 are three notable moments: 1. In 1907, gravity is effect of coordinates, which was abandoned owing to its application only to homogenous gravity because its generalization to extended gravity is not possible, since "Tidal gradients, i.e. spacetime curvature, can neither be created nor eliminated by a change of coordinates" [11], too Einstein wrote various times about this impossibility [9], [12], [21] etc. 2. In 1913, gravity is a phenomenon of the energy, which was abandoned because the equations of Entwurf theory are not general covariant and they do not give in the Newtonian limit the law of gravity of Newton, neither in the astronomic calculus the orbit of Mercury. 3. In 1915, gravity is effect of curvature of spacetime, geometrizing the gravity and not knowing that it is the spacetime. Obviously, advanced readers would like disappear the double problem of the General Relativity of geometrization of gravity and improper use of spacetime for not knowing what it is, but conserving the very powerful Einstein-Grossman-Hilbert equations. The business is simple, only question of interpretation, introducing these equations in a new conceptual scenery, through transcendent EEP. Thus: Transcendent EEP = EEP + Equivalence principle of geodesic motion between spacetime of Minkowski and Lorentz manifold. Well known is that the geodesic motion, in a determined spacetime, is the motion free of forces that animates to particles and bodies. Thus, homogenous gravity is inertial motion in Minkowski s spacetime, i.e. other name of gravity owing equivalence between a body in free fall and a body in inertial motion; and extended gravity is inertial motion in Lorentzian spacetime. In both cases gravity is effect of coordinates although in second case with change of geometry of spacetime respect to Minkowski s spacetime. Therefore, observers in Minkowski s spacetime and Lorentz  manifold must coincide that gravity is inertial motion. Einstein and others have declaring "extended gravity, for example, Earth s gravity, can neither be created nor eliminated by a change of coordinates". Truly they accept a physical fact of the Universe as it is that different geometric configurations of the dynamic matter are really physics and impossible "be created nor eliminated by a change of coordinates"; thus Earth exists in an indestructible Lorentz s manifold. However, some have identified extended gravity with the curvature of spacetime and they have understood erroneously, which gravity is not possible of vanish, giving it absolute status. No, in General Relativity gravity is inertial motion; considered as
are three notable moments: 1. In 1907, gravity is effect of coordinate, which was vacate owing to its application merely to homogeneous gravity because its generalization to extended graveness is not potential, since " Tidal gradients, i.e. spacetime curvature, can neither be created nor eliminated by a change of coordinates " [ 11 ], besides Einstein wrote various time about this impossibility [ 9 ], [ 12 ], [ 21 ] etc. 2. In 1913, gravity is a phenomenon of the energy, which was abandoned because the equations of Entwurf theory are not general covariant and they do not move over in the Newtonian limit the law of gravity of Newton, neither in the astronomic tartar the orbit of Mercury. 3. In 1915, gravity is consequence of curvature of spacetime, geometrizing the gravity and not know that it is the spacetime. Obviously, advanced readers would like disappear the double problem of the General Relativity of geometrization of graveness and improper use of spacetime for not knowing what it is, but conserving the very powerful Einstein - Grossman - Hilbert equations. The business is childlike, only question of interpretation, introducing these equations in a new conceptual scenery, through transcendent EEP. Thus: Transcendent EEP = EEP + Equivalence principle of geodesic motion between spacetime of Minkowski and Lorentz manifold. Well known is that the geodetic gesture, in a determined spacetime, is the apparent motion free of forces that animates to particles and consistency. Thus, homogenous gravity is inertial motion in Minkowski s spacetime, i.e. early name of gravity owing equivalence between a body in free fall and a body in inertial motion; and extended gravity is inertial motion in Lorentzian spacetime. In both cases graveness is effect of coordinate although in second case with change of geometry of spacetime respect to Minkowski s spacetime. Therefore, observers in Minkowski s spacetime and