How the Intensity of Geomagnetic Storms can be

How the Intensity of Geomagnetic Storms can be Determined from Solar Data Vasyl Yurchyshyn, Big Bear Solar Observatory, 40386 North Shore Lane, Big Bear City, CA 92314, vayur@bbso. njit. edu Coronal Mass Ejections (CMEs) are correlated with geomagnetic storms, which are a response of the magnetosphere to an action of the southward interplanetary magnetic field (IMF). We discuss a new method to produce forecast of the intensity of a geomagnetic storm at least 1 day in advance based solar data. F 1 We used the functions F 1 and F 2 to analyze the March 13, 1989 geomagnetic storm (solid line in the figure on the right shows corresponding Dst index). This was a three step storm, therefore we assume that three CMEs may have caused it. First, we determined the source regions and the initial speed of the CMEs, then we calculated the Bz in the corresponding magnetic clouds and the range of the Dst index during the storms (blue boxes). ΔDst 1 ΔDst 2 Dst Index, n. T 1. We found that the CME projection speed is related to the Bz in IMF : Predicted Range of the Dst Fig. 1 The hourly averaged Bz measured at the front of an ejecta (ACE, GSM) vs the projected speed of CMEs. The solid line is an exponential fit: F 1=Bz[[n. T]=12. 3+0. 7 exp(V/404). The dashed lines show r. m. s=7 n. T. 2. In turn, the Bz in IMF defines the intensity (the Dst Index) of a storm F 2 The X 4. 5/3 B flare at 18: 46 UT on March 10, 1989 produced 1 st CME, which arrived on March 13 at 02: 00 UT. Its travel speed was about 760 km/s, while the initial speed was 1000 km/s. Bz predicted: -10 … -24 n. T Dst predicted: -100 … -180 n. T The X 1. 0/2 B flare on March 11 at 15: 33 UT produced 2 nd CME, which arrived on March 13 at 10: 00 UT. Its travel speed was about 990 km/s, while the initial speed was 1100 km/s. Bz predicted: -13 … -27 n. T Dst predicted: (-120 … -190)+ΔDst 1 = -210…-280 Fig. 2 The Dst index vs the hourly averaged Bz. The solid line is a 3 rd degree polinominal fit, F 2, and the dashed lines show r. m. s=33 n. T. The M 6. 7/1 n flare on March 12 at 08: 16 UT produced 3 rd CME, which arrived on March 14 at 19: 00 UT. Its travel speed was about 1200 km/s, while the initial speed was 1400 km/s. Bz predicted: -28 … -42 n. T Dst predicted: (-250 … -330)+ΔDst 2 = -400…-480 March 13 -15, 1989, Time, UT Storm Forecast Routine is Based on the F 1 and F 2 • Sign of the Bz in the IMF, sign • CME’s projected speed, V • The intensity of the Bz: Bz=F 1(V) x sign • The intensity of a geomagnetic storm Dst = F 2(Bz) • Publishing the results at: bbso. njit. edu/ ~vayur/halo_cme