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Itinerary 2.3, page 2. - On the tides.
--- 2.3.7 ---
When cumulative-dissipative processes are evident.
These processes can be recorded when they become evident. This occurs under at least three conditions:
(1) when the water is still, but not stagnant, and the two processes alternate, in a more or less orderly fashion, almost to the point of unison (NB: keep in mind that the alternation of the two processes produces a continuous change in volume, and an apparently frenetic movement, but the water remains still);
(2) when the water moves relative to the Moon at one of the critical angular velocities for water;
(3) that the values of (2) are also long-lasting, that is, their variation /hr is zero, or very close to zero—as shown in the graph.
Example.
The phenomenon occurred on March 18, 2011, at 10:59 a.m., at point c of the calendar, at the critical angular velocity of 139.4 deltini/hr.
At that date and time, the phenomenon I call "water figures" (when the shapes tend toward squares) occurred. In other circumstances, "density waves" appear instead (when the shapes tend toward rectangles or stripes).
Under very specific conditions, when the water is completely still, the phenomenon can also occur in the open sea.
--- 2.3.8 ---
Only on some occasions.
On some occasions—when the angular velocity relative to the Moon reaches one of the critical angular velocities, and perhaps also for some other reason that needs to be studied—the phenomenon of water figures and density waves, which I have interpreted as follows, occurs.
It occurs when all the water molecules, stationary and in harmony with each other, in a significant volume of at least one cubic meter, alternate in unison, in close time, between the two phases—cumulative and dissipative.
As the videos show, the difference in volume occupied by water in the two phases—cumulative and dissipative—is considerable.
A gamble.
At this point, I'd be inclined to bet that the greatest volume is reached in the cumulative phase, without ruling out that the opposite could happen. So it's best not to bet.
When it happens.
The phenomenon would occur when the motion of a large number of water molecules relative to the Moon persists for a prolonged period at a critical angular velocity valid for water, thus making the variation in its density visible, even in a limited area.
To summarize, I recall two conditions for the phenomenon. It can occur: (1) when the movement of non-stagnant water is very small; and (2) when the motion of many water molecules relative to the Moon persists, for a prolonged period, at one of the critical angular velocities at which this phenomenon can occur.
Consequently, the phenomenon is best defined when the angular velocity relative to the Moon varies only slightly, and consequently the duration of a critical angular velocity value, when it occurs, lasts a long time.
This can happen near points a, b, c, and d of the calendar used for the seeds, but also far from these points, on rare occasions.