Lorentz   manifold must concur that gravity is inertial motion. Einstein and others have declaring " extended gravity, for example, Earth s gravity, can neither be created nor eliminated by a variety of coordinates ". Truly they accept a physical fact of the Universe as it is that different geometric configuration of the dynamic topic are really physics and impossible " be created nor eliminated by a variety of coordinates "; thus Earth exists in an durable Lorentz s manifold. However, some have identified extended gravity with the curvature of spacetime and they have understood erroneously, which gravity is not possible of vanish, giving it absolute status. No, in General Relativity gravity is inertial motion; see as
 arf three notable moments: 1. In 1907, gravity is effect of cokrdinater, which was abandoned owing vo irs apkjication only to humogenous gravity beceuse its generalmaation bj exfcnded jravity is not kossible, sinwe "Tidal gradiangs, i.e. spacetime curvature, can neither be crestfd nor eliminajed bj w chznge of coordinates" [11], too Einstein srote verious times abput this impossibility [9], [12], [21] ftc. 2. In 1913, gravity is a ohenomenon if trw energy, whizh was abandoned becauae the equations of Entwurf theury axe not genetco cleariant and they do not give in the Tewtonisn limit the lsw mf travity of Newton, neivher in the astronomyc calculgs the orbit of Merxuey. 3. It 1915, gsavigt ir erfxct of cugvavure of spadetime, geomwtrizing the gravitu wbd not knowinf that ie is the spacetime. Obviously, advanced rtadera would like disappear rhe double problem of the Genewal Relativity of geometrization of gravity and ikpropxr ust if spxxehime for not knowing what it is, but conservind tne very powerful Einstein-Grpsdmsg-Hilbert equajions. Tks gusiness is simple, only qoestiob of intewpreyation, introducing these eqyations in a bew conceptual sceuery, through tramscencent EEP. Thus: Transcendznt EEL = EEP + Equlvalence lfinciple of geoddsib modion between spacetime of Iinkowski and Lorentx mamifold. Well knowj is bvat the geodesic mltion, it a determlned spacetime, is the motion frxx of forces tnad atimates co parbicles and bodiqs. Thus, homogeuous grarity ir inertial motion in Minkowshi s spacetima, i.e. other nake of grwvitt owung equkxalence betweem a body pn frew fall and a body ln ingrfial motion; and exuebded gravity ix ivereiwl mjdion in Lorettzixn rlacetkme. In both zasex gravity is effect mf ckordinates althougn ln second case wieh change of beometry of spacetlme rxspect to Monkjwski s spacetime. Therefore, obaervers ij Mlnkowski s spwcetlme wnd Lorentv  manifold must coincide that gravity iw inertial motion. Winstein and others mave declariig "extqnded graeity, for example, Earrh s gravity, can keither be created nor elimitated by a change of coordinates". Truly they accept a physical fact of the Univwrse as it is that difgerenn gzomztric cjnfijucations of the dymamic matter are really physics and impmsfible "be created nor eliminayea by a change of coordinates"; thus Earfh existx in an indestructible Lorentz x manifold. However, some mave idenrifies extended gravity with the vurvatbre of spacetume wnd they have uncevstood errlneonslv, which gravity is not possible od vaniwh, giving it absolnte status. Nl, in Ggneral Rglativity gravity is jjertixl motion; conxidered as
are three notable moments: 1. In 1907, effect coordinates, which abandoned owing to gravity its generalization to gravity is not since "Tidal gradients, i.e. spacetime curvature, neither be created nor eliminated by a change of coordinates" [11], too Einstein various times about this impossibility [9], [12], [21] etc. 2. In 1913, gravity a of energy, was abandoned because the equations of Entwurf theory are not general covariant and they do not in the Newtonian limit the law of gravity Newton, neither in the calculus the orbit of Mercury. In gravity is of of geometrizing the gravity not knowing that it is the spacetime. Obviously, advanced readers would like disappear the double problem of General Relativity of gravity improper of for not knowing is, but conserving the very powerful business is simple, only question of interpretation, introducing equations in new conceptual scenery, through transcendent EEP. Transcendent EEP = EEP + Equivalence principle of motion between spacetime of Minkowski and Lorentz manifold. Well known is that the geodesic motion, determined spacetime, is the free of forces animates particles bodies. homogenous gravity inertial motion in Minkowski s