Enigma of the Birth and Evolution of Solar Systems May Be Solved by Invoking Planetary-Satellite Dynamics

From ancient times there has been a quest to understand the position of human kind in the cosmic order and to develop predictive system which could warn us of the impending natural calamity. In a continuing quest for an accurate predictive system, in Greek times Ptolemy kept our Planet at the center of the Universe and propagated the Geo-centric World View [Gale (2005-2006), Lawson (2004)]. In 16th century at the height of Renaissance, in a paradigm shift work but which was very much in keeping with common-sense , Nicolaus Copernicus, mathematician, astronomer and catholic monk, presented his book “De revolutionibus orbium coelestium (on the Revolution of the Heavenly Spheres)” first printed in 1542 in Nuremberg, Holy Roman Empire of the German Nation[Hawking (2005), Kuhn (1957), Windleband (1958), Crowe (1990)]. It offered a new framework for calculating the positions of the planets and this computational framework was tied to a Helio-centric World View [Hawking (2005)].


The discovery of first extra-solar system 1
In 1986, two proposals came from the University of Arizona and the University of Perkin-Elmer for space based direct imaging of Extra-Solar Systems using 16m-infrared telescope and optical telescope respectively. [Shiga 2004, Zimmerman 2004. Atmospheric turbulence smears the star's light into an arcsecond blob and reduces the resolution therefore ground based imaging of exo-planets was impossible.
Enigma of the Birth and Evolution of Solar Systems May Be Solved by Invoking Planetary-Satellite Dynamics 75 Adaptive Optics overcomes the atmospheric turbulence. Adaptive optics measures the scrambling due to air turbulence with a special sensor, then sends the information to a flexible mirror that deforms and undulates many times a second to tidy up the image. The rapid changes in the shape of the mirror exactly compensates the distorting effect of the churning atmosphere.
Recently extreme adaptive optics has been developed. It replaces hundreds of tiny pistons that reshape current flexible mirrors with thousands of smaller ones, and correct the incoming light not hundreds but thousands of times a second. This would spot a young glowing Jupiter in a much wider orbits. The road to another earth lies through another Jupiter, hence the presence of wide orbit Jupiter will mark the stars which should be closely examined first for earth like planets and then for life and intelligence.
In 1991 the first extra-solar system around a Pulsar was discovered by Alexander Wolszczan and Dale Frail. This pulsar is PSR1257+12, a rapidly rotating neutron star about 1.4M Θ and at a distance of 2000 to 3000 light years of our Earth. In this solar-system three planets were observed. The two planets have orbital period of a few months, small eccentricities and masses a few times as large as the mass of Earth. Third planet, innermost planet, has a period of one month and the mass is that of our Moon. In 1994, 60-inch telescope on Palomar Mountain, coupled with primitive adaptive-optics system, imaged a brown dwarf orbiting the star Gliese 229. The brown dwarf was orbiting the host star at a semi-major axis of 40AU(Astronomical Unit) where 1AU is 1.5×10 8 km. The same system was photographed by Hubble Space Telescope. The ground-based imaging of this binary-star was confirmed by space image. This established the technical feasibility of taking ground-based images of sub-stellar objects using telescopes fitted with adaptiveoptics.
In 1995 Mayor and Quiloz discovered the first exo-planet orbiting the star 51Pegasi. They used ELODIE spectrograph. In this the wobbling motion of the host star is used to detect the companion object. The wobbling motion of the host star gives rise to an effective radial velocity along the line-of-sight. Hence light coming from the host star experiences Doppler Effect. When the host star is approaching us , we record a blue shifted light and when host star is receding we record a blue shifted light. The recording of the alternate blue and red shift along the time axis gives the orbital period of the exo-planet and the magnitude of the shift gives us the mass of the host star. Since we may not be having an edge-on view of the orbital plane and the orientation radius vector of the orbital plane may be at an angle i, the angle of inclination of the orientation vector with respect to the line-of-sight, therefore the mass observed is MSini. We do not get the true mass of the exo-planet unless we have an edge-on view.
In 51Pegasi extra-solar system, we have the exo-planet orbiting the host star at a semi-major axis of 4.8 million miles. The orbital period is 4.2 days. This exo-planet is named 51 Pegasi.b. The mass observed, i.e. MSini , was more massive than that of Saturn.
One of the biggest drawback of Doppler Method of detection is that only Gas Giants of the size of Jupiter and Saturn can be detected.
ELODIE spectrograph has been further improved into CORALIE echlie spectrograph mounted on the 1.2m-Euler Swiss telescope at La Silla Observatory, ESO, Chile. This has been refined and exo-planets of Uranus mass have also been detected.
In 1999, a planet around HD209458 was detected by transit method. The actual mass and the size of the planet orbiting HD 209458 has been determined by combining the transit method and Doppler shift method. The density has been inferred and it is established that HD 209458b is a gas giant primarily constituted of Hydrogen just as Jupiter and Saturn are.
In 2001  Both these discoveries were too close to the host star for comfort. In the classical model there was no place for gas giants to be orbiting closer than 1 to 2 AU. These exo-planets were called hot-jupiters and they defied the conventional wisdom.  December 11-17, 2011 Pg.15.] Generally the exo-planets have eccentricities equal to zero. That is they are orbiting in perfect circular orbits like our nine planets. But there are other exo-planets which are in highly elliptical orbits like comets. Planets have been found orbiting binary stars, in circum-binary configuration, as well as in three star-systems. [Doyle et. al. (2011), Welsh et.al(2012]. Planets have been found orbiting pulsars.
The only exoplanet with an orbital period larger than that of Jupiter is the one orbiting 55Cancri. Its MSini = 4M J and its orbital period is 14 years. A two part space mission, TPF will detect from Earth-size planets and search for signs of habitability.

