Re: [EVGRAY] Re: Magnetic flux annihilation-reconnect phenomenon

Database ID: 111650
2019-01-10T18:21:34-06:00
Norman Wootan <[email protected]>

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Lets look at the actual make up of the magnetic flux lines. 
https://van.physics.illinois.edu/qa/listing.php?id=414

https://www.reddit.com/r/askscience/comments/30fari/what_is_a_magnetic_field_made_of/ 
Interesting note here  "Take the magnetic field created by the earth for 
example. This field is very big. If virtual photons can travel all the 
way around the field in a time shorter than planck time, aren't they 
moving faster than the speed of light?"   Ah Ha!   Super Light, Super 
luminal velocities.

https://www.youtube.com/watch?v=cYA0bntrjsk&feature=youtu.be

https://www.youtube.com/watch?v=3P-FGw5KUeo&feature=youtu.be

https://www.youtube.com/watch?v=crfY2vzVMbI&feature=youtu.be

https://www.youtube.com/watch?v=rst9EcF9ryk&feature=youtu.be

https://www.youtube.com/watch?v=hk1cOffTgdk&feature=youtu.be The Best!

On 1/10/2019 4:55 PM, Norman Wootan wrote:
>
> Thank You, Bert Pool for this new soc. 
> https://scienceblog.com/505176/scientists-inch-closer-to-fusion-energy-with-discovery-of-a-process-that-stabilizes-plasmas/
>
> On 1/10/2019 7:58 AM, Norman Wootan [email protected] [EVGRAY] wrote:
>>
>>
>>   Alfvén wave
>>
>> An *Alfvén wave* is a wave that occurs in a plasma 
>> <https://www.plasma-universe.com/Plasma> (or conducting fluid), 
>> resulting from the interaction of the magnetic fields and electric 
>> currents <https://www.plasma-universe.com/Electric_current> within 
>> it, causing an oscillation of the ions. Alfvén wrote in a letter to 
>> the journal /Nature/ in 1942:
>>
>>     "If a conducting liquid is placed in a constant magnetic field,
>>     every motion of the liquid gives rise to an E.M.F. which produces
>>     electric currents. Owing to the magnetic field, these currents
>>     give mechanical forces which change the state of motion of the
>>     liquid. Thus a kind of combined electromagnetic-hydrodynamic wave
>>     is produced."^[1]
>>     <https://www.plasma-universe.com/Alfv%C3%A9n_wave#cite_note-alfven1942-1>
>>
>>
>> Alfvén waves initiated the field of magnetohydrodynamics 
>> <https://www.plasma-universe.com/Magnetohydrodynamics> which 
>> subsequently earned Alfvén a Nobel Prize.
>>
>> Put some thought behind this statement  "A conductive liquid"!!
>>
>> On 1/10/2019 7:41 AM, Norman Wootan wrote:
>>>
>>> https://en.wikipedia.org/wiki/Hannes_Alfv%C3%A9n Please read this 
>>> mans research and see how he was often rejected by fellow physicists.
>>>
>>> On 1/10/2019 7:31 AM, Norman Wootan wrote:
>>>>
>>>> http://aa.springer.de/papers/7324002/2300449.pdf Still researching 
>>>> the importance of the Alfven waves in plasma.
>>>>
>>>> On 1/10/2019 6:51 AM, Norman Wootan wrote:
>>>>>
>>>>> Moray, Jon Gentry and Warren asked pertinent questions regarding 
>>>>> velocities, magnetic flux etc. in plasma events so I did a search 
>>>>> as to whether Alfven waves have a frequency.  This site pretty 
>>>>> well defines a lot of plasma info that we need. See: 
>>>>> https://www.britannica.com/science/plasma-state-of-matter#ref507092
>>>>>
>>>>> On 1/10/2019 6:29 AM, Warren Keillor [email protected] 
>>>>> [EVGRAY] wrote:
>>>>>> Norman
>>>>>> Hooper's work looks very compelling. At his time of 
>>>>>> experimentation, super conductors were not a reality as they are 
>>>>>> now. The fact that a resistance free conductor might accelerate  
>>>>>> a potential's velocity, after going through a resistor, suggests 
>>>>>> an analogy to fluid dynamics, much like Bernuili's principle 
>>>>>> application of a venturi to gases.
