ࡱ> `!$ڪNE @ gxcdd``N` 2 ĜL0##0KQ* W A?d 3zjx|K2B* Rj :@u!f0100X@V ȝATNA 27)?$WQS!>obRi3vq%0b-ϫD7! ~ Ay8gN7Xf(Kb2G(./rLp`a 0c]  3AlM̆oq]_l99sp1d?R@aP[& ;zT)zBGX{oitgUyQG}z 3/;Y7n)럍QWq aZ~c~v-k7{U;!o!IcCl :8 {2-L 8 MkR㉗LD>^vi[x*Tk# X^cÔG.v&${EV]Pz,@?H`!\8>zo.O}p D } h*xcdd``Vbd``baV d,FYzP1n:&&6! KA?H1:ʎ ㆪaM,,He` @201W&00p_QaŪXkhZ P.P16J`roR%y d^Hfnj_jBP~nb@.Nǘ̼T,& \ 1dfȄL.hxs``b#RpeqIj.C \E.B ~`sr`!{gͺiK0 excdd``>$d@9`,&FF(`TIe A?d fĒʂT @_L ĺEܘA,a kL̀&!rof01d++&1X|#+|-MlW6AVJN(7HEr~LąE$qH83O*2E='b:+XE>L wW&CF+zG!f$Kp~|!>TSX!|, g Ev#]Lpw5Іۻ (?U^U ķ XxG<% *G ^F ) n``;F&&\{ {:@ĞB a hd0`!.Qb03$:B` 4excdd``^$d@9`,&FF(`TI%WRcgbR v/ fĒʂT @_L ĺER@,a KL *'031d++&1X|#+|-$V1lWsHf%'_R_c:83O*G=O`ce)27)?a)B8$qMʄM̄C*%,aQP{zqІ,T*oV y,CBO8|jKa;?fK֤-*7;0l O \Ы,xh5w차g}O&Z-xCZGYqߑt#llU]_`AWq  U.jV\}\R1ǴQ6[wz&/m=M^._eK׳kt]h:, .b~hܒZxZzkdv'UunnQХ חH~IŸ.$@Bpk_oѩq4 ιGs,vC1{O} 4j%㍽`+0_'F0=RпhA I0'`!;> o1e`T xڥTk@&&6MTx"A[JAR""-*nZšЋQxԣzA?cwQ* Rj`hep3NB<ϵ4% ol;q!Tޫ9* bB!z@G9¤`Cؗj$xK~ߤ+ eq<2p6\tMM7Amp] ?K[*č_ {Bw;N?]L;u3[FyL{;r>ЉOyU lOhml1|uQLg?AiC燽so,+xO z}{ #_Vtaq?Ʊ`!}1{nPkE%8@ e fdKxcdd``a 2 ĜL0##0KQ* Wä&d3H1)fY;@<6@=P5< %! 8 :@u!f010m` wfjQ9B&&ܤu > 1X +|-?ɞb&#.#[, eUh^Hfnj_jBP~nbn4j&7S!61Z2O`r`YRfQ|O 631-ǖ#4.v0oA+KRs~ePdk)Yݗ`S%l`!]zjBɴk  H+xcdd``fcd``baV d,FYzP1n:X,56~) @ /*k UXRY`7S?&lebabMa`HRx*İb@`# 5w3U RXlbb@>@lblm&4ܸa 4=xĤ\Y\˰d.P"CXhy.Ā+f~`e`![Edj,{hkDL )xcdd``Vbd``baV d,FYzP1n:&lB@?b u  UXRY7S?&lebabMa`&%ÊU7r1,j]b mĕޤJt@$ȼbr<12@]Ps701YřyXL٥\ 1b_l3Y.+2!, \84=X|Ĥ\Y\ː2C 1,|r`!}!fu{UiP((^@  KxuJA\NX-D/؋AL*+Xu! $6| _0S߳{w=w5K_؉(zB9(0mOY{|&CuMSS-vZ c4FF[8[:iV כpmni1uof|`yW#3{Do6m?~bp6u*EufZr<F'tj /91֙t$:N8X?JX?FDLΝ$T9xXϥKKu|zOb ѻ: ֥He.}TA{%ƺP#ma]Kh>z5 6~u=muI<7a7za@ z'xX例Ka^m֍Z>a}_1"1awZeVa=TyXa=\u**k'te c|dNGPcBMlka=951}'z T5XO34]S3;Y2ivM9ƽnX5K),|]3 j*2k5Իk&tyʌ.7lsLJ.6{8+t9LK កrsV(~MBIڌ@Ϗ$h*:4uIz$}HyDQ AE̓ ef#s"P%$jFk~ӽ|kX9m{%PeϥFup%!" fr3ނ)ڱnQv(ڱމq)( _(#䒌~QG>RR`\ ՠg"if@"i%HZz.R$]UHZ.ĬtdzM1c滫6`4Q"j++Eݫu >,:$X_efO+> M(1֝@3@ 4Ei TEשudIE'A׉ ㊮]'AKu(怪YY XP5S6T;MU'1ַ4uhPv:Rb4#@TETkXkaT}}h; _~ lm2+N1A$E$콊(K.PNE;AAqoe)qk. ͊7?i{w1h_ݻi)uoik.3h[7țg~ޠ{{=Sb={u+wu)w vU &(']@ΊY;t+%;a?տ_~ +!ߗVn"g<βYU7񴺗v<|u(_g8(_>&zi&<]1 ?~*~TegFqfw }g5N}pg꾔q̑ cffG$<LLMI fcbt>8;kp/{D]54wSwJ;}4ݼ?oݙy&I()=.='%# G0| 8wXNo-\Uh<" =v] 8~~?s_2~q՚'3=OXW J ,cɯcq7Y5"-cTBNfB`~NQzdxU{8j:6+0&sD0ݮֆ>cOKᖴY@8gSaNNA^ 9+Dfjc}^iuKFV]TF[mlAN)i 8JZ#Zd9Y)#3Ƥefo[i'抽.{hMW~[Ջ?gg\`!8[ cƊ̕8i1xڝOA߼-BmEpP(G$4b1KlIkŋ %IB8! 뼙)rqI}f[qkbG!cQ0 C=d(שu  IAHbp8h<wFL [`:xe=1 )J.VZвHRigϢZ&22"Ųj.W7E+*SWRPNB׼~ÛX{ru{ _ܒ,/wMYs/P?xhRQEZՆg4'֠jX#g3g%5|[rORQg}Qe.O&ɷ8^PD]5(vBVV۫x?]`x\`!yr6lW8  eGx}Q1K@}%M,X"QMwA`;:X%bB!8 #:tؽ"JqQ0~w ;{{w6`oC.˦1"! $(s\q7ͫg#dT|Ϩeڣ=vr:>0@oIwer =K}eti9?S3od,8΁ے3л\[\>vP^ε2Y6Yu^?Hºv!(S($ji4~q?p =(ұ:n;F,ԯ {E\AΘ顔C'v-{nՙu\[.כ\~r5k#Pcbt~j7&_"~ ybevvcxmV|s.Jax"k4}VcK8 LGfg y{_0{?sRԹTDuRoCFzUR\tQ|KQ]JUbM:C|>WkyR >+%4or~\A`!hMrp$8vH #%2xڝR1K@~Ih .