10.08.2013 Views

III. Gm-C Filtering - Epublications - Université de Limoges

III. Gm-C Filtering - Epublications - Université de Limoges

III. Gm-C Filtering - Epublications - Université de Limoges

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

A parallel self resonating circuit is then obtained consi<strong>de</strong>ring a parallel capacitor Cp to<br />

the gyrator. This leads to a resonant frequency given by:<br />

filter.<br />

g m1g<br />

m2<br />

ω . (<strong>III</strong>.37)<br />

CC<br />

0 =<br />

p<br />

A filter using a gyrator as a resonant element is called in the literature a Gyrator-C<br />

Figure 72 <strong>de</strong>picts a fourth or<strong>de</strong>r high-pass filter. The equivalent gyrator-C filter is<br />

obtained transforming the inductors of the circuit into gyrators.<br />

Figure 72. Synthesis of a filter using gyrators<br />

II.4.a.ii Impact of Real Elements<br />

Though previous transconductances were consi<strong>de</strong>red as i<strong>de</strong>al, imperfections appear<br />

when implementing the <strong>de</strong>sign. It can be either an input capacitance (for instance the Cgs of a<br />

MOS realizing the gm) or a non-infinite output resistance. This leads to the schematic shown<br />

in Figure 73, where C2 takes into account the real mo<strong>de</strong>l of the transconductance as well as<br />

the internal no<strong>de</strong> capacitance of the gyrator.<br />

- 59 -

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!