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Vendredi 23 janvier 2009. Periodic Solution Of Maxwell Propagation-TV Antenna. The equation of propagation of Potential V of Electromagnetic field of MAXWELL PROPAGATION or COULUMBIAN POTENTIAL by this PDE. Vxx -(epsi*µ)Vtt =0 with no charge in espace. I set a Fourrier Serial Periodic Solution. V(x,t)=Ao A(x)sinwt B(x)Coswt=A(x)Sin(wt -kx). The ODE-PDE equations from are. Axx (k 2)A =0. 2k(dA/dx) (epsi*µ)(W 2)A =0. Solution Amplitude A(x)=B1coskx B2sinkx. If x,y,z K=(k1,k2,k3). Orsay,lyon 1,manheim?

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Blog-BookScience-NDao | blog-bookscience-ndao.blogspot.com Reviews
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Vendredi 23 janvier 2009. Periodic Solution Of Maxwell Propagation-TV Antenna. The equation of propagation of Potential V of Electromagnetic field of MAXWELL PROPAGATION or COULUMBIAN POTENTIAL by this PDE. Vxx -(epsi*µ)Vtt =0 with no charge in espace. I set a Fourrier Serial Periodic Solution. V(x,t)=Ao A(x)sinwt B(x)Coswt=A(x)Sin(wt -kx). The ODE-PDE equations from are. Axx (k 2)A =0. 2k(dA/dx) (epsi*µ)(W 2)A =0. Solution Amplitude A(x)=B1coskx B2sinkx. If x,y,z K=(k1,k2,k3). Orsay,lyon 1,manheim?
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Blog-BookScience-NDao | blog-bookscience-ndao.blogspot.com Reviews

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Vendredi 23 janvier 2009. Periodic Solution Of Maxwell Propagation-TV Antenna. The equation of propagation of Potential V of Electromagnetic field of MAXWELL PROPAGATION or COULUMBIAN POTENTIAL by this PDE. Vxx -(epsi*µ)Vtt =0 with no charge in espace. I set a Fourrier Serial Periodic Solution. V(x,t)=Ao A(x)sinwt B(x)Coswt=A(x)Sin(wt -kx). The ODE-PDE equations from are. Axx (k 2)A =0. 2k(dA/dx) (epsi*µ)(W 2)A =0. Solution Amplitude A(x)=B1coskx B2sinkx. If x,y,z K=(k1,k2,k3). Orsay,lyon 1,manheim?

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blog-bookscience-ndao.blogspot.com blog-bookscience-ndao.blogspot.com
1

Blog-BookScience-NDao: WHY BRAIN THEORY AND NOT CARDIAC

http://blog-bookscience-ndao.blogspot.com/2008/11/why-brain-theory-and-not-cardiac.html

Lundi 3 novembre 2008. WHY BRAIN THEORY AND NOT CARDIAC. 1-Brain is composed SPINO (Function 1),CORTEX(Function 2) etc. Xn 1=F(Xn,K) -E. X state K parameters E treshold. If F sup E Xn 1=1 If F inf E Xn 1=0. From state Xo The Strategical Control is to set The FIXED POINT for recognizing signal. 4-Control Function with LJAPUNOV STRATEGY. Inscription à : Publier les commentaires (Atom). WHY BRAIN THEORY AND NOT CARDIAC. Foundation Of Cardiac Theory-3. Afficher mon profil complet.

2

Blog-BookScience-NDao: novembre 2008

http://blog-bookscience-ndao.blogspot.com/2008_11_01_archive.html

Lundi 3 novembre 2008. WHY BRAIN THEORY AND NOT CARDIAC. 1-Brain is composed SPINO (Function 1),CORTEX(Function 2) etc. Xn 1=F(Xn,K) -E. X state K parameters E treshold. If F sup E Xn 1=1 If F inf E Xn 1=0. From state Xo The Strategical Control is to set The FIXED POINT for recognizing signal. 4-Control Function with LJAPUNOV STRATEGY. MODEL CARDIOYTHMOR(WAIT VIDEO IN CONSTRUCTION WOOD ART ENGINERING). M l 2 Z"= -M l g sinZ K Xs l 2 Cos 2 Z -l W 2 R 2 *1/e sin Wt. MXs" = -KXs W 2 R 2 1/e Sin Wt -l Z' 2.

3

Blog-BookScience-NDao: octobre 2008

http://blog-bookscience-ndao.blogspot.com/2008_10_01_archive.html

Vendredi 24 octobre 2008. FOUNDATION OF CARDIAC THEORY-2. 1-Ressources:also Leo Chua(chao),Bernard Picinbono(signal france),Jean Louis Lions(PDE france) ,IEEE CSS,IEEE CAS. DX/dt=F(X,K) dX/dt=F(X,K) Io. Control Cardiac frequency F Io=0. Control cardiac frequency F with electrical stimulation Io. Cardiac Frequency F control of Pacemaker. Data Holter analyze and modeling,F frequency,P pressure,R respiratory,M mass ,l lenght patient,T temperature ,d debt. F=G(P,R,d,T,M,T). F(n 1)=G(F(n=,P,R,d,T,M,l). 5-exis...

4

Blog-BookScience-NDao: décembre 2008

http://blog-bookscience-ndao.blogspot.com/2008_12_01_archive.html

Mercredi 3 décembre 2008. Confrontation Automatic and Book Of Abraham and Marsden. TAUPE:in 1977 Exodus demonstration,line war music system,in 1978 Taupe change with advanced acoustic rock reggae with Album Babylon by Bus-afraid to Taupe and not afraid to people- -11 is bas? BONUS:bonus to team Marianty Ionel for number of functions. Functions Automatic:impedance system R,L,C- variables V and I- function H=(1/2)lI 2 (1/2)CV 2 (1/2)RI 2- If exist system where H=constant? END OF COURSE THE PROF LEAVES AMPHI.

5

Blog-BookScience-NDao: Confrontation Propagation VI1 and Maxwel Potential Propagation

http://blog-bookscience-ndao.blogspot.com/2009/01/confrontation-propagation-vi1-and.html

Jeudi 22 janvier 2009. Confrontation Propagation VI1 and Maxwel Potential Propagation. You Know university Orsay ,you know university lyon,standfaod manheim and OBAMA come in train at wash. Equation Propagation Maxwell potential. Vxx -(epsi*µ)Vtt= -d/epsi d charge. See my potential propagation VI1 on my google books author:dit papa lamine ndao. Or www.heart-simulator.com. Propagation VI1 has potential V and electrical field E=grad V the question if Potential VI1 verify equation of maxwell.

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Vendredi 23 janvier 2009. Periodic Solution Of Maxwell Propagation-TV Antenna. The equation of propagation of Potential V of Electromagnetic field of MAXWELL PROPAGATION or COULUMBIAN POTENTIAL by this PDE. Vxx -(epsi*µ)Vtt =0 with no charge in espace. I set a Fourrier Serial Periodic Solution. V(x,t)=Ao A(x)sinwt B(x)Coswt=A(x)Sin(wt -kx). The ODE-PDE equations from are. Axx (k 2)A =0. 2k(dA/dx) (epsi*µ)(W 2)A =0. Solution Amplitude A(x)=B1coskx B2sinkx. If x,y,z K=(k1,k2,k3). Orsay,lyon 1,manheim?

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