`"V@VW'gAp BWHݥT]z;{2б1 @u6MDy& IB+)'EIF4j Մ9&d\?s(4DYJd1q4MhU>dp"X|)ۻN+EV)썏Jg!{2ihʼ/+y b<ɥ~(fD>bcv%P/,%gw._8*䖌Ûs>0q[S|?3G̏jn"exuVyߓQ^{a_M|17gw)T !X_A!.;UBz7 S(#S`!j>i}4>s N=X hxcdd``g 2 ĜL0##0KQ* W􀙁]RcgbR v6@=P5< %!@5 @_L ĺEz@,a kȝATNA $37X/\!(?71aŪXkyO7LF]F\= a~?|g=`{+a&nf<1 Ma`x*_{Z 2?ጰ7#n{16^;d~S8l+) Zq;121)W2xePdk-υÀ2vm&(  , 3 Rwnanie Equation.30,Microsoft Equation 3.0-Rwnanie Equation.30,Microsoft Equation 3.01Rwnanie Equation.30,Microsoft Equation 3.0BRwnanie Equation.30,Microsoft Equation 3.0 Rwnanie Equation.30,Microsoft Equation 3.0!Rwnanie Equation.30,Microsoft Equation 3.0"Rwnanie Equation.30,Microsoft Equation 3.0&Rwnanie Equation.30,Microsoft Equation 3.0'Rwnanie Equation.30,Microsoft Equation 3.0(Rwnanie Equation.30,Microsoft Equation 3.0)Rwnanie Equation.30,Microsoft Equation 3.0C)Rwnanie Equation.30,Microsoft Equation 3.0/Rwnanie Equation.30,Microsoft Equation 3.0/ 0DArialNew X@,o0,0$DSymbolew X@,o0,0$ DTimes New Roman,o0,0$@ . @n?" dd@  @@`` 0! 9   #  @K]#4 7!)#"$%&2'*+ ,"o2$$ڪNE 2$Ɗ\01:#(-}Q2$8>zo.O}p dR2${gͺiK02$.Qb03$:2$LC_Kx2$> o1eC] $2$1{nPkE% 2$zjBɴke%2$Edj,{hkc2$!fu{UiP((2$!?2Vb=GL=I r2$[ cƊ̕@> 2$7kZ!972Gv~"2$5m0. {Jjc! 8#2$r6lW&2$j?%@ӝ 8v'2$33-)sϭxa)2$hMrp$8v#+$2$j>i}4>s N=, 0AA`3@ 3N)Z ʚ;Y@8ʚ;g4YdYdD0ppp@ <4ddddp~00@ 80___PPT10 pp?  %! Euclidean Reality Theory  Spectacular Conclusions and New ProblemsDD(C  Witold Nawrot+Singularities and their new interpretation.,,(+  &New rules of composition of velocities '&((& &New rules of composition of velocities''(& &New rules of composition of velocities''(& &The new transformation of coordinates ''($  &The new transformation of coordinates ''($ .3We have now the new transformation of coordinates 44(@$  The Lorentz Transformation$ +The Lorentz Transformation$   The Lorentz Transformation$ #The Lorentz Transformation$ ! #The Lorentz Transformation is wrong$$(H " #The Lorentz Transformation is wrong$$(H $$The Lorentz Transformation is wrotng%%(H &The recession of galaxies6 0The recession of galaxies6 '$The recession of galaxies SIMPLE????&%( (6  (Dark side of the UniverseH *Problems of the FER model ,Conclusions from the new model(  9Acceleration of bodies to the speed interpreted as the speed of light is possible. This effect can be an experimental test for correctness of the model. The Lorentz Transformation, although mathematically correct, cannot be applied to a description of any physical problem because of its non-physical character. :Z:E F    7 #   -Conclusions from the new model(  MThe recession of galaxies can be described very simply as only an effect of an observation, and not as actual acceleration. In the FER, without the observer we are only able to describe a class of points or trajectories of a body. Determining a single point or trajectory from the class is possible only if the observer is chosen. NZN          F  ` 33` Sf3f` 33g` f` www3PP` ZXdbmo` \ғ3y`Ӣ` 3f3ff` 3f3FKf` hk]wwwfܹ` ff>>\`Y{ff` R>&- {p_/̴>?" dd@,|?" dd@   " @ ` n?" dd@   @@``PR    @ ` ` p>> tl(    6t  `}  PKliknij, aby edytowa styl wzorca tytuBu) )  0  `  Kliknij, aby edytowa style wzorca tekstu Drugi poziom Trzeci poziom Czwarty poziom Pity poziom*   a  0荏 ^ `  >*  0 ^   @*  0t ^ `  @*H  0޽h ? 