2025? Life Finder
The space-based Life Finder will search newfound Earths for signs of biological activity. Planets have been orbiting very close to their parent star so much so that they are slowly evaporating due to the heat and solar wind from their parent star. These are the hot Jupiters referred to above. As mentioned these defy the common wisdom of planet formation. By the year 2000, dozen exoplanets discovered and majority of them were hot Jupiters.
The catalog of exoplanets is growing and hot-jupiters seem to be an exception. The average planet size is falling and orbital distance is growing. That is exo-planets are being discovered farther and farther away from their parent star. Table 3. gives a chronological order of the milestones achieved in exo-planetary studies

Conditions conducive to exo-planet growth
In general it is found that single star system favour planet growth. Heavier stars favor giant planet growth while lighter stars favour terrestrial planet growth [Thommes et.al.(2008)] The extra-solar systems have a much larger probability in younger and more metal-rich regions of the spiral galaxies. The parent stars of exo-planets have higher metallicity [Santos 2005]. They have a higher abundance of elements heavier than hydrogen and helium.
The time factor is also very important. There is a very narrow time slot of few million years after the birth of the solar nebula in which the planets can be formed. The building blocks of planets are dust and gas. The dust particles of the accretion disc are continuously spiraling into the parent star by Poynting-Robertson drag and gas-dust smaller than 0.1 micron are being pushed out by solar radiation insolation by the process known as photo-evaporation [Ardila 2004].
In our Solar System there exists dusty debris disk in the asteroid belt. This causes the zodiacal light hence it is called zodiacal belt of dusty debris. This extends from 3AU to 10AU. There also exists Kuiper Belt of dusty debris from 30AU to 100AU. Similar dusty debris disk surround the stars with planetary system. These have been imaged by IRAS(infra red astronomical satellites) in 1983.It carried out complete survey of the sky in mid to far infra-red wavelength from 12 to 100 microns. The star itself is too hot, about 1000 Kelvin, to emit at far IR. But an accompanying debris disk will heat up and reradiate at far IR. This will give a bump in the stellar spectrum. The excess energy at infrared wavelength invariably indicate the presence of dusty debris disk. These debris disks are tenuous and faint but they have definite IR hazy glow. A gap in the debris disk is the signature of a protoplanet orbiting the parent star. The planet is in formative stage.
The dust in the debris disk either comes from the collisions of the initial leftover planetismals during planet formation or could be coming from collisions of comets and asteroids much after the formation has been completed. This debris disk generally range from 100AU to 1000AU and their composition is similar to that of our comets. The central part is a gap.
Ground based detectors cannot observe IR because of the absorption effect of the atmosphere. Milllimetric radiations reach the surface of the Earth. Therefore Submillimeter Common-User Bolometer Arrays (SCUBA) are used on the ground observatory for detecting the mm radiation coming from the debris disk of the stars. A combination of IR and mm wavelengths observations made by Hubble Space Telescope, SCUBA and IR detectors from the ground observatories have established that a dozen stars possess the dusty debris disk including Beta Pictoris. These debris disks are the analogue of Kuiper belt debris and hence are cooler than expected.
The debris disk depend on the age. Young stars in formative stage possess a much larger and heavier dusty debris disk as compared to our Solar System which is 4.56Gy.In our Solar System much of the debris has been used up in planet formation and the residual has spiraled in due to Poynting-Robertson(PR) drag or photoevaporated. The dust presently seen in asteroid belt and Kuiper belt is the result of collision and evaporation of comets and asteroids. They are continuously being removed by PR drag and by photoevporation and they are also being replenished by collisions and evaporation. Hence the young stars have a much larger debris disk.  The discovery of earth-like exo-planet would be the Holy Grail of astrobiology-a place where life started from scratch independently of life on Earth. The strategy is to first detect an earth-like exoplanet in the Goldilock zone of some star nearby say within 100 lightyears and then use terrestrial planet finder (TPF) to detect the biomarkers in the atmosphere of the given exoplanet.

Evolution of solar system building material
In NASA's DEEP IMPACT mission a 820 pound impactor collided with Comet Tempel 1. By the study of Comet material it was concluded that it was made of the pristine constituents of early solar system. This pristine material consisted of fragile organic material. This material includes polycyclic aromatic hydrocarbons(carbon based molecules found on charred barbeque grills and automobile exhaust on Earth).
On the other hand, the asteroids are the leftovers of planet formation and they therefore represent a more evolved form of matter. About 4000 Asteroids have been categorized. The Asteroid belt exists from 2.1AU to 3.3AU. Asteroids are coplanar with Ecliptic Plane. They move in the same direction as the Planets.
In terrestrial planets there is a metallic core and surrounding basaltic-granitic mantle.
But a Solar System which is in transition like HD113766 and which has a dusty disk has material in between the primitive kind contained in comets and more evolved kind found in asteroids.
Planet bearing Extra Solar Systems invariably have an environment rich in metal [Santos 2005]. The stars with twice the metallicity have 25% chance of harbouring a planet whereas stars with Sun's metallicity has only 5% chance.
There is a very narrow time slot of tens of millions of year in which Gas Giants birth and growth must take place. The dust part is continuously spiraling inward due to Poynting -Robertson photo assisted drag and gas-dust particle smaller than 0.1 micron are pushed out by the solar radiation insolation also known as photo evaporation.. Thus the gas-dust circumstellar disc is dissipated after tens of millions of years. If the opportunity is not seized for the birth and evolution of Gas Giants then no planetary formation would take place. The formation of Gas Giants is essential for Earth-like terrestrial planets.

