Gravity: Pulling or Pushing?

 Mankind alone amongst the beasts demonstrably examines and actively seeks to understand and quantify his existence. Until he examines the physical, spiritual and mental as an integrated whole, the Question will not be answered.  Until viewed wholistically, any answers can make no sense because the Questions themselves are not understood. -- Craig Berry

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-- What is gravity when push comes to shove? --
 

 Essentially it is accepted that the greater the mass of a body, the greater is the gravitational field of that body.   The problem is that of gravity itself.   What actually makes or causes gravity?   For the sake of this explanation, allow me to assign some simple arbitrary values to the forces involved for the sake of illustration.

 As a dynamic stream of Psi energy encounters a resistant object, it is resisted in its transit of that object.   This gives the said object a Psi resistance value; evidenced by its attendant gravitational field and resultant (quantifiable) mass.  For the sake of this exercise, I will label the resistance provided by a mass to be a [value].  To extrapolate this thought, if there is no Psi resistance, there is no measurable mass.  It is the resistance of an object to the transit of Psi energy which gives it mass. Something which is completely Psi transparent will have no mass.

 I will assign the essentially omni-directional dynamic free energy or dynamic flow of the Psi Field an arbitrary value of 1000.   Assuming that the Psi force is moving in all directions, it is reasonable to assume that, given a lack of an intervening Psi resistant mass, the Psi Field will retain its omni-directional integrity and energetic dynamic essentially without reduction.   

Gravity is typically thought of as an attractant force as a result of mass.   Its observable effect is apparently attraction and based on this observational interpretation gravity has remained a field of attraction to science. 

To argue the Psi Field theory, I will assign the earth and moon arbitrary “Psi mass values” of 3.0 and 1.0 respectively.

 In our first illustration (figure 1), we have a someone standing on the surface of the earth (which has a mass of 3).   From above, 1000 units are propelling (each particle with mass) the person into the planetary mass and attempting to make the person’s molecules conform to the planetary sphere, which is the most Psi neutral shape.   Opposing this 'planetary' thrust is the counterpoised Psi Field that has expended a minute amount of its energy traversing the planetary body, but is still able to counter the unimpeded 1000 propelling the person down with an effective counter-propulsion of 997.  Thus the person only experiences a true Psi disparity (gravity) of  3  acting on their body’s own Psi resistant mass; propelling them towards the planetary Psi centre (see figure 1).  

 

 Figure 1 

 For the sake of further examples, I will refer to the phenomena of disparity in counterpoised Psi ‘flows’ as a “Psi shadow” for reasons which will be obvious shortly.  It is important to realise at this point that it is each particle of the body which has mass that is being acted upon by Psi and not the surfaces of the body’s physical boundaries.  For those 'reading ahead', the Psi shadow is indeed gravity in all its glory.

To raise an obvious point from the above example, the shape of the sphere is the only shape that can survive for long under dynamic Psi pressure on a large and fluid scale.  The only logical planetary shape that can be formed in a Psi resistant mass is a sphere.  Any other shape contains a longer axis which in turn offers a greater  resistance.  This imbalance will work to shorten all axis of the object until the  resistance of all axis have achieved a state of equilibrium (see figure 2).  The final extrapolation of this diagram (figure 2) will result in the shape conforming to one where all mass is equidistant from the centre (i.e. a sphere) where no single axis offers greater resistance than any other. 

Figure 2

To give another example of Psi as the dynamic source of gravity, let us examine the tides of the oceans.   Before exploring the phenomena of oceanic tides, let me take you on a quick illustrative detour for a moment.   If you push on opposite sides of a water filled balloon, the water will rush to the area where resistance is least and will continue to do so until the point where a pressure-static equilibrium has been established, regardless of shape.   With this established, we will move on.

 Water on an uninfluenced planetary body, without the gravitational effects of another celestial body, will do its best to conform concentrically to the mass centre of the body (i.e. become part of the static mass of the sphere).   On earth we have two main influential celestial bodies creating  shadows dramatically effecting our planet; the Sun and Moon. To recap, we have assigned our planetary body a Psi mass of 3 and our moon a mass of 1.  The sun will be assigned a mass of 6. (Yes, the sun's relative mass is roughly 332, 830 times that of earth, but this is a "diagrammatic illustration" of its effect here on earth.)

When the moon is full (the lunar disk fully visible) the masses of the sun and moon are essentially in a  state of axial opposition.   Assume that of the moon exerts a Psi shadow of -1 and that the sun casts Psi shadow to the value of -6.   With a force of 1000 pushing upon the sides of the planetary mass, the mass of water is squeezed effectively towards the places where the Psi influence is lesser (figure 3).   In this case, into the shadows cast by the influencing celestial masses of the sun and moon in the Psi field as a repelling force rather than as an attracting force.

 Psi Field illustrrations - Figure 3

Figure 3

Before this example is discounted as too simplistic, let us examine the phases of the moon and the tides resulting.

  •  A new moon (the visible disk fully in shadow) produces the highest of all tides, with sun and moon conjunct, casting the strongest, multiplied Psi shadow.

  • A full moon (the visible disk fully illuminated) produces the next highest tides, with sun and moon axially opposed, casting axially opposing Psi shadows.

  • Waxing and waning quarters (with the visible disk partially illuminated to approx 50%) produce the least tidal fluctuations, with the sun and moon obliquely positioned, where their  effects are not multiplied by their alignments.

 Gravimeters work by quantifying relative strengths in the planet’s gravitational field.  Gravity is observed as being stronger over denser materials.  A model proposing an increase in the local Psi shadow due to a higher localised resistance, thereby resulting in a stronger apparent gravity fits the observed phenomena well.   

 In cases where gravitational fields are observed as dynamic and striated, an attractant model fails to account for the observed variations.  A Psi Field model allows and can even predict (via relative mass variations within the body) the ‘projected’ Psi shadows essentially emanating from the centre of mass.

 

Accretion of space bound bodies is another area where the attractant model of gravity fails when considering the formation of the distant outer planets.

 

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