3380___PPT10.@v}I  Projekt domy[lny}  $(  r  S <>  r  S > `    H  0޽h ? 33___PPT10i.0I+D=' = @B +  o(   7  <Y The new approach to the issue of physical reality, consisting in the description of space with the help of hypothetical Euclidean dimensions which cannot be directly observed, provides many new conclusions and indicates some new problems. Some of the conclusions are contradictory with predictions of the RT; however, neither these nor the other conclusions have been experimentally verified yet.  : " N  2 D       $ H  0޽h ? 33___PPT10i. `Z+D=' = @B + L0   ` G (  r  s *C"? `  s *"`x  c $ `}   9  <  ds2=dt2-(dx2+dy2+dz2)            9  <쌉E T  dt2=ds2+(dx2+dy2+dz2)            0  <x   0ds=0 while dt,dx,dy,dz`"0V    3  "    0 $The Lorentzian space-time (observed)% 2%H     08 xX The singularities are possible 2H Z   <U  w  0dt`"0 while ds,dx,dy,dz`"0 3& 3 3     "    08 hX  The FER reality (objective) 23$     0   "The singularities are not possible# 2#3H v   04׉  According to the FER model the singularities are not the real limitations of physical phenomena but only the limitations of the observation.X 29C        H  0޽h ? 33___PPT10i.G+D=' = @B +# L0 "p'8n(  x  c $TÉ `}   ^  6((^  6v  s ,A 3??"?K 3^  677j  S A  -??"? t  -^  6++j  S A  1??"?   1^  6((j  S A  B??"?  B@B  C >p @B  C >~ ~ FB  S >p E @B  C >a @B  C >Q Q T 2   c C0ENGFH\#J Q `TjT`T E0`TjT`T E0 `T E0 x 2 ! s BOC1ENGj+HS$JQ `T`TOC1`T`TOC1OC1q2 " c CmENGHH JQ `T`T`TktPm`T`T`TktPm`TktPmJ # 3 ĉ Xa 6  $ 3 U Xb 6  % 3 UQJ-V Xg 6  & 3 U ~   Dx F  ' 3 U"    Dt F  ( 3 TU ~   Dx F  ) 3 LU   Dt F  * 3 U  !trajectory of the observed body 6"  6 * + 3 |U 4u* $trajectory of the observer in rest F%"  Z  , 3 |yU4  $trajectory of the observer in motion%%Z LB - c $D  a LB .@ c $D 4  /0 NA C? ?S" Q : C U 1 <\U @ 5SRTX 2 0]M  4 <UYy 5FERX 5 0ov%RB 6 s *D>X 7 0>( 8 <(U! 5FERH  0޽h ??0 ! " 33___PPT10i.0+D=' = @B +5 L0 4,(    c `U0e0e #" 0e `}  U   JA "? UH  0޽h ? 33___PPT10i.@;+D=' = @B + L0 $(  $ $ c  (U0e0e #" 0e `}  U $ $ 00Ufk  Experimental test: Products of decay of particles can depend from the energy of the particle With a certain, strictly defined energy, one of the products of the decay should be a particle moving with the speed of light( 2] ~     > $ <5U  T The new rules of composition of velocities should be a result of a certain new transformation of velocities different from the Lorentz transformation       H $ 0޽h ? 33___PPT10i.