Lundquist Magnetic Reynolds Number Calculator

Lundquist number S = μ₀·L·v_A/η plasma MHD calculator. Stig Lundquist 1949. ENEA DTT, ITER Frascati, INAF IAPS magnetic reconnection.

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Lundquist magnetic Reynolds number calculator plasma MHD

The Lundquist number S calculator determines the fundamental dimensionless parameter of magnetohydrodynamics (MHD) measuring the ratio of resistive timescale τ_η to Alfvén timescale τ_A in a magnetized plasma, per the formulation by Swedish physicist Stig Lundquist 1949 Physical Review 76, 1805 "Experimental Investigations of Magneto-Hydrodynamic Waves" Uppsala University. The Lundquist number S is a variant of the magnetic Reynolds number Rm built with Alfvén velocity v_A instead of flow velocity v. The classic formula: S = μ₀·L·v_A / η = τ_η / τ_A, with L = characteristic length scale (m), v_A = B / √(μ₀·ρ) Alfvén velocity (m/s), η = magnetic resistivity (Ω·m), μ₀ = 4π×10⁻⁷ T·m/A vacuum permeability. Equivalently: S = L·v_A / D_m with D_m = η/μ₀ magnetic diffusivity (m²/s). The general magnetic Reynolds number: Rm = μ₀·L·v / η with v flow velocity (Lundquist uses v=v_A specifically). MHD physics: for S >> 1 → ideal MHD (frozen-flux Alfvén theorem 1942, magnetic field lines frozen in plasma move with it); S << 1 → resistive diffusion dominates (field lines relax via ohmic dissipation);

S ~ 1 → magnetic reconnection (topology change). Typical S values:

  • Solar corona L=10⁸ m, v_A=10⁶ m/s, η=10⁻⁶ Ω·m → S ≈ 10¹³ (ideal MHD)
  • Tokamak ITER L=2 m, v_A=10⁷ m/s, η=10⁻¹⁰ Ω·m → S ≈ 10⁹
  • Solar wind L=10⁸ m, v_A=5×10⁴ m/s, η=10⁻⁹ Ω·m → S ≈ 10¹²
  • Lab plasma L=0.1 m, v_A=10⁵ m/s → S ≈ 10⁵
  • Galactic dynamo L=10²⁰ m → S ≈ 10²⁰. Magnetic reconnection: Sweet-Parker 1957-58 τ_rec = τ_A · √S (slow for large S, collisional scaling); Petschek 1964 τ_rec ~ τ_A · ln(S) (fast, X-point with shocks); Plasmoid instability Loureiro 2007 for S > 10⁴ turbulent reconnection regime. Physical applications:
  • MHD plasma simulations (GIZMO, FLASH, PLUTO INAF code)
  • Solar flares CME magnetic reconnection
  • Tokamak instability ELMs Edge Localized Modes
  • Magnetar magnetosphere SGR
  • Accretion disks AGN/X-ray binaries
  • Galactic dynamo amplification μG fields
  • Magnetic reconnection diagnostics solar flares. Italian applications:
  • ENEA Frascati DTT Divertor Tokamak Test 2028 (Italian Energy Agency Centro Ricerche Frascati Rome)
  • FTU Frascati Tokamak Upgrade 1989-2020 (8 T field deuterium, highest density tokamak ENEA)
  • ITER France 2025 Cadarache + Ansaldo Nucleare Genoa (Italy 25% ENEA + INFN + CNR)
  • INFN Frascati 1957 LNF National Labs Bruno Touschek ADA 1961 storage rings
  • INAF IAPS Rome 2010 Astrophysics Planetology Space plasma MHD physics
  • Solar Orbiter ESA 2020 ASI 25% corona-chromosphere reconnection Metis EUI
  • BepiColombo ESA-JAXA 2018 ASI 35% Mercury magnetosphere MHD plasma
  • AGILE satellite ASI 2007 AGN gamma-ray flares blazars. Italian space plasma research: INAF Trieste 1898 solar physics IBIS Interferometric BIdimensional Spectropolarimeter; Athena ESA 2035 X-IFU INAF Palermo 25% AGN cluster ICM reconnection; LiteBIRD ESA 2032 INAF + ASI CMB B-modes inflation; Cineca Marconi100 30 PFlops + Leonardo 250 PFlops 2023 N-body MHD plasma simulations 5th TOP500 worldwide; ICTP Trieste 1964 + SISSA 1978 MHD astrophysical plasma. Italian Physics Nobel: Carlo Rubbia 1984 CERN W and Z bosons UA1 + ENEA president 1999-2005 nuclear fusion. PNRR 2021-2026: Mission 2 green hydrogen nuclear fusion; Mission 4 Component 2 research €6.9B