>>>>>> The idea of dielectric conductors is a mind smasher, inverting 
>>>>>> our entire circuit thoughts.
>>>>>> Generally, pretty radical concepts, in a zone to set us up for 
>>>>>> quantum physics thinking. Whew!
>>>>>> Cheers Warren
>>>>>>
>>>>>> Sent from Yahoo Mail on Android 
>>>>>> <https://go.onelink.me/107872968?pid=InProduct&c=Global_Internal_YGrowth_AndroidEmailSig__AndroidUsers&af_wl=ym&af_sub1=Internal&af_sub2=Global_YGrowth&af_sub3=EmailSignature>
>>>>>>
>>>>>>     On Wed, 9 Jan 2019 at 3:17 PM, Norman Wootan [email protected]
>>>>>>     [EVGRAY]
>>>>>>     <[email protected]> wrote:
>>>>>>
>>>>>>     Good question Warren! Nobody really knows how the potential
>>>>>>     and current manifest in the conductor passing through a flux
>>>>>>     field. Your question is valid cause there very well may be
>>>>>>     some sort of reconnect occurring here. Theory was, that the
>>>>>>     flux field was photon stream which enabled pairing to produce
>>>>>>     electrons and attending current. There is still so much that
>>>>>>     we don't know but things are getting interesting.   Read that
>>>>>>     last doc that I posted for it is very enlightening on this
>>>>>>     subject.  See:
>>>>>>     http://www.tfcbooks.com/mall/more/temp/x565-hen.htm This is
>>>>>>     one of Oles favorites.
>>>>>>
>>>>>>     On 1/9/2019 9:09 AM, Warren Keillor
>>>>>>     [email protected]
>>>>>>     <mailto:[email protected]> [EVGRAY] wrote:
>>>>>>>
>>>>>>>     Norman
>>>>>>>
>>>>>>>     I wonder if, in a down to earth , practical manner, the
>>>>>>>     connect/re-connect plays a role in, for instance, the
>>>>>>>     Kromery, where one slides the magnets at right angles to
>>>>>>>     their locked together state.
>>>>>>>     Initially, I need both hands to grasp the flywheel to turn
>>>>>>>     my Kromery.
>>>>>>>     Once turning, one finger's friction on the rim, easily
>>>>>>>     rotates the flywheel, regardless of the load.
>>>>>>>     Too fast, then eddy currents start warming the magnetic coil
>>>>>>>     cores.
>>>>>>>     Are we cutting those magnetic lines?
>>>>>>>     Cheers Warren
>>>>>>>     Sent from Yahoo Mail on Android
>>>>>>>     <https://go.onelink.me/107872968?pid=InProduct&c=Global_Internal_YGrowth_AndroidEmailSig__AndroidUsers&af_wl=ym&af_sub1=Internal&af_sub2=Global_YGrowth&af_sub3=EmailSignature>
>>>>>>>
>>>>>>>         On Wed, 9 Jan 2019 at 9:25 AM, Norman Wootan
>>>>>>>         [email protected] <mailto:[email protected]> [EVGRAY]
>>>>>>>         <[email protected]> <mailto:[email protected]>
>>>>>>>         wrote:
>>>>>>>
>>>>>>>         http://young.caltech.edu/Collisionless_Magnetic_Reconnection.html
>>>>>>>
>>>>>>>         On 1/9/2019 8:21 AM, Norman Wootan wrote:
>>>>>>>>
>>>>>>>>         https://phys.org/news/2017-10-hidden-mechanics-magnetic-field-reconnection.html
>>>>>>>>
>>>>>>>>         On 1/9/2019 8:14 AM, Norman Wootan wrote:
>>>>>>>>>
>>>>>>>>>         https://gss.pppl.gov/talks/reconnection%20lecture%201.pdf
>>>>>>>>>
>>>>>>>>>         On 1/9/2019 8:09 AM, Norman Wootan wrote:
>>>>>>>>>>
>>>>>>>>>>         https://link.springer.com/chapter/10.1007%2F978-94-009-0545-0_14