The difficulties in discovering exo-planets
Doppler shift technique is the most convenient method of detecting Jupiter sized planets in tight orbits around their parent stars. The other methods are enumerated in Table 5.

Method Description
Terrestrial direct imaging Largest telescopes such as Keck, Gemini and Subaru are being used for direct imaging. Orbital architecture can be determined hence true mass is known. Easier to detect gas giants in wide orbits like ours. Young stars are ideal target as their companion planet would be glowing brightly in infra red wavelength because of the accretion generated heat.

Space direct imaging
William SPARKS(Space Telescope Science Institute) is using Hubble Space Telescope's Advanced Camera for Surveys for direct imaging. Orbital architecture can be determined hence true mass is known. Easier to detect gas giants in wide orbits like ours. Young stars are ideal target as their companion planet would be glowing brightly in infra red wavelength because of the accretion generated heat.
Radial Velocity technique or Radiovelocimetry or reflex motion of solar type stars A color change in the star light betrays the wobble caused by the companion planet. When star is approaching, light experiences a blue shift and when star is receding, light experiences red shift. This is also known as Doppler Shift technique.
There is uncertainty about the orbital angle of inclination hence real mass is indeterminent. Only the lower limit of the true mass is determined. Easier to detect gas giants in tight orbit.

Astrometric method
Recording the proper motion of the star on the celestial sphere i.e. the dome of the sky. Most sensitive for gas giants in nearby stars. Since 2-D picture is obtained therefore actual mass is determined. Wide orbit planets produce larger amplitude of the proper motion of stars hence easier to detect but wide orbit means longer orbital period hence a longer timeline of observations.

Transit photometry method
If the planet lies in the orbital plane of the star and we have an edge on view then the planet transit or Venus transit-like will cause a periodic square-well shaped dip in the star's brightness. It gives the estimate of planet size and the orbital period. The mass will have to be determined by astrometric or Doppler shift technique.

Gravitational microlensing
This method is used for detecting very faint stellar and sub-stellar bodies within our galaxy. A massive body intervening the space between the source and observer causes gravitational bending of light from the source leading to the brightening of the image of the source. If the intervening body is a star with a planet then the lining up of the source planet, intervening star and the observer will lead to considerable brightening up of the image of the source. As planet moves out of the line of sight, the brightening will diminish. The

Method
Description period of fluctuation in the image of the source is the orbital period and the amount of fluctuation gives the mass of the planet.

Lyot method
Suppresses 98.5% of the starlight by the use of a coronagraph and images the companion planet at near-IR wavelength or images the starlight reflected by the companion planet or by the circumstellar debris disk.

Nulling interferometry.
Large binocular telescope is used for canceling the starlight by nulling interference and image the exo-planet or the debris disk. Starlight are collected by two mirrors but with a path difference of half wavelength. This results into destructive interference along the central line of sight but it is constructive interference off the line of sight. Radio emissions similar to those from Jupiter.
Radio emissions similar to those from Jupiter could reveal the presence of planets. Time is the greatest difficulties. The orbital periods of Jupiter and Saturn are 12 and 29.5 years. Hence one will have to wait for that long to measure its periodicity.
Second is the resolution of the Doppler Technique. With the present resolution we could keep looking for century and not detect a Saturn of that mass and of that semi-major axis.
The masses of Jupiter and Saturn are 318 and 95M E and those of Neptune and Uranus are 17.2 and 14.6 M E . The amplitude of Doppler oscillation is proportional to (MSinα)/a 1/2 . Hence observational bias is towards heavier masses and shorter semi-major axis.  Table 6. A comparative study of the radial velocity of the host star for different combinations of star-planets.
As seen from the Table (6), with decreasing mass of the planet and increasing mass of the host star, the amplitude of oscillation of the radial velocity decreases. As the amplitude of oscillation decreases it becomes increasingly difficult to decipher the periodic planetary signal in the presence of various noise sources that produce random fluctuations in star's apparent radial velocity.
Recently HARPS spectrometer has been developed by the Swiss team which discovered the first exoplanet Pegasi 51. This spectrometer has the required precision to decipher the tiny Doppler shift due to 0.1 m/s radial velocity of the host star harboring an earthlike planet. The instrument is kept in high vacuum and precisely controlled low temperature so that the sources of noise can be eliminated and optical stability may be imparted for obtaining the required precision. Through HARPS only Mu Arae's planet, 14 times M E, was detected.
By Astrometric measurements , the inclination of the planetary orbit and orbit-globe parameters can be determined. Astrometry is the precise measurement of two-dimensional stellar positions on the celestial sphere. The astrometric studies complement the radial velocity method. Through this method the ellipse traced by the centroid of the star during one orbital period of the planet can be exactly determined. From this ellipse the angle of inclination α and other globe-orbit parameters can be determined.
Space Interferometry Mission scheduled for 2009 will give sufficient accuracy to astrometric method for discovering a new planet.