@;+D=' = @B +  ,(  ,r , S KU `}  U l , c $X?C"?4Y:B , 3 Ԕ:B , 3 >  x :B , 3 Ԕ:B  , 3 Ԕxx :B  , 3 >2  , c C0ENGFH\#J Q `TjT`T E0`TjT`T E0 `T E0  2  , s BOC1ENGj+HS$JQ `T`TOC1`T`TOC1OC1)2  , c CmENGHH JQ `T`T`TktPm`T`T`TktPm`TktPmP , 3 SUxP Xa 6  , 3 XUwz Xb 6  , 3 ;U  Xg 6  , 3 @)UPq 3  Dx F  , 3 dhU A   Dt F  , 3 mUf 8I  Dx F  , 3 U  A u  Dt F  , 3 Up-. !trajectory of the observed body 6"  6 * , 3 @U   $trajectory of the observer in rest F%"  Z  , 3 U5U $trajectory of the observer in motion%%Z j , S A  ??"?   j , S A !??"? Gx  !j , S A "??"? Gw  "LB , c $D  LB ,@ c $DF (H , 0޽h ??0 , , , 33___PPT10i.)+D=' = @B +#  :2 "4(  4r  4 s *C"?px 4 0C"?p x 4 c $U `}  U j 4 S A &??"?] = &j 4 S A '??"?P 0 'j 4 S A (??"?p|  (j 4 S A )??"? '  )^2 !4 6Ԕc f  "4 0 a The new transformation of coordinates does not predict the length s contractionP(2P   H 4 0޽h ? 33___PPT10i.)+D=' = @B +    (  x  c $&f     6T  ,$0 `However&  (  6 V & ,$0 NIn the FER we can also derive the classical Lorentz transformation& .FF(   H  0޽h ? 33  ___PPT10 .)+M i5DT ' = @B D ' = @BA?%,( < +O%,( < +DJ' =%(D' =%(D' =A@BB-BB0B@ A%(D' =1:Bvisible*o3>+B#style.visibility<* %(D' =-g6B fade*<3<* D%' =+4 8?pCBB+#ppt_w*sin(2.5*pi*$)CB?B*Y3>B ppt_w<* D' =+4 8?\CB#ppt_hBCB#ppt_hB*Y3>B ppt_h<* D' =%(D' =%(DD' =A@BBBB0B%(D' =1:Bvisible*o3>+B#style.visibility<* %(D' =-s6Bcircle(in)*<3<* +p+0+  ++0+  +  8(  8r 8 S 'gP   @ p8 C X?P RB v8 s *DL= TXB w8 0DԔ3: RB x8 s *DE3 XB y8 0DԔ:6 E |8 0h_ lF  6x  2 8 0{ b  3x 2 8 08H G / 6t  2 8 0pC G * 3t 22 8 C"ENGΌJ"Q `TLwL`T"`TLwL`T""L`T""\T2 8 B#ENGYBH{7[IJQ k+V`T#JM[Tk+V`T#JM[T#JM[T^  8 0sZ 4j 2 8 0w  4j 22 8 CjmENGf4HEhAJ Q Q`TuM#jmQ`TuM#jm M#jm  R2 8 s *;;2 8 B_TCUTENG8H.XJQ `T`T_TUT`T`T_TUT_TUT? < R2 8 s * Po  8 02%  Observers xt and x t are moving with velocity V=sinj relative to each other&M 24  8 0   x-axis of observer xt is perpendicular to t axis of observer s x t frame.K 2J   8 0   x -axis of observer x t is perpendicular to t axis of observer s xt frame.K 2J  d 8 0tnq1 VFrames of the xt and x t observers in FER:,(2,l H 8 0޽h ?O@8888 33___PPT10i.d+D=' = @B +  `11"(  x  c $0.nV     PA ?"?v}   PA?"?m   PA?"?   @  C X?tN.B   S\ S4B  # o.B 4B  # o.\ S.B   o6  6 .B   SB .B   oS 6 .2    d b  B  6  6  B  S_ 6 .2   /<w.2    Y .2   /m w.2   X H .2   /w  3 j s  @x   3 i  @t }  3 0=  ` ;t }  3 y    ;x .2    S .2   4m |2  s B!ENGe7CHZI JQ U`T!M^TU`T!M^T !M^T L 2  S C ENG,4J Q Q`TuM`T Q`TuM`T M`T oM2  B1TC"ENGTHQ5I1TJQ `TY"`TY"1TY"1T  2  B{C]TENGҐHI{J]TQ rr{]T{]Tg    3 xU2 gs  EA & }  3 lf  ;B } ! 3   ;P } " 3 ز^ ;O  # 3 tX @t  $ 3 8] c  Vt 2  % 3 -  Vx 2  & 3 P H  Ix * ' 3 ~  >j  ( 3 (W~ >j  ) 3 t$+ t  Rj 0  * 3   +  Rj 0 } + 3   ;t  , 3  T  Nx *RB - s *D>`) RB . s *D>`8 RB / s *D>. e @ 0 C X?kt 1 0k fCoordinates of point P in frames xt and x t in FER4(24l  H  0޽h ?O@ 33___PPT10i.d+D=' = @B +  4?dG(  d@ 0d C X?]x d c $,;{   @ d C X?tG.B d  S\ S4B d # o.B 4B  d # o.