>>>>>>>>>>
>>>>>>>>>>
>>>>>>>>>>
>>>>>>>>>>
>>>>>>>>>>         Recent
>>>>>>>>>>         Developments
>>>>>>>>>>         in
>>>>>>>>>>         the
>>>>>>>>>>         Theory
>>>>>>>>>>         of
>>>>>>>>>>         Magnetic
>>>>>>>>>>         Reconnection
>>>>>>>>>>         Dieter
>>>>>>>>>>         Biskamp
>>>>>>>>>>         Max-Planck-Institut
>>>>>>>>>>         fiir
>>>>>>>>>>         Plasmaphysik
>>>>>>>>>>         8046
>>>>>>>>>>         Garching
>>>>>>>>>>         bei
>>>>>>>>>>         Miinchen,
>>>>>>>>>>         Federal
>>>>>>>>>>         Republic
>>>>>>>>>>         of
>>>>>>>>>>         Germany
>>>>>>>>>>         Abstract
>>>>>>>>>>         The
>>>>>>>>>>         talk
>>>>>>>>>>         briefly
>>>>>>>>>>         reviews
>>>>>>>>>>         previous
>>>>>>>>>>         stationary
>>>>>>>>>>         models,
>>>>>>>>>>         mainly
>>>>>>>>>>         configurations
>>>>>>>>>>         of
>>>>>>>>>>         the
>>>>>>>>>>         Petschek
>>>>>>>>>>         type,
>>>>>>>>>>         pointing
>>>>>>>>>>         out
>>>>>>>>>>         their
>>>>>>>>>>         shortcomings
>>>>>>>>>>         and
>>>>>>>>>>         basic
>>>>>>>>>>         failure
>>>>>>>>>>         in
>>>>>>>>>>         accounting
>>>>>>>>>>         for
>>>>>>>>>>         fast
>>>>>>>>>>         magnetic
>>>>>>>>>>         reconnection
>>>>>>>>>>         in
>>>>>>>>>>         the
>>>>>>>>>>         limit
>>>>>>>>>>         of
>>>>>>>>>>         large
>>>>>>>>>>         magnetic
>>>>>>>>>>         Reynolds
>>>>>>>>>>         number.
>>>>>>>>>>         It
>>>>>>>>>>         is
>>>>>>>>>>         shown
>>>>>>>>>>         that
>>>>>>>>>>         in
>>>>>>>>>>         this
>>>>>>>>>>         limit
>>>>>>>>>>         no
>>>>>>>>>>         relevant
>>>>>>>>>>         stationary
>>>>>>>>>>         states
>>>>>>>>>>         exist.
>>>>>>>>>>         Instead
>>>>>>>>>>         strong
>>>>>>>>>>         small-scale
>>>>>>>>>>         MHD
>>>>>>>>>>         turbulence
>>>>>>>>>>         develops
>>>>>>>>>>         even
>>>>>>>>>>         in
>>>>>>>>>>         2D
>>>>>>>>>>         geometry,
>>>>>>>>>>         giving
>>>>>>>>>>         rise
>>>>>>>>>>         to
>>>>>>>>>>         energy
>>>>>>>>>>         dissipation
>>>>>>>>>>         and
>>>>>>>>>>         reconnection
>>>>>>>>>>         rates
>>>>>>>>>>         independent
>>>>>>>>>>         of
>>>>>>>>>>         the
>>>>>>>>>>         value
>>>>>>>>>>         of
>>>>>>>>>>         the
>>>>>>>>>>         collisional
>>>>>>>>>>         re-
>>>>>>>>>>         sistivity.
>>>>>>>>>>         I
>>>>>>>>>>         Introduction
>>>>>>>>>>         In
>>>>>>>>>>         the
>>>>>>>>>>         last
>>>>>>>>>>         decade
>>>>>>>>>>         it
>>>>>>>>>>         has
>>>>>>>>>>         been realized
>>>>>>>>>>         that
>>>>>>>>>>         the
>>>>>>>>>>         presence
>>>>>>>>>>         of
>>>>>>>>>>         magnetic
>>>>>>>>>>         fields
>>>>>>>>>>         is
>>>>>>>>>>         a
>>>>>>>>>>         ubiquitous
>>>>>>>>>>         phenomenon
>>>>>>>>>>         in
>>>>>>>>>>         cosmic
>>>>>>>>>>         systems.