The classical model of the birth and evolution of a solar system
From the three new Neptune-like planets [Schwarzschild 2004] the scientists conclude the following: i. The shock waves of a Supernova explosion sets a giant cloud of gas and dust , passing nearby, into a spinning mode. The rapid spin cannot be accommodated by one hydrostatic star hence it results into the fragmentation of the cloud into binary or multiple star system. Even the new multiple system cannot accommodate the excess angular momentum and the individual clouds are flattened out as pancake shaped disc of accretions. The central part collapses into a proto-star surrounded by a thick disk of gas and dust. From these Keplerian debris disks the planets are born. The solar insolation is causing the photoevaporation of gas out of the system and the dust particles are spiraling inward due to Poynting-Richardson Drag and settling down in the midplane of the disc. Thus gas is blown out and the host star vicinity is filled with heavy suspension of dust particles larger than a micron size. These micron size dust randomly collide and stick together building up km-sized planetismals. But before the build up can take place the random collision may result in repeated breakups preventing the formation of planetismals. But if there is heavy dust suspension, with the gas blown out, runaway gravitational accretion takes place resulting into full scale terrestrial planets.
So there are two scenarios: a. The first scenario is the earliest stage of planet formation when the protostar is not experiencing full scale thermonuclear fusion . At that stage there is a very light density suspension of dust in a thick envelope of gas. The gravitation is too weak and gravitational accretion is prevented. But snowline criteria is not applicable as thermonuclear furnace is not switched on yet. Hence the dust is coated with ice which is amorphous and hence sticky (Ordinary ice is a open-pack hexagonal crystalline structure and is non-sticky whereas ice at -230ºc is fluffy amorphous structure. If small ceramic ball is covered with fluffy, amorphous ice falling from a height of 12 cm it bounces to 1 cm whereas ball covered with crystalline ice bounces to 8 cm. The colder, more disordered ice absorbs more of the energy of the impact because the molecules rearrange themselves during the collision. Therefore the dust particles coated with amorphous ice will stick together rather than rebounce). Through collision and agglomeration (or sticking), km-sized planetismals are formed which are then set on the path of gravitational accretion. Once 10M E cores have formed the gravitational field is strong enough to cause the wrapping of these icy-rocky cores with thick envelopes of gas resulting first into gas giants and subsequently into ice giants. b. The second scenario is when gas has been exhausted both by the process of gas giants and ice giants formation and also by photoevaporation. At this stage lack of gas assists runaway gravitational accretion of the thick dust suspension into terrestrial planets. Radioactive dating of the core by Hf-W has established that Earth and Mars were formed 29 million years and 13 million years respectively after the birth of the solar nebula [Cameron 2002, Yin et al 2002, Kleine et al 2002. There was an extended core formation period. The interior of the planet is heated partly due to Helmholtz Contraction(or gravitational energy release) and partly due to radioactivity particularly that of 26 Al. Accumlative collision between small bodies produce the planet. When a small body collides into a large body the core of the small body gets embedded into the mantle of the large body. The heat of impact melts the interior and molten iron core of the smaller body percolates to the core of the larger body. ii. According to core-accretion theory or dust bunny theory, by agglomeration-accretion a rock or ice core is formed of mass 10 M + . Beyond that critical mass the core rapidly envelopes itself by gravitationally captured gas from the surrounding circumstellar disk. This process terminates with the formation of a gap in the circumstellar disc.
Douglas Lin(University of California, Santa Cruz) says " Many incipient gas giants won't make it to jovian mass before the disk dissipates after a few million years. So we can expect lots of failed Jupiters to show up as Neptune".
The farther the planet is the longer it takes to form. Infact it may be 100 billion years whereas the lifetime of the debris disk may be only several million years.
Computer models of Jonathen Lunine give the following picture:


In the inner part of the solar system debris disk is dense. In this dense part, the gas giants are formed in first million years through a chain of core formation and gas accretion;  In the next ten million years the leftover rock and dust accreted to form the moonsized embryos. Dust clumps together into gravel, gravels to rock and rocks to hundred of planetary embryos moving in tidy, sedate circular orbits. The collisions stop.  Jupiter's influence that is gas giant's influence have two effects:  It churns an orderly set of embryos into an unruly, colliding swarm which through collision and accretion evolves into a set of terrestrial planets like our Earth and Mars in another 10 to 20 million years but these rocky planets are bone dry;  Gas Giants in outer regions would cause icy embryos to veer inward and collide with newly evolved rocky planets. In the process water is transferred to the inner rocky planet;  Gas Giants also act as bodyguards for these small watery worlds. There are large chunks of residual rock an ice which are on the loose and which would smash the inner rocky planets in next 100 million years. Gas Giants with its powerful gravitational fields took direct hit from these marauder chunks, some were flung out of the system and most others were herded into the asteroid belt; iii. According to gas instability theory there is an abrupt formation of gas giants. The gravitational instability in the circumstellar disc leads to gas-giant formation. There is no unfinished middleweights planets. iv. In classical theory the explanation given for the infernally tight orbits of the hot jupiters is the following: These must have formed much farther away beyond the snow-line which is about 1AU. Subsequently the tidal interaction with the protoplanetary disc caused the hot Jupiter to spiral in. This protoplanetary disc itself dissipates off due to Poynting-Robertson drag and due to photo-evaporation. So the inward migration must be fast before the dust-gas protoplanetary disc dissipates off [Schwarzschild 2004]. This is too contrived a situation. But in the new planetary-satellite model this naturally occurs.

