Showing posts with label Declination. Show all posts
Showing posts with label Declination. Show all posts

Monday, April 13, 2026

The S&P 500 versus the Speed of the True Lunar Node

Financial markets correlate closely with the 4–14 day cycle of the retrograde–stationary–direct motion of the True Lunar Node (North Node). This cycle can be depicted best by charting the Speed of the True Lunar Node against the S&P 500 (where "speed" refers to the geocentric motion in degrees of longitude per day).

S&P 500 (daily candles) vs True and Mean Lunar Node Speed, December 2025 to June 2026.
On March 30, 2026 — the date of the major stock market low shown in the chart above — the True Lunar Node was positioned at approximately 3°–4° Pisces (retrograde) in the Buttonwood Agreement NYSE natal chart (May 17, 1792, 8:52 AM LMT, New York). Using the Placidus house system, it fell in the 11th house, the sector governing groups, large-scale public participation, collective sentiment, international alliances, and speculative market trends driven by the masses.
Expect potential short-term changes in trend when the True Lunar Nodal Speed (blue solid line in the chart above)

► equals the Mean Lunar Nodal Speed (red horizontal dashed line), or
► is at 0 (grey horizontal dashed line), or 
► reaches maximum and minimum extremes.
 
The absolute maximum of the True Lunar Nodal Speed is approximately +0.0015 degrees of geocentric longitude per day (brief direct motion); the absolute minimum is -0.1074 degrees per day (peak retrograde motion). Standstills (stations) of the True Lunar Node occur when its geocentric speed in longitude momentarily reaches zero, as it oscillates around its mean retrograde motion due to solar and planetary perturbations. 
 
 
The True Node is predominantly retrograde (negative speed, averaging –0.053°/day) but regularly slows, stations (speed = 0°/day), and briefly moves direct (positive speed, up to +0.0015°/day) for hours to days before resuming retrograde motion. These stations are most pronounced and prolonged near eclipse seasons (roughly every 173 days), when solar perturbations on the lunar orbit are strongest.

The S&P 500 versus the Speed of the True Lunar Node (solid blue line)
and the Speed of the Mean Lunar Node (blue dashed line), 2014 to 2016.
In addition to the phenomenon of eclipses, there is a period of approximately ±2 weeks around the equinoxes, when Earth crosses the ecliptic from south to north (spring) and vice versa (fall). During these intervals, geomagnetic activity tends to be relatively strong, though highly variable and unpredictable, as solar emissions impact both hemispheres in an unbalanced manner.
 The S&P 500 versus the Speed of the True Lunar Node (solid blue line), November 2015 to April 2016.
 
The S&P 500 versus the Speed of the True Lunar Node and Eclipse Crash Windows, October 2014 to December 2015. 
The physical wobbling and oscillation of the Moon in its orbit around Earth and the Sun are driven by square aspects and conjunctions in both longitude and declination relative to the Sun and Earth. Around solar and lunar eclipses, the lunar nodes undergo rapid transitions between direct motion (speed above zero), retrograde motion (below zero), and near-standstill phases (at or very close to zero), as indicated by the blue-shaded time frames in the charts above. During these periods, financial markets commonly exhibit sentiment extremes and elevated volatility.
Approximately every 86.5 days, a so-called Moon Wobble occurs when the Sun is conjunct, opposite, or square (0°, 90°, 180°, 270°) to the True Lunar Node. The lunar node begins wobbling about two weeks before the exact event and remains unstable until roughly one week afterward. When coupled with solar or lunar eclipses, the wobble effect can be extended. As the Sun approaches conjunction or opposition to the lunar node, its motion is nearly blocked (as indicated by the bluish shaded areas). These periods are potential crash windows in financial markets. 
 
The S&P 500 versus the Sun conjunct, opposite, and square (0°, 90°, 180°, 270°) to the True Lunar Node, 2011 to 2015. 
 
The Moon's Nodal Wobble refers primarily to the retrograde precession of the lunar orbital nodes—the points where the Moon's orbit intersects the ecliptic plane. This line of nodes completes a full 360° cycle westward (retrograde) relative to the vernal equinox in approximately 18.613 years, at a mean rate of about 19.35° per year or 0.053° per day.
 