>>>>>>>>>>         On
>>>>>>>>>>         the
>>>>>>>>>>         one
>>>>>>>>>>         hand,
>>>>>>>>>>         magnetic
>>>>>>>>>>         fields
>>>>>>>>>>         serve
>>>>>>>>>>         as
>>>>>>>>>>         a large
>>>>>>>>>>         energy
>>>>>>>>>>         reservoir
>>>>>>>>>>         which
>>>>>>>>>>         may
>>>>>>>>>>         be
>>>>>>>>>>         tapped
>>>>>>>>>>         in
>>>>>>>>>>         a fast
>>>>>>>>>>         dynamic
>>>>>>>>>>         process
>>>>>>>>>>         leading
>>>>>>>>>>         to
>>>>>>>>>>         various
>>>>>>>>>>         kinds
>>>>>>>>>>         of
>>>>>>>>>>         explosive
>>>>>>>>>>         events
>>>>>>>>>>         such
>>>>>>>>>>         as
>>>>>>>>>>         flares.
>>>>>>>>>>         On
>>>>>>>>>>         the
>>>>>>>>>>         other
>>>>>>>>>>         hand,
>>>>>>>>>>         magnetic
>>>>>>>>>>         fields
>>>>>>>>>>         tend
>>>>>>>>>>         to
>>>>>>>>>>         be
>>>>>>>>>>         compressed
>>>>>>>>>>         in
>>>>>>>>>>         processes
>>>>>>>>>>         such
>>>>>>>>>>         as
>>>>>>>>>>         protostar
>>>>>>>>>>         formation
>>>>>>>>>>         and
>>>>>>>>>>         are
>>>>>>>>>>         computed
>>>>>>>>>>         to
>>>>>>>>>>         dominate
>>>>>>>>>>         the
>>>>>>>>>>         dynamics
>>>>>>>>>>         in
>>>>>>>>>>         the
>>>>>>>>>>         later
>>>>>>>>>>         phases
>>>>>>>>>>         in
>>>>>>>>>>         a nonrealistic
>>>>>>>>>>         way
>>>>>>>>>>         if
>>>>>>>>>>         not
>>>>>>>>>>         dissipated
>>>>>>>>>>         sufficiently
>>>>>>>>>>         fast.
>>>>>>>>>>         To
>>>>>>>>>>         account
>>>>>>>>>>         for
>>>>>>>>>>         such
>>>>>>>>>>         processes of
>>>>>>>>>>         fast
>>>>>>>>>>         magnetic
>>>>>>>>>>         field
>>>>>>>>>>         annihilation
>>>>>>>>>>         is
>>>>>>>>>>         the
>>>>>>>>>>         main
>>>>>>>>>>         objective
>>>>>>>>>>         of
>>>>>>>>>>         the
>>>>>>>>>>         theory
>>>>>>>>>>         of
>>>>>>>>>>         magnetic
>>>>>>>>>>         reconnect
>>>>>>>>>>         ion.
>>>>>>>>>>         The
>>>>>>>>>>         term
>>>>>>>>>>         magnetic
>>>>>>>>>>         reconnect
>>>>>>>>>>         ion
>>>>>>>>>>         refers
>>>>>>>>>>         to
>>>>>>>>>>         the
>>>>>>>>>>         picture
>>>>>>>>>>         of
>>>>>>>>>>         magnetic
>>>>>>>>>>         field
>>>>>>>>>>         lines.
>>>>>>>>>>         These
>>>>>>>>>>         have
>>>>>>>>>>         a well-defined
>>>>>>>>>>         meaning
>>>>>>>>>>         in
>>>>>>>>>>         a highly
>>>>>>>>>>         conducting
>>>>>>>>>>         fluid,
>>>>>>>>>>         viz.
