PART 2- Section A: Density Change with celestial body movement

Introduction

In Part 1, with section 1 & 2 it has been established the shell nature of celestial bodies, where a celestial body can be a moon like small satellite or a big galaxy. Material in every celestial body spread across different layers and the density within the body decreases from center to outer layers. As every celestial body floats into one of its mother body layer (Eg. the solar system is the mother body to Earth), there is a boundary separating celestial body from its mother body. At this boundary the density of outermost layer is equal to density of the mother body layer. In section 3, it is shown how a body loses its outer layers when it travels towards high density layers of its mother body. Now here in this part 2, we will see how a celestial body layer can get outer layer bodies which are orbiting this celestial body towards its high density layers and how the material density in each layer can increase with the movement of the celestial body towards center of mother body.

Section 1: Increase in number of bodies in layers of the body moving towards high density layers 

The 2^nd scenario of celestial body behavior explained at the end of part 1 is critical to the new hypothesis on origin of Universe or existence of Universe. When celestial body, C travelling towards the center of mother body, M, c’, the moon of C can act in both ways, 1. ether to leave C and become a satellite to M or 2. give up the outer layer, which is holding it back from moving along with C. For this c’ needs to move closer to center of C. By doing so, c’ reduces its size and loses its mass too. And the stellar body C as a whole increases its density as it loses large volume space with a fraction of loss in mass in the form of outer layer.

Fig.2.1.1. The Moon C, along with its sub-moon c’ moving towards planet M behaves in either of the two ways depicted in scenario 1 &2. C loses c’ to M’s outer layer as c’ is unwilling to give up its outer layer materials are shown in scenario 1. It is shown with body scenario 2, that c’ is carried in by C even at the high density space of M, which happened as c’ maintains to arrive at high density  space of C by losing its outer low density layer materials.

The behavior of c’ is the key in deciding the fate of C as a whole. And this needs to be observed thoroughly.

If C doesn't travel towards higher densities of M, the question of c’ leaving or not, doesn't arise. But if C travels towards higher densities, c’ must behave in either of two ways as discussed above. If c’ does able to give up its outer layer then it can still act like the moon of C and can go along with C towards M. If c’ is not able to lose its outer layer it cannot follow C and needs to be get-away from C and become a moon to M inside M’s outer layer.

The phenomenon explained here can be applied to Earth system along with Moon. Moon is the natural satellite of Earth, which orbits around Earth in one of Earth’s material layers defined by certain density. If we assume this layer as outer most layer of Earth then, if Earth system moves towards Sun then either of two situations explained in fig 2.1.1 is a possibility. One situation can arise where Moon can leave Earth system and becomes a planet of Sun, where as in second situation by losing its outer layers Moon will come pretty much closer to Earth. Either one of these two situations is driven by Moon’s 'holding capability of its outer layers' or the Earth’s holding capability of Moon. If Earth’s holding capability is weaker than the Moon’s holding capability then Moon leaves Earth system and vice versa.

The phenomenon of Fig.2.1.1 is extension of Earth-Moon system, where Moon also has one sub moon with same atmospheric layers as Moon(C) and Earth (M). The scenario 2 of Fig.2.1.1 explains how the sub moon, c’ comes closer to C by losing its outer layers. If c’ is as big as C then we can call them as twin moon system like twin planets. This is not an uncommon phenomenon universe where scientists identified lot of twin stars. They can have common outer layer. In this case we call C and c’ as C₁ and C₂ respectively. As shown in Fig.2.1.2, when this twin moon system moves towards M by having scenario-2 situation, C₁ and C₂ come further closer to each other by losing their common outer layer and turning their inner layer a common layer to both C₁ and C₂.

Fig. 2.1.2: When twin moons C₁ and C₂ having a common outer layer moves towards high density layer of their mother body, they come closer and their immediate inner layer becomes their common layer as the outer layer lost

Further extension of this idea gives more insight into how the bodies inside a mother body get affected when the mother body goes in to high density layers or inner layers of its mother body. If we assume few sub moons(3^rd order bodies) orbit inside last two outermost layers of C₁ and C₂ (which are the 2^nd order bodies), such that c’₁ , and c’₂ in outer most common layer of C₁ and C₂ and in immediate inner layer d’₁ , and d’₂ orbit successively in each individual layer of the C₁ and C₂ . Fig.2.1.3. is referred for better clarity. When 1^st order body, i.e., the Earth system moves towards the inner layer of it mother body, if this system entirely follows the scenario 2, the c’₁ , and c’₂ of outer most common layer come into immediate high density layer of C₁ and C₂ where as this layer is now a common layer for  C₁ and C₂ . As the inner layer became the common layer for C₁ and C₂  , d’₁ , and d’₂ becomes common bodies to both C₁ and C₂ and upon the entry of  c’₁ , and c’₂ due to their inward movement all c’₁ ,  c’₂ , d’₁ , and d’₂ co-exist in the common layer. Now we may call combination of C₁ and C₂ as new body C₁₂. In this way the outer layer of these 2^nd order bodies becomes denser by not only due to loss of the outermost layer but also due to the entry of outer layer bodies with their increased outer layer densities. Here if we take the mass of bodies in calculating the density of a layer this layer density increases. But the mass of incoming bodies is nothing to do with true density of material layers. If we observe a unit space of that layer it remains unaffected by the incoming outer body. But if we see the number of bodies such as c’_1, c’₂ and d’₁ types their number has increased in the outer layer.

Fig.2.1.3: When the twin moons are having still smaller moons in their layers, during their inner layer is turning into the common layer for them, the outer layer moons (c’₁ and c’₂) too come in to the inner layer by losing their outer layers. At the same time the inner layer individual moons (d’₁ and d’₂) become common moons for both C₁ and C₂. So all four moons in two layers co-exist in single common inner layer, which is now outermost layer for C₁₂.

If the combination body C₁₂ further goes deep down into inner layer of its mother body M, these 2^nd order bodies all c’₁ ,  c’₂ , d’₁ and d’₂ may still go down in high density layer by losing their outer layers and may join the high density bodies e’₁ ,  e’₂ and e’₃. If mother body further goes down, the c’₁ and c’₂ bodies may not able to carried in further and the combination body C₁₂ may not able to carry them further. In that case, scenario 1 is prevalent and the body C₁₂ may lose c’₁ or c’₂ or both.

If we apply this phenomenon to bigger celestial bodies like galaxies and clusters of galaxies we could see this kind of phenomenon happening over there. While Galaxies move in to higher density areas of universe when scenario 2 is applicable the number of stars and planets will increase in outer arms of Galaxy.

The density change in the material layers in celestial bodies also can be established but for before that we need to get clarity on several things which we do in section 2.