The extra-solar planets which donot fit in any model
Lately many exoplanets have been discovered apart from hot-jupiters which donot fit any Model of planet birth and evolution and hence present a conundrum. * Initially it was thought that Giant planets must have formed in colder region far from their parent stars. Icy nuggets act as seeds that accumulate enough dust to build up to a critical mass where by runaway accretion it is enveloped by a large mass of gas giving birth to gas giants. These icy nuggets can form only beyond snowline [Sasselov & Lecar 2000]. But in HD 188753 this could not have happened. This is because the secondary system of star pair would truncate the disk to 1.3AU leaving nothing beyond in the colder region that could nucleate and grow into a giant planet. "Giant planets in circumstellar disks can migrate inward from their initial formation positions. Radial migration is caused by inward torques between the planet and disk, by outward torque between the planet and the spinning star and by outward torques due to Roche lobe overflow and consequent mass loss from the planet." [Trilling, Benz et al 1998]. Through numerical solutions it has been shown that taking all the torques into consideration, Jupiter-mass planets can stably arrive and survive at small heliocentric distance just as hot-jupiters do in scorchingly tight orbits.  (1) Equation (1) has two roots and hence planet -satellite systems have two geo-synchronous. Only at these two Geo-synchronous orbits the system is in equilibrium because the orbits are non-dissipative. Elsewhere the system is dissipative hence in non-equilibrum either spiraling out to the outer geo-synchronous orbit or spiraling inward to its certain doom. The inner Geo-synchronous orbit lies at energy maxima whereas the outer Geosynchronous orbit is at energy minima. Therefore the inner geo-orbit is an unstable equilibrium orbit and the outer geo-orbit is a stable equilibrium orbit.
When the natural satellite is at the inner geo-orbit it is easily perturbed by solar wind or cosmic particles or solar insolation. It tumbles out on an expanding outward spiral path or it falls short of the inner geo-orbit on inward collapsing spiral path. Inward collapsing spiral path is entirely a runaway path. The outward spiral path, because of energy conservation, is initially an impulsive gravitational runaway phase which quickly terminates because of tidal dissipation in the central host body due to tidal streching and squeezing . This runaway phase is the gravitational sling shot phase. After the gravitational sling shot phase, the natural satellite coasts on its own towards the outer geo orbit. Our Moon is on a midway course in its journey towards the outer geo-orbit. Charon, a satellite of Pluto, has already arrived at the outer geo-orbit. The satellite may remain stay put in the outer geo-orbit as Charon is doing or it may be deflected as our Moon will be.

The new hypothesis-gravitational sling shot model of planet-satellite system
The Authors did the Keplerian-approximated analysis of Earth-Moon, Mars-Deimos-Phobos and Pluto-Charon [Sharma & Ishwar 2004A, Sharma, Rangesh & Ishwar 2009. The Authors were able to generate the outward expanding spiral path of Moon as shown in Figure 1.
In a sequel paper on the New Perspective of the Solar System [Sharma & Ishwar 2004B, Sharma 2011, it was established that Planets experience a similar kind of impulsive slingshot phase due to Sun as our Moon does due to Earth. This leads to new paradigm on the birth and evolution of our as well as extra Solar Systems.

THe phenomena of gravitational slingshot
Planet fly-by, gravity assist is routinely used to boost the mission spacecrafts to explore the far reaches of our solar system [Dukla, Cacioppo & Gangopadhyaya 2004, Jones 2005, Epstein 2005, Cook 2005]. Voyager I and II used the boost provided by Jupiter to reach Uranus and Neptune. Cassini has utilized 4 such assists to reach Saturn.
A space-craft which passes " behind" the moon gets an increase in its velocity(and orbital energy) relative to the primary body. In effect the primary body launches the space craft on an outward spiral path. If the spacecraft flies "infront" of a moon, the speed and the orbital energy decreases. Traveling "above" and "below" a moon alters the direction modifying only the orientation (and angular momentum magnitude). Intermediate flyby orientation change both energy and angular momentum. Accompanying these actions there are reciprocal reactions in the corresponding moon.
The above slingshot effect is in a three body problem. In a three body problem , the heaviest body is the primary body. With respect to the primary body the secondary system of two bodies are analyzed.
In case of planet flyby, planet is the primary body and the moon-spacecraft constitute the secondary system.
While analyzing the planetary satellites, Sun is the primary body and planet-satellite is the secondary system. But in our Keplerian approximate analysis, Sun has been neglected without any loss of generality and without any loss of accuracy. In fact the general trend of evolution of our Moon has been correctly analyzed [Sharma, B. K. and Ishwar, B " Basic Mechanics of Planet-Satellite Interaction with special reference to Earth-Moon System", 2004, http://arXiv.org/abs/0805.0100].
While analyzing the Sun-planet system, galactic center is the primary body and Sun-planet is the secondary system. But in our analysis the galactic center has been neglected and we have essentially analyzed Sun-planet as a two body problem.
In a similar fashion in the analysis of Planet Flyby-Gravity Assist Maneuvers, Planet is the primary body. The planet can be neglected and moon-spacecraft can be treated as a two body problem and the same results can be obtained without any loss of accuracy or generality. This will be done in a future paper.
The gravitational sling shot becomes clearer if we look at the radial acceleration and radial velocity profile.