Italian Lundquist number plasma table

Physical systemL (m)v_A (m/s)η (Ω·m)S LundquistItalian application
Solar corona10⁸10⁶10⁻⁶10¹³Solar Orbiter ESA ASI Metis
Solar wind 1 AU10⁸5×10⁴10⁻⁹10¹²BepiColombo ESA-JAXA ASI
Tokamak ITER210⁷10⁻¹⁰10⁹ITER France ENEA 25%
FTU Frascati Tokamak0.95×10⁶10⁻⁹10⁷ENEA Frascati 1989-2020
DTT Frascati 20281.28×10⁶10⁻¹⁰10⁸ENEA Centro Ricerche
Lab plasma0.110⁵10⁻⁵10⁵INFN Frascati LNF 1957
Mercury magnetosphere2×10⁶2×10⁵10⁻⁸10¹⁰BepiColombo MPO ASI 35%
AGN accretion disk10¹³10⁵10⁻⁸10¹⁵Athena ESA 2035 INAF
Magnetar SGR 1806-2010⁴10⁸10⁻¹²10¹³AGILE ASI 2007 INAF
Galactic dynamo10²⁰10⁴10⁻⁸10²⁰INAF Trieste 1898 IBIS

(Source: Lundquist 1949 Phys. Rev. 76, 1805 + Sweet 1958 Parker 1957 + Petschek 1964 + Loureiro 2007 plasmoid + ENEA Frascati 2025 + INAF IAPS Rome).

Italian Lundquist calculation examples

  • Solar corona X-class flare reconnection Solar Orbiter ESA 2020 ASI 25% Metis EUI: L = 10⁸ m (1 solar radius), v_A = 10⁶ m/s (B = 10 G ρ = 10⁻¹² kg/m³), η = 10⁻⁶ Ω·m (Spitzer T=10⁶ K). S = μ₀·L·v_A/η = (4π×10⁻⁷)·10⁸·10⁶/10⁻⁶ = 1.26×10¹³. τ_A = L/v_A = 100 s, τ_η = L²/(η/μ₀) = 1.3×10¹⁹ s (>> universe age). Sweet-Parker τ_rec = τ_A·√S ≈ 3.5×10⁷ s = 1 year (TOO SLOW for observed CME 1 hour). Petschek τ_rec = τ_A·ln(S) ≈ 3,000 s = 50 min (matches CME observed)
  • Tokamak ITER France 2025 Cadarache ENEA 25% + Ansaldo Nucleare Genoa: L = 2 m, v_A = 10⁷ m/s (B = 5.3 T D-T plasma), η = 10⁻¹⁰ Ω·m (T = 150 mln K). S = (4π×10⁻⁷)·2·10⁷/10⁻¹⁰ = 2.5×10⁹. Plasmoid instability for S > 10⁴ → turbulent reconnection ELMs Edge Localized Modes (controlled via RMP Resonant Magnetic Perturbations)
  • FTU Frascati Tokamak Upgrade 1989-2020 ENEA 8 Tesla: L = 0.9 m, v_A = 5×10⁶ m/s, η = 10⁻⁹. S = 5.7×10⁶
  • DTT Divertor Tokamak Test ENEA Frascati 2028: L = 1.2 m, v_A = 8×10⁶ m/s, η = 10⁻¹⁰. S = 1.2×10⁸
  • Mercury magnetosphere BepiColombo MPO ESA-JAXA 2018 ASI 35%: L = 2×10⁶ m, v_A = 2×10⁵ m/s, η = 10⁻⁸. S = 5×10¹⁰. Substorm reconnection magnetotail Mercury (1 g vs Earth 30%)
  • AGN accretion disk Athena ESA 2035 X-IFU INAF Palermo 25%: L = 10¹³ m, v_A = 10⁵ m/s, η = 10⁻⁸. S = 1.3×10¹⁵. MRI Magnetorotational Instability Balbus-Hawley 1991 angular momentum transport
  • Lab plasma INFN Frascati LNF 1957: L = 0.1 m, v_A = 10⁵ m/s, η = 10⁻⁵. S = 1.3×10⁵. Z-pinch magnetic confinement experiments