>>>>>>>>>>         thin
>>>>>>>>>>         magnetic
>>>>>>>>>>         flux
>>>>>>>>>>         tubes
>>>>>>>>>>         which
>>>>>>>>>>         are
>>>>>>>>>>         carried
>>>>>>>>>>         along
>>>>>>>>>>         with
>>>>>>>>>>         the
>>>>>>>>>>         fluid,
>>>>>>>>>>         maintaining
>>>>>>>>>>         their
>>>>>>>>>>         individuality,
>>>>>>>>>>         though
>>>>>>>>>>         they
>>>>>>>>>>         may
>>>>>>>>>>         be
>>>>>>>>>>         wound
>>>>>>>>>>         in
>>>>>>>>>>         a very
>>>>>>>>>>         complex
>>>>>>>>>>         manner.
>>>>>>>>>>         Only
>>>>>>>>>>         owing
>>>>>>>>>>         to
>>>>>>>>>>         finite
>>>>>>>>>>         electrical
>>>>>>>>>>         resistivity
>>>>>>>>>>         or
>>>>>>>>>>         some
>>>>>>>>>>         equivalent
>>>>>>>>>>         process
>>>>>>>>>>         may
>>>>>>>>>>         two
>>>>>>>>>>         field
>>>>>>>>>>         lines
>>>>>>>>>>         coming
>>>>>>>>>>         close
>>>>>>>>>>         together
>>>>>>>>>>         lose
>>>>>>>>>>         their
>>>>>>>>>>         identities
>>>>>>>>>>         by
>>>>>>>>>>         being
>>>>>>>>>>         cut
>>>>>>>>>>         and
>>>>>>>>>>         reconnected
>>>>>>>>>>         in
>>>>>>>>>>         a different
>>>>>>>>>>         way.
>>>>>>>>>>         Though
>>>>>>>>>>         this
>>>>>>>>>>         is
>>>>>>>>>>         a local
>>>>>>>>>>         process,
>>>>>>>>>>         it
>>>>>>>>>>         leads
>>>>>>>>>>         to
>>>>>>>>>>         a change
>>>>>>>>>>         of
>>>>>>>>>>         field
>>>>>>>>>>         topology
>>>>>>>>>>         permitting
>>>>>>>>>>         new
>>>>>>>>>>         types
>>>>>>>>>>         of
>>>>>>>>>>         large-scale
>>>>>>>>>>         plasma
>>>>>>>>>>         motions
>>>>>>>>>>         that
>>>>>>>>>>         would
>>>>>>>>>>         otherwise
>>>>>>>>>>         be
>>>>>>>>>>         inhibited.
>>>>>>>>>>         The
>>>>>>>>>>         255
>>>>>>>>>>         w.
>>>>>>>>>>         BrinbMnn
>>>>>>>>>>         et
>>>>>>>>>>         al.
>>>>>>>>>>         (eds.J,
>>>>>>>>>>         Physical
>>>>>>>>>>         Processes
>>>>>>>>>>         in
>>>>>>>>>>         Hot
>>>>>>>>>>         Cosmic
>>>>>>>>>>         PlIlsmas,
>>>>>>>>>>         255-269.
>>>>>>>>>>         e
>>>>>>>>>>         1990
>>>>>>>>>>         Kluwer
>>>>>>>>>>         Academic
>>>>>>>>>>         Publishers.
>>>>>>>>>>         256
>>>>>>>>>>         change
>>>>>>>>>>         of
>>>>>>>>>>         the
>>>>>>>>>>         magnetic
>>>>>>>>>>         field
>>>>>>>>>>         is described
>>>>>>>>>>         by
>>>>>>>>>>         Faraday's
>>>>>>>>>>         law:
>>>>>>>>>>         oB
>>>>>>>>>>         (
>>>>>>>>>>         ...
>>>>>>>>>>         )
>>>>>>>>>>         2'"
>>>>>>>>>>         7it=VX
>>>>>>>>>>         iixB
>>>>>>>>>>         +
>>>>>>>>>>         'IV
>>>>>>>>>>         B.