This "wobble" or instability in nodal speed reflects heightened perturbations when the Sun's gravitational influence on the Moon's orbital plane is strongest. The True Node may exhibit rapid fluctuations in direction and speed (retrograde-stationary-direct), magnifying energetic or disruptive effects in observational contexts. Mean nodes remain steadily retrograde but also decelerate noticeably.
 
The Draconic Month—also known as the nodical or draconic lunar month—has a mean length of 27.212220 days (27 days, 5 hours, 5 minutes, and 35.8 seconds) and is one of the five distinct lunar orbital periods used in astronomy and astrology.
This Precession causes the Moon's maximum declination to vary between roughly ±18.3° (minor lunar standstill) and ±28.6° (major lunar standstill) over the cycle, influencing eclipse patterns, tidal extremes, and the apparent "wobble" in the Moon's orbital orientation as viewed from Earth. A secondary, shorter-term perturbation arises from solar gravitational effects, causing the True (osculating) Node to oscillate around the mean node by up to about ±1.5° with a dominant period of roughly 173 days.
The Moon's Extreme Declinations represent the annual instants of greatest northern (positive) and southern (negative) geocentric declination, which delineate the progression of the 18.613-year lunar standstill cycle. These events reach their peak values (±28.43°) during the major lunar standstill in 2025 and their minimum values (±18.33°) during the minor lunar standstill in 2034.
The Moon's Extreme Declinations and Standstill Cycle, 2025 to 2035.
These values reflect the combined effects of the Moon’s orbital inclination (≈5.15°) and the 18.613-year nodal precession relative to the ecliptic. During major standstill years the extremes approach the sum of the obliquity of the ecliptic (≈23.44°) plus the orbital inclination; during minor standstill years they approach the difference. The listed times mark the precise moments of zero declination rate of change (local extrema).
Eclipses occur when the Sun aligns closely with the lunar nodes (conjunction or opposition) near a new or full Moon, aligning the Sun, Earth, and Moon in three dimensions. Around these times—typically twice yearly in eclipse seasons separated by about 173 days—the True Node's geocentric motion slows markedly, often becoming stationary or briefly direct (positive speed) before resuming retrograde motion.
 
As observed from Earth, the Sun crosses both lunar nodes as it travels along the ecliptic. The interval between successive returns of the Sun to the same node is known as the draconic (or eclipse) year, approximately 346.6201 days. Hence, there are about 12.74 draconic months in one eclipse year, and 13.42 draconic months in one tropical (or solar) year. 

Equinoxes mark when the Sun crosses the celestial equator, aligning its apparent position with the intersection of the ecliptic and equator. The lunar nodes' alignment with equinox points modulates the Moon's Extreme Declinations and Standstill Cycles. When a node coincides near an equinox, it accentuates the 18.613-year nodal cycle's effects on lunar rising/setting azimuths and tidal variations. The True Node's oscillatory behavior can interact with these seasonal alignments, though without the pronounced speed reversal seen at eclipses. 
 
See also:

Monday, December 1, 2025

2026 Turning Points in the Geocentric and Heliocentric Bradley Indices

The Bradley Index (also known as Bradley Siderograph, or Bradley Barometer) is a financial astrology indicator created by American astronomer Donald Bradley in the 1940s. The Heliocentric Bradley Index is an adaptation of the original geocentric concept, using heliocentric planetary positions instead (more on the calculation HERE).
 
Geocentric and Heliocentric Bradley Indexes for 2026.
 
Bradley Indices are often misinterpreted, with many linking the slopes directly to market trends. Tops and bottoms can signal potential turning points in price, whether a peak or a trough. The importance of these turn dates is not dependent on the magnitude of the change before or after the turn, meaning that even moderate shifts can be just as significant as larger ones. 
 
Q4 2025.
 
Q1 2026.
 
Q2 2026
 
Q3 2026.  
 
Q4 2026.  

Abbreviations:
geo = Geocentric Bradley Turning Point; helio = Heliocentric Bradley Turning Point; (L) = low; (H) = high. 
Dates are calculated for EST/EDT; expect turning points to be exact within ±1 day.
 