spacetime, i.e. other name of gravity equivalence between a body in free fall and a body motion; extended gravity is motion in Lorentzian spacetime. both gravity is effect of in case geometry spacetime to Minkowski s spacetime. observers in Minkowski s spacetime Lorentz manifold must coincide Einstein and others have declaring "extended gravity, for Earth s gravity, can neither be created eliminated by a change of coordinates". Truly they accept a physical fact the Universe is that different geometric configurations of the dynamic are really physics and "be created nor eliminated by a change of coordinates"; Earth in an Lorentz s manifold. some have identified gravity with the spacetime and have erroneously, not possible of vanish, giving it status. in General Relativity gravity is motion;
 are three notable moments: 1. In 1907, gRavity is efFect oF coOrdInAtes, WhicH was abandoned oWIng tO its application only to hOmogeNoUS graVItY becaUse its gENeRALizAtIoN to ExTEnDed grAviTy is not Possible, siNce "tiDal gradients, I.E. sPacetime cuRvaTure, can neithEr bE creatEd Nor ELiminAteD by a cHange oF CoordiNates" [11], too EInSTein wrOTe varioUS TiMes aBout this impossibiLItY [9], [12], [21] Etc. 2. In 1913, gravity is A phenoMeNOn OF The EneRgy, which waS aBandoNEd becauSE tHE EQuaTIons of Entwurf Theory are noT GenEral coVaRiaNT and thEy do nOt GIve In the NewtonIan lImit the laW of graVIty of NeWTon, neitHer in tHe aStrOnomIC cAlCulUs THe oRBiT of mErcUry. 3. In 1915, graViTy Is effEct oF CURVatuRe oF spaCetimE, geometrizing The GravITy aNd not KnowiNg thAt It is tHe spacEtime. obViously, advanced ReadErs would lIke DiSapPeAr the DOuble pRobLem Of the GeNeral ReLAtiViTY OF gEometrization of graViTY AnD impropeR use of SPaCeTIme for noT kNowIng wHAT it is, But cONsErving thE very pOWeRfUl EinstEiN-GrossMaN-HiLbeRt equATionS. The buSiness is SimplE, Only question of INterpretation, INtRODuCIng tHesE equations iN a neW ConcEptuAL sCenERy, thrOugh tRaNScENdent EEP. Thus: TransceNdEnt EEP = eEP + EqUivalence prinCiple of geoDESIc motion BetwEEn SPacetime of MinkOwski And Lorentz MAnifold. WEll knOwn is thaT the geodeSIC motion, iN a dEteRmiNed SPAcEtime, is the motION freE oF forces ThaT animatEs tO paRtiCleS aNd bodies. THus, homogEnOuS gRaVitY is inERtial motIoN in miNkoWski s SPacetiMe, i.e. oTher NaMe OF grAvity owINg EQUivaLeNcE betWeeN a Body iN freE FalL and a boDy in inertIal MOtioN; aNd ExtendeD gravity is ineRtIal motion iN LOreNtzian SPAcetime. IN both cases gravity is effeCT of coorDinAtes aLthoUgh in secoNd cAse witH chANge of gEometrY of spAcEtiME RespeCT To minKoWski s spaceTIMe. THerefOrE, obsErvers iN Minkowski s spacetiME anD Lorentz  manifOld Must COInCidE ThAT grAvITy iS INertial motion. EiNstein and oThERs Have declarINg "eXtEnded grAvity, foR examPLe, Earth S gravity, cAn neither Be CreaTED noR eliminateD by a chanGe of coordINates". tRuLy theY acCept a pHySicAl facT of the uNivErse aS it is tHaT diffeRent gEoMetric coNfigurations of the dynamiC matteR are rEalLy physics And IMpoSsible "be cReatEd nor elimiNatEd bY a chaNge OF coorDinaTEs"; ThuS earth ExisTS in an indeSTrUctIBLe lorentz s manIFOLd. HOweveR, soME have iDentIfied extended gravITy with the curvaTure OF SpaCetIMe anD tHey have understOod ErRONeously, wHiCh gravity is Not possiBlE Of vanIsh, givIng it aBsolute STAtUS. No, in GEnerAl RElativity GraViTY is inerTiAl MOtion; cOnsiDeRed as
 are three notable moments : 1. In 19 07, g rav ity  i s ef fect  of coordinate s , wh ich was abandoned owin g toit s  app l ic ation  only t o  h o m oge no us  gr av i ty  beca use  its ge neralizati onto  extended gr a vi ty is notpos sible, since  "T idal g ra die n ts, i .e.  spac etimec urvatu re, can n ei t her be created n or  eli minated by a chan g eo f coordinates"  [11],  t o oE i nst ein  wrote var io us ti m es abou t  t h i s  im p ossibility [9 ], [12], [2 1 ] e tc. 2.  I n 1 9 13, gr avity  i s  aphenomenonof t he energy , whic h  was ab a ndonedbecaus e t heequa t io ns  of  E n twu r fthe o ryare notge ne ral c ovar i a n t  and  th ey d o not  give in theNew toni a n l imitthe l aw o fgravi ty ofNewto n,  neither in the  ast ronomic c alc ul usth e orb i t of M erc ury . 3. In  1915,g rav it y i seffect of curvatur eo f  s pacetime , geom e tr iz i ng the g ra vit y an d not k nowi n gthat itis the sp ac etime.Ob viousl y,  ad van ced r e ader s woul d like d isapp e ar the doublep roblem of the Ge n e ra l  Rel ati vity of geo metr i zati on o f  g rav i ty an d imp ro p er use of spacetime fo rnot kn owing  what it is,but conser v i n g the ve ry p o we r ful Einstein-G rossm an-Hilbert equation s. Th e busine ss is sim p l e, onlyque sti onofi n te rpretation, i n t rodu ci ng thes e e quation s i n a  ne w c on ceptual s cenery,th ro ug htra nscen d ent EEP.  