Return ratio

The return ratio of a dependent source in a linear electrical circuit is the negative of the ratio of the current (voltage) returned to the site of the dependent source to the current (voltage) of a replacement independent source. The terms loop gain and return ratio are often used interchangeably; however, they are necessarily equivalent only in the case of a single feedback loop system with unilateral blocks.

The return ratio of a dependent source in a linear electrical circuit is the negative of the ratio of the current (voltage) returned to the site of the dependent source to the current (voltage) of a replacement independent source. The terms loop gain and return ratio are often used interchangeably; however, they are necessarily equivalent only in the case of a single feedback loop system with unilateral blocks.

Calculating the return ratio

The steps for calculating the return ratio of a source are as follows: Set all independent sources to zero. Select the dependent source for which the return ratio is sought. Place an independent source of the same type (voltage or current) and polarity in parallel with the selected dependent source. Move the dependent source to the side of the inserted source and cut the two leads joining the dependent source to the independent source. For a voltage source the return ratio is minus the ratio of the voltage across the dependent source divided by the voltage of the independent replacement source. For a current source, short-circuit the broken leads of the dependent source. The return ratio is minus the ratio of the resulting short-circuit current to the current of the independent replacement source.

Example: Collector-to-base biased bipolar amplifier

free and short-circuiting broken leads]] Figure 1 (top right) shows a bipolar amplifier with feedback bias resistor R f driven by a Norton signal source. Figure 2 (left panel) shows the corresponding small-signal circuit obtained by replacing the transistor with its hybrid-pi model. The objective is to find the return ratio of the dependent current source in this amplifier. To reach the objective, the steps outlined above are followed. Figure 2 (center panel) shows the application of these steps up to Step 4, with the dependent source moved to the left of the inserted source of value i t , and the leads targeted for cutting marked with an x. Figure 2 (right panel) shows the circuit set up for calculation of the return ratio T, which is T = - \frac {i_r} {i_t} \ . The return current is i_r = g_m v_{\pi} \ . The feedback current in R f is found by current division to be: i_f = \frac {R_D//r_O} {R_D//r_O +R_F +r_{\pi}// R_S} \ i_t \ . The base-emitter voltage v π is then, from Ohm's law: v_{\pi} = -i_f \ ( r_{\pi}// R_S ) \ . Consequently, T = g_m (r_{\pi}// R_S ) \ \frac {R_D//r_O} {R_D//r_O +R_F +r_{\pi}// R_S}\ . G = \frac {v_{out}} {i_{in}} = \frac {(1-g_m R_F)R_1 R_2} {R_F+R_1+R_2+g_m R_1R_2} \ , with R 1 = R S || r π and R 2 = R D || r O . This expression can be rewritten in the form used by the asymptotic gain model, which expresses the overall gain of a feedback amplifier in terms of several independent factors that are often more easily derived separately than the overall gain itself, and that often provide insight into the circuit. This form is: G = \ G_{ \infty } \frac {T} {1+T} + G_0 \frac {1} { 1+T} \ \ , where the so-called asymptotic gain G ∞ is the gain at infinite g m , namely: G_{\infty} = - R_F \ , and the so-called feed forward or direct feedthrough G 0 is the gain for zero g m , namely: G_{0} = \frac { R_1 R_2 } {R_F +R_1 +R_2}\ . For additional applications of this method, see asymptotic gain model and Blackman's theorem.

References

See also

Asymptotic gain model Blackman's theorem Extra element theorem

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