Geomagnetic storms and active geomagnetic conditions are about half as likely through mid-July compared to their more frequent occurrence during the equinox seasons.
Although we are in the prime northern hemisphere 6 meter sporadic-E season through mid-July, solar maximum effects are causing less frequent and shorter duration long distance sporadic-E propagation beyond 2200 km than occurred during solar minimum and continued through 2022.
The 2300Z Penticton 10.7 cm observed solar flux index was 209 and is likely to remain about the same through Saturday.
SILSO’s latest Estimated International Sunspot Number was 272 and is likely to remain about the same through Saturday.
The visible solar disk has one large, three medium, nine small and four very small active regions containing 105 sunspots with a total sunspot area of 1190 micro solar hemispheres (about seven times the surface area of the Earth).
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 an X-class solar flare 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 of S1-class minor solar radiation storms through Saturday with minimal impact on propagation crossing polar regions.
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 from June through September in the northern hemisphere is always mildly to moderately degraded 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 mostly normal through Saturday. Short path propagation between North America and east Asia after about 0930Z is likely to be normal through Friday and mostly normal on Saturday.
30 meter propagation crossing the auroral ovals and polar regions is likely to be mostly normal through Saturday with possible mild degradation during local nighttime hours. 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 mostly normal through Saturday with possible mild degradation during local nighttime hours. 20 meter long distance propagation 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 mostly normal through Saturday with possible mild degradation during local nighttime hours. 17 and 15 meter long path propagation from North America to southeast and east Asia from about 1100Z to 1400Z is likely to be mostly normal through Saturday .
12 and 10 meter propagation is likely to be mostly normal through Saturday with possible mild degradation during local nighttime hours. 12 and 10 meter long path propagation from North America to southeast and east Asia from about 1100Z to 1400Z is likely to be mostly normal through Saturday .
Thermally driven high velocity thermospheric winds at the F2 region altitude blow from the high temperature dayside hemisphere to the low 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 the northern hemisphere to less than 24 MHz through mid-September and less than 28 MHz through late September.
There is a slight chance of brief, isolated, geographically focused 6 meter trans-Atlantic sporadic-E propagation from about 1100-2200Z between mid-latitude U.S states and Europe, North Africa and the Middle East. There is a very slight chance of 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) from about 1400-1800Z. There is a very slight chance of F2 trans-equatorial propagation (TEP) from the southern tier of U.S. states to South America from about 2000-0200Z. There is a very slight chance of 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, VK9, VP6, ZL and ZL7) from about 1900-0300Z. There is a very chance that more northerly U.S. stations may couple into TEP and oblique-TEP via geographically focused brief intervals of sporadic-E propagation. TEP may be significantly enhanced 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 14 minutes later and sunset seven minutes later 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 absorbing D region.
Although we are in the prime northern hemisphere 6 meter sporadic-E season through mid-July, solar maximum effects are causing less frequent and shorter duration long distance sporadic-E propagation beyond 2200 km than occurred during solar minimum and continued through 2022.
The 2300Z Penticton 10.7 cm observed solar flux index was 209 and is likely to remain about the same through Saturday.
SILSO’s latest Estimated International Sunspot Number was 272 and is likely to remain about the same through Saturday.
The visible solar disk has one large, three medium, nine small and four very small active regions containing 105 sunspots with a total sunspot area of 1190 micro solar hemispheres (about seven times the surface area of the Earth).
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 an X-class solar flare 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 of S1-class minor solar radiation storms through Saturday with minimal impact on propagation crossing polar regions.
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 from June through September in the northern hemisphere is always mildly to moderately degraded 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 mostly normal through Saturday. Short path propagation between North America and east Asia after about 0930Z is likely to be normal through Friday and mostly normal on Saturday.
30 meter propagation crossing the auroral ovals and polar regions is likely to be mostly normal through Saturday with possible mild degradation during local nighttime hours. 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 mostly normal through Saturday with possible mild degradation during local nighttime hours. 20 meter long distance propagation 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 mostly normal through Saturday with possible mild degradation during local nighttime hours. 17 and 15 meter long path propagation from North America to southeast and east Asia from about 1100Z to 1400Z is likely to be mostly normal through Saturday .
12 and 10 meter propagation is likely to be mostly normal through Saturday with possible mild degradation during local nighttime hours. 12 and 10 meter long path propagation from North America to southeast and east Asia from about 1100Z to 1400Z is likely to be mostly normal through Saturday .
Thermally driven high velocity thermospheric winds at the F2 region altitude blow from the high temperature dayside hemisphere to the low 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 the northern hemisphere to less than 24 MHz through mid-September and less than 28 MHz through late September.
There is a slight chance of brief, isolated, geographically focused 6 meter trans-Atlantic sporadic-E propagation from about 1100-2200Z between mid-latitude U.S states and Europe, North Africa and the Middle East. There is a very slight chance of 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) from about 1400-1800Z. There is a very slight chance of F2 trans-equatorial propagation (TEP) from the southern tier of U.S. states to South America from about 2000-0200Z. There is a very slight chance of 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, VK9, VP6, ZL and ZL7) from about 1900-0300Z. There is a very chance that more northerly U.S. stations may couple into TEP and oblique-TEP via geographically focused brief intervals of sporadic-E propagation. TEP may be significantly enhanced 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 14 minutes later and sunset seven minutes later 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 absorbing D region.
Comment