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Bron: Leigh Westin, The Other Dimension,
NCGR Declination SIG Newsletter - Volume 6, No.3, Autumn
2001; published here with the permission of Leigh Westin.
Recently I was asked to explain the three parallel
aspects mentioned by Charles Jayne in the second chapter
of his treatise, Declination, the Hidden Aspect.
Charles Jayne was a brilliant and greatly respected
astrologer, but this was not an easy passage to understand.
For some the letter identification, B, A and E might
have been confusing because of the normal inclination
to associate value with alphabetical order.
However, Jayne chose the letters for an entirely different
reason.
- The 'B' parallel referred to a Bodily
parallel.
- The 'A' to a parallel by Antiscion
in celestial longitude
- The 'E', a parallel by Ecliptic, again
in celestial longitude.
To understand ecliptic intercept or 'EI' as
Jayne referred to it, one must acknowledge the relationship
between declination and celestial longitude and that
they can be equated.
It seems to be forgotten that the celestial coordinates
such as declination, right ascension, celestial longitude
and latitude, are measurements devised to describe the
view of the heavens that we have from Earth by man,
rather than being edits from God; and for that reason
to some the idea of equating declination and celestial
longitude is crossing a perceived-to-be forbidden boundary
between the equatorial and ecliptic systems.
But this is simply not thinking through the reason the
two systems exist.
One of the most important bodies we use all the time,
the Sun, has only these two coordinates, declination
and celestial longitude; and when considered together,
the Sun itself actually crosses that perceived-to-be-forbidden
boundary between celestial longitude and declination.
The path of the Sun which is basically the same year
after year can be traced on one since curve in the heavens,
any point of which will be both declination and celestial
longitude, thus how they can be equated. In fact this
is the source of the ancient technique of the antiscion
relationship.
At the same time there is really no path of the Sun
and to refer to this body in such manner can be quite
confusing because everyone knows, it is not the Sun
that is moving but rather Earth.
Thus we need to get beyond the illusion to what is really
happening - that celestial longitude represents where
Earth is in its orbit around the Sun and that declination
represents the point of Earth's surface that is simultaneously
being presented to the vertical rays of the Sun.
Now we are talking reality and at least to my way of
thinking, it's must easier to understand.
Year after year when Earth is at any particular position
around the Sun (in celestial longitude), the same declination
or degree of its decline will be aligned with the Sun.
These are fairly constant equivalents, changing only
about 4 degrees in declination over a 40,000-year cycle.
Ecliptic intercept refers to the association
of a particular position of celestial longitude always
being associated with a particular position of declination.
Those that everyone is familiar with are the Solstice
Points, 0° Cancer or Capricorn that corresponds to maximum
declination, which right now is about 23°26', also the
Equinoxes, 0° Aries and Libra, associated with 00°00
declination.
Every declination point between 0° and 23°26' is also
associated with celestial longitude positions. For example
17°31' in north declination corresponds to 19 Taurus
09 and 10 Leo 51.
Because these share the same declination, they are said
to be reflections of each other or in antiscion relationship.
In south declination at 17°31' the corresponding celestial
longitudes are 19 Scorpio 09 and 10 Aquarius 51. The
ecliptic intercepts then of 17°31' north declination
are 19 Taurus 09 and 10 Leo 51; in south declination
the ecliptic intercepts of 17°31' are 19 Scorpio 09
and 10 Aquarius 51.
Anyone can check this out in an ephemeris for any year.
For year after year the positions for the apparent Sun
in celestial longitude and declination will equate as
described above.
When the Sun is found at 17°31' declination, its celestial
longitude will be one of the four positions cited depending
on whether it is north or south declination, thus an
ecliptic intercept.
Now that we are armed with a little background, let's
get on to the three types of parallels as described
by Jayne.
- Parallel 1. The 'B' parallel.
- Statement from Jayne's book: "Any body
having the same or nearly the same, declination
as Mars would then be bodily parallel to Mars."
- Explanation: The 'B' parallel standing for
'body' meant simply two celestial bodies at the
same declination in one hemisphere, north or south,
thus a bodily parallel, and cited by Jayne as
the most powerful of the three types.
- Example: Mars at 17N31 declination and
any celestial body at or about 17N31.
- Parallel 2. The second parallel was referenced as
'A' representing 'antiscion.'
