19 | June | 2010 | SCIFIre@lismQuest.com

how to support guidance systems in the shared data interactions of spacetime

By Henryk Szubinski

TURNING AGAINST GRAVITY

4 FREEDOOMS

5TH FRAMEWORK : THE FREEDOOM OF KNOWLEDGE MOOVEMENT

CHORDIS6

THE 7TH FRAMEWORK CHORDIS

MINIMAL ECCESSANCE TO THE UNIVERSE BY A DISSONATED VALUE THAT EVERYONE USES AS THE TYPE OPEN FASED DISPLACEMENT TROUGH IT AS THE TYPE ALTERED UNIVERSE HISTORIES:

a human relations with the objective universe position of a observer with the spacetime where all laws are maintained so that all data on spacetime can be maintained as functional on any additional alterations. This then is a hunam point of view for the data verticals that define the process of warping at the right side of the illustrations as the difference between universal relations in observations by data

x+ 1

so that the space time = 1+relativity Area

and the thread levels = difference A + 1 / 1-A (x+1)

basic black hole and the spacetime in rotation about the universal core values so that the event horizon is defined as the thread of a type rotation similar to a bolt.so that the rotations in the vertical = a doughnut type spacetime that is open.

basic data on the altered cir sector quadrance resultance of a non involved / involved prismartic effect where both the refraction through a prism can be observed as well as the altered position singularity of the altered vector non prismat displacement.

A ATOMIC MODEL FOR THE EXPANSIONS OF CORE UNIVERSE VALUES IN PULSATIONS AND CONTRACTIONS SUCH AS WITH HEAT DEATH OF THE UNIVERSE BY DISPLACEING TEMPERATURE THROUGH THE WARPS IN DOUGHNUT FORMAT FORCE AS WELL AS BIG CRUNCH SIMILARITY OF TRANSLATIONAL VECTORISATIONS.

electrons will be shown to cover all the electron orbitals by the motion of a divisive time process in a mobius path around the dougnut as well as the proton and neutrons doing the same with the core value doughnut motion:

The effects are alterability by mobius motion in linked influence to the orbital doughnuts:

such as a singualr process effect to displace influence beyond the 4th orbital INV = the full motion 3 D of the orbital doughnut so that the process in 3 D = motion involvance by the influence of the 3 D responsive core motion = a proton neutron alterations of the radial similarity by opposition of thoose rotations = 3 S

where does all the matterr dark matter go when the universe has expanded; well the type mobius strips would have a shadow when the format mobius = a dimensional solid form such as a doughnut.

the doughnuts will be related to as prisms that conclude the motion of refractions and reflections as well as polarisations as the apperance of the particles by a format of opposed backgrounds.

THE PROCESS VECTORS SHOWN ARE THE SAME AS THE VALUES ON THE PENDLUM AS A FORMAT TO BE OVERIDED WITH THE DOUGHNUT TURN OF ITS MOTION INVERTIVES

expansional displacement by relations of isolated force parameters of the universe H2O in non big crunch value relations difference universe

THE ACTUAL THEORY THAT DEFINES THE BIG BANG WITH THE BIG CRUCH WOULD EQUATE THE NON OBSERVATIONALITY OF THE PROCESS BY BEEING INCLUDED IN THE PROCESS OF A POSITIONAL INCLUSION OFF THE PROCESS OBSERVATIONS BY THE NEW TYPE 1,2,3 FORMAT THAT DEFINES THE PROCESS AS A COMPUTATIONAL THEORY WHICH BALANCES THE 2 VECTORS AND THEIR 3 VECTOR MUTUAL DISSAPEARANCE OF THE OBSERVER WITHOUT SUCH A THEORY:

THE TYPE THEORIES ON THSI FORMAT WILL THEN CAUSE A DISSONATED DISRUPTION OF THE BIG CRUNC &/OR BIG BANG AS BEING DISSORDERED IN ITS EXACT CENTRATIONS:

Is there any difference between a simulated reality and a “real” one? …. Tipler’s Omega Point Theory is predicated on an eventual Big Crunch, ….. The inhabitants of a simulated universewould have no way of knowing that one day of … embedded in pi (in its base-11 expansion) by the creators of the universe. …

Illustration of a pendulum.

True entropy-energy in its primordial forms as the expansion of space or …. but itsrelationship to other physical quantities or parameters has never been understood. … Thevalue of G determines the time scale (lifetime) of the Universe both …. possibility if theUniverse does not collapse in a “Big Crunch“. …

Linearizations of a pendulum.