Italian plasma fusion MHD research

Italian MHD plasma research:

  • ENEA Centro Ricerche Frascati Rome 1960 Italian Agency Energy New Technologies Sustainable Economic Development: FTU Frascati Tokamak Upgrade 1989-2020 8 Tesla highest field record, deuterium plasma record density; DTT Divertor Tokamak Test 2028 first-of-its-kind divertor exhaust heat resolution (€500 mln PNRR + Eurofusion); RFX-mod2 Padua 2024 Reversed Field Pinch Consorzio RFX CNR-INFN-University 2 MA plasma current
  • INFN National Institute Nuclear Physics Frascati 1957 LNF Laboratori Nazionali Bruno Touschek ADA 1961 + ADONE 1969 e+e- storage rings (DAΦNE 2002); 23 national sections (Rome Sapienza/Tor Vergata, Milan Bicocca, Padua, Pisa, Bologna, Turin, Naples, Pavia, Genoa, Bari, Trieste, Catania, Lecce, Cagliari, Perugia); €50M annual budget
  • INAF National Institute Astrophysics Rome 2002 Monte Porzio Catone (16 observatories): IAPS Rome 2010 Astrophysics Planetology Space plasma MHD + space missions; Trieste 1898 solar physics IBIS Sunspot 2003 + Planck CMB 2009-2018; Capodimonte Naples 1812 VST KIDS dark matter; Catania-Etna 1880 solar; Padua 1761 Galileo Asiago 1979 Copernico 182 cm; Brera Milan 1762; Arcetri Florence 1872; Bologna Loiano 1936; Palermo 1790; Cagliari 1899 SRT 64 m radio
  • Italian solar telescopes: IBIS Interferometric BIdimensional Spectropolarimeter Sacramento Peak NM AURA INAF Arcetri-Catania magnetic photosphere-chromosphere spectroscopy; EST European Solar Telescope 4 m Canary Islands 2030 Italy 15% INAF + ENEA; SST Swedish Solar Telescope INAF collaboration
  • ASI Rome 1988 plasma missions: Solar Orbiter ESA 2020 ASI 25% 0.28 AU minimum solar distance, Italian instruments Metis coronagraph INAF Padua-Turin + EUI INAF + STIX X-ray; Parker Solar Probe NASA 2018 9.86 R_sun 2024; BepiColombo ESA-JAXA 2018 ASI 35% MPO Mercury orbiter 2026 magnetosphere MHD plasma SERENA INAF + ISA accelerometer; AGILE ASI 2007-2024 gamma-ray observatory INAF + INFN AGN flares blazar; Athena ESA 2035 X-IFU calorimeter INAF Palermo 25% AGN cluster ICM accretion disk magnetic reconnection; LiteBIRD JAXA-ESA 2032 CMB B-modes inflation INAF Trieste + ASI
  • ITER International Thermonuclear Experimental Reactor France Cadarache 2025 first plasma 2025 D-T fusion 500 MW (Italy 25% via EU EUROfusion + ENEA + INFN + CNR + Consorzio RFX Padua; Ansaldo Nucleare Genoa vacuum vessel + TF coils; Walter Tosto Chieti mechanical components; SIMIC Camerano; Criotec Turin; OCEM Energy Bologna)
  • Cineca Bologna 1969 Marconi100 30 PFlops + Leonardo HPC pre-exascale 250 PFlops 2023 5th TOP500 worldwide MHD plasma magnetar AGN GRMHD simulations
  • ICTP Trieste 1964 International Centre Theoretical Physics Abdus Salam Nobel 1979 + SISSA Trieste 1978 MHD astrophysics. Italian Physics Nobel: Carlo Rubbia 1984 CERN Pavia University W and Z bosons UA1 + ENEA president 1999-2005 nuclear fusion project. Italian R&D tax bonuses 2025-2026: R&D Tax Credit L. 160/2019 art. 1 c. 200 up to 25% research innovation plasma fusion expenses; Patent Box L. 178/2020 50% income from MHD software algorithm patents; Industry/Transition 5.0 Tax Credit DL 39/2024 art. 38 up to 35% energy efficiency fusion green hydrogen investments; PNRR Mission 2 Component 2 hydrogen nuclear fusion; Mission 4 Component 2 research €6.9B fundamental and applied