However, there is more.
- Statement from Jayne: In addition, a planet
bodily at A, whose ecliptic intercept is at H,
is in antiscion parallel (an A parallel) to P.
- Explanation: Jayne was stating a planet bodily
at any declination, and at, for example, 15Tau00
would be in antiscion parallel to any body at
15Leo00. This is simply the antiscion relationship
using celestial longitude rather than declination.
As for strength, he cites such as being more indirect
and less powerful than the 'B' or bodily parallel.
- Example: Mars at 17N31 declination, celestial
longitude 15 Leo 00; another celestial body
at 15 Tau 00, and any declination.
- Parallel 3. The 'E' or ecliptic parallel.
- Statement: In an E parallel, the second body
is bodily parallel to the ecliptic intercept of
P.
- Explanation: The 'E' or ecliptic parallel is
a celestial body at any celestial longitude but
with declination equivalent in celestial longitude
to another body's declination equivalent in celestial
longitude.
This he states to be the most indirect or least
powerful of all the three types.
- Example: Mars at 17N31 declination and any
celestial longitude; another celestial body
at any declination and 19 Tau 09 or 10 Leo
51 in celestial longitude, both of which are
the longitude or solar equivalents or the
ecliptic intercepts of 17N31 declination.
This has been an explanation, as I understand it, of
Jayne's description of three types of parallels. Jayne
wrote this while Kt Boehrer was in the midst of her
innovative research on out-of-bound bodies.
Until then no one knew how to approach the out-of-bounds
factors. Now that we have that research, there has been
a broadening of our understanding in many areas.
One of the most important factors concerning the above
information is the strength Jayne attributed
to each type of parallel, with the bodily parallel
being the most powerful and a conjunction in longitude
and parallel in declination simultaneously being even
stronger.
However, he ascribes the 'antiscion parallel' computed
in celestial longitude positions as being weaker and
the 'ecliptic parallel, the coordination of celestial
longitude translated into declination, being weaker
yet.
He further indicates that a contra-parallel works
through the same methodology.
Personally, I fully ascribe to the power of the 'B'
or bodily parallel.
On the other hand, the 'A' parallel or antiscion works
in declination with no doubt, but unless the bodies
are actually parallel, I do not ascribe to the antiscion
relationship in celestial longitude alone.
The rationale is simply that the antiscion relationship
originated from declination, the mirror points of the
same declination for two different positions in celestial
longitude, not the other way around. Sometimes the methodology
works, but in other instances, it seems to fall on a
dumb note. When it does work, I have found celestial
longitude is within 5 degrees of the longitude equivalent
of the body's existing declination. When it doesn't
seem to work, celestial longitude is more than five
degrees away from the longitude equivalent of the existing
declination.
There could be a relationship between Jayne's finding
that the antiscion parallel in celestial longitude is
of a weaker nature than a bodily parallel and that which
I've found. In a way we are both discussing a weaken
condition much like two bodies in celestial longitude
in wide orb of a conjunction. However, the deciding
factor of parallels is not celestial longitude, the
deciding factor is the body's declination. The same
scenario exists for the 'E' or ecliptic parallel and
which Jayne termed even weaker than the 'A' or antiscon
parallel.
There is a great difference in changing declination
into celestial longitude and the reverse, changing celestial
longitude into declination as must be done with the
'E' type parallel as described. The former no question
works, but the latter, like the antiscion relationship
when computed only in celestial longitude, sometimes
falls on a dumb note-again perhaps for the same rationale,
that its existing celestial longitude is more than a
5 degree orb from its solar equivalent in declination.
Even further though, celestial longitude could be
likening to the environment around Earth since this
in a way is Earth's walking path around the Sun. An
energy can be thrown in its path and certainly affect
it but it may be a side glancing hit as celestial longitude
and its partner measurement celestial latitude are keyed
only to Earth's path with imaginary poles. On the other
hand, it takes a transmission onto Earth's body for
energy to be fully incorporated. Of the two measurements
related directly to Earth (described in ephemeredes
as the Sun) celestial longitude or declination, only
through declination does this occur. Unlike a celestial
longitude measurement, declination is a measurement
directly associated with Earth's physical body by being
keyed to Earth's geocentric equator and positive and
negative magnetic poles.
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©Copyright, 2001 Leigh Westin
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