Transistor Basics is a free introductory textbook on transistors and their basic applications. See the editorial for more information....

Input and Output Impedance Matching

Author: Leonard Krugman

Equations 3-13 and 3-21 indicate that the input resistance is affected by the load resistance and, conversely, the output resistance depends on the generator internal resistance.

Thus, starting with a given load resistance, if the generator resistance is changed to match the input resistance, the output resistance of the transistor changes, thus requiring a change in load resistance, and so on. In the following analysis, the proper values of generator and load resistance which satisfy both the input and output matching conditions at the same time are determined. Let r1 equal the proper value of input resistance and generator resistance. Let r2 equal the image matched value for the transistor output resistance and the load resistance. Then: r1 = Rg = ri and r2 = RL = ro. Substituting for RL and r1 in equation 3-13

transistor_basics_03-82.gif

Eq. (3-26)

Solving in terms of r12r21

(r1 - r11) (r2 + r22) = - r12r21

Eq. (3-27)

Substituting for Rg and ro in equation 3-21

transistor_basics_03-83.gif

Eq. (3-28)

Again solving in terms of r12r21

(r2 - r22) (r1 + r11) = - r12r21

Eq. (3-29)

Equating equations 3-27 and 3-29

(r1 - r11) (r2 + r22) = (r2 - r22) (r1 + r11)

Eq. (3-30)

Cross multiplying and cancelling equal terms,

r1r2 - r2r11 + r1r22 -r11r22 = r1r2 - r1r22 + r2r11 - r11r22

2r1r22 = 2r2r11

Eq. (3-31)

or

transistor_basics_03-85.gif

Eq. (3-32)

This latter equation indicates that matching the input and output resistances for maximum power gain requires their values to be in the same ratio as the open-circuit characteristics of the transistor.

The absolute value of the generator internal resistance and its matched input resistance in terms of transistor open-circuit parameters can now be determined. Substituting the equality transistor_basics_03-84.gif into equation 3-26,

transistor_basics_03-86.gif

Eq. (3-33)

transistor_basics_03-87.gif

Eq. (3-34)

transistor_basics_03-88.gif

Eq. (3-35)

transistor_basics_03-89.gif

Eq. (3-36)

In terms of the stability factor, transistor_basics_03-90.gif, which will be defined later in the chapter, the input image resistance

transistor_basics_03-91.gif

Eq. (3-37)

For the typical point-contact transistor previously considered, when r11 = 250 ohms, r12 = 100 ohms, r21 = 24,000 ohms, and r22 = 12,000 ohms, the numerical value of r1 is

transistor_basics_03-92.gif

For the typical junction transistor, when r11 = 550 ohms, r12 = 500 ohms, r21 = 1,900,000 ohms, and r22 = 2,000,000 ohms,

transistor_basics_03-93.gif

The output image resistance of a transistor can be determined in a similar fashion from the ratio

transistor_basics_03-94.gif

Substituting this equality into equation 3-28

transistor_basics_03-95.gif

Eq. (3-38)

transistor_basics_03-96.gif

Eq. (3-39A)

transistor_basics_03-97.gif

Eq. (3-39B)

transistor_basics_03-98.gif

Eq. (3-40)

In terms of the stability factor transistor_basics_03-99.gif; the output image resistance

transistor_basics_03-100.gif

Eq. (3-41)

For the typical point-contact transistor,

transistor_basics_03-101.gif

Forthe typical junction transistor

transistor_basics_03-102.gif

These values may be checked on the RL vs ri and Rg vs ro characteristics plotted for these typical transistors in Figs. 3-11, 3-12, 3-14, and 3-15.


Last Update: 2010-11-17