\ S.B  d  o6  6 .B  d  SB .B  d  oS 6 .2  d   d b  B d 6  6  B d S_ 6 .2 d  /<w.2 d   Y .2 d  /m w.2 d  X H .2 d  /w d 3 lj s  @x  d 3 Xi  @t } d 3 =  ` ;t } d 3 y    ;x .2 d   S .2 d  4m |2 d s B!ENGe7CHZI JQ U`T!M^TU`T!M^T !M^T L 2 d S C ENG,4J Q Q`TuM`T Q`TuM`T M`T oM2 d B1TC"ENGTHQ5I1TJQ `TY"`TY"1TY"1T  2 d B{C]TENGҐHI{J]TQ rr{]T{]Tg   d 3 @2 gs  EA & }  d 3  f  ;B } !d 3   ;P } "d 3 x^ ;O  #d 3 tX Nt * $d 3 ] c  Vt 2  %d 3 `$-  Vx 2 } &d 3 0*P H  ;x  'd 3 P/~  >j  (d 3 `3W~ >j  )d 3 7$+ t  Rj 0  *d 3 =  +  Rj 0  +d 3 4B  It * ,d 3 G T  @x  9d BK:  X &&   < 8d 3 A?m^ :d 6< 7d 3 A?v  ;d BhQm   (10) N & &     < 6d 3 A? ) RB S TRB =d s *D>L^LRB >d s *D>Le Tt ?d 0dZk fCoordinates of point P in frames xt and x t in FER4(24l  H d 0޽h ?O@dddd 33___PPT10i.d+D=' = @B +  /'6|(  |x | c $v `}   ^ -| 6u 4| 0{{9 AWe have two transformations, derived in FER, excluding each otherB 2B $ 5| 0 w_ (One of the transformations must be wrong() 2 P 6| 0@ _G  Which of them and why???(2 6H | 0޽h ? 33___PPT10i.d+D=' = @B +E  \TJh(  hr h s *X?C"?+  FB  h S >O  Q r h S d}   4B h # i FB h S >ll :B  h 3 oli 4B  h # oP l ! 4B  h # o P 42  h # '  x 42 h #  42 h # L h S \h  @t  h S Th   ;t  h S (h^ jf  ;x 42 h #  R< 42 h #  2 h c C ENG,4J Q Q`TuM`T Q`TuM`T M`T jt2 h B1TC"ENGTHQ5I1TJQ `TY"`TY"1TY"1T; >  h S h  ;B  h S hO r  ;P  h S Thz ;O  h S  hF  @t  h S MhQ   ;x  h S h >j  h S hi /  >j  h S 0h'@ B C ;t  h C .U L  eTrajectory of point P  :2  h 3 jN F2 !h S  "h <  0While defining the coordinates xt of point P we are assuming that trajectory of point P is perpendicular to the space axis of the coordinate system xt. (we remember that in FER the space-axis of an observer - now placed in xt frame -must be perpendicular to the trajectory of observed body  here the trajectory of point P)JFp 8                H h 0޽h ??0hh h 33___PPT10i..@^+D=' = @B +   \p(  px p c $ `}   F ?p S X?L 4B @p # S :B Ap 3 oyS FB Bp S >dv | FB Cp S >y 42 Dp # ! q .B Ep  I  I .B Fp   I 42 Gp # 42 Hp # ( bh 42 Ip # L & 42 Jp # Y Kp S Kp@ C  @x  Lp S Lp  @t  Mp S Mp  ;t 2 Np c C ENG,4J Q Q`TuM`T Q`TuM`T M`T wv2 Op B1TC"ENGTHQ5I1TJQ `TY"`TY"1TY"1T4 =  Pp S DPp* H  ;A  Qp S TQp >  ;P  Rp S Rp ;O  Sp S Sp  @t  Tp S 8TpD  @t  Up S PUp7| + @x  Vp S  Vp >j  Wp S ԭWpb $  >j  Xp S Xp  @x  Yp S C"? @ etrajectory of point P  2 Zp CGnENGtҝHAZI`TJmNQ  ͢>Gn@5 ͢>Gn@5`TmN>Gn@5`TmNU  F2 [p S  -p=  \p <̺  FWhile defining the coordinates x t of point P we are assuming that trajectory of point P is perpendicular to the space axis of the coordinate system x t . (we remember that in FER the space-axis of an observer - now placed in x t frame - must be perpendicular to the trajectory of observed body  here the trajectory of point P)`Lr S[,   :            H p 0޽h ??0NpOp Zp 33___PPT10i..