JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 106,NO. A8, PAGES 15,797-15,801, AUGUST 1, 2001 A historyof early work on the heliosphericmagneticfield E. N. Parker EnricoFermiInstitute,andDepartments of PhysicsandAstronomy Universityof Chicago,Chicago,Illinois Abstract. The ideaof a magnetic fieldin spacearoundEarthbegan400 yearsagowithGilbert's recognition thatthemagneticfieldof Earthextendsoutwardintospaceto formwhatwe nowcall themagnetosphere. Theconcept of thesolarwindandtheheliosphere haditsfirstglimmerings withtherecognition, about270 yearsago,thatgeomagnetic activityis correlated with solar activity.It wassuggested abouta 100yearsagothattheconnection is throughsolarcorpuscular radiationwith velocitiesof the orderof 103km/s. The observedaccelerationof comettails indicated theuniversalnatureof solarcorpuscular radiation,givingriseto thefirstspeculation on theexistence of theheliosphere. Thehydrodynamic expansion of themilliondegreesolarcorona wasthenshownto providethesolarwind (solarcorpuscular radiation),stretchingoutthe magneticfields of the Sunto fill the heliosphere with a spiralmagneticfield. The adventof the spaceagesoonverified the solarwind andmagneticfield with directmeasurements. 1. Early Concepts period of about4 months,whereasthe magneticfluctuationAB occurs in an hour. Hence Kelvin concluded that a solar cause is The scientific pursuit of magnetic fields in interplanetary impossible. He ignoredthe suggestion that the geomagnetic space(the heliosphere)beganabout400 years ago with research variationsmight be the result of a beam of solarcorpuscular on the form of the geomagneticfield. The crucialstepwas made radiation. by Gilbert [1600] who first recognizedthat Earth possessesa The concept of isolated collimated (cold) beams of solar dipole magneticfield extendingfar out into spaceand declining in intensityas 1/r3with distancer from the centerof Earth. Geomagnetic fluctuations were discovered and associatedwith auroral activity throughthe coordinatedwork of Graham [ 1724] and Celsius[ 1741]. De Mairan [ 1754] suggestedthat Earth orbits through the extended corona of the Sun, and it is the entry of solarcoronalparticlesinto the geomagneticfield that causesthe fluctuationsand the aurora. This prescientconceptwas basedon the mistakenidea that the zodiacal light representsthe outward extension of the corona observedclose to the Sun during an eclipse of the Sun. The zodiacal light extendsfar beyond the orbit of Earth. As the reader will soon see, the association of the corpuscularemission of protons and electrons (103 krn/s) developedthroughthe last decadeof the nineteenthcenturyand the first half of the twentiethcentury[cf Chapmanand Ferraro, 1933, 1940] as the causeof geomagneticstormsand enhanced aurora. The ideasbeganto take form with the discoveryof the electronand the superficialresemblance of the auroralrays to cathoderay streamersin the laboratory Crooke's tube. The velocity(103km/s)of the corpuscular radiationwasestimated from the delay of a couple of days betweena flare event at the Sun and the associated geomagneticactivity. The ultimatestep in the concept of solar corpuscularradiation was Biermann's [1951, 1957] realization that the solar corpuscularradiation is responsiblefor the observedstrongantisolaraccelerationof the zodiacallight with interplanetaryfree electrons(a concepttotally unknown to de Mairan) persisteduntil about 1962 when direct gaseouscomet tails. Since all comet tails show this acceleration, measurementsin spaceshowedotherwise. Brief historiesof the Biermann pointed out that the Sun emits solar corpuscular developmentof geomagneticactivity [Chapman,1967] and space radiation in all directions at all times. That is to say, the science[Parker, 2000] are available in the literature. corpuscular radiation is notconfined tobeams created by special It must be appreciatedthat interplanetaryspacewas regarded events on the Sun, but rather is a universal and continuing as a hard vacuum by many physicists, the zodiacal light property of the Sun. Assumingthat the principal interactionof