Geocentric and Heliocentric Turning Points:    
2025         Dec 05 (Fri) = helio (L)
    Dec 09 (Tue) = helio (H)
    Dec 22 (Mon) = geo (L)
    Dec 23 (Tue) = helio (H)
    Dec 24 (Wed) = geo (L)
    Dec 27 (Sat) = helio (H)
2026        Jan 02 (Fri) = geo (L)
    Jan 08 (Thu) = helio (H)
    Jan 16 (Fri) = geo (L)
    Jan 17 (Sat) = helio (H)
    Jan 19 (Mon) = geo (H)
    Jan 21 (Wed) = helio (H)
    Jan 25 (Sun) = geo (H)
    Jan 26 (Mon) = helio (H)
    Jan 31 (Sat) = geo (H)
    Feb 05 (Thu) = helio (H)
    Feb 08 (Sun) = geo (H)
    Feb 12 (Thu) = helio (H)
    Feb 16 (Mon) = geo (H)
    Feb 21 (Sat) = helio (H)
    Feb 26 (Thu) = geo (H)
    Mar 03 (Tue) = helio (H)
    Mar 07 (Sat) = geo (H)
    Mar 08 (Sun) = helio (H)
    Mar 16 (Mon) = geo (H)
    Mar 18 (Wed) = helio (H)
    Mar 25 (Wed) = geo (H)
    Mar 31 (Tue) = helio (H)
    Apr 03 (Fri) = geo (H)
    Apr 10 (Fri) = helio (H)
    Apr 14 (Tue) = geo (H)
    Apr 15 (Wed) = helio (H)
    Apr 18 (Sat) = geo (H)
    Apr 24 (Fri) = helio (H)
    May 04 (Mon) = geo (H)
    May 07 (Thu) = helio (H)
    May 08 (Fri) = geo (H)
    May 11 (Mon) = helio (H)
    May 16 (Sat) = geo (H)
    May 18 (Mon) = helio (H)
    May 21 (Thu) = geo (H)
    May 25 (Mon) = helio (H)
    May 28 (Thu) = geo (H)
    May 31 (Sun) = helio (H)
    Jun 06 (Sat) = geo (H)
    Jun 10 (Wed) = helio (H)
    Jun 11 (Thu) = geo (H)
    Jun 16 (Tue) = helio (H)
    Jun 19 (Fri) = geo (H)
    Jun 21 (Sun) = helio (H)
    Jun 22 (Mon) = geo (H)
    Jun 26 (Fri) = helio (H)
    Jul 04 (Sat) = geo (H)
    Jul 13 (Mon) = helio (H)
    Jul 14 (Tue) = geo (H)
    Jul 14 (Tue) = helio (H)
    Jul 16 (Thu) = geo (H)
    Jul 19 (Sun) = helio (H)
    Jul 21 (Tue) = geo (H)
    Jul 26 (Sun) = helio (H)
    Jul 27 (Mon) = geo (H)
    Jul 28 (Tue) = helio (H)
    Jul 31 (Fri) = geo (H)
    Aug 08 (Sat) = helio (H)
    Aug 12 (Wed) = geo (H)
    Aug 13 (Thu) = helio (H)
    Aug 17 (Mon) = geo (H)
    Aug 22 (Sat) = helio (H)
    Aug 27 (Thu) = geo (H)
    Aug 27 (Thu) = helio (H)
    Sep 03 (Thu) = geo (H)
    Sep 03 (Thu) = helio (H)
    Sep 07 (Mon) = geo (H)
    Sep 10 (Thu) = helio (H)
    Sep 13 (Sun) = geo (H)
    Sep 18 (Fri) = helio (H)
    Sep 22 (Tue) = geo (H)
    Sep 23 (Wed) = helio (H)
    Oct 02 (Fri) = geo (H)
    Oct 02 (Fri) = helio (H)
    Oct 09 (Fri) = geo (H)
    Oct 12 (Mon) = helio (H)
    Oct 16 (Fri) = geo (H)
    Oct 17 (Sat) = helio (H)
    Oct 17 (Sat) = geo (H)
    Oct 21 (Wed) = helio (H)
    Oct 25 (Sun) = geo (H)
    Oct 27 (Tue) = helio (H)
    Oct 29 (Thu) = geo (H)
    Oct 30 (Fri) = helio (H)
    Oct 31 (Sat) = geo (H)
    Nov 02 (Mon) = helio (H)
    Nov 05 (Thu) = geo (H)
    Nov 08 (Sun) = helio (H)
    Nov 13 (Fri) = geo (H)
    Nov 17 (Tue) = helio (H)
    Nov 18 (Wed) = geo (H)
    Nov 23 (Mon) = helio (H)
    Nov 26 (Thu) = geo (H)
    Nov 26 (Thu) = helio (H)
    Nov 27 (Fri) = geo (H)
    Nov 29 (Sun) = helio (H)
    Nov 30 (Mon) = geo (H)
    Dec 01 (Tue) = helio (H)
    Dec 04 (Fri) = geo (H)
    Dec 08 (Tue) = helio (H)
    Dec 11 (Fri) = geo (H)
    Dec 15 (Tue) = helio (H)
    Dec 19 (Sat) = geo (H)
    Dec 20 (Sun) = helio (H)
    Dec 29 (Tue) = geo (H)
2027         Jan 03 (Sun) = helio (H)
    Jan 09 (Sat) = geo (H)
    Jan 12 (Tue) = helio (H)
    Jan 15 (Fri) = geo (H)
    Jan 24 (Sun) = helio (H)
 