Fig. 2. Radial Acceleration Profile of Moon (Within a G1 the Moon is accelerated inward.
Beyond a G1 the Moon is rapidly accelerated outward under the influence of an impulsive gravitational torque due to rapid transfer of spin rotational energy. The maxima of the outward radial acceleration occurs at a 1 . (This is the peak of the impulsive sling shot torque.)

Setting up of the time integral equation.
In setting up the time integral equation the first step is to set up the radial velocity expression which has been derived in SOM_Appendix A.
The radial velocity expression is as follows:   (2) Where K is the structure constant and M is the structure exponent. All the other symbols are defined as before. Equation 2 gives the radial velocity of natural Satellite Iapetus with respect to Saturn.
Between a G1 and a G2 , ω/Ω is greater than Unity hence radial velocity is positive and recessive.
At less than a G1 , ω/Ω is less than Unity hence radial velocity is negative and secondary approaches primary.
At greater than a G2 , ω/Ω is negative which is physically not possible in a prograde system hence system is untenable and it is a forbidden state.
Spin to Orbital velocity equation yields a root when it is in second mean motion resonance (MMR) position. That is: This gives a root at a 2 which is gravitation resonance point and I assume that after the secondary undergoes gravitational sling shot impetus, it attains maximum recession velocity at this point. After this maxima, recession velocity continuously decreases until it reaches zero magnitude at outer Clarke's Orbit as shown in Figure 3.
Thus as is evident from Eq.2, recession velocity is zero at a G1 and a G2 . From a G1 to a 2 , the system is in conservative phase and secondary experiences a powerful sling-shot impulsive torque which imparts sufficient rotational energy to the secondary by virtue of which the secondary coasts on its own from a 2 to a G2 during which time the system is in dissipative phase, Secondary is exerting a tidal drag on the central body and all the rotational energy released by the central body as a result of de-spinning is lost as tidal heat, but not completely. This tidal heat is produced during tidal deformation of both the components of the binary if the secondary is not in synchronous orbit. Our Moon is presently in synchronous orbit hence it is not undergoing tidal heating but Earth is undergoing tidal heating.
When the secondary tumbles into sub-synchronous orbit it experiences a negative radial velocity which launches it on a collapsing spiral and the system is spun-up . In this collapsing phase, secondary exerts an accelerating tidal torque on the central body and Since Eq.2 has a maxima at a 2 therefore the first derivative of Eq. 2 has a zero at a 2 . Equating the first derivative of Eq.2 to zero we get: From Eq.4, structure exponent 'M' is calculated.
We donot yet know the structure constant K. We make an intelligent guess of V max and calculate the value of 'K' from Eq. 2 equated to V max at semi-major axis 'a 2 '.
Using these values of 'K' and 'M' the time integral equation is set up and tested for the age of the system.
This transit time should be of the order of 4.5Gy in the case of Iapetus because that is the age of Iapetus. [ Castillo-Rogez et al (2007)]. Through several iterations we arrive at the correct value of K.

Theoretical verification of the experimentally observed 'lengthening of day' curve of our planet Earth by primary-centric analysis 3
Since the birth of Earth-Moon System, Earth's spin has been slowing down and Moon has been receding. Earth's spin has slowed down from 5 hours to 24 hours today and Moon has receded from 15,000Km to the present Lunar Orbit of 384,400Km.
John West Wells through the study of daily and annual bands of Coral fossils and other marine creaturs in bygone era has obtained ten length of day of bygone eras [Wells 1963, Wells 1966]. These benchmarks are tabulated in Table ( Kaula & Harris [1975] have determined the synodic month through the studies of marine creatures. The results are tabulated in Table (10).
One benchmark has been provided by Charles P. Sonnett et al through the study of tidalies in ancient canals and estuaries [Sonett & Chan 1998 ]. He gives an estimate of 4 18.9 E T  hours mean solar day length at about 900 million years B.P. in Proterozoic Eon, pre-Cambrian Age.

