This forecast derived from today 's NOAA/SWPC web pages and 15 other online sources (the URLs at the end of this forecast) is published five days a week (M-F) in The Daily DX .
All days and times in this forecast are in UTC (Zulu) time.
Global 6 meter F2 propagation may begin by late October if solar flux values continue to persist well above 200. 6 meter Trans-Equatorial F2 Propagation (TEP) is likely to occur regularly from September through November. 6 meter sporadic-E propagation beyond 2200 km is extremely unlikely until December.
The 2300Z Penticton 10.7 cm observed solar flux index was 240 and is likely to remain about the same through Saturday.
SILSO’s latest Estimated International Sunspot Number was 230 and is likely to remain about the same through Saturday.
The visible solar disk has one growing large active region, one stable large region, two growing medium active regions, one stable medium active region, two stable small active regions, one decaying small active region and two decaying very small active regions containing 90 sunspots with a total sunspot area of 2240 micro solar hemispheres (about 13 times the surface area of the Earth).
Solar wind speed is likely to be about 400 km/second or less through at least Saturday.
Mostly quiet geomagnetic conditions are likely through Saturday.
M-class solar flares are likely to cause a few minutes of minor to moderate radio blackouts of propagation paths crossing the sunlit side of the Earth through Saturday. There is a slight chance that X-class solar flares may cause about an hour of widespread blackouts of propagation paths crossing the sunlit side of the Earth through Saturday.
There is a slight chance that S1-class solar radiation storms may cause brief, minor degradation of propagation crossing the northern hemisphere polar region through Saturday.
160 and 80 meter propagation from North America to VK/ZL and the South Pacific is likely to be normal through Saturday . 160 and 80 meter long distance propagation in the northern hemisphere is always mildly to moderately degraded through September by E region blanketing of low angle F2 propagation until at least several hours after sunset.
40 meter short path propagation from North America to the Middle East and south Asia after 0030Z is likely to be normal through Saturday. Short path propagation between North America and east Asia after about 0930Z is likely to be normal through Saturday.
30 meter propagation crossing the auroral ovals and polar regions is likely to be normal through Saturday. Daytime 30 meter long distance propagation is always mildly to moderately degraded within several hours of local noon by E-region blanketing of low angle F2 propagation.
20 meter propagation crossing the auroral ovals and polar regions is likely to be normal through Saturday. 20 meter propagation beyond 2200 km in the northern hemisphere from June through September is always moderately degraded within several hours of local noon by E-region blanketing of low angle F2 propagation.
17 and 15 meter propagation crossing the auroral ovals and polar regions is likely to be normal through Saturday. 17 and 15 meter long path propagation from North America to southeast and east Asia from about 1100Z to 1400Z is likely to be normal through Saturday.
12 and 10 meter propagation is likely to be normal through Saturday. 12 and 10 meter long path propagation from North America to southeast and east Asia from about 1100Z to 1400Z is likely to be normal through Saturday.
Thermally driven high velocity seasonal thermospheric winds at F2 region altitude blow from the high temperature dayside hemisphere to the lower temperature nightside hemisphere reducing the volume of neutral atomic oxygen available to be ionized in the F2 region during daytime hours, lowering the MUF for F2 propagation crossing high latitudes to mostly less than 28 MHz through about mid-September.
Brief, isolated, geographically focused 6 meter trans-Atlantic sporadic-E propagation is extremely unlikely from about 1100-2200Z between mid-latitude U.S states and Europe, North Africa and the Middle East. Brief geographically focused 6 meter F2 propagation enhanced by TEP over Africa from the southern tier of US states to the Indian Ocean, equatorial and southern Africa (e.g., 3B8. 3B9, 7Q, D2, FR, V5, ZD7 and ZS) is extremely unlikely from about 1400-1800Z. F2 trans-equatorial propagation (TEP) from the southern tier of U.S. states to South America is extremely unlikely from about 2000-0200Z. Above-the-MUF oblique-TEP F2 propagation from the southern tier of US states to the south Pacific (e.g., 3D2, 5W, E5, FK, FO, VK4, VP6 and ZL) is extremely unlikely from about 1900-0300Z. It is extremely unlikely that more northerly U.S. stations may couple into TEP and oblique-TEP via geographically focused brief intervals of sporadic-E propagation. There is a chance of TEP propagation from about 2000-0200Z during the initial phase of strong to severe geomagnetic storms then degrading several hours after initial enhancement.
Sustained southward orientation (-Bz) of the north-south component of the interplanetary magnetic field (IMF) plays a crucial but unpredictable role in triggering all geomagnetic storms. Brief minor to moderate geomagnetic
storms may be gradually triggered when the IMF is sustained in a southward orientation (-Bz) with IMF field strength of about 5 nanoteslas or more for at least a few hours coincident with the influence of a geoeffective coronal hole high speed stream or CME. More frequent, longer duration, minor to severe geomagnetic storms may be triggered suddenly and unpredictably when the IMF is sustained in a southward orientation (-Bz) with IMF field strength of about 5 nanoteslas or more for a period of several hours or more coincident with the influence of a geoeffective CME and solar wind speed of about 500 km/second or more.
Mid-latitude northern hemisphere sunrise is 43 minutes later and sunset is 42 minutes earlier than it was on June 20th . Sunrise is about two hours earlier and sunset is about two hours later at the altitude of the refracting F2 region. Sunrise is about one hour earlier, and sunset is about one hour later at the altitude of the daytime absorbing D region.
