© 1957 by Oxford University Press
THE PERIODIC SOLUTIONS OF THE DIFFERENTIAL EQUATION OF A RESISTANCE-CAPACITANCE OSCILLATOR
( Northampton Polytechnic London )
A third-order differential equation is considered of a form which arises in con-nexion with a resistance-capacity oscillator, the equation being normalized to the form
![]() |
and µ are small parameters which in the main part of the discussion are re-lated by
= µ2, and g(D) is a particular polynomial operator of the third degree.
The procedure previously applied to a second-order equation with unsymmetrical non-linear damping, is usexd to obtain the periodic solutions having the period of the forcing term when
is near to 1, i.e. for the case of fundamental resonance. It is shown that the resonance curves are of the same form as those obtained for the second-order equation and that the stability of the periodic solutions is determined by variational equations which are likewise identical in form to those previously obtained for the second-order equation.