Comparative study of lengthening of day curve of our Earth by theory and observation
As seen from the superposition of the two lengthening of day curves, there is remarkable match between Observation and Theory in the recent past after the Pre-Cambrian Explosion of plant and animal life but in the remote past, particularly in early Archean Eon, Earth seems to be spinning much slower than predicted by theory. This implies that rotational inertia was much higher than what has been assumed in this analysis. In fact there are evidence to show that early Earth was much less stratified as compared to modern Earth. It was more like Venus [Allegre, Calnde 1994, Taylor, Rose & Mclennan 1996.
Through out the analysis C, the Principal Moment of Inertia, has been assumed to be constant whereas infact it was evolving since the Giant Impact [Runcorn 1966].
In the first phase of planet formation, Earth was an undifferentiated mass of gas, rocks and metals much like Venus. At the point of Giant Impact, the impactor caused a massive heating which led to melting and magmatic formation of total Earth. The heavier metals, Iron and Nickel, settled down to the metallic core and lighter rocky materials formed the mantle. The mantle consisted of Basalt and Sodium rich Granite.
Due to Giant Impact, Earth gained extra angular momentum. This led to a very short spin period of 5 hours. It has been calculated that the oblateness at the inception must have been 1% [SOM_Appendix D, Kamble 1966] whereas the modern oblateness is 0.3%. Taking these two factors into account C of Earth must have been much higher than the modern value of 37 2 8.02 10 kg m  . In this paper the early C has been taken as 37 2 9.9 10 kg m  .
After Achaean Eon the general cooling of Earth over a period of 2 billion years led to slower plate-tectonic movement. The 100 continental-oceanic plates coalesced into 12 plates initially and into 13 plates subsequently. The slower plate tectonic engine led to deep recycling of the continental crust and hence to complete magmatic distillation and differentiation of the internal structure into multi-layered onion like structure. Thus at the boundary of Archean Eon and Proterozoic Eon a definite transition occurred in the internal structure.
Before this boundary, the mantle and the outer crust was less differentiated. It was composed of a mixture of Basalt and Sodium-rich granite. After this boundary a slower plate-tectonic dynamo helped create the onion-like internal structure with sharply differentiated basaltic mantle and potassium-rich granitic crust. This highly heterogenous internal structure and less oblate geometry leads to the modern value of C equal to 37 2 8.02 10 kg m  .
The form the evolving C is as follows: Here f[(t-2E9)_] is defined as a step function which is 0 before 2 billion years and is Unity at 2 billion years and at greater times.
The profile of evolution of C with time is obtained in Fig. (7) : As can be seen in Fig. (9), there is a much closer fit except for a large deviation at 2.5Gyrs after the Giant impact. This is due to step change in Moment of Inertia, C, at 2Gyrs after the Giant Impact. It would have been more realistic to assume a gradual change in C at the boundary of Archean and Proterozoic Eon. This correction will be made in a sequel paper.

A new perspective of birth and evolution of our solar system & extra solar systems
The new perspective holds that: i. before the thermonuclear furnace turns on that is before full scale fusion reaction begins, in the inner region of the solar system by a process of agglomeration-accretion the icy-rocky core is formed. As soon as it reaches a critical mass of 10M E , it rapidly wraps itself with Hydrogen and Helium gas which is available in abundance in the gasdust debris . As it grows to 300M E , a gaping hole is formed in the disk. This paucity of gas terminates the runaway gas accretion. As we see, the necessity of a snow line does not arise as the inner region is sufficiently cold (100 kelvin) to keep the dust coated with amorphous ice which eliminates impact rebounce and permits agglomeration to take place unhindered to km size planetismal. ii. by the above process sequentially the four jovian planets are born i.e. one after another.
As the first Gas Giant is formed, because of initial slingshot effect, caused by our Sun, Jupiter spirals out and makes space for the formation of the next gas giant namely Saturn. As Saturn spirals out, the Ice Giants namely Neptune and Uranus are formed. iii. Just as Jupiter spirals out to wide orbits, it is equally probable that the gas giant may be perturbed within the inner geo-orbit in other solar systems. Those tumbling short of inner geo-orbit get launched on inward collapsing spiral path doomed to their certain distruction. They become hot jupiters in scorchingly tight orbit. In course of planet discovery, many examples of hot jupiters have turned up. iv. the planet formation sequence follows the descending order of mass. The heaviest (i.e.Jupiter) being born the first and the lightest ( i.e. Neptune) the last; v. the time factor of evolution is inversely proportional to the mass i.e. the massive giants evolve out of their initial orbit very rapidly whereas the lightest one remaining almost stay put. This implies that Jupiter spirals out of the maternity ward very rapidly whereas the terrestrial planets remain orbiting where they were born; vi. in the first phase, Gas Giants and Ice Giants are formed when there is abundance of gas and dust. In course of birth and evolution of these massive planets the disk is dissipated of gas partly due to the accretion by the jovian cores and partly due to photoevaporation. The remnant disk is largely populated by planetismals. In the second phase the rocky planetismals gravitationally collapse to form the terrestrial planets in a sequence according to the descending order of mass. Earth was formed the first and Mercury the last. Pluto is a recently captured body. It has not been formed insitu.

