This page content is an attempt to tie together some of the ‘obvious’ connections, between image projection, image reproduction, chromatic aberration, colour manifestation, plane polarised light, converging/diverging lens & mirrors, and planes of
This page content is an attempt to tie together some of the ‘obvious’ connections, between image projection, image reproduction, chromatic aberration, colour manifestation, plane polarised light, converging/diverging lens & mirrors, and planes of symmetry. The operation of a telescope is a great tool to understanding the effect of electricity and polarisation on the inert gas condition. As the octave seed, the inert gas contains within itself the other elemental expressions. It is the application of graduated polarising condition which causes those elemental expressions to extend out from the 2D inert gas into the 3D perceived universe.
Fig : 1 represent the two main lens types. The convex lens will impart the following properties to the simulated universe,
- generation & compression of the light streams
- centripetal focus to a single focal point/axis
- heat & accumulate light density
- lens thickness implies greater expression of N/S pole axis
The concave lens will thus reverse all of the above properties.
- radiate & expand the light rays
- centrifugally unwind from a central point/axis out towards the expanse of space
- cool & redistribute light over a large area, increasing nebulosity
Both these lens types are created as a result of polarity and curvature. Consider the fig : 1a as follows,
When a disturbance is introduced to the calm condition of Stillness curvature is immediately imparted into the simulation.
Curvature = Polarisation = Motion
When light moves from left to right it will appears to expand and radiate, while light moving from right to left will appear through the same curvature to compress and generate.
The same curvature will thus produce two effects depending on direction. So, when applied to the cone of polarity generation is achieved in the direction of the apex, but, radiative expansion will be apparent towards the cone base.
An important consequence of fig : 1a is that there is always a two-directional effect present, one which is compressing and the other which is expanding. These opposed light stream will experience close ‘contact’ at the anode where the curvature/polarity is greatest, but, experience a more open relaxed ‘contact’ towards the cone base. This is why anodes (suns) are incandescent while cathodes (space) are cold.
There are a number of way to interpret the motion within this cone of polarity. For now, think of it as you might a boat crossing a pond. the boat is located at the dividing fulcrum. ahead of the boat a bow wave compresses to create the positive anode condition, while in the boats wake the waves are elongated to create the negative cathode condition. Later, we will look at this model in terms of its ‘thermodynamic’ significance.
It is a well known property of convex optics, that if an object is positioned at 2f (twice the focal length) from the lens then an inverted, identical image will be produced at 2f!! This will be a real image, being the product of converging lines. In other words, think of those converging lines as a compressive, generative effect giving rise to a real image albeit inverted. These effects are a result of light behaving as if passing through a biconvex lens system.
The implication of Fig : 2 is that north/south hemispheres are mirror images, with the dividing equator acting like a biconvex lens.
The result of the division process indicated in fig : 2a is exactly analogous to this convex lens inversion highlighted in fig : 2.
You might describe the inverted image at 2f as an inside-out copy of the original image, but, one could not say it was an unwinding, radiative, negative image!
WR would describe the characteristics of fig : 2 as a single negative cathode (biconvex lens) divided into two anodes, one the inversion of the other.
Opposite mate are NOT simply mirror images…
they are also INVERTED/inside-out images South is therefore an inside-out mirror image of North
If the red apex manifests in sector 1 of the cubic model, then the blue apex will manifest as the diagonal, inverted, same sized, real opposite in sector 8!!
The same effect can be achieved if light passed through a biconvex lens positioned at the center of the wave field.
In fact, fig : 3 explains in the simplest fashion how images of the original seed idea can manifest at opposite corners of the cubic wave field.
Fig : 3a may indicate this inverted image relationship evident with bi-convex lenses. This image also indicate how ‘un-empty’ space actually is. Depending on the detector used, more and more structure is revealed which otherwise would remain hidden from visual perception.
Every cubic wave field centered by a sun, will have, surrounding that sun, a zone of curved potential.
This curved potential distribution will behave like converging lenses looking inwards towards the hub, and conversely when looking in the opposite direction light will diverge away from the centering hub. Light coming from space tow