“Einstein of information theory” to illuminate the relation of …… parameter values (“genes”) of our evo devo universe may provide results analogous to changes geneticists …… About six billion years ago, universe expansion began to accelerate. …. A universe that ended in a “Big Crunch,” for example, would …

17 Feb 2008 … What is the force behind the big bang if not the greater probability of disorder… In relation to the universe’s expansion being attributable to the big bang, … one can ask if this is termed as a contraction WRT the isolated body? …. In this sense no physical observer actually ‘makes it’ to the big crunch. …

(IOW, the paper galaxies exert no gravitational force on each other. …… to Earth (Traveling at the same speed in relation to earth on its return journey …. 3) A better way to observe theexpansion of the universe is to read what Edwin …. The idea that the universe could collapse into a “Big Crunch” and then …

I have a friend who doesn’t believe in the expansion of the Universe. …… I believe there is noattractive force between photons (other than …… What is angular scaling (degrees) inrelation to the band filtering of a piece of the …… round the Universe in the time between the Big Bang and the Big Crunch! …

2 Jan 2010 … 2) Coriolis effect; the difference in ground heating (caused by the …… The gas giants have no CO2 or H2O, mostly Nitrogen, ….. In the mean time, however, see if you can prove that the universe, in it’s entirety, …… in relation to ANOTHER object. What exactly are you trying to convince …

What if there was no “big bang” and there will be no “big crunch“? ….. (the value followingrelationship, not the is of identity) to be: E = m c λυ. …… The difference between the electrode and the ion creates a force of attraction. …. and there is a resultant expansion of the universe, …

9 Feb 2007 … ‘Will the universe collapse again and lead to another Big Bang? …. in nature as evidenced in the observed spontaneous expansion of the universe, ….. has no relationto the determinism or indeterminism of the laws of …. For ex: there is no difference between consciousness and awareness to some. …

3) – According to these facts, distance of light displacement are only the …… Relation + entre + la + structure + spatiale + du + matériau + et + de + …… So, with no force, how all matter of the universe at this end-point can ….. + universe + expansion, + and + black + holes (Mexico) – big + crunch (UK) …

Our theory of isolated elementary particles is based on non-linear …… of spacetime is characterized by the relation between differences in time …… that means a displacementof 7 days per millennium. Its value of …… have a global influence on universe’s expansionand provokes an artificial “Big Crunch“. …

In mathematics, a linear function (or map) $f (x)$ is one which satisfies both of the following properties:

additivity, $\textstyle f(x + y)\ = f(x)\ + f(y);$

homogeneity, $\textstyle f(\alpha x)\ = \alpha f(x).$

(Additivity implies homogeneity for any rational α, and, for continuous functions, for any real α. For a complex α, homogeneity does not follow from additivity; for example, an antilinear map is additive but not homogeneous.)

An equation written as

$f(x) = C\,$

is called linear if $f (x)$ is a linear map (as defined above) and nonlinear otherwise. The equation is called homogeneous if $C = 0$ .

The definition $f (x) = C$ is very general in that $x$ can be any sensible mathematical object (number, vector, function, etc), and the function $f (x)$ can literally be any mapping, including integration or differentiation with associated constraints (such as boundary values). If $f (x)$ contains differentiation of $x$ , the result will be a differential equation.

A classic, extensively studied nonlinear problem is the dynamics of a pendulum under influence of gravity. Using Lagrangian mechanics, it may be shown^[1] that the motion of a pendulum can be described by the dimensionless nonlinear equation

$\frac{d^2 \theta}{d t^2} + \sin(\theta) = 0\,$

where gravity points “downwards” and $θ$ is the angle the pendulum forms with its rest position, as shown in the figure at right. One approach to “solving” this equation is to use $d θ / d t$ as an integrating factor, which would eventually yield

$\int \frac{d \theta}{\sqrt{C_0 + 2 \cos(\theta)}} = t + C_1\,$

which is an implicit solution involving an elliptic integral. This “solution” generally does not have many uses because most of the nature of the solution is hidden in the nonelementary integral (nonelementary even if $C 0 = 0$ ).

Another way to approach the problem is to linearize any nonlinearities (the sine function term in this case) at the various points of interest through Taylor expansions. For example, the linearization at $θ = 0$ , called the small angle approximation, is

$\frac{d^2 \theta}{d t^2} + \theta = 0\,$

since $\sin(\theta) \approx \theta$ for $\theta \approx 0$ . This is a simple harmonic oscillator corresponding to oscillations of the pendulum near the bottom of its path. Another linearization would be at $θ = π$ , corresponding to the pendulum being straight up:

$\frac{d^2 \theta}{d t^2} + \pi - \theta = 0\,$

since $\sin(\theta) \approx \pi - \theta$ for $\theta \approx \pi$ . The solution to this problem involves hyperbolic sinusoids, and note that unlike the small angle approximation, this approximation is unstable, meaning that $| θ |$ will usually grow without limit, though bounded solutions are possible. This corresponds to the difficulty of balancing a pendulum upright, it is literally an unstable state.