notwithstanding. Space was consideredto be so empty that the corpuscularradiation with the comet tail gas is through electrostatic potentialdifferences of 109voltsor morecouldbe charge exchange, Biermann estimated that the corpuscular postulated without fear of ridicule. To cite an extreme case, radiation has a density of the order of 500-1000 protons and Kelvin asserted that solar activity could not be the cause of electrons/cm 3at the orbit of Earth. This agreedwith the 500 geomagnetic fluctuations AB in spite of the overwhelming electrons/cm 3 estimated fromthebrightness of thezodiacallight evidenceof a connectionwith a 2-day delay. Kelvin considered on the assumptionthat the light is scatteredsunlight from free AB at Earth as the superpositionof a AB in a solar dipole magnetic field. Extrapolating backto theSunwith 1/r3implieda electrons. In fact, the zodiacal light is principally sunlight AB at theSunsome107timeslargerthanthemodestAB - 3x10'3 scatteredby dust grains. What is more, the solar corpuscular gaussobserved at Earth,thatis, 3x104gaussat theSun.Overthe radiationinteractswith the comet ions and electronsprincipally 1033 cm3volumeof theSun,thisrepresents a magnetic energyof through the magnetic field carried with corpuscularradiation. 4x104øergs,equivalent to the solaroutput(4x1033 ergs/s)overa However these quantitative points were not understooduntil later. The essentialstepwas the recognitionthat the corpuscular radiationfrom the Sun is an everydayphenomenonand doesnot Copyrl.gbt 2000 by the AmericanGeophysicalUnion. dependupon specialflare eventsat the Sun. Now there are two obviousplacesto look for the sourceof the Papernumber2000JA000100 interplanetarymagneticfield. One is the interstellaror galactic 0148-0227/00/2000JA000100509.00 15,797 15,798 PARKER: A HISTORY OF EARLY WORK ON THE HELlOSPHERIC MAGNETIC FIELD magneticfield, whichmay extendthroughthe solarsystem,and the other is the Sun itself. Hilther [1949] and Hall [1949] observedthe systematicplanepolarizationof starlightthat has beenreddenedby passagethroughinterstellardust,indicating thatnonspherical dustgrainsarepreferentially alignedby some large-scalefield. Spitzer and Tukey [1951] and Davis and Greenstein[ 1951]madethepointthattheonlyplausiblefieldis a galacticmagneticfield orientedmoreor lessalongthe galactic arm. They proposedferromagneticgrainsor paramagnetic grains, respectively. It was not possibleto deducethe field strength from the degree of polarization without precise knowledge of thecomposition andshapeof theindividual grains, but numbersof the orderof 10'5 gausswereoftenmentioned. Fermi [1949, 1954] appealedto the galacticmagneticfield to confinethe galacticcosmicrays, and, in fact, suggested that cosmicray particlesare acceleratedby bouncingoff Alfv6n wavesand other movingdisturbances in the galacticmagnet .Simpson[1951, 1954; Simpson,Fonger, and Treiman, 1953] developed the neutron monitor to measure the cosmic ray intensity at energies in the range 1 - 10 GeV, where the variationsAI are much larger. Simpsonestablishedfive cosmic ray neutronmonitorsfrom Huancayo,Peru, on the geomagnetic equator,wherethe geomagneticfield admitsparticlesonly above about10 GeV, to Chicago,wherethe geomagnetic cutoffis about 2 GeV. In this way he used the geomagneticdipole field as a magneticspectrometer.By intercalibratingand intercomparing AI at thesestations,he was ableto showthe energydependence of the Forbushdecreaseand of the 11-yearvariationof the mean cosmicray intensitywith the magneticsunspotcycle. He found that the energy dependencecould be explainedby neither an electrostaticpotentialin interplanetaryspacenor by an increase in the geomagneticcutoff energy. He noted,then, that the only remainingpossibilityis manipulationof interplanetarymagnetic field by solar corpuscularradiationin sucha way as to partially field. excludethe lower energyparticles. However, it soon became clear that the interstellarmagnetic A number of magnetic effects were proposed. Alfvdn [1956, field doesnot penetrateinto interplanetaryspace,becauseof the 1958] pointed