Difference between revisions of "TF EIM Chapt3"
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:<math>\left | \frac{V_{out}}{V_{in}}\right | = \sqrt{\left [ \frac{R_L + i \left ( \omega L - \frac{1}{\omega C}\right)}{R + R_L + i \left ( \omega L - \frac{1}{\omega C}\right)}\right ]\left [ \frac{R_L + i \left ( \omega L - \frac{1}{\omega C}\right)}{R + R_L + i \left ( \omega L - \frac{1}{\omega C}\right)}\right ]^*}</math> | :<math>\left | \frac{V_{out}}{V_{in}}\right | = \sqrt{\left [ \frac{R_L + i \left ( \omega L - \frac{1}{\omega C}\right)}{R + R_L + i \left ( \omega L - \frac{1}{\omega C}\right)}\right ]\left [ \frac{R_L + i \left ( \omega L - \frac{1}{\omega C}\right)}{R + R_L + i \left ( \omega L - \frac{1}{\omega C}\right)}\right ]^*}</math> | ||
− | :<math>\left | \frac{V_{out}}{V_{in}}\right | = \sqrt{\left [ \frac{R_L^2+ \left ( \omega L - \frac{1}{\omega C}\right)^2}{R + R_L | + | :<math>\left | \frac{V_{out}}{V_{in}}\right | = \sqrt{\left [ \frac{R_L^2+ \left ( \omega L - \frac{1}{\omega C}\right)^2}{R + R_L R_L^2+ \left ( \omega L - \frac{1}{\omega C}\right)^2}</math> |
=== Phase shift=== | === Phase shift=== |