Geocentric Turning Points:
2025         Dec 22 (Mon) = geo (L)
2026        Jan 19 (Mon) = geo (H)
    Feb 08 (Sun) = geo (L)
    Mar 07 (Sat) = geo (H)
    Mar 16 (Mon) = geo (L)
    Mar 25 (Wed) = geo (H)
    Apr 03 (Fri) = geo (L)
    Apr 15 (Wed) = geo (H)
    Apr 24 (Fri) = geo (L)
    May 18 (Mon) = geo (H)
    May 28 (Thu) = geo (L)
    Jun 22 (Mon) = geo (H)
    Jul 14 (Tue) = geo (L)
    Jul 27 (Mon) = geo (H)
    Jul 28 (Tue) = geo (L)
    Aug 13 (Thu) = geo (H)
    Aug 27 (Thu) = geo (L)
    Sep 03 (Thu) = geo (H)
    Sep 07 (Mon) = geo (L)
    Sep 10 (Thu) = geo (H)
    Sep 18 (Fri) = geo (L)
    Sep 22 (Tue) = geo (H)
    Oct 02 (Fri) = geo (L)
    Oct 09 (Fri) = geo (H)
    Oct 17 (Sat) = geo (L)
    Oct 21 (Wed) = geo (H)
    Oct 29 (Thu) = geo (L)
    Nov 05 (Thu) = geo (H)
    Nov 17 (Tue) = geo (L)
    Nov 26 (Thu) = geo (H)
    Dec 04 (Fri) = geo (L)
    Dec 11 (Fri) = geo (H)
    Dec 15 (Tue) = geo (L)
    Dec 19 (Sat) = geo (H)
    Dec 29 (Tue) = geo (L)
2027        Jan 15 (Fri) = geo (H)  
 