out that the abrupt expansionof Hale's 40-gauss powerful outwardsweepof the solarcorpuscularradiation. With dipole field of the Sun would adiabaticallydecelerateand dilute thenumbersavailableat thetime(500 protons andelectrons/cm 3 the cosmicrays, producinga reductionin measuredintensitynot and 1000 kin/s) Davis [1955] estimated that the interstellar unlike the Forbush decrease. A particularly naYveidea was magneticfield (10'5 gauss)is pushedaway to a distanceof proposedby Parker [1956], who suggestedthat interplanetary several hundredAU. Hence, it would appearthat the Sun must plasmacloudscontainingmagneticfields might be capturedby be the sourceof any interplanetarymagneticfields. the gravitational field of Earth, thereby forming a temporary The magnetic fields of the Sun were first detected and magneticbarrier around the geomagneticdipole and inhibiting measured by Hale [1908] through their Zeeman effect in the arrival of the lower energy cosmicrays. Fortunately,it was sunspots,where the field strengthsare commonly 2000-3000 soon recognized that the feeble gravitational field of Earth is gauss. Hale [1913] also thoughtthat he detectedpolar fields of grosslyinadequatefor the taskandthe idea wasabandoned. the general order of 40 gauss, indicating that the Sun has a Morrison [1959] suggestedthat a plasma cloud containinga general dipole magnetic field. In fact, when Babcock and closed tangled internal magnetic field is emitted by the Sun. Babcock [1955] began systematic mapping of the solar Expanding out through interplanetary space, the cosmic rays photosphericmagnetic fields, the polar fields of the Sun proved within the cloud are adiabaticallydeceleratedand diluted, so that to be only 10 gauss or less, reversing every 11 years near the a Forbushdecreaseis observedas the cloudengulfsEarth. Gold peak of the sunspotcycle. Re-examinationof Hale's old plates [1959] suggestedthat a plasmacloud is emitted from a bipolar indicateda noiselevel of the orderof 40 gauss. active region on the Sun, stretchingthe bipolar field out through interplanetaryspaceto provide an expandingmagnetictongue, 2. Indirect Evidence whose interior would contain a decelerated and diminished cosmic ray intensity. The Forbush decreaseoccurswhen the Now 50 years ago the only direct probes of interplanetary tongueengulfsEarth. conditions were the solar corpuscularradiation impacting the The great cosmicray flare of February23, 1956 providedan geomagneticfield and the observedvariationsAI [Forbush,1937, unanticipated and effectiveopportunityfor probinginterplanetary 1954] of the galactic cosmic ray intensity. Unfortunately, the magnetic conditions. Meyer, et al. [1956] used the time corpuscular radiation gave no clue as to the interplanetary variationsrecordedby the five neutronmonitor stations,plus a magnetic field, whereas the cosmic ray variations were clearly sixth on shipboard(on the way to Antarctica) in the harbor at the result of someform of interplanetaryelectromagneticeffect Wellington,New Zealandto determinethe energyspectrum.The on an otherwise steady external field of galactic cosmic rays. promptarrival of solarcosmicraysat preciselydeterminedtimes Forbushmade his historic ground-basedmeasurements with ion at different terrestriallongitudesand latitudesshowedthat the chambers,which respondprimarily to the muonsproducedby first arrivals came straightfrom the Sun. The intensitypeaked, collisionsof the incoming protonsat the top of the atmosphere. and the directionality disappeared, after about 15 min, Thus the ion chamberstrack the intensityof incomingcosmicray subsequently decliningast'3/2for a few hoursbeforegoingover protonswith energiesof the orderof 10-15 GeV andhigher. Of into an exponential decline exp(-t/'c). It was clear that any particularinterestwas the occasionalabruptintensitydrop of a interplanetarymagneticfield betweenEarth and Sun was more or few percentover a periodof hours,graduallyrecoveringover the less radial. The simplestmodel for the declining phasewas a next several days, usually simultaneouslywith a geomagnetic