Coordinate variables and n- dimensional Graceli .
Imagine a system of coordinates where the 0 point to the ends has a bend to one side following a fixed angle variation curve equal or variable angle , or waves that change according to time and the acceleration variable.
Since this bending may be coordinated at all .
With this system we have a coordinate variables . And that spatial coordinates Graceli are not two , but three . Where have the latitude , longitude and height .

Even with the coordinates which values ​​have stopped and the results are multipliable a 0 [ zero ] , forming voids between the shapes being the same or multipliable by 1 [ one] , where the values ​​do not change, forming a system in that interval equal , ie repeating points and do not vary , thus have a system where bends occur in a straight movements with system holes.

With this coordinate system variables , and even relating to observers at distant points , which increases when an object approaches the observer , and decreases as it moves away from the observer b .
Or even a curve for an observer is concave and the other is convex .

The function fx is a curve as the acceleration of the movement of each coordinate . Coupled with the rotation of coordinates.
Fx + [ mc + rc ] = [ a coordinated wave motion ] + [ rotation coordinate ] .

The Gaussian function for bell would become a variable function over time and with the acceleration of each coordinate .

That is, we no longer have the shape of a bell , nor the function of Fermat spiral one , becomes a variable manner.

Ie have variable functions with variable shapes .




Graceli function for sequential and statistical curve .

Graceli function to variations of shapes and movements
E (t + 2kπ ) = E (t ) + [ a2 ] . [V / T ] / [ ct ] + logx / x n ... + [ G s1 ] + [ * 0 * GS2 ] ... n * i / t or [ c / t ] ==
E (t + 2kπ ) = E (t ) + [ a2 ] . [V / T ] / [ ct ] + logx / x n ... + [ Y s1 * 0 ] + [ * YS2 ] ... n * i / t or [ c / t ] =
E (t + 2kπ ) = E (t ) + [ a2 ] . [V / T ] / [ ct ] + logx / x n ... + [ K s1 ] + [ * 0 * ks2 ] n ... * I / T or [ c / t ] ==
E (t + 2kπ ) = E (t ) + [ a2 ] . [V / T ] / [ ct ] + logx / x n ... + [ BS1 * 0 ] + [ * BS2 ] n ... * i / t or [ c / t ] =

Where we have an infinitesimal statistical

Graceli theory for non- uniform particles , energies , thermal and radioactive waves, fields and actions . And quantum entanglement .

Ie , the nature does not follow an egalitarian uniformity at all points within particles , fields , thermal and radioactive waves, etc. .

For infinitesimal curves in differential curves.

Graceli sequential function for all types of functions and curves .