Heliocentric Turning Points:
2025         Dec 05 (Fri) = helio (L)
    Dec 09 (Tue) = helio (H)
    Dec 23 (Tue) = helio (L)
    Dec 24 (Wed) = helio (H)
    Dec 27 (Sat) = helio (L)
2026         Jan 02 (Fri) = helio (H)
    Jan 08 (Thu) = helio (L)
    Jan 16 (Fri) = helio (H)
    Jan 17 (Sat) = helio (L)
    Jan 21 (Wed) = helio (H)
    Jan 25 (Sun) = helio (L)
    Jan 26 (Mon) = helio (H)
    Jan 31 (Sat) = helio (L)
    Feb 05 (Thu) = helio (H)
    Feb 12 (Thu) = helio (L)
    Feb 16 (Mon) = helio (H)
    Feb 21 (Sat) = helio (L)
    Feb 26 (Thu) = helio (H)
    Mar 03 (Tue) = helio (L)
    Mar 08 (Sun) = helio (H)
    Mar 18 (Wed) = helio (L)
    Mar 31 (Tue) = helio (H)
    Apr 10 (Fri) = helio (L)
    Apr 14 (Tue) = helio (H)
    Apr 18 (Sat) = helio (L)
    May 04 (Mon) = helio (H)
    May 07 (Thu) = helio (L)
    May 08 (Fri) = helio (H)
    May 11 (Mon) = helio (L)
    May 16 (Sat) = helio (H)
    May 21 (Thu) = helio (L)
    May 25 (Mon) = helio (H)
    May 31 (Sun) = helio (L)
    Jun 06 (Sat) = helio (H)
    Jun 10 (Wed) = helio (L)
    Jun 11 (Thu) = helio (H)
    Jun 16 (Tue) = helio (L)
    Jun 19 (Fri) = helio (H)
    Jun 21 (Sun) = helio (L)
    Jun 26 (Fri) = helio (H)
    Jul 04 (Sat) = helio (L)
    Jul 13 (Mon) = helio (H)
    Jul 14 (Tue) = helio (L)
    Jul 16 (Thu) = helio (H)
    Jul 19 (Sun) = helio (L)
    Jul 21 (Tue) = helio (H)
    Jul 26 (Sun) = helio (L)
    Jul 31 (Fri) = helio (H)
    Aug 08 (Sat) = helio (L)
    Aug 12 (Wed) = helio (H)
    Aug 17 (Mon) = helio (L)
    Aug 22 (Sat) = helio (H)
    Aug 27 (Thu) = helio (L)
    Sep 03 (Thu) = helio (H)
    Sep 13 (Sun) = helio (L)
    Sep 23 (Wed) = helio (H)
    Oct 02 (Fri) = helio (L)
    Oct 12 (Mon) = helio (H)
    Oct 16 (Fri) = helio (L)
    Oct 17 (Sat) = helio (H)
    Oct 25 (Sun) = helio (L)
    Oct 27 (Tue) = helio (H)
    Oct 30 (Fri) = helio (L)
    Oct 31 (Sat) = helio (H)
    Nov 02 (Mon) = helio (L)
    Nov 08 (Sun) = helio (H)
    Nov 13 (Fri) = helio (L)
    Nov 18 (Wed) = helio (H)
    Nov 23 (Mon) = helio (L)
    Nov 26 (Thu) = helio (H)
    Nov 27 (Fri) = helio (L)
    Nov 29 (Sun) = helio (H)
    Nov 30 (Mon) = helio (L)
    Dec 01 (Tue) = helio (H)
    Dec 08 (Tue) = helio (L)
    Dec 20 (Sun) = helio (H)
2027         Jan 03 (Sun) = helio (L)
    Jan 09 (Sat) = helio (H)
    Jan 12 (Tue) = helio (L)
    Jan 24 (Sun) = helio (H)


 
 
In bull markets, New Moons are often bottoms, and Full Moons are tops.
In bear markets, New Moons are often tops, and Full Moons are bottoms.
 
"The Bradley Indicator and Why I Don’t Use It."

Sunday, November 30, 2025

Cosmic Cluster Days | December 2025

Heliocentric Cosmic Cluster Days (CCDs) and financial markets do not display a consistent polarity or directional bias. The 'noise channel' serves as a signal filter, with the upper and lower limits of the channel being empirically defined. That said, swing directions, along with swing highs and lows also within the 'noise channel,' may correlate with or coincide with short-term market trends and reversals.
 
Cosmic Cluster Days  |   Composite Line  |  Noise Channel 
  = Full Moon | = New Moon |   = Lunar Declination max North and  = max South立春Solar Terms
 
Cosmic Cluster Days in December 2025: 
Nov 30 (Sun)Dec 01 (Mon) into Jan 1 (Thu) continuously above the Noise Channel (except of Dec 20). 
Major Peaks and Troughs: Dec 4 (Thu) | Dec 9 (Tue) | Dec 16 (Tue) | Dec 20 (Sat).
   