uniform diffusive magnetic barrier beginning at about 1.5 AU storm, generally known as a Forbush decreasein honor of its andextendingout to perhaps5 AU. Collectively, the cosmicray variationssuggesteda variety of discoverer. The similarity and close tracking of the two phenomena suggestedto Forbush that the geomagnetic storm interplanetarymagneticfield scenariosat different times. The may somehow increase the geomagneticcutoff energy at each indirect inferences from cosmic rays, comet tails, and latitude, thereby reducing the intensity of the incoming cosmic geomagneticvariationswere insufficientto pin down the precise rays. But whatever the mechanismfor the manipulationof the form and behavior of the interplanetary magnetic field. cosmic rays, the Forbushdecreaseclearly indicatedthe heavy Presumably, the magnetic field is dominated by the solar handof solarcorpuscularradiation. corpuscularradiation,but the origin of the corpuscularradiation PARKER' A HISTORY OF EARLY WORK ON THE HELlOSPHERIC MAGNETIC FIELD 15,799 was unclear. There were vague thoughts about corpuscular idealized case of a precisely radial solar wind with uniform emissionfrom sunspots, M regions,flares,etc., all confounded by velocity v beyondsomeradiusr = a near the Sun. A smokepot Biermann's revelation that the Sun emits solar corpuscular placedat somepoint (00, tp0 ) on the spherer = a rotatingwith the radiation at all times and at all heliocentric latitudes. angularvelocity fl of the Sun at the polar angle 00 producesa line of smokein the wind with the spiralconicalform 0=00, r- a = (v/•)(qo- q00).The magneticline of forcethroughthe smokepot 3. Solar Wind The next advance was made by Chapman [1959], who calculatedthe extremely high thermal conductivity and small thermalemissionof the million degreecoronalgas. He showed, then, that the corona, strongly bound by gravity near the Sun, extendsfar beyond the orbit of Earth, with the temperatureT lies everywherein the line of smoke,so that the field line has the same Archimedian spiral form as the line of smoke. The magneticfield intensityis determinedby the field at r = a by decliningoutwardonly as 1/r2/7.The ghostof de Mairanmust havebeenpleasedwith the result. Parker [ 1958] noted two fundamentaldifficulties with the idea that Chapman'scoronacould remain static. The first difficulty arosefrom integrationof theequationfor staticequilibrium, dp/dr+ GMoM/r 2 = O, (1) wherep = 2NkT representsthe pressureof ionized hydrogenat a temperatureT and numberdensityN, M 0 is the massof the Sun, and M is the mass of a hydrogen atom. The result is nonvanishingpressurep at r =oofor the simple reasonthat far from the Sun the slow decline of the temperatureleads to the thermal energy per ion exceeding the gravitational binding energyof the Sun. The seconddifficulty was that a tenuousstatic coronawould not permit the passageof Biermann'suniversalsolarcorpuscular radiation. Even if there were no transversemagnetic fields in space,the two-streamplasmainstabilitywould quickly arrestthe flow of one plasma through the other. It was evident that, somehow,the stronglybound and seeminglystatic coronanear the Sun must becomethe corpuscularradiationat large distance. If the coronacannotbe static,suppose,then, that them is a steady radial velocity v(r), so that, insteadof the static equilibrium equation,we havethe momentumequation NMvdv/dr+ dp/dr+ GMoM/r2 = 0, Br(r,O,qo) = Br[a,O,qo - •(r-a)/v](a/r)2, (3) B0(r,0,q0)= 0, (4) B,(r,O,qo) = B•[r,0,q0- •(r-a)/v]a2• sinO/vr. (5) In the real heliospherethe solar wind velocity is not uniform around the Sun, nor is it always constantin time at any given heliographic longitude of the rotating Sun. So the magnetic structurein interplanetaryspaceis complicatedby divergingflow (at high latitude), convergingflow (at low latitude), fast spiral streams overtaking slow spiral streams, and blast waves (nowadays recognized as coronal mass ejections). These possibilitieswere sketchedat some length [cf. Parker, 1963, Chaps.9, 10, 11 andreferences therein;Sarahbai,1963]. One of the mostinterestingaspectshasturnedout to be the overtakingof slow regions of wind by fast regions, providing forward and backwardpropagatingshocksalongthe spiralzonesof collision. Burlaga [1997] has followed these effects over the years as spacecrafthave venturedfarther out throughthe solar system, finding that the phenomenonprovidesa sawtoothstructureof the solarwind and magneticfield at the orbit of Jupiterand beyond. The large fluctuationsin the otherwisespiralmagneticfield were investigatedby Belcher and Davis [1971] and the dynamicsof the deflection of the solar wind was treatedby Carovillano and Siscoe [ 1969]. 