- #1
Master1022
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- TL;DR Summary
- Topic: Two port network filter synthesis; filter transformation from low pass to band-stop equivalent. This question is specifically about transforming an inductor and capacitor to their band stop equivalent circuit components. I have a question about the derivation of the values of these circuit components
Hi,
Context:
I was looking through some circuits material in the topic of filter synthesis for two port networks. For simplicity, these networks have been synthesized for normalized conditions: 1 rad/s cut-off frequency and a termination resistor of 1 ## \Omega ##. An example filter is shown in the image below - the 1 ## \Omega ## termination resistor can be seen.
I was reading about the transformation of LPF (filter) circuits to band stop (filter) circuits. The transformation is given by: (where ## s_n ## is normalised, and ## \omega_0 ## is the target cut-off value)
Question 1:
Then below I read the following (shown in the image below). For the inductor transformation, am I correct in thinking that the penultimate expression should instead read:
[tex] \frac{1}{s L_{e1} + \frac{1}{s C_{e1}}} [/tex]
That is, the ## L_{e1} ## and ## C_{e1} ## should be swapped around. When I asked about it, I was told that I was "definitely wrong", but I am struggling to see why.
Question 2:
If we wanted to transfer both the filter type (LPF --> Band stop) and the filter values (i.e. change from normalized values of 1 rad/s cut-off to arbitrary value), how would I transform the circuit values? For the inductors, would I:
1. Transform the inductor via ## L_{new} = \frac{R_0 L_n}{\omega_0} ##
2. Then transform ## L_{new} s_n ## as shown in the image above
or have I misunderstood this?
Any help would be greatly appreciated. I can provide more information if required to clarify the post.
Context:
I was looking through some circuits material in the topic of filter synthesis for two port networks. For simplicity, these networks have been synthesized for normalized conditions: 1 rad/s cut-off frequency and a termination resistor of 1 ## \Omega ##. An example filter is shown in the image below - the 1 ## \Omega ## termination resistor can be seen.
I was reading about the transformation of LPF (filter) circuits to band stop (filter) circuits. The transformation is given by: (where ## s_n ## is normalised, and ## \omega_0 ## is the target cut-off value)
Question 1:
Then below I read the following (shown in the image below). For the inductor transformation, am I correct in thinking that the penultimate expression should instead read:
[tex] \frac