@^+D=' = @B +     "t> (  tx t c $  `    !t < t The Lorentz Transformation does not allow to describe the coordinates of any real body, but it describes only the coordinates of a point being the intersection of the trajectories of different bodies. From mathematical point of view, the Lorentz Transfor-mation is correct in every single point of the space. From physical point of view, the Lorentz Transformation is useless because it does not describe any real body The mistake consists in fact that in FER we can not determine the space axis without knowing trajectory of the observed body. We derived the Lorentz transformation in FER applying the rule valid for SRT only, where determinig of coordinates of a body, without knowing its world line, was possible.  6=4 j n+   =   ! $           +               H t 0޽h ? 33___PPT10i..@^+D=' = @B +N  e]((  r  S 5u   F  S X?ZFB  S o rF :B  3 o > FB  S o  FB  S o # FB  S o E .2    $ .2    * d   S  +  Dr1 $  S 0? oV "  Dr2 $2  s C=ENG:J=Q `Tz/:`T=`Tz/:`T==/:`T==l    S n P  Jj1 &  S . 9n  Jj2 &2  s CENGJQ j`T*iQ`Tj`T*iQ`TQ`T    S <   =t   S B  0axis of time and the trajectory of an observer H  .2   =  w ~  6C"?  0H  >Big Bang 2 Xr  03jJB t82  CtoENGyH] $J=Q m`T-r98Dtom`T-r98Dto=r98Dto=s p R2 ! s * L- 2 " C$fENGHXTJ(Q Ƚ`TffR$fȽ`TffR$f(fR$f(  ! R2 # s *~ M  & 0Dc8 aThe galaxies created during Big Bang are moving, in FER, along trajectories having common origin.b 2b b M ' 0R"p Observer which is moving along black trajectory observes, in point t, galaxies which are moving along trajectories green and red.( 2B>    ( 0H Rc &Directions in FER, perceived by the observer as the space-dimensions, are different for each observed galaxy, and are perpendicular to the trajectories of the observed galaxies  they are equal to r1 and r2.B 2   H  0޽h ?O@ " 33___PPT10i.2w+D=' = @B +   !1(  x  c $CR `}  R @  C X? % @B  C oWk? o 4B  # os 7s @B  C os @B  C oZ s @B  C o> n  2   2  Q # ]   C GR $  Dr1 $  C $MR  hO  Dr2 $2  c C=ENG:J=Q `Tz/:`T=`Tz/:`T==/:`T==7 s   C QR9  Jj1 &  C VR2gn  Jj2 &2  c CENGJQ j`T*iQ`Tj`T*iQ`TQ`T o   C |Rn   =t   C 8R[    0axis of time and the trajectory of an observer H  X  C R? C ntrajectory of an observed galaxy 1 and its t1  axis $8, Z X  C (R##N ntrajectory of an observed galaxy 2 and its t2  axis $8, Z  2   B~  6C"?j  S A ??"?/ ; |   0RN  >Big Bang 2 Xr  03jJ mx 2  CtoENGyH] $J=Q m`T-r98Dtom`T-r98Dto=r98Dto=>i^R2  s *E2  C$fENGHXTJ(Q Ƚ`TffR$fȽ`TffR$f(fR$f( R2  s *IF z  0|RJj5 jt  age of the Universe  our point on the trajectory6 26t    0R:J+Z >H  Hubble s constant and H=1/t 2 >  ! 0R9 X  TObserved velocities of galaxies are equal to sinus of angle between the trajectoriesU 2U0   B H  0޽h ?O@  33___PPT10i.2w+D=' = @B +  0!(  x  c $RP&f   R ~  6C"?  0DR7J| ( 2 ! 