4. Space Observations (2) Observationalstudiesof the solar wind and its magnetic field got underwaywith Explorer 10, on an orbit that carriedit out to together withthecondition thatNvr2= constantfor conservation about15 Re (Re is the radiusof Earth)in the generaldirectionof solarwinddensityof 500 H ions/cm 3at of particles. With the million degreetemperatureextendingfar theSun. The presumed out into space,the only solutionstartingat small r with small v velocities of 500-1000 km/s suggested that the sunward and strong gravitational binding and extending smoothly and boundaryof the geomagneticfield was pushedin to about5 Re, continuouslyto p = 0 at r = oo is the supersonicexpansion so Explorer 10 would be well out in the wind for most of the solutionprovidingthe solarwind [cf. Parker, 1958, 1963, 1965, time. It was baffling, therefore,to find only an intermittentwind 1969; Hundhausen, 1972; Roberts and Soward, 1972]. of 4 - 8 H atoms/cm 3 and 200 - 400 km/s alternatingwith With the generalhydrodynamicexpansionof the solarcorona as the origin of the solarcorpuscularradiationit was immediately clearthat the interplanetarymagneticfield is madeup of the solar magneticfieldswhereverthey are not strongenoughat the Sunto preventthe free expansionof the corona[Parker, 1958]. That is relativelysteadymagneticfieldsof 10-4gauss[Heppneret al., 1963] and no wind for irregularperiodsof the orderof an hour. At first sight it suggesteda solar wind loosely filled with magneticfilamentsfrom the Sun. However,it was soonpointed to say,theactivecorona is forciblyconfined by thestrong (-102 4-8 H atoms/cm •, thenthe sunwardmagnetopause lies at 10-15 gauss)bipolarmagneticfields of the activeregions,whereasthe coronais able to pushits way out throughthe relatively weak (-10 gauss) fields of the broad active regions. So the interplanetarymagneticfield arisesprimarily from the forced extensionof the quiet regionfields. Coronalexpansionand the resulting solar wind create the heliosphereand fill it with magneticfield drawn out from the Sun and extendedto the outer boundaryat some 100- 200 AU. The basic character of the interplanetary or heliospheric magnetic field is easily illustrated [Parker, 1958] for the Re rather than 5 Re. Thus Explorer 10 was moving along the bouncing sunward magnetopause,which alternatelyretreated, exposingthe spacecraftto shockedsolar wind, and advanced, placingthe spacecraft within the shelterof the geomagnetic field. out [Bonetti et al., 1963)] that if the solar wind density is only Bonetti et al. [1963] sketched the configuration, with the upstream bow shock and the comet shaped magnetosphere extendingin the antisolardirection. The next spacecraftto explore the interplanetarymagnetic field was the Mariner 2 mission to Venus. It provided the first long-term quantitativerecord of the solar wind velocity and 15,800 PARKER: A HISTORY OF EARLY WORK ON THE-HELlOSPHERIC MAGNETIC FIELD Subsequentstudiesshowedthat the signof the interplanetary density[Snyderand Neugebauer,1964; Neugebauerand Snyder, 1966, 1967]. Unfortunately, the Mariner spacecraftwas not magnetic field correlates best with the fields of the Sun at magnetically clean, there being active electric currentloops as latitudes of about +30 ø and-30 ø, showing how the corona is well as magneticstructuralmaterial, so that the magnetometer confined by the strongmagnetic fields of the active regions at was able to recordrapidmagneticfluctuations AB -0.6x10 -4 low latitude so