User:Balaji.sivaraj

Electflux mathtunning

That havebeen there to exact age past info of the charge attract over observation matalic crytal reflection refraction with variance of cycliccharge coils to create the flux. Between electrons charge and flux to connect probagation using gravity and froce calculate and apply the mathematics

ectronic Circuits

Different Frequency 30 hz to 3000 Ghz - Frequency in the form of Loop and Spiral Uplink Downlink Bandwidth Travel free space propagation Propagation Mathematics Vector Algebra Divergence & Strokes Cartesian Curvilinear cylindrical and spherical Laplacian Curls and Curls on curls. Electrical Fields Ohms Law Joules Law Amperes Law Newtons Force Field infinite Lines Field Finite Lines Field Metals Field of Multiple Point of the Charge. Field Metal of Symmetry. Magnetic Field Faradays Law of electromagnetic induction Induced EMF Intensity E in terms of the vector potential A Moving conductor in a time independent Magnetic Field Flux Lines Ampere law flux Tuning Magnetic Flux and Magnetic flux density B Biot savarts law Magnetic Field of a linear conductor of infinite Length. Magnetic Field of a circular current Carrying Loop Magnetic Field of a Solenoid Magnetic Flux Density inside an infinitely long cylinder containing a uniform current density Magatential vector potential Line Integral of the Vector potential a over a closed curve. Magnetic Field adjacent to a thin long sheet of current Force two thin long parallel sheets of current.

EMF Displacement Current Maxwell�s Equation Plane wave propagation Using Alpha beta gamma waves Dielectric and conductor binomials Dielectric and conductors Small element and vector - Az cos theta Az Sin Theta Small element E R 2sin 2 Small element E theta Small element H Flux sin theta - U Im dl sino/4 pie caswt1 d/dr (-w/c) + U im dl cos wt1 cos w t1 (-sino) Far Field Near Field Wave Equation in terms of electromagnetic potential and their solution Volt charge and density Radiation pattern current element and dipole s1 r s2 V =1/4 Pie e0 jw(q / s1 -q/s2) S1 = r + l/2cos theta S2= r - l/2cos theta {1/r+c/jwr2} Volts Er Electrical Radiation = - Jw Ar � dv/dr E Theta = - Jwa theta - 1/r dV/D Theta H flux Near Field Far Field Quasi Stationary region Im lcos theta /2 Pie E theta [ 1/r3] E theta 1/r3 H flux 1/r2 Radiation from infinttesimal dipole or an infinitesimal oscillating current az U e power -Jbr Im dl /4 pier d/dr d/d theta az cos theta az sin theta d/d theta � sin theta d/dr (e power -Jbr) (-Jb) Er n di electric E0 n di electric H flux n di electric Far field Near Field P = E X H P= 1/2 ar e theta H flux � a theta Er H flux Pr Az [ Binomials- E x az [Binomials )