0t_R'  qThe increase of velocity of galaxies is only an effect of the way in which we perform the observations. It has nothing to do with any actual acceleration.8(2g 3  z  H  0޽h ? 33___PPT10i.2w+D=' = @B +   7 / @ (  r  S xR `}  R F  S X?:  3 H :B  3 o 0x 4B  # o 4B  # .c- 4B  # ZF 7 4B  # 6y, 4B  # ZU E r  08RԔ Y  j Big Bang D   C R/  Dark side of the Universe  this half of the Uni-verse can not be seen from Earth  TR   C R0  zBoundary of the observed Universe is perpendicular to the Earth s trajectory PP    C R) 7C Trajectory of the Earth 6 %  C  R; E i 7Fluctuations of the boundary of the observed Universe 88l   C  (RF   -Fluctuations of the trajectory of the Earth  .+Z  .B   [Qv .B @   .B     .B     .B    o E .B @   * E H  0޽h ? 33___PPT10i.6K+D=' = @B +   "P~(  r  S kR `}  R 4B  # Ԕ` ` FB  S ԔO.B   u u ` :2  3 K; FB  S ԔKd FB  S ԔTa 4 .B   r$u e .B   p ` 42  # NR42  # pL 42  # ^   S xqRP  ET &   S 8wR?  Trajectory of the observer .  6   |G, WWTrajectory of body ATimes New Roman8  ~Y;. WWTrajectory of body CTimes New Roman3   |d, WWTrajectory of body BTimes New Romanv  S PįF4$!?O/᎜$wIb8GcQAWI(AVDBZ+%;lvx\is;͛f}̛}' ]@*],4H@4R1Ke)H:]a]Bis3|+{_հ )AX^PN:% vac^YE}f3ZXw{a '8q]ڪ'R!2!_ҶC!g/K15D o@6rn)^}}H<ˁ 0 A}QzzVQo}]}*⿏eġe>*d/|fZgj<u )ojl?{ֲyq/k'Uk8 <:jX=k ` k5@Z)kڸT<҈G#uݟ# B@r|86_{kO^Y`Mo9vm \!u(C|V i⏖_!|}mWqWX-_{j|n~P4'BЇD~7& ܲکXbwݽ{\g¢B8yw> F#!'22 }WkݓD$5S"ƓV6N;V٦z [@pc68$nu(f*{+e"^+ Z碠,5bAkcf>QLvNvu'LNrhP>ľ[_AUثUW#Uv951=&{HS}R_Y@ 8wc]1#O p쏶zk6 7 !:Bv{6Z(й=;1NNӐ:gѐcțm n;Ѓ&z`r tJP$!8(IR1Qa5ݨtMD״qG3rz}fw>˙/y&mVziz[Aʺ$P#?;uq0}Pٹ?ЌFm~7|T|$pjGRpuEo+z)x2Ǽv)+2rH4$)hHM"' *g9yWQ?.3OYY}X3YiǏ#>Vgo|<_׫+'2w~mofNgwpߝ͢7سۯ c0{m>D. }8I %35۰`"+YAU$w#sWew8PgjvU98aV|֦B6ODg"Kn-꘡iC\ZD[}9Hvۣy< jod<^pA(9> cdi=ƣʭU<}ZLz#>i|(#Co(mGW7 0c!=v_0Zw`Ho@#G} (jmEeؙ,Bg"_Ý' aٗoϮ6ԗ.ž^K9hoJHmjJeh?_?brpgR>ct;d@%e,&aPFk}9^PIp |d'xr}2fHYyی԰_'⑤lgSg;5Jq˨t_NO3`M/k/eIE6lnIWifcb!|L |d׼t\MYsOzfk]6Zf1qŃ&t+'`ᗯIJ~o+wf? e1j5hyCzGJx`xrUkxXAOA~3[PEBM#^<`bTɃŴa -6!<lyR%`a6L@"vQ3%܎k  &11xP ?0f9,I+o?~#9;܌QX߽2(Rk]{xa_R翐Qxo׀F)82_Gb+5R!tN}>nwTkvqyvs#{i/io q" uـtO}kt}|aDADMΦCg:Z!`3D!ܵni11&aͲԯ jt |,XCmYg&G ij#IL"_Q Xz`!e,ZG.J.Rɩ=*@;7SK䴡t*n`0dwFeZ;{woLZY)b1Wˬ_#޷e7$p3rUD1}5lPq1d)X%Iɹ/ApA9Ǯ0̄*qkh7g = әt2uE" kS36جJ _]rVޛvYk DE+)ʂ!8Eb[Qd>lzaT91&gL%e,Hv?i ssxXOA~3[]XD!V"^8`0Z# <ie -4Dɻ4xфC<)Mٺ4l~Λ~ٮ{ip$=Pmic>C-}~H/ @8d#@UW_s}l;6cscerF VO+d|s=? | ̩uIՏc$ߪ;;s$,c^DVMS E%OI#_ѿQ0uoE yAD`|٧a kҖ*ԟT&D f;dzr؍''wT@eϪ.}A }4C/}闖% G{4z~^1# atsH*{}y{Hsh\ԇL47k1Qc/ׂQy9Z?NUAne7f֖23O>MEؿ1/&b)%(DTG72Xo7K1f٤d=~YM#Rlh)IH>@}`q_'g[!߃iq-#.o4u{ǧ+Wz5M96݈tւUdw̰e$dE<8?9Mc _\'>3P&P}xhQM)=d*O+6=^PBcѴtFv,n!aH_9%$Yf|ow:EŢyb9{[5'ɟJng[91݌G^yA-XXO}?{oq_yws"szNw'&=xX=LTA=(p NB)8AEba3;=<3RCІBŊX ΐ;gvȻH0]ٟٙ=>~hX^%|1$ -5-I 8VFUb&D)M4fb}A r6< Y}xlv\\gTS!LUY#o2? .~S ~=~ߌu:A*_p}ͷ^ z@yB(>30q<6Fy(;YAƂ J&bqPs ЈԄt餞CZWq txXSW;%/ksgc?_<{._x)ʉ]?ߘ|rCA3ݲ")Ga0ozzm."g[CzaD1M0&G3jNjh3_ĝB."