>>>>>>>>>>         (1)
>>>>>>>>>>         Here
>>>>>>>>>>         the
>>>>>>>>>>         ratio
>>>>>>>>>>         of
>>>>>>>>>>         the
>>>>>>>>>>         diffusion
>>>>>>>>>>         term
>>>>>>>>>>         and
>>>>>>>>>>         the
>>>>>>>>>>         convection
>>>>>>>>>>         term
>>>>>>>>>>         (2)
>>>>>>>>>>         is
>>>>>>>>>>         a convenient
>>>>>>>>>>         dimensionless
>>>>>>>>>>         measure
>>>>>>>>>>         of
>>>>>>>>>>         the
>>>>>>>>>>         resistivity,
>>>>>>>>>>         Rm
>>>>>>>>>>         being
>>>>>>>>>>         the
>>>>>>>>>>         magnetic
>>>>>>>>>>         Reynolds
>>>>>>>>>>         number.
>>>>>>>>>>         In
>>>>>>>>>>         practically
>>>>>>>>>>         all
>>>>>>>>>>         astrophysical
>>>>>>>>>>         plasmas
>>>>>>>>>>         Rm
>>>>>>>>>>         is large,
>>>>>>>>>>         essentially
>>>>>>>>>>         because
>>>>>>>>>>         of
>>>>>>>>>>         the
>>>>>>>>>>         large
>>>>>>>>>>         scales
>>>>>>>>>>         L.
>>>>>>>>>>         Hence
>>>>>>>>>>         magnetic
>>>>>>>>>>         diffusion
>>>>>>>>>>         is
>>>>>>>>>>         in
>>>>>>>>>>         general
>>>>>>>>>>         a very
>>>>>>>>>>         weak
>>>>>>>>>>         process.
>>>>>>>>>>         Magnetic
>>>>>>>>>>         processes
>>>>>>>>>>         such
>>>>>>>>>>         as
>>>>>>>>>>         solar
>>>>>>>>>>         flares,
>>>>>>>>>>         however,
>>>>>>>>>>         seem
>>>>>>>>>>         to
>>>>>>>>>>         require
>>>>>>>>>>         fast
>>>>>>>>>>         reconnection
>>>>>>>>>>         with
>>>>>>>>>>         time
>>>>>>>>>>         scales
>>>>>>>>>>         practically
>>>>>>>>>>         independent
>>>>>>>>>>         of
>>>>>>>>>>         Rm.
>>>>>>>>>>         The
>>>>>>>>>>         main
>>>>>>>>>>         theoretical
>>>>>>>>>>         problem
>>>>>>>>>>         therefore
>>>>>>>>>>         is
>>>>>>>>>>         to
>>>>>>>>>>         find
>>>>>>>>>>         models
>>>>>>>>>>         allowing
>>>>>>>>>>         sufficiently
>>>>>>>>>>         high
>>>>>>>>>>         reconnect
>>>>>>>>>>         ion
>>>>>>>>>>         rates.
>>>>>>>>>>         Fast
>>>>>>>>>>         reconnection
>>>>>>>>>>         is
>>>>>>>>>>         not
>>>>>>>>>>         a diffuse
>>>>>>>>>>         process,
>>>>>>>>>>         but
>>>>>>>>>>         is
>>>>>>>>>>         strongly
>>>>>>>>>>         localized
>>>>>>>>>>         in
>>>>>>>>>>         current
>>>>>>>>>>         sheets.
>>>>>>>>>>         Such
>>>>>>>>>>         current
>>>>>>>>>>         sheets
>>>>>>>>>>         may
>>>>>>>>>>         arise
>>>>>>>>>>         at
>>>>>>>>>>         any
>>>>>>>>>>         point
>>>>>>>>>>         with
>>>>>>>>>>         non-vanishing
>>>>>>>>>>         magnetic
>>>>>>>>>>         shear
>>>>>>>>>>         and
>>>>>>>>>>         a velocity
>>>>>>>>>>         gradient
>>>>>>>>>>         along
>>>>>>>>>>         the
>>>>>>>>>>         direction
>>>>>>>>>>         of
>>>>>>>>>>         the
>>>>>>>>>>         shear
>>>>>>>>>>         perpendicular
>>>>>>>>>>         to
>>>>>>>>>>         the
>>>>>>>>>>         field,
>>>>>>>>>>         i.e.
