∼ 1.4 by averaging , , and over an ensemble of model storms characterized by different (but statistically equivalent) sets of substorm‐onset times.
    Type of Medium: Online Resource
    ISSN: 0094-8276 , 1944-8007
    Language: English
    Publisher: American Geophysical Union (AGU)
    Publication Date: 1992
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    detail.hit.zdb_id: 7403-2
    SSG: 16,13
    Library Location Call Number Volume/Issue/Year Availability
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  • 4
    Online Resource
    Online Resource
    American Geophysical Union (AGU) ; 1993
    In:  Geophysical Research Letters Vol. 20, No. 16 ( 1993-08-20), p. 1727-1730
    In: Geophysical Research Letters, American Geophysical Union (AGU), Vol. 20, No. 16 ( 1993-08-20), p. 1727-1730
    Type of Medium: Online Resource
    ISSN: 0094-8276
    Language: English
    Publisher: American Geophysical Union (AGU)
    Publication Date: 1993
    detail.hit.zdb_id: 2021599-X
    detail.hit.zdb_id: 7403-2
    SSG: 16,13
    Library Location Call Number Volume/Issue/Year Availability
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