For previous CCDs, click [HERE]. For background on the author, the concept, and the calculation method, click [HERE].
 
Geocentric and Heliocentric Bradley Turning Points in 2025, click [
HERE]. 
Sensitive Degrees of the Sun, click [HERE].
Planet Speed (Retrogradity), click [HERE].   
Planetary Declinations, click [HERE].
Lunation Cycle, click [HERE].  

The
So
Lunar Rhythm
in December 2025.
 

Saturday, November 1, 2025

Cosmic Cluster Days | November 2025

Heliocentric Cosmic Cluster Days (CCDs) and financial markets do not display a consistent polarity or directional bias. The 'noise channel' serves as a signal filter, with the upper and lower limits of the channel being empirically defined. That said, swing directions, along with swing highs and lows also within the 'noise channel,' may correlate with or coincide with short-term market trends and reversals.
 
Cosmic Cluster Days  |   Composite Line  |  Noise Channel 
  = Full Moon | = New Moon |   = Lunar Declination max North and  = max South立春Solar Terms
 
Cosmic Cluster Days in November 2025: 
Oct 28 (Tue) | Nov 07 (Fri) into Nov 16 (Sun), and Nov 18 (Tue) into Jan 19, 2026 (Mon) continuously above
the Noise Channel. Major Peaks and Troughs: Nov 12 (Wed) | Nov 17 (Mon) | Nov 21 (Fri) | Nov 23 (Sun).
   
For previous CCDs, click [HERE]. For background on the author, the concept, and the calculation method, click [HERE].
 
Geocentric and Heliocentric Bradley Turning Points in 2025, click [HERE]. 
Sensitive Degrees of the Sun, click [HERE].
Planet Speed (Retrogradity), click [HERE].   
Planetary Declinations, click [HERE].
Lunation Cycle, click [HERE].  

The SoLunar Rhythm  in November 2025.
PrimeTimes charts the Sun's fixed cycles (Dawn, High-Noon, Dusk) against the Moon's shifting overhead/underfoot periods. It uses two strength factors—proximity (Perigee/Apogee) and angle (High/Low Cycle)—to rate daily potential (0-100). Analyzing every minute, the system identifies overlaps where potent lunar and solar times coincide, giving an accurate, composite forecast.

Wednesday, October 1, 2025

Cosmic Cluster Days | October 2025

Heliocentric Cosmic Cluster Days (CCDs) and financial markets do not display a consistent polarity or directional bias. The 'noise channel' serves as a signal filter, with the upper and lower limits of the channel being empirically defined. That said, swing directions, along with swing highs and lows also within the 'noise channel,' may correlate with or coincide with short-term market trends and reversals.
 
Cosmic Cluster Days
  |   Composite Line  |  Noise Channel 
  = Full Moon | = New Moon |   = Lunar Declination max North and  = max South立春Solar Terms
 
Cosmic Cluster Days in October 2025: 
Sep 24 (Wed) | Oct 02 (Thu) | Oct 20 (Mon) | Oct 21 (Tue) | Oct 26 (Sun) | Oct 28 (Tue) | Nov 07 (Fri)
   
For previous CCDs, click [HERE]. For background on the author, the concept, and the calculation method, click [HERE].
 
Geocentric and Heliocentric Bradley Turning Points in Q4, 2025.
 Oct 02 (Thu) = helio (L) | Oct 05 (Sun) = helio (H) | Oct 08 (Wed) = geo (L) | Oct 15 (Wed) = helio (L) | Oct 24 (Fri) = helio (H) | 
Oct 28 (Tue) = geo (H) | Oct 29 (Wed) = helio (L) | 2025 Oct 30 (Thu) = helio (H) | Nov 02 (Sun) = helio (L) 
 
Geocentric and Heliocentric Bradley Turning Points in 2025, click [HERE]. 
Sensitive Degrees of the Sun, click [HERE].
Planet Speed (Retrogradity), click [HERE].   
Planetary Declinations, click [HERE].
Lunation Cycle, click [HERE].