Small Signal Model of the diode ο§ In certain applications a diode is biased to operate at a point on the forward i-v curve. ο§ A small AC signal is superimposed on the DC quantities. 1. Determine DC operating point (VD and ID), using one of the models discussed, 2. For small signal operation around the dc bias point: The diode is modeled by a resistance equal to the inverse of the slope of the tangent to the i-v curve at the bias point. Consider the circuit shown: ππ· π‘ = ππ· + ππ π‘ is the total voltage applied: ππ· ≡ the dc value ππ π‘ ≡ the small signal value ππ· π‘ = πΌπ· + ππ π‘ is the total current: πΌπ· ≡ the dc value ππ π‘ ≡ the small signal value 1. DC analysis: iD Turn off the small signal: ⇒ ππ· π‘ = ππ· The current through the diode will be only dc: ππ· ππ· π‘ = πΌπ· = πΌπ exp( ) πππ Bias Point Q ID vD 0.5 0.6 V V VD 0.7 V 0.8 V When the signal ππ π‘ is applied: ο§ Total voltage across the diode: ππ· π‘ = ππ· + ππ π‘ ο§ Total instantaneous current: ππ· π‘ = πΌπ exp( ππ· π‘ = πΌπ exp ππ· +π π π‘ ππ· π‘ = πΌπ· exp πππ ππ π‘ πππ ο When ππ βͺ πππ ; ππ· π‘ = πΌπ· exp ππ π‘ πππ ππ· π‘ = πΌπ exp : ππ· πππ × exp ππ π‘ π ππ ) → πππ (1) ππ π ππ βͺ 1 ⇒ exp ≅ πΌπ· (1 + ππ π‘ πππ ): ππ π‘ πππ ≅1+ ππ π‘ πππ (2) This represents the small signal approximation: where the exponential dependence is approximated by a linear relation ππ· π‘ ≅ πΌπ· + πΌπ· π ππ ππ π‘ = πΌπ· + ππ (π‘): Thus we have a small signal current ππ (π‘) superimposed on the dc current πΌπ· πΌπ· ππ π‘ ≅ ππ π‘ πππ The quantity πΌπ· π ππ relating ππ to π£π has the dimension of conductance; it is: the diode small signal conductance Its inverse: ππ = πππ πΌπ· is the diode small signal resistance ππ or or incremental resistance ππ the dynamic resistance ππ Graphical Interpretation of the small signal approximation ππ = 1 π ππ· π π£ π· π =πΌ π· π· This small signal resistance represents the inverse of the slope of the ππ· − π£π − π£π· curve at the operating point Q. Equivalent circuit model for the diode for small changes around bias point Q. The incremental resistance rd is the inverse of the slope of the tangent at Q, and VD0 is the intercept of the tangent on the vD axis: ππ· π‘ = ππ· + ππ π‘ = ππ·0 + ππ β ππ· π‘ ππ· + ππ π‘ = ππ·0 + ππ β πΌπ· + ππ π‘ ππ· + ππ π‘ = ππ·0 + ππ β πΌπ· + ππ β ππ π‘ DC: ππ· = ππ·0 + ππ β πΌπ· AC: ππ π‘ = ππ β ππ π‘ Large Signal Equivalent Circuit The Small Signal Equivalent Circuit: is as shown Small Signal Equivalent Circuit Replace Diode by its large signal equivalent circuit dc Analysis Small signal analysis High frequency small signal equivalent circuit We add the capacitance to consider the delay between the signal voltage applied and the signal current