that the wind at Earth comesmainly from the free gaussin the interplanetarymagneticfield carriedpastthe space coronalexpansionat middlelatitudes[Wilcox, 1968; Wilcoxand craft in the 500 km/s wind [Davis et al., 1964], but there was no Howard, 1968; Wilcox and Colburn, 1969]. This brief history traces the investigationand thinking on conditionsin space,especiallythe magneticfieldsin space,from the early daysof indirectprobingand inferringto the later direct studiesthat becamepossiblewith the dawningof the spaceage. The hydrodynamicexpansionof the solarcoronaprovesto be the of the field. Thus it was that Ness et al. [1964] succeededin controlling factor, stretchingout the weak regions of solar making the first measurementsof the mean interplanetary magneticfield all the way out throughthe heliosphere,through magneticfield at the orbit of Earth.The measuredfield fluctuated the presumed termination shock, and into the subsonic rapidly, with AB- B. From their detailed measurements, downstreamwake in the local interstellarwind. The following however,theyfounda meanfieldB- 0.6x10-4gauss inclinedto paper by N. F. Ness picks up where the presenthistorical theradialdirection by theexpected spiralangle(•t = tan4(rf•/v)) narrative leaves off, carrying the space exploration of the of 300-45ø dependingupon the prevailingwind velocityat the interplanetary magneticfield into the fascinating detailsomitted time. Thus the interplanetarymagneticfield is nearly radial in the grosspictureoutlinehere. inside the orbit of Earth and more nearly azimuthalbeyondthe Acknowledgments.JanetG. Luhmannthanksboth of the orbit of Mars. One couldbegin to seethe basisfor the behavior refereesfor their assistance in evaluatingthispaper. of the solarcosmicraysof February23, 1956. The long-termmonitoringof the interplanetary magneticfield References got underwayat that time, subsequently accumulating the variety of effectsarisingfrom the irregularitiesof the solarwind. The Alfv6n, H., The Sun'sgeneralmagneticfield, Teiius,8, 1, 1956. Phenomena immediate interest,however, was in tracing the field back to its Alfv6n, H., Interplanetarymagneticfield, in Electromagnetic in CosmicalPhysics, IAU Symp.No. 6, editedby B. Lehnert,pp. 284origins at the Sun. For it must be appreciatedthat the way to determinethemeanfield. Thus it remainedfor the InterplanetaryMonitoringPlatform1 to be carefullydesigned,undercontinuedpressureandpersuasion from N. F. Ness, to allow the necessaryprecision magnetic measurementsof both the mean and the fluctuationcomponents observations of the solar wind at the orbit of Earth and the observations of the coronaand magneticfieldsat the Sun do not showpreciselywhat partsof the coronaare able to expandto providethe solarwind observedat theorbitof Earth. Note thenthat a simplel/r2 radialextrapolation of a radial magneticfield backto the surfaceof the Sunprovidesa factorof about5x104,sothatthemean0.6x10'4gaussat theorbitof Earth becomesabout 3 gaussat the Sun. In fact, the quiet region(and nowadaysthe coronalhole) fields are typically10 gauss,but over only a fractionof the solarsurface,sotheirfieldsspreadout over the entire4•; solid anglefilled by the solarwind at large distance from the Sun, providingan equivalentmeanfield at the Sun of only a few gauss. Thus the mean field at the orbit of Earth checksout aboutright, asnearlyasonecantell. A curiousfeatureof the interplanetaryfield was the tendency to pointawayfrom the Sunfor abouta weekandthentowardthe Sun for about a week, then away again, etc., so that the field in the plane of the ecliptic, and presumablyalso in the equatorial planeof the Sun,showedfour distinctsectorsrotatingwith the 27 day period of the Sun (as viewed from the orbitingEarth and spacecraft). In some years there were only two sectors,each rotating by in about 2 weeks. A detailed study by Ness and Wilcox [1964; Wilcox and Ness, 1965, 1968] and Schattenet al. [1969] showedthat the interplanetarymagneticfield is stretched out from the large unipolarmagneticregionson the Sun. 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