>>>>>>>>>>         virtually
>>>>>>>>>>         everywhere
>>>>>>>>>>         in
>>>>>>>>>>         the
>>>>>>>>>>         plasma,
>>>>>>>>>>         as
>>>>>>>>>>         visualized
>>>>>>>>>>         in
>>>>>>>>>>         Fig.
>>>>>>>>>>         1.
>>>>>>>>>>         The
>>>>>>>>>>         simplest
>>>>>>>>>>         models
>>>>>>>>>>         are
>>>>>>>>>>         quasi-stationary
>>>>>>>>>>         configurations
>>>>>>>>>>         with
>>>>>>>>>>         one
>>>>>>>>>>         current
>>>>>>>>>>         sheet
>>>>>>>>>>         at
>>>>>>>>>>         a well
>>>>>>>>>>         defined
>>>>>>>>>>         location
>>>>>>>>>>         determined
>>>>>>>>>>         by
>>>>>>>>>>         the
>>>>>>>>>>         overall
>>>>>>>>>>         geometry,
>>>>>>>>>>         which
>>>>>>>>>>         have
>>>>>>>>>>         been
>>>>>>>>>>         investigated
>>>>>>>>>>         in
>>>>>>>>>>         the
>>>>>>>>>>         conventional
>>>>>>>>>>         theory
>>>>>>>>>>         of
>>>>>>>>>>         magnetic
>>>>>>>>>>         reconnection.
>>>>>>>>>>         The
>>>>>>>>>>         basic
>>>>>>>>>>         assumption
>>>>>>>>>>         in
>>>>>>>>>>         these
>>>>>>>>>>         theoretical
>>>>>>>>>>         approaches is
>>>>>>>>>>         the
>>>>>>>>>>         existence
>>>>>>>>>>         of
>>>>>>>>>>         a two-dimensional
>>>>>>>>>>         subsystem
>>>>>>>>>>         around
>>>>>>>>>>         an
>>>>>>>>>>         X-type
>>>>>>>>>>         magnetic
>>>>>>>>>>         neutral
>>>>>>>>>>         point
>>>>>>>>>>         which
>>>>>>>>>>         is
>>>>>>>>>>         small
>>>>>>>>>>         compared
>>>>>>>>>>         with
>>>>>>>>>>         the
>>>>>>>>>>         global
>>>>>>>>>>         magnetic
>>>>>>>>>>         configuration
>>>>>>>>>>         but
>>>>>>>>>>         large
>>>>>>>>>>         compared
>>>>>>>>>>         with
>>>>>>>>>>         the
>>>>>>>>>>         so-called
>>>>>>>>>>         diffusion
>>>>>>>>>>         region
>>>>>>>>>>         around
>>>>>>>>>>         the
>>>>>>>>>>         neutral
>>>>>>>>>>         point,
>>>>>>>>>>         where
>>>>>>>>>>         the
>>>>>>>>>>         diffusion
>>>>>>>>>>         term
>>>>>>>>>>         in
>>>>>>>>>>         (1)
>>>>>>>>>>         is
>>>>>>>>>>         important.
>>>>>>>>>>         In
>>>>>>>>>>         this
>>>>>>>>>>         subsystem
>>>>>>>>>>         conditions
>>>>>>>>>>         would
>>>>>>>>>>         rapidly
>>>>>>>>>>         adjust
>>>>>>>>>>         to
>>>>>>>>>>         changes
>>>>>>>>>>         in
>>>>>>>>>>         the
>>>>>>>>>>         global
>>>>>>>>>>         configuration,
>>>>>>>>>>         so
>>>>>>>>>>         that
>>>>>>>>>>         the
>>>>>>>>>>         evolution
>>>>>>>>>>         of
>>>>>>>>>>         the
>>>>>>>>>>         latter
>>>>>>>>>>         would
>>>>>>>>>>         correspond
>>>>>>>>>>         to
>>>>>>>>>>         a sequence
>>>>>>>>>>         of
>>>>>>>>>>         stationary
>>>>>>>>>>         states
>>>>>>>>>>         in
>>>>>>>>>>         the
>>>>>>>>>>         former
>>>>>>>>>>         which
>>>>>>>>>>         are
>>>>>>>>>>         steady-state
>>>>>>>>>>         solutions
>>>>>>>>>>         with
>>>>>>>>>>         the
>>>>>>>>>>         boundary
>>>>>>>>>>         conditions
>>>>>>>>>>         determined
>>>>>>>>>>         by
>>>>>>>>>>         the
>>>>>>>>>>         global
>>>>>>>>>>         system.