Observational proofs in support of gravitational sling shot model
In recent days four observations strongly suggest that in remote past Jupiter and the gas giants may have experienced gravitational sling shot and they may have been launched on an outward spiral path just the way Moon has been launched or for that matter all planetary natural satellites have been launched.
a. 700 Hilda asteroids in elliptical orbit [Franklin et al 2004].The asteroid belt is populated with hundred thousands of rocky remnants leftover from planet formation. These are called asteroids and they lie between Mars and Jupiter orbit between a radii of 3AU to 10AU. Most of the asteroids are in near circular orbits. There are 700 odd asteroids known as Hilda which are in highly elliptical orbit and these eccentricities could have been imparted only by a migrating Jupiter set on an expanding spiral path. The migrating Jupiter first ejected some proto-Hilda asteroids out of the system and next elongated the orbits of the residual asteroids. The migrating Jupiter could have also set the planetary embryos on unruly chaotic paths which led to frequent collisions and accretion resulting into terrestrial rocky planets. b. Through computer simulation studies [Tsiganis, Gomes, Morbidelli & Lavison 2005] it has been shown that our planetary system, with initial quasi-circular, coplanar orbits, would have evolved to the current orbital configurations provided Jupiter and Saturn crossed the 1:2 mean motion resonance (MMR). When the ratio of the orbital periods of Jupiter and Saturn is 1:2 it is the strongest resonance point. At all integer ratios resonance is obtained but the maximum is obtained at 1:2.  . These are asteroids which are in he same orbit as that of Jupiter but they are leading or lagging by 60º in their coorbital motion. d. The petrology record on our Moon suggests that a cataclysmic spike in the cratering rate occurred approximately 700 million years after the planets formed . With the present evidence we assume the birth of our Solar Nebula at 4.56Gya. The formation of Gas Giants and Ice Giants was completed in first 5 millon years and Earth was completed in first 30 million years. This puts the date of completion of Giant Planets at 4.555Gya and the date of completion of the Terrestrial Planets particularly Earth at 30 million years after the solar nebula was born that is at 4.53Gya. At 4.53Gya, the Giant Impact occurred and from the impact generated circumterrestrial debris, Moon was born beyond Roche's Limit at 16,000Km orbital radius. By gravitational sling shot effect it was launched on an outward spiral path. Presently Moon is at the semi-major axis of 3,84,400Km with a recession velocity of 3.7cm/year. Towards the end of planet formation phase, the residual debris of the solar nebula was being rapidly sucked in or swept out of the system. This resulted in heavy meteoritic bombardment of all the big sub-stellar objects including our Moon. Through Apollo Mission studies it has been determined that there is a sharp increase in the bombardment rate and hence in the cratering rate around the period of 4.5 to 3.855Gya. From this it is concluded that there was a cataclysmic Late Heavy Bombardment of all big sub-stellar bodies, including our Moon, at about 700 My after the completion of formation of Jupiter and Saturn.
As the planet formation was completed , the gaseous circumsolar nebula was dissipated by gravity accretion and finally by photoevaporation. According to Tsiganis et al [2005], Jupiter and Saturn were born at 5.45AU and 8AU respectively where the orbital period ratio that P S / P J was less than 2. According to them the resulting interaction with massive disk of residual planetismals Jupiter and Saturn spiraled out on diverging path crossing 1:2MMR(P S / P J = 2) point at 8.65AU and today the ratio is little less than 2.5. At the 1:2MMR crossing due to gravitational resonance their orbits became eccentric. This abrupt transition temporarily destabilized the giant planets, leading to a short phase of close encounters among Saturn, Uranus and Neptune. As a result of these encounters, and of the interactions of the ice giants with the disk, Uranus and Neptune reached their current heliocentric distances of 19.3AU and 30AU. And Jupiter and Saturn evolved to the current orbital eccentricities of 6% and 9%. The same planetary evolution can explain LHB provided Jupiter and Saturn crossed 1:2MMR 700My after their formation. That is LHB occurred at 3.855Gya.

Future direction of investigation
This new perspective on Solar System birth and evolution based on planetary satellite dynamics is called Primary-centric World View. This Primary-centric View has led to the fractal Architecture of the Universe [Sharma 2012A]. The Primary-centric View has been applied to Kepler-16b, Kepler 34b and Kepler 35b to explain its circum-binary architecture [Sharma 2012B]. The Primary-centric View has also been used to test the validity Iapetus's hypothetical sub-satellite [Sharma 2012C]. The Author has utilized the primary-centric view to work out the probable evolutionary history of PSR J1719 -1438 and its compacted companion at a distance of 4000ly [Sharma 2012D)]. Presently I am applying this World View to see if star binaries, pulsar binaries, pulsar-black hole, Galaxy of Stars, Clusters and Super-Clusters fall in this frame work or not . A positive test for all these binaries and galaxy of stars will give us a new approach to the dynamics of the Universe.

References
Allegre The all-encompassing term Space Science was coined to describe all of the various fields of research in science: Physics and astronomy, aerospace engineering and spacecraft technologies, advanced computing and radio communication systems, that are concerned with the study of the Universe, and generally means either excluding the Earth or outside of the Earth's atmosphere. This special volume on Space Science was built throughout a scientifically rigorous selection process of each contributed chapter. Its structure drives the reader into a fascinating journey starting from the surface of our planet to reach a boundary where something lurks at the edge of the observable, light-emitting Universe, presenting four Sections running over a timely review on space exploration and the role being played by newcomer nations, an overview on Earth's early evolution during its long ancient ice age, a reanalysis of some aspects of satellites and planetary dynamics, to end up with intriguing discussions on recent advances in physics of cosmic microwave background radiation and cosmology.

How to reference
In order to correctly reference this scholarly work, feel free to copy and paste the following: Bijay . Enigma of the Birth and Evolution of Solar Systems May Be Solved by Invoking Planetary-Satellite Dynamics, Space Science, Dr. Herman J. Mosquera Cuesta (Ed.), ISBN: 978-953-51-0423-0, InTech, Available from: http://www.intechopen.com/books/space-science/the-dynamics-of-planetarysatellites-and-the-generalization-of-the-same-provides-a-new-theory-of-bir