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Home , Magnetic reconnection

CLASSICAL MODELS OF MAGNETIC RECONNECTION

YUNQI , 2019.4.26 TUTOR: XUENING BAI CONTENTS

• Introductions to magnetic reconnection

• Sweet-Parker Model: a classical perspective

• Petschek’s Model: a faster reconnection

• Summary INTRODUCTION: WHAT IS MAGNETIC RECONNECTION?

• Magnetic reconnection is a physical process occurring in highly conducting plasmas in which the magnetic topology is rearranged and magnetic energy is converted to kinetic energy, thermal energy, and particle acceleration.

• A magnetic reconnection process in solar flares: https:// en.wikipedia.org/wiki/ File:SDO_Observes_a_Reconnection_Event.ogv

• experiments INTRODUCTION: WHAT IS MAGNETIC RECONNECTION?

•

• accretion disks

• Plusars & Magnetars

reconnection region&

(ANATOLY SPITKOVSKY, 2006) INTRODUCTION: WHAT IS MAGNETIC RECONNECTION?

• Characteristics

• change the magnetic topology (further relaxation can release more energy)

• generate an electric field which accelerates particles parallel to

• dissipate magnetic energy (direct heating)

• accelerate , i.e. convert magnetic energy into kinetic energy INTRODUCTION: A SHORT HISTORY

• In 1946, Giovanelli suggested reconnection as a mechanism for particle acceleration in solar flares.

• 1957-58, Sweet and Parker developed the first quantitive model, currently known as Sweet-Parker model.

• 1961 Dungey investigated the interaction between a dipole () and the surrounding (interplanetary) magnetic field which included reconnection.

• 1964 Petschek proposed another model in order to overcome the slow reconnection rate of the Sweet-Parker model.

• … SWEET-PARKERS MODEL: A CLASSICAL PERSPECTIVE

incoming plasma • Magnetic reconnection with velocity vR happens when two plasma coming closer to each other, and the magnetic field lines are able to rearrange their outflow plasma structure, bringing the plasma inside the reconnection region reconnection region outside by the electric field. Alfven speed vA SWEET-PARKER MODEL: A CLASSICAL PERSPECTIVE

• Some typical values of the magnetohydrodynamic(MHD) regime

c2 • Magnetic diffusivity: η = 4πσ

B 6 • Alfven speed: vA = ∼ 10 cm/s μ0ρ LvA • S = Lunquidst number: η c / 4 π the ratio of the global Ohmic 2 diffusion time τ d i f f ≡ L / η to the global Alfven time τ A ≡ L / v A , typically S ∼ 1012 SWEET-PARKER MODEL: A CLASSICAL PERSPECTIVE

• How does reconnection happen?

• Ideal flux freezing: slow moving plasmas Ideal condition for flux freezing: PLASMA ηct INCOMING l = < δ vR 4π PLASMA OUTFLOWING • Reconnection vA happens if: l ∼ δ

reconnection region SWEET-PARKER MODEL: A CLASSICAL PERSPECTIVE

• How does reconnection happen?

• restrictions on current layer: 2L current density: j ≈ B/4πδ

v HOT v Ohmic heating rate (CGS): 2δ PLASMA 2 ηcB INCREASING ηcj2 = 2 2 PRESSURE (4π) δ current layer geometry Heating timescale: τA = L/vA • pressure relation:

2 2 p = ηcj τA < B0 /8π → δ > L/ S DEFINE: δ S P = L / S

Lv • Lundquist number: S = A ηc/4π SWEET-PARKER MODEL: A CLASSICAL PERSPECTIVE

• How does reconnection happen?

• reconnection speed: plasma flux conservation δ v v = SP v = A R L A S PLASMA INCOMING • with given Alfven vR speed PLASMA ηc OUTFLOWING v = R vA 4πδSP SWEET-PARKER MODEL: A CLASSICAL PERSPECTIVE

• How does reconnection happen?

• adiabatic heating and Ohmic heating

Recall that: δ > δ S P , Ohmic heating is 2.4 not sufficient for producing the 2.2 excess pressure because p ∼ 1/ δ2 , adiabatic heating is required. 2 1.8 SP / / In Sweet-Parkers Model, δ must / 1.6 decrease to provide such mechanic. 1.4 • time evolution for δ 1.2 2v t 2 2 2 2 A 1 δ − δSP = (δ0 − δSP)exp(− ) 0 1 2 3 4 5 v t/L L A SWEET-PARKER MODEL: A CLASSICAL PERSPECTIVE

• Time scale for reconnection

τSP ∼ L/vR = L S/vA 2L • consider an actual , L ∼ 104km v HOT v 2δ PLASMA 7 vA ∼ 2.7 × 10 cm/s Lv current layer geometry S = A ∼ 2.7 × 1012 ηc/4π

6 τSP ∼ 2 × 10 s ∼ month

• typical time: minutes to hours for a solar flare, making Sweet- Parker model a terribly long reconnection model. PETSCHEK’S MODEL: A FASTER RECONNECTION

• Reconnection occurs in a smaller scale, such as near a point. L* < L L v = v R L* SP Shock Wave • Plasma fluid doesn’t have to T reach the current sheet to flow out. It is considered to be dragged out the reconnection region by the tension generated by the curved magnetic field line. PETSCHEK’S MODEL: A FASTER RECONNECTION

• Petschek derived that the reconnection speed satisfies: δ where L* is a free parameter, vR = vA L* can this be true?

• Restrictions on L * : current densities in the shock are finite, π vA π v v = A R 3 vR(max) ≈ 8 ln[(vR/vA) S] 8 ln S

8τA • check it for the Sun! τ = ln S = 30 s < < τ , works perfectly P π SP for fast reconnection process. PETSCHEK’S MODEL: A FASTER RECONNECTION

• dynamics do not allow a shock structure

• Numerical simulations shows this model is unstable

• η needs to increase around the reconnection point, which is not expected as the background resistivity varying rapidly around certain point. SUMMARY

• Magnetic reconnection releases magnetic energy, accelerates plasma, and changes topology of the magnetic field.

• First quantitive model: Sweet-Parker Model, though its slow for reconnection.

• Fast reconnection model by Petschek, unstable in MHD simulations, require increasing magnetic diffusivity near reconnection point. REFERENCE

• Zweibel, E. G., & Yamada, M. (2009). Magnetic reconnection in astrophysical and laboratory plasmas. Annual review of astronomy and astrophysics, 47, 291-332.

• Parker, E. N. (1957). Sweet's mechanism for merging magnetic fields in conducting fluids. Journal of Geophysical Research, 62(4), 509-520.

• Sweet, P. A. (1958). 14. The neutral point theory of solar flares. In Symposium- International Astronomical Union (Vol. 6, pp. 123-134). Cambridge University Press.

• Kulsrud, R. M. (2005). Plasma for astrophysics. Princeton University Press.

• https://en.wikipedia.org/wiki/Magnetic_reconnection

• Gunnar Hornig, An introduction to magnetic reconnection, STFC Summer School Glasgow