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THE BASIC EQUATION
Although the equations describing the operation of the vacuum tube
are derived in many text books, the derivation is repeated here so that
a form more suitable for use with G-Curves can be shown. With these
equations and the G-Curves, the performance of a vacuum tube in its
circuit may be calculated at any point within the operating area.The total instantaneous value of the plate current in a tube is a
function of the tube parameters and can be expressed as:ib = f ( eb, ec1, ec2, . . . )
The unspecified parameters are functions of such things as filament
voltage, tube geometry, temperature, and many other factors. Holding
the unspecified parameters constant, a series expansion of the above
equation in terms of partial derivatives of ‘f ‘ can be written. These par-
tial derivatives are the commonly used conductance parameters in the
following equation:ip = ( gm1* eg1 ) + ( gm2* eg2 ) + . . . + ( gp* ep ) (3)
where the g's are the values of the partial derivatives. This is the basic
equation from which equations for use with the G-Curve technique are
derived. For triodes, it reduces to:ip = ( gm* eg ) + ( gp* ep ) (4)
RESISTANCE-COUPLED AMPLIFIER EQUATIONS
The triode R-C amplifier circuit is shown in Fig. 2-1. For the present
analysis Rk1 may be assumed equal to zero, or a short circuit. Because
supply voltage Ebb is constant, plate voltage change ep is equal but
opposite in polarity to the output voltage change, i.e. :ep = -eL = -ip* RL
Using this to eliminate ip from Equation 4 gives:
ep = ( -gm* RL* eg ) / [ 1 + ( gp* RL )]
and the equation for amplification follows immediately:
K = ep / eg = ( -gm* RL ) / [1 + ( gp* RL )] (5)
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Copyright 2008 for Phyllis K. Pullen, M.D.,
by Robert J. Legg