terça-feira, 25 de março de 2014



Analytical Geometry Graceli oscillatory . And Graceli calculation .


Graceli coordinate system n- dimensional . And Graceli mathematical relativity .


Analytical Geometry Graceli oscillatory .

Geometry Graceli coordinate movements of oscillatory waves to variations of moves to east, west , north, south divided by time .


0 point onwards has a movement to n , s , l , or the east, west , north, south divided by time .

With a variation oscillatory movement to either side with respect to time in each coordinate x and y .

With this we have forms that vary the oscillation range of the coordinates in the form of waves in all directions . That is, a four-dimensional coordinate system Graceli .

Where frequency range and are divided by time.

 These oscillations can follow the formulas :
 

Logx /x n...


Logx /x n... * [[log h/h n… * logj /j n...]n...].


Logx /x n... * [[log h/h n… * logj /j n...]n...]*[*P +R[AF], *P –R,0.


Logx /x n... * [[log h/h n… * logj /j n...]n...]*[*P +R[AF], *P –R,0 [AF]+ [osc k.
                            
freq osc. F / c/t].


or differential or integral functions , such as:


                                            + Lat, long , altu + movement.





functions with extensions [ extension ] points for distances d .

areas for [ d ] multiplied by the distance exponent 2 for spheres by pi ..

For volumes multiplied by the exponent 3 .


P = extensions = distance forming in points differential and integral function.

F [ x ] = functions.
or

 integral.


  
                                                     * P . of points, lines , curves , bells , wave forms .

                    
        

     2


                                                                       2
                                                                 * P [ in areas ] .



             
                      
        


 
                                                                   3
                                                               * P [ volumes to ] .



For differential .

F [x] * p . of points, lines , curves , bells , wave forms .

             2
F [x] * p [ in areas ] .




             
               3
F [ x ] * p [ for volumes ] .





Graceli coordinate system.

 Dimensional .

Latitude , longitude , height .
Latitude , longitude and movement .



Four-dimensional .
Latitude , longitude , height and movement / t . [ k range , and frequency f waves ] .

Five dimensions .

Latitude , longitude , height , movement / T , flows .

Six dimensions.

Latitude , longitude , height , movement / t , and transcendental flows [ / + R / -R , / 0 ] .



Mathematical relativity Graceli by graceli coordinates.

Change of position , location, forms , movements , precession , oscillation, variable flows of shapes , growth and decrescimentos parts , like a balloon that inflates and part wilt deformations . Rotation, translation and displacement, and oscillatory precession.

Horseshoes , cups, boxes , objects , and quadrimensionais dimensional images .


Variations in relation to positions of observers . Where one observes a form of an object . Where a person behind a glass see the bottom of the glass and the mouth of the front glass.


With this addition to the object , curves , straight lines , we deformations and displacements . And parts that disappear when multiplied by 0 [ zero ] , making a geometric system of transcendental parts .
 And also with forms in relation to positions of observers .


Graceli geometry of shapes , areas and volumes of flows and oscillatory movements .

For oscillatory areas.

For forms of extensions .

Example .


Area : A = 4πrs2 * logx / x ... n * [ [ log h / hn logj ... * / j ... n ] ... n ] * [ * P + R [ AF ] * P - value , 0 [ AF ] + [ k osc . , fo F / c / t ] * [ d ] .

                                                                                                    
Area : A = 4πrs2 * logx / x ... n * [ [ log h / hn logj ... * / j ... n ] ... n ] * [ * P + R [ AF ] * P - value , 0 [ AF ] + [ k osc . , fo F / c / t ] .


                             





for oscillatory volumes.
                                                                                                                                                      
Página 3  * Logx / x ... n * [ [ log h / hn logj ... * / j ... n ] ... n ] * [ * P + R [ AF ] , P * -R , 0 [ AF ] + [ k osc . , fo F / c / t ] .

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