Difference between revisions of "Active Filters"

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\end{align}
 
\end{align}
 
</math>|{{EquationRef|1}}}}
 
</math>|{{EquationRef|1}}}}
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If we let <math>Q=\omega_0 RC = \tfrac{R}{\omega_0 L}</math> and <math>\omega_0 = \tfrac{1}{\sqrt{LC}}</math>, then we can rewrite our expression for <math>H\left(s\right)</math> as:
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{{NumBlk|::|<math>
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H\left(s\right) = \frac{s\cdot\frac{\omega_0}{Q}}{s^2 + s\cdot\frac{\omega_0}{Q} + \omega_0^2}
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</math>|{{EquationRef|2}}}}

Revision as of 15:33, 24 March 2021

Passive RLC filters are simple and easy to design and use. However, can we implement them on-chip? Let us look at a simple example to give us a bit more insight regarding this question.

Example: A passive band-pass filter

Consider the filter shown in Fig. 1.

We can write the transfer function as:

 

 

 

 

(1)

If we let and , then we can rewrite our expression for as:

 

 

 

 

(2)