How variable are Birkeland currents?
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Abstract
Abstract I address the problem of estimating the time-rate-of-change of high-latitude Birkeland currents by using a string-of-pearls formation of satellites. Space series are calculated by linear interpolation of measurements made at the revisit times of the satellites. A lower bound on the total time derivative can be estimated as a function of distance along the orbit. Space series of the vertical component of electric current density, used as a proxy for field-aligned (Birkeland) current density at high latitude, are estimated from the along-track spatial derivative of Swarm magnetic field measurements residual to the CHAOS-7 internal field model. The results reveal non-negligible total time derivatives over periods shorter than 2 mins. Auroral Birkeland current densities derived from single-satellite traversals of magnetic field gradients can change dramatically in the time it takes a single satellite to cross a large-scale current system. In one example, during an overflight by the Swarm satellites of the THEMIS Fort Yukon all-sky imager on 1 December 2013, the vertical current density poleward of a visually quiescent auroral arc changes from
$$\sim 0.3\ \mu \,\hbox {A}/\hbox {m}^{2}$$
∼
0.3
μ
A
/
m
2
upward to
$$\sim 1.0\ \mu \,\hbox {A}/\hbox {m}^{2}$$
∼
1.0
μ
A
/
m
2
downward in 13.7 s (corresponding to an along-track separation of Swarm A and B of 104 km). The variability of Auroral Birkeland currents, between 25 November 2013 and 31 December 2013, as estimated by the median of
$$|dj_z/dt|$$
|
d
j
z
/
d
t
|
, reaches
$$15\ \hbox {nA}/\hbox {m}^{2}/\textrm{s}$$
15
nA
/
m
2
/
s
in the northern dayside auroral zone and exceeds
$$30\ \hbox {nA}/\hbox {m}^{2}/\textrm{s}$$
30
nA
/
m
2
/
s
in the pre-noon sector of the southern hemisphere.
Graphic Abstract