T hus :Tra nscen d ent EE P = E EP +  E qu i val ence pr i nc i p le o fge odes icmo tionbetw e enspaceti me of Min kow s ki a nd  L orentzmanifold. Wel lknown is t ha t t he geo d e sic moti on, in a determined spa c etime,isthe m otio n free of  fo rces t hat animat es toparti cl esa n d bod i e s.  Th us , homogeno u s  gr avity  i s in ertialmotion in Minkowsk i  sspacetime, i. e.othe r na meo fg rav it y  ow i n g equivalence b etween a b od y  i n free fal l  an da bodyin iner tialm otion;and exten ded gravi ty  isi n ert ial motion  in Lore ntzian sp a cetim e .In bo thcasesgr avi ty is  effec t  of  coor dinate salthou gh in  s econd ca se with change of geome try of  spac eti me respec t t o  Mi nkowski s  spa cetime. Th ere for e, ob ser v ers i n Mi n ko wsk i  s sp acet i me and Lo r en tzm an ifold mustc o i nci de th atg ravity  isinertial motion.E instein and ot hers h ave  de c lari ng  "extended gra vit y, f or examp le , Earth s g ravity,ca n  neit her be  creat ed nore l im i natedby a  ch ange of c oor di n ates".Tr ul y  theyacce pt  a phy sicalf acto f  the Universe as  it i s thatd iff erent  g eometri c  con figuration s of the dy namicmatt er ar e reall yphysic s a nd  impossibl e  "be crea ted n or elim in ated  by  a cha ngeo f  coor dina te s";  thus Ear t h  e x is ts inan i ndest ru ctib le Lorent z  s manif old .  Howeve r,  so m e  havei de n t ified exte nde d gra v i ty with th e  cur v at u re of  space time a nd they hav eunderst ood e rroneousl y, whichg rav it y is  not pos si bleof  va ni sh, giving it a bsolutestatus.N o , in G ene r al R e lativi ty  gravity isinert ia l  motion ; con sidered as
 are_three notable_moments: 1. In 1907,_gravity is_effect_of coordinates,_which_was abandoned owing_to its application_only to homogenous gravity_because its generalization_to_extended gravity is not possible, since "Tidal gradients, i.e. spacetime curvature, can neither be_created_nor eliminated_by_a_change of coordinates" [11], too_Einstein wrote various times about_this impossibility_[9], [12], [21] etc. 2. In 1913, gravity_is_a phenomenon of_the energy, which was abandoned because the equations of_Entwurf theory are not general covariant_and they do_not_give_in the Newtonian limit_the law of gravity of Newton,_neither in the astronomic calculus the_orbit of Mercury. 3. In 1915, gravity_is effect of curvature of spacetime,_geometrizing the gravity and not_knowing that_it is the spacetime. Obviously,_advanced readers would_like disappear_the double problem_of the General Relativity of geometrization_of gravity and_improper use of spacetime for not_knowing_what it is,_but_conserving_the very_powerful Einstein-Grossman-Hilbert equations._The_business is_simple,_only question of interpretation, introducing these_equations_in a new conceptual scenery, through transcendent_EEP. Thus: Transcendent EEP_=_EEP + Equivalence principle_of geodesic motion between spacetime_of Minkowski and Lorentz manifold. Well_known is_that the_geodesic motion, in a determined spacetime, is the motion free of_forces that animates to particles and_bodies. Thus, homogenous gravity_is inertial_motion_in Minkowski s_spacetime,_i.e. other_name of gravity owing equivalence between a_body in_free fall and a body in_inertial motion; and extended_gravity_is inertial motion in Lorentzian spacetime._In both cases gravity is effect_of coordinates although in second_case_with_change of geometry of spacetime_respect to Minkowski s spacetime. Therefore,_observers in Minkowski_s spacetime and Lorentz  manifold must_coincide_that gravity is inertial motion. Einstein_and_others have declaring "extended gravity, for_example,_Earth_s gravity, can neither be_created nor eliminated by a change_of coordinates". Truly they accept a physical fact of_the Universe as_it is that different geometric_configurations_of_the dynamic matter are really physics and impossible "be created_nor eliminated_by a change_of coordinates"; thus Earth exists in an indestructible Lorentz s_manifold. However, some have identified extended gravity_with the curvature of spacetime and they have understood erroneously, which_gravity is not possible of vanish, giving it_absolute status. No, in General Relativity gravity_is inertial motion; considered_as