10/23/2019

EMSC GSNAT Report 10-24-2019

By: Gordon Rutherford
Global Events >2.5m











Lunar Resonant Geometries - 10/24/2019

By: Gordon Rutherford

Solar Rotating  Magnetic Field


Solar Rotating  Magnetic Field
MUST be Dead Rock Body Material, Not Active Dynamo
Solar Magnetic Field Polarity at Heliocentric Positions
- **Earth (Mantle/ Moon)
   Para-Magnetic = HIGH
- Mars Para-Magnetic = Neutral
- Mercury Dia-Magnetic = LOW
   (Resonating at HIGH)

** = Earth Core (Dynamo/Ferro-Magnetic)
Mantle = Cooled Para-Magnetic Rock
(Para-Magnetic)



GEOCENTRIC LUNAR MAGNETIC 
RESONANT GEOMETRIES

GEOCENTRIC LUNAR MAGNETIC RESONANT GEOMETRIES
NASA JPL Horizons Ephemeris Data, concentrating on Lunar Resonant Geometries
- Jupiter at Western Elongation
- Saturn at 120 degrees from the Moon
- Neptune at Lunar Opposition

NASA JPL Data
- Lunar Resonant Focus


COMBINATIONAL GEOMETRIES
Geocentric Positions relative to the Positions 
surrounding the Earth, in 360 degrees. 
- EARTH CROSSING URANUS CONNECTED PATH TO THE SUN
- Jupiter and Neptune at Western Elongation
*** URANUS AND SATURN AT NEAR 120 DEGREES APART ***

- MAGNETIC OPPOSITION during JUPITER AND NEPTUNE
- MAGNETIC OPPOSITION during URANUS AND SATURN
*** = added after reviewing reports

NASA JPL Data
- Geocentric Combinational Geometries


Solar Report - 10/24/2019

By: Gordon Rutherford




:Product: Forecast Discussion
:Issued: 2019 Oct 25 0030 UTC
# Prepared by the U.S. Dept. of Commerce, NOAA, Space Weather Prediction Center #


Solar Wind (24 hr Summary)
Solar wind parameters were at background levels until ~24/0600 UTC. Just after 24/0600 UTC, a CIR ahead of a positive polarity CH HSS, began interacting with Earths magnetosphere, causing enhancements in the solar wind environment. At ~24/1030 UTC, solar wind speeds increased to near 500 km/s, total field reached 14 nT, and the Bz component saw a maximum southward deflection to -12 nT. Phi remained mostly negative until just after 24/1100 UTC, when it rotated into a mostly positive
orientation. Wind speeds did eventually reach over 600 km/s late in the period as CH HSS effects increased.



Forecast...
Solar wind parameters are expected to remain enhanced on 25 Oct due to persistent CH HSS influences. CH HSS effects are projected to begin tapering off on 26-27 Oct as the CH HSS transits out of a geoeffective position.



Geospace (24 hr Summary)
The geomagnetic field was quiet to active due to CIR/CH HSS effects.



.Forecast...
The geomagnetic field is expected to be at mostly unsettled to active levels, with isolated G1 (minor) storm periods on 25 Oct. Conditions should begin to taper off on 26-27 Oct to active conditions or less, as the CH begins rotating away from a geoeffective position.

Solar Activity (24 hr Summary)
Solar activity was very low. No Earth-directed CMEs were observed in available satellite imagery.

.Forecast...
Solar activity is expected to persist at very low levels on 25-27 Oct.

Energetic Particle (24 hr Summary)
The greater than 2 MeV electron flux was at normal levels and the greater than 10 MeV proton flux was at background levels.

.Forecast...
The greater than 2 MeV electron flux is expected to increase from normal to high levels on 25 Oct as a positive polarity CH HSS moves into a geoeffective position. Electron flux levels are expected to remain at
high levels on 26-27 Oct. The greater than 10 MeV proton flux is expected to continue at background levels throughout the forecast period.




Lunar Report - 10/24/2019

By: Gordon Rutherford



NORTHERN HEMISPHERE AVERAGE
Moonrise  3:29 am
Median  10:03 am
Moonset   16:40 pm



TODAY - THURSDAY, OCTOBER 24, 2019
The Moon today is in a Waning Crescent phase. In this phase the Moon’s illumination is growing smaller each day until the New Moon. During this phase the Moon is getting closer to the Sun as viewed from Earth and the night side of the Moon is facing the Earth with only a small edge of the Moon being illuminated. This phase is best viewed an hour or 2 before the sunrise and can be quite beautiful if you're willing to get up early. It can also be a great time to see the features of the Moon's surface. Along the edge where the illuminated portion meets the dark side, the craters and mountains cast long shadows making them easier to observe with a telescope or binoculars.


Lunar orbit position on 24 October 2019 Thursday 12:00 UTC


Beaver Moon after 19 days
Next Full Moon is the Beaver Moon of November 2019 after 19 days on 12 November 2019 at 13:34.

Moon before perigee
13 days after point of apogee on 10 October 2019 at 18:29. The lunar orbit is getting closer, while the Moon is moving inward the Earth. It will keep this direction for the next day, until it get to the point of next perigee on 26 October 2019 at 10:41

Moon after northern standstill
4 days after previous North standstill on 20 October 2019 at 08:07, when Moon has reached northern declination of ∠22.947°. Next 8 days the lunar orbit moves southward to face South declination of ∠-23.047° in the next southern standstill on 2 November 2019 at 00:33



Neap tide
There is low ocean tide on this date. Sun and Moon gravitational forces are not aligned, but meet at big angle, so their combined tidal force is weak.



Distance to Moon 363 497 km
Moon is 363 497 km (225 867 mi) away from Earth on this date. Moon moves closer next day until perigee, when Earth-Moon distance will reach 361 316 km (224 511 mi).




New Moon in 3 days
After 3 days on 28 October 2019 at 03:38, the Moon will be in New Moon geocentric conjunction with the Sun and this alignment forms next Sun-Moon-Earth syzygy.



WORKS CITED
https://www.moongiant.com/phase/today/
https://lunaf.com/lunar-calendar/
https://www.calendar-365.com/moon/current-moon-phase.html
https://www.moontracks.com/declinations.html
https://www.timeanddate.com/moon/usa/miami