F O R M A T  F O R  C O N T I N I U M  U M L I M I T E D

By Henryk Szubinski….

(a space ship freighter concept)

 

 

WORK HERE  concerns the calculations of background space time relations on three basis of a mean value cold dark matter format by using the mean value resultant of the background, foreground,and real speace time values;

background formats

[------------------alter Hyper node

[------------------predefined start values

[-------------------in toxicative sections.

background formats 2

]——————-alter diffuse access alter connect

]——————redistribute

]——————defunctionate actuality

background section 3

[---------------------hyper divisive improbability

[---------------------alter hyper projective diffuse

[--------------------redistribute string theory Obtuse angles

foreground value 1)

[------------------------prodefine hyper actualise

[--------------------------prodefinitions superior numbers of

[-----------------hyper generate

foreground set 2;

]————————–redefined symmetry

]————————-redefine alternate ATLAS

]————————-system project point

foreground set 3 ):

]—————————–definition high stability sections

]—————————alterations of mass=D.f.S

]—————————-projective

Real background set 1);and the real foreground sets;2)

——————–response diffuse————–hyper

——————–alterance D.f.= E.x———–sectional

——————–spacial hyper ————–implicit drive

——————multi definitions———intact sections (probability drive reversal)

mulst system compiled data theory;

B.g / F.g = root R.g ( 3 – F)

A fair basis of everything by a similar value that has to be space…Right ?…every event has a similar look to it,,cant be that difficult to derive space time everywhere when it is one continuiim.. Just juxtaposing background with foreground and real ground on 3 levels would give a mean value space time as the usable comparative to any space time object..

the resultants could be used in;

cold matter

dark matter

dark energy

luminescence spread effects

 

Spacetime entails a new concept of distance. Whereas distances in Euclidean spaces are entirely spatial and always positive, in special relativity, the concept of distance is quantified in terms of the space-time interval between two events, which occur in two locations at two times:

s^2 = c^2\Delta t^2 - \Delta r^2\,   (spacetime interval),

where:

c is the speed of light,
Δt and Δr denote differences of the time and space coordinates, respectively, between the events.

(Note that the choice of signs for s2 above follows the Landau-Lifshitz spacelike convention. Other treatments reverse the sign of s2.)

Space-time intervals may be classified into three distinct types based on whether the temporal separation (c2Δt2) or the spatial separation (Δr2) of the two events is greater.

Certain types of worldlines (called geodesics of the spacetime) are the shortest paths between any two events, with distance being defined in terms of spacetime intervals. The concept of geodesics becomes critical in general relativity, since geodesic motion may be thought of as “pure motion” (inertial motion) in spacetime, that is, free from any external influences.

[edit] Time-like interval

\begin{align} \\   c^2\Delta t^2 &> \Delta r^2 \\             s^2 &> 0 \\ \end{align}

For two events separated by a time-like interval, enough time passes between them for there to be a cause-effect relationship between the two events. For a particle traveling at less than the speed of light, any two events which occur to or by the particle must be separated by a time-like interval. Event pairs with time-like separation define a positive squared spacetime interval (s2 > 0) and may be said to occur in each other’s future or past. There exists a reference frame such that the two events are observed to occur in the same spatial location, but there is no reference frame in which the two events can occur at the same time.
The measure of a time-like spacetime interval is described by the proper time:

 

a luminescence of string theory seems to imply the shadow zone of a limited spread on the values of intensity and the ability to cast its own shadow by a minimal involvance of the background complexity of the apparent impossibility of a light sourece to cast its own shadow…

 

 

\Delta\tau = \sqrt{\Delta t^2 - \frac{\Delta r^2}{c^2}}

 

In physics, spacetime (or space–time) is any mathematical model that combines space and time into a single continuum. Spacetime is usually interpreted with space being three-dimensional and time playing the role of a fourth dimension that is of a different sort than the spatial dimensions. According to certain Euclidean space perceptions, the universe has three dimensions of space and one dimension of time. By combining space and time into a single manifold, physicists have significantly simplified a large number of physical theories, as well as described in a more uniform way the workings of the universe at both the supergalactic and subatomic levels.

In classical mechanics, the use of Euclidean space instead of spacetime is appropriate, as time is treated as universal and constant, being independent of the state of motion of an observer. In relativistic contexts, however, time cannot be separated from the three dimensions of space, because the rate at which time passes depends on an object’s velocity relative to the speed of light and also on the strength of intense gravitational fields, which can slow the passage of time.

 

Spacetime entails a new concept of distance. Whereas distances in Euclidean spaces are entirely spatial and always positive, in special relativity, the concept of distance is quantified in terms of the space-time interval between two events, which occur in two locations at two times:

s^2 = c^2\Delta t^2 - \Delta r^2\,   (spacetime interval),

formats for luminescence seems to model the dimensional object in 3 dimensions by a shadow effect when a brighter luminescence and a lower intensity luminescence is involved…

 

where:

c is the speed of light,
Δt and Δr denote differences of the time and space coordinates, respectively, between the events.

(Note that the choice of signs for s2 above follows the Landau-Lifshitz spacelike convention. Other treatments reverse the sign of s2.)