?95rQED% ),mTJGq$CpMa51tT1;bb~X}WF,UDos>_>_zr a<31K[K0c3pVohlӃE` my)+`O"Nˮ]:%_4^zɢFHh>־?*56ʮ屔w/yG " ځim6Hss޸>P=ޢJ SVu]Ue7N2!@bg xp^RЀ3ÿ lHbP  LPÄ!1 4axĐ% y@( XyT0cH!-,\#3+SrRIp101"X}" 0e(#!dԧAP{=t 9e!~[a?h i-}pb/ d1;4̀-/x 8\\_V`gr Vp-,M,ca=c/ QL؋B25Xb fpN ]?L K)BcFFf..F06[b <MiRSf&g3b`)[t1 ?!hR&SR\ZTSd%( tJ8")8ve(,3RYz?*[2 j?Pk xp^RЀ3ÿ lHbP  LPÄ!1 4axĐ% y@( XyT0cH! ^#3HV30d'2b`bDD`;PtGC y'bOzC? rB x}Vh9020-2qRD?F`Ja悤=/$>%e*f&秕(0\\ KK2|GϘBb]Bk1 d(A1/IɌ\\LSKl^ 4yBM BM@\Բ ڴV28 C# I(dHIO ?X?(RYz;A2gR6KM xp^RЀ3ÿ lHbP  LPÄ!1 4axĐ% y@( XyT0cH!p7~w'A2ş!!$;#'\;H_h?+ ?k?H} i@c?^V,BFˁiTI{y_H}.KLUL./O+Q03`J+&d1p01Mĺ01KrqzqɌ\\LS+l&u _PS1gqS&fFd /,Ԥ ejҤ ?X?(RYz;AFQS eABxVkA3h6 "vQ/mr(BBO=I]7_b']AyxDn*eY.jcMRHaX62P`3VK@xE?/z._λgx=kɧ P=OPM4i(ԿXc&q'_ _림7R)"m\_~L~-ր Ǜe.0QUi1=#qЌBN=RVb tq5]iP4$O{}Q?Tc]VPs(~A@>NaBk,>ρ.օG^a߁3C(oϟ#0CRGU #eC&\Ԙ+pM 5Ǹ1"*ά+=o>PѫHeѪ?5؉˝.HECs806KJ##_kx%ܱQZ33F}bVWP:4j폢9͘PgJ暚ۍj.$jYWk>4^w͇A{)I*|);̋ xp^RЀ3ÿ lHbP  LPÄ!1 4axĐ% y@( XyT0cH!pw'A2ş!!$;#'\;H_h?+ ?k?H} i@c?^V,BFˁi-}`5A%J `bd0Rbj fg`  dBQ2CLfPDWBR`ؕ%Pʈ**6H@C~?ZxXkA;6mAT b(4BM6mZ(x$xzP(z _ ޤb{3qVRj2͛7}uo7< 2J*w>k(dL ʨW|]dt_AKݷ˘d SȘ%峆vho?κٿd} pos?^cwSv؎FD"MY-T VW OSфMU/{ _=4uQM(oM0^C{hdn2o4*g.Q7aDoaj!B$>L%@;£!u<0*@PDڏG0O3rL";6gsX5 jӇ zR~ Ңh ci!N{LD#'wxtu|/d]m>_~QnAW3hOf,Bo`1+|A`:>ӍnX-Bգ#7 !v%sVm 7}DdXILgġ%wnaB5rrMbKNnMfܞq5>yz+#TVrz"NP|M(T <r &0 ^!dgakG8G2^w3oa~i oNr^tiv.xy|zˏ+;&6<~!J`4Z`\A"]0Oh+'0 `h    $,DEuclidean Reality Theory Spectacular Conclusions and New ProblemsWitekWitek42Microsoft PowerPoint@@l?@`Eq@ qGGdg  *1  x--$ww--'@Arial-. -2 IEuclidean Reality Theory n  ."System-@Arial-.  2 .-@Arial-. 12 8Spectacular Conclusions and   .-@Arial-. 2 New Problems .-@Arial-. 2 Witold Nawrot    .-՜.+,0t     Pokaz na ekranieHANAKOM ArialSymbolTimes New RomanProjekt domylnyMicrosoft Equation 3.0DEuclidean Reality Theory Spectacular Conclusions and New ProblemsSlajd 2,Singularities and their new interpretation.'New rules of composition of velocities'New rules of composition of velocities'New rules of composition of velocities'The new transformation of coordinates 'The new transformation of coordinates 4We have now the new transformation of coordinates The Lorentz TransformationThe Lorentz TransformationThe Lorentz TransformationThe Lorentz Transformation$The Lorentz Transformation is wrong$The Lorentz Transformation is wrong%The Lorentz Transformation is wrotngThe recession of galaxiesThe recession of galaxies%The recession of galaxies SIMPLE????Dark side of the UniverseProblems of the FER modelConclusions from the new modelConclusions from the new model Uywane czcionkiSzablon projektuOsadzone serwery OLETytuy slajdw_ WitekWitek  !"#$%&'()*+,-./0123456789:;<=>?@ABCDEFGHIJKLMNOPQRSTUVWXYZ[\]^_`abcdefghijklmnopqrstuvwxyz{|}~Root EntrydO)Pictures.Current UserSummaryInformation(PowerPoint Document(1DocumentSummaryInformation8