Element Equations for 2-terminal elements f R (v, i , t ) 0 v i fC (v, q, t ) 0 q i q v f m ( , q, t ) 0 memristor inductor capacitor resistor f L ( , i, t ) 0 Ø Resistor: An element that has an algebraic equation between v and i. Inductor: An element that has an algebraic equation between Ø and i. Capacitor: An element that has an algebraic equation between v and q. Memristor: An element that has an algebraic equation between Ø and q. 2-Terminal Capacitors and Inductors linear and time-invariant Capacitor Inductor q (t ) C v(t ) (t ) L i (t ) dv(t ) i (t ) C dt di (t ) v(t ) L dt In order to model nonlinear and or time-varying capacitors and inductors (q ) and ( ) are used: t q(t ) ˆ i ( )d t [C] (t ) ˆ v( )d [Wb] L.O. Chua, C.A. Desoer, S.E. Kuh. “Linear and Nonlinear Circuits” Mc.Graw Hill, 1987, New York Capacitor f C ( q, v ) 0 charge-controlled v vˆ( q ) voltage-controlled q qˆ (v) If qˆ (v ) is differentiable dq d (qˆ (v)) dv ˆ i dt dv dt dv C (v) ˆ dqˆ (v) i C (v ) dv dt Inductor f L ( , i) 0 flux-controlled i iˆ( ) current-controlled ˆ(i ) ˆ If (i ) is differentiable d d (ˆ(i )) di ˆ v dt di dt dˆ(i ) di v L(i ) L(i ) ˆ di dt Capacitor Linear and time-invariant Inductor Nonlinear and time-invariant L.O. Chua, C.A. Desoer, S.E. Kuh. “Linear and Nonlinear Circuits” Mc.Graw Hill, 1987, New York Capacitor Linear and time-varying Inductor q(t ) C (t )v(t ) (t ) L(t )i(t ) dv(t ) dC (t ) i (t ) C (t ) v(t ) dt dt v(t ) L(t ) q(t ) (2 sin t )v(t ) C (t ) 2 sin t (t ) (2 sin t )i(t ) L(t ) 2 sin t di (t ) dv(t ) v ( t ) ( 2 sin t ) (cos t )i (t ) i (t ) (2 sin t ) (cos t )v(t ) dt dt L.O. Chua, C.A. Desoer, S.E. Kuh. “Linear and Nonlinear Circuits” Mc.Graw Hill, 1987, New York di (t ) dL(t ) i (t ) dt dt First-Order Linear Circuits RTH iC vC vTH EE+KVL dvC iC C CvC dt vC vTH vC RTH C RTH C GN vL iL iN di vL L L LiL dt i i iL L N GN L GN L EE+KCL State Equations, Kalman (1960) x ax bu, x(0) x0 L.O. Chua, C.A. Desoer, S.E. Kuh. “Linear and Nonlinear Circuits” Mc.Graw Hill, 1987, New York Solutions of First-Order Differential Equations x ax dx ax dt x(0) x0 x (t ) C t dx adt x 0 ln x(t) - lnC = at x(t) ln = at C x(t ) Ceat t x (0) Cea 0 x(t ) eat x0 x ax bu x (0) x0 Assumption: x(t ) S (t )e at d ( S (t )e at ) a ( S (t )e at ) bu(t) dt dS(t) at at aS (t )e e aS (t )e at bu(t) dt t dS(t) at e bu(t) dt t dS(t) e at bu(t) dt Assumption: x(t ) S (t )e S (t ) e a bu()d S (0) 0 t x (t ) S (0)e at e a ( t ) bu ( ) d , at t 0 0 0 x (0) S (0)e a 0 e a ( t ) bu ( ) d , 0 t x (t ) e at x (0) e a ( t ) bu ( ) d 0 t x (t ) e x (0) e at a ( t ) bu ( ) d 0 zero-input response zero-state response t Solutions of First-Order Differential Equations x ax bu x (0) x0 t x (t ) e at x (0) e a ( t ) bu ( ) d 0 zero-input response zero-state response If a<0 then z.i. response and probably some part of the z.s. Response converge to zero as time goes to infinity. This part of the solution is called transient solution (geçici çözüm). The remaining part in z.s. solution (which does not converge to zero) is called the steady state solution t (kalıcı çözüm). x (t ) e at x (0) e a ( t ) bu ( ) d 0 transient solution steady solution First-Order Linear Circuits x ax bu, x(0) x0 t x(t ) e x(0) e a ( t )bu ( )d at 0 RTH vC t vC 0 e VTH t RTH C vTH vTH e vC t vC 0 vTH e RTH iC vC vTH t RTH C t RTH C transient solution dvC CvC dt vC vTH vC = + RTH C RTH C iC C L.O. Chua, C.A. Desoer, S.E. Kuh. “Linear and Nonlinear Circuits” Mc.Graw Hill, 1987, New York vTH steady solution An Example Find the transient dynamic behaviour of the voltage buffer! L.O. Chua, C.A. Desoer, S.E. Kuh. “Linear and Nonlinear Circuits” Mc.Graw Hill, 1987, New York An Example L.O. Chua, C.A. Desoer, S.E. Kuh. “Linear and Nonlinear Circuits” Mc.Graw Hill, 1987, New York
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