magnetic reconnection
Definition: A non-ideal plasma process that changes magnetic connectivity and converts stored field energy into heat, flows, and accelerated particles.
Why it matters here: Magnetic reconnection is the topological rearrangement of magnetic field lines at a thin current sheet where oppositely directed field components meet, allowing previously separate field lines to reconnect into a lower-energy configuration; the energy difference between the pre- and post-reconnection field configurations is released as particle acceleration, plasma heating, and radiation -- the physical origin of a flare’s energy.
Relationship: Use this term alongside free magnetic energy; the lecture's quantitative model is summarized below.
\[ E_{\rm free} \sim \frac{B^2}{2\mu_0}\,V, \qquad \text{GOES class} = \frac{\text{peak 1-8\,\AA\ flux (W/m}^2)}{10^{-4}\,\text{W/m}^2}\ (\text{X-class}) \]
Boundary or common confusion: Treating the order-of-magnitude free-energy estimate as a precise flare-energy prediction. This lecture’s E_free~(B^2/2mu0)V calculation depends sensitively on the assumed active-region volume and the fraction of the field that is genuinely non-potential (free) rather than potential -- both are order-of-magnitude, level 3 estimates here, explicitly disclosed, not precise measurements of AR12673’s actual pre-flare field.
free magnetic energy
Definition: Magnetic energy stored above the minimum-energy potential field compatible with the measured boundary conditions.
Why it matters here: A magnetic field configuration with the lowest possible energy for a given set of boundary conditions is called a potential field (current-free); any additional energy stored in currents/shear above this potential-field baseline is the free energy available to power eruptive phenomena.
Relationship: Use this term alongside potential field; the lecture's quantitative model is summarized below.
\[ E_{\rm free} \sim \frac{B^2}{2\mu_0}\,V, \qquad \text{GOES class} = \frac{\text{peak 1-8\,\AA\ flux (W/m}^2)}{10^{-4}\,\text{W/m}^2}\ (\text{X-class}) \]
Boundary or common confusion: Treating the order-of-magnitude free-energy estimate as a precise flare-energy prediction. This lecture’s E_free~(B^2/2mu0)V calculation depends sensitively on the assumed active-region volume and the fraction of the field that is genuinely non-potential (free) rather than potential -- both are order-of-magnitude, level 3 estimates here, explicitly disclosed, not precise measurements of AR12673’s actual pre-flare field.
potential field
Definition: A current-free magnetic field that minimizes magnetic energy for specified normal-field boundary conditions.
Why it matters here: A magnetic field configuration with the lowest possible energy for a given set of boundary conditions is called a potential field (current-free); any additional energy stored in currents/shear above this potential-field baseline is the free energy available to power eruptive phenomena.
Relationship: Use this term alongside non-potential (sheared) field; the lecture's quantitative model is summarized below.
\[ E_{\rm free} \sim \frac{B^2}{2\mu_0}\,V, \qquad \text{GOES class} = \frac{\text{peak 1-8\,\AA\ flux (W/m}^2)}{10^{-4}\,\text{W/m}^2}\ (\text{X-class}) \]
Boundary or common confusion: Treating the order-of-magnitude free-energy estimate as a precise flare-energy prediction. This lecture’s E_free~(B^2/2mu0)V calculation depends sensitively on the assumed active-region volume and the fraction of the field that is genuinely non-potential (free) rather than potential -- both are order-of-magnitude, level 3 estimates here, explicitly disclosed, not precise measurements of AR12673’s actual pre-flare field.
non-potential (sheared) field
Definition: A current-carrying magnetic configuration displaced from the potential state by shear or twist and therefore able to store free energy.
Why it matters here: Active regions with strongly sheared or twisted magnetic field (evidence of stored free energy, directly observable in vector magnetograms, Unit 5) are strongly statistically associated with subsequent large flares, supporting the free-energy-release picture.
Relationship: Use this term alongside GOES classification; the lecture's quantitative model is summarized below.
\[ E_{\rm free} \sim \frac{B^2}{2\mu_0}\,V, \qquad \text{GOES class} = \frac{\text{peak 1-8\,\AA\ flux (W/m}^2)}{10^{-4}\,\text{W/m}^2}\ (\text{X-class}) \]
Boundary or common confusion: Treating the order-of-magnitude free-energy estimate as a precise flare-energy prediction. This lecture’s E_free~(B^2/2mu0)V calculation depends sensitively on the assumed active-region volume and the fraction of the field that is genuinely non-potential (free) rather than potential -- both are order-of-magnitude, level 3 estimates here, explicitly disclosed, not precise measurements of AR12673’s actual pre-flare field.
GOES classification
Definition: The A-B-C-M-X flare scale defined by peak 1-8 angstrom soft X-ray irradiance at Earth, with each letter class spanning a decade.
Why it matters here: The GOES soft X-ray flare classification scheme spans nine orders of magnitude in peak 1-8 Angstrom X-ray flux, from the smallest recorded A-class flares (~10^-8 W/m^2) to the largest recorded X-class flares; the real X9.3 flare of 6 September 2017 (Lecture 06) had a peak flux of 9.3e-04 W/m^2 -- by definition, an "X9.3" flare has flux 9.3 x 10^-4 W/m^2, since GOES X-class flares are defined as flux/(10^-4 W/m^2).
Relationship: Use this term alongside soft X-ray flux; the lecture's quantitative model is summarized below.
\[ E_{\rm free} \sim \frac{B^2}{2\mu_0}\,V, \qquad \text{GOES class} = \frac{\text{peak 1-8\,\AA\ flux (W/m}^2)}{10^{-4}\,\text{W/m}^2}\ (\text{X-class}) \]
Boundary or common confusion: Treating the order-of-magnitude free-energy estimate as a precise flare-energy prediction. This lecture’s E_free~(B^2/2mu0)V calculation depends sensitively on the assumed active-region volume and the fraction of the field that is genuinely non-potential (free) rather than potential -- both are order-of-magnitude, level 3 estimates here, explicitly disclosed, not precise measurements of AR12673’s actual pre-flare field.
soft X-ray flux
Definition: Radiant power per unit area measured in a low-energy X-ray band; GOES uses the 1-8 angstrom band for operational flare classification.
Why it matters here: The GOES soft X-ray flare classification scheme spans nine orders of magnitude in peak 1-8 Angstrom X-ray flux, from the smallest recorded A-class flares (~10^-8 W/m^2) to the largest recorded X-class flares; the real X9.3 flare of 6 September 2017 (Lecture 06) had a peak flux of 9.3e-04 W/m^2 -- by definition, an "X9.3" flare has flux 9.3 x 10^-4 W/m^2, since GOES X-class flares are defined as flux/(10^-4 W/m^2).
Relationship: Use this term alongside magnetic reconnection; the lecture's quantitative model is summarized below.
\[ E_{\rm free} \sim \frac{B^2}{2\mu_0}\,V, \qquad \text{GOES class} = \frac{\text{peak 1-8\,\AA\ flux (W/m}^2)}{10^{-4}\,\text{W/m}^2}\ (\text{X-class}) \]
Boundary or common confusion: Treating the order-of-magnitude free-energy estimate as a precise flare-energy prediction. This lecture’s E_free~(B^2/2mu0)V calculation depends sensitively on the assumed active-region volume and the fraction of the field that is genuinely non-potential (free) rather than potential -- both are order-of-magnitude, level 3 estimates here, explicitly disclosed, not precise measurements of AR12673’s actual pre-flare field.