>>>>>>>>>>         This
>>>>>>>>>>         is
>>>>>>>>>>         the
>>>>>>>>>>         idea
>>>>>>>>>>         of
>>>>>>>>>>         stationary
>>>>>>>>>>         forced
>>>>>>>>>>         reconnection.
>>>>>>>>>>         The
>>>>>>>>>>         prototype
>>>>>>>>>>         of
>>>>>>>>>>         such
>>>>>>>>>>         configurations
>>>>>>>>>>         is Petschek's
>>>>>>>>>>         reconnection
>>>>>>>>>>         model
>>>>>>>>>>         1),
>>>>>>>>>>         which
>>>>>>>>>>         is given
>>>>>>>>>>         schematically
>>>>>>>>>>         in
>>>>>>>>>>         Fig.
>>>>>>>>>>         2.
>>>>>>>>>>         In
>>>>>>>>>>         fact,
>>>>>>>>>>         much
>>>>>>>>>>         of
>>>>>>>>>>         the
>>>>>>>>>>         theoretical
>>>>>>>>>>         work
>>>>>>>>>>         on
>>>>>>>>>>         magnetic
>>>>>>>>>>         reconnection
>>>>>>>>>>         2
>>>>>>>>>>         ),3)
>>>>>>>>>>         consists
>>>>>>>>>>         of
>>>>>>>>>>         modifications
>>>>>>>>>>         and
>>>>>>>>>>         refinements
>>>>>>>>>>         of
>>>>>>>>>>         this
>>>>>>>>>>         model.
>>>>>>>>>>         The
>>>>>>>>>>         theory
>>>>>>>>>>         is based
>>>>>>>>>>         on
>>>>>>>>>>         the
>>>>>>>>>>         effect
>>>>>>>>>>         that
>>>>>>>>>>         the
>>>>>>>>>>         motion
>>>>>>>>>>         of
>>>>>>>>>>         a plasma
>>>>>>>>>>         may
>>>>>>>>>>         be
>>>>>>>>>>         supersonic
>>>>>>>>>>         at
>>>>>>>>>>         arbitrarily
>>>>>>>>>>         low
>>>>>>>>>>         speed
>>>>>>>>>>         with
>>>>>>>>>>         respect
>>>>>>>>>>         to
>>>>>>>>>>         the
>>>>>>>>>>         slow
>>>>>>>>>>         mode
>>>>>>>>>>         . Hence,
>>>>>>>>>>         by
>>>>>>>>>>         analogy
>>>>>>>>>>         with
>>>>>>>>>>         a system
>>>>>>>>>>         of
>>>>>>>>>>         two
>>>>>>>>>>         supersonic
>>>>>>>>>>         gas
>>>>>>>>>>         jets
>>>>>>>
>>

References

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To [email protected], Mbking42 <[email protected]>, Jon Gentry <[email protected]>, Bert Pool <[email protected]>, Bob Paddock <[email protected]>, joel mcclain <[email protected]>, Lane Wootan <[email protected]>, Toby Grotz <[email protected]>, Walt <[email protected]>, Phil Rembold <[email protected]>, Angel Alvarez <[email protected]>, Fredric Fletcher <[email protected]>, Jeane Manning <[email protected]>
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Message-ID <[email protected]>
Date Thu, 10 Jan 2019 18:21:34 -0600
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Subject Re: [EVGRAY] Re: Magnetic flux annihilation-reconnect phenomenon
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From Norman Wootan <[email protected]>