All days and times in this forecast are in UTC (Zulu) time.
Global 6 meter F2 propagation may begin by late October if solar flux values continue to persist well above 200. 6 meter Trans-Equatorial F2 Propagation (TEP) is likely to occur regularly from September through November. 6 meter sporadic-E propagation beyond 2200 km is extremely unlikely until December.
The 2300Z Penticton 10.7 cm observed solar flux index was 240 and is likely to remain about the same through Saturday.
SILSO’s latest Estimated International Sunspot Number was 230 and is likely to remain about the same through Saturday.
The visible solar disk has one growing large active region, one stable large region, two growing medium active regions, one stable medium active region, two stable small active regions, one decaying small active region and two decaying very small active regions containing 90 sunspots with a total sunspot area of 2240 micro solar hemispheres (about 13 times the surface area of the Earth).
Solar wind speed is likely to be about 400 km/second or less through at least Saturday.
Mostly quiet geomagnetic conditions are likely through Saturday.
M-class solar flares are likely to cause a few minutes of minor to moderate radio blackouts of propagation paths crossing the sunlit side of the Earth through Saturday. There is a slight chance that X-class solar flares may cause about an hour of widespread blackouts of propagation paths crossing the sunlit side of the Earth through Saturday.
There is a slight chance that S1-class solar radiation storms may cause brief, minor degradation of propagation crossing the northern hemisphere polar region through Saturday.
160 and 80 meter propagation from North America to VK/ZL and the South Pacific is likely to be normal through Saturday . 160 and 80 meter long distance propagation in the northern hemisphere is always mildly to moderately degraded through September by E region blanketing of low angle F2 propagation until at least several hours after sunset.
40 meter short path propagation from North America to the Middle East and south Asia after 0030Z is likely to be normal through Saturday. Short path propagation between North America and east Asia after about 0930Z is likely to be normal through Saturday.
30 meter propagation crossing the auroral ovals and polar regions is likely to be normal through Saturday. Daytime 30 meter long distance propagation is always mildly to moderately degraded within several hours of local noon by E-region blanketing of low angle F2 propagation.
20 meter propagation crossing the auroral ovals and polar regions is likely to be normal through Saturday. 20 meter propagation beyond 2200 km in the northern hemisphere from June through September is always moderately degraded within several hours of local noon by E-region blanketing of low angle F2 propagation.
17 and 15 meter propagation crossing the auroral ovals and polar regions is likely to be normal through Saturday. 17 and 15 meter long path propagation from North America to southeast and east Asia from about 1100Z to 1400Z is likely to be normal through Saturday.
12 and 10 meter propagation is likely to be normal through Saturday. 12 and 10 meter long path propagation from North America to southeast and east Asia from about 1100Z to 1400Z is likely to be normal through Saturday.
Thermally driven high velocity seasonal thermospheric winds at F2 region altitude blow from the high temperature dayside hemisphere to the lower temperature nightside hemisphere reducing the volume of neutral atomic oxygen available to be ionized in the F2 region during daytime hours, lowering the MUF for F2 propagation crossing high latitudes to mostly less than 28 MHz through about mid-September.
Brief, isolated, geographically focused 6 meter trans-Atlantic sporadic-E propagation is extremely unlikely from about 1100-2200Z between mid-latitude U.S states and Europe, North Africa and the Middle East. Brief geographically focused 6 meter F2 propagation enhanced by TEP over Africa from the southern tier of US states to the Indian Ocean, equatorial and southern Africa (e.g., 3B8. 3B9, 7Q, D2, FR, V5, ZD7 and ZS) is extremely unlikely from about 1400-1800Z. F2 trans-equatorial propagation (TEP) from the southern tier of U.S. states to South America is extremely unlikely from about 2000-0200Z. Above-the-MUF oblique-TEP F2 propagation from the southern tier of US states to the south Pacific (e.g., 3D2, 5W, E5, FK, FO, VK4, VP6 and ZL) is extremely unlikely from about 1900-0300Z. It is extremely unlikely that more northerly U.S. stations may couple into TEP and oblique-TEP via geographically focused brief intervals of sporadic-E propagation. There is a chance of TEP propagation from about 2000-0200Z during the initial phase of strong to severe geomagnetic storms then degrading several hours after initial enhancement.
Sustained southward orientation (-Bz) of the north-south component of the interplanetary magnetic field (IMF) plays a crucial but unpredictable role in triggering all geomagnetic storms. Brief minor to moderate geomagnetic
storms may be gradually triggered when the IMF is sustained in a southward orientation (-Bz) with IMF field strength of about 5 nanoteslas or more for at least a few hours coincident with the influence of a geoeffective coronal hole high speed stream or CME. More frequent, longer duration, minor to severe geomagnetic storms may be triggered suddenly and unpredictably when the IMF is sustained in a southward orientation (-Bz) with IMF field strength of about 5 nanoteslas or more for a period of several hours or more coincident with the influence of a geoeffective CME and solar wind speed of about 500 km/second or more.
Mid-latitude northern hemisphere sunrise is 43 minutes later and sunset is 42 minutes earlier than it was on June 20th . Sunrise is about two hours earlier and sunset is about two hours later at the altitude of the refracting F2 region. Sunrise is about one hour earlier, and sunset is about one hour later at the altitude of the daytime absorbing D region.
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