Updated July 2026

Frequently Asked Questions

What is Lundquist number S?

Lundquist number S is fundamental dimensionless MHD parameter measuring ratio resistive timescale τ_η to Alfvén timescale τ_A in magnetized plasma. Formulated Stig Lundquist 1949 Phys. Rev. 76, 1805 Uppsala. Variant magnetic Reynolds number built with Alfvén velocity v_A instead flow v. For S>>1 ideal MHD frozen-flux Alfvén theorem; S<<1 resistive diffusion dominates.

Lundquist number formula?

S = μ₀·L·v_A/η = τ_η/τ_A where L length scale m, v_A = B/√(μ₀·ρ) Alfvén velocity m/s, η magnetic resistivity Ω·m, μ₀ = 4π×10⁻⁷ T·m/A. Equivalent S = L·v_A/D_m with D_m = η/μ₀ magnetic diffusivity. General magnetic Reynolds Rm = μ₀·L·v/η with flow v. Lundquist uses v=v_A specifically for plasma physics.

Typical S Lundquist values?

Solar corona L=10⁸ m v_A=10⁶ m/s η=10⁻⁶ → S ≈ 10¹³; Tokamak ITER L=2 m v_A=10⁷ m/s η=10⁻¹⁰ → S ≈ 10⁹; Solar wind L=10⁸ m v_A=5×10⁴ → S ≈ 10¹²; Lab plasma L=0.1 m → S ≈ 10⁵; Galactic dynamo L=10²⁰ m → S ≈ 10²⁰. ITER ENEA Italy 25% Cadarache 2025 first plasma.

MHD magnetic reconnection?

Sweet-Parker 1957-58 τ_rec = τ_A·√S very slow large S collisional scaling. Petschek 1964 τ_rec ~ τ_A·ln(S) fast X-point with shocks. Plasmoid instability Loureiro 2007 for S>10⁴ turbulent reconnection regime. Solar flares CME ENEA Solar Orbiter ASI Metis EUI. Tokamak ELMs Edge Localized Modes ITER FTU DTT Frascati.

ENEA DTT Frascati 2028?

Divertor Tokamak Test ENEA Centro Ricerche Frascati Rome 2028 first-of-its-kind divertor exhaust heat resolution plasma fusion. €500 mln PNRR Eurofusion. L=1.2 m v_A=8×10⁶ m/s η=10⁻¹⁰ → S=1.2×10⁸. FTU Frascati 1989-2020 8 T magnetic field record. ITER France Cadarache 2025 Italy 25% Ansaldo Nucleare Genoa vacuum vessel TF coils.

Solar Orbiter ASI plasma?

Solar Orbiter ESA 2020 ASI 25% 0.28 AU minimum solar distance, Italian instruments Metis coronagraph INAF Padua-Turin + EUI extreme UV imager + STIX X-ray. Corona-chromosphere magnetic reconnection S=10¹³. BepiColombo ESA-JAXA 2018 ASI 35% MPO Mercury 2026 magnetosphere SERENA INAF. Athena ESA 2035 X-IFU INAF Palermo AGN.

Lundquist number applications?

Applications: 1) MHD plasma simulations GIZMO FLASH PLUTO INAF code Cineca Leonardo 250 PFlops; 2) Solar flares CME magnetic reconnection; 3) Tokamak ELMs ITER FTU DTT; 4) Magnetar SGR magnetosphere AGILE ASI; 5) Accretion disks AGN Athena ESA 2035 INAF Palermo 25%; 6) Galactic dynamo amplification μG; 7) Solar magnetic reconnection diagnostics.

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