Principles of Electricity and Electromagnetism |
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Page 503
... component of the plate poten- Eod.c.cutoff grid potential = Eb / μP ip Eo Lic KEC Eg -ec Simplified approximate dynamic characteristic ip - Speg - Sp ( eg + ep / μp ) Saturation region ec 20 ic angle -πως ὁ π / + 20 π 5π / 32K 7π / 3 ...
... component of the plate poten- Eod.c.cutoff grid potential = Eb / μP ip Eo Lic KEC Eg -ec Simplified approximate dynamic characteristic ip - Speg - Sp ( eg + ep / μp ) Saturation region ec 20 ic angle -πως ὁ π / + 20 π 5π / 32K 7π / 3 ...
Page 535
... component of H is given by the function o ( t − 2 ) , g ' C the equation becomes = Kof ' where the primes indicate ... component along the y axis with a corresponding magnetic component in the direction of -x . As these components ...
... component of H is given by the function o ( t − 2 ) , g ' C the equation becomes = Kof ' where the primes indicate ... component along the y axis with a corresponding magnetic component in the direction of -x . As these components ...
Page 540
... component , this component must vanish for n ' and n " , or ' = " 0. Thus all the ray vectors lie in the plane perpendicular to the surface that contains the incident ray . For equality of the r component of n and n ' it is necessary ...
... component , this component must vanish for n ' and n " , or ' = " 0. Thus all the ray vectors lie in the plane perpendicular to the surface that contains the incident ray . For equality of the r component of n and n ' it is necessary ...
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alternating current alternating-current ampere amplifier amplitude angle angular anode antenna applied approximately armature assumed atom axis calculated capacity cathode cell characteristic charge circuit coefficient coil component condenser conducting conductor considered constant curl current flowing curve deflection density determined dielectric dielectric constant direct-current direction dynamic resistance effective electric field electromagnetic electromotive force electrons electrostatic element energy equal equation flux force frequency function galvanometer grad harmonic hence impedance induction integral ions known length linear load magnetic field magnetic moment magnitude maximum measured meter negative obtained ohms oscillations output parallel phase plane plate current positive potential difference potentiometer quantities R₁ radiation radius ratio reactance region represents resistance resonant rotation scalar shown in Fig solution surface temperature terminals theorem torque transconductance triode tube unit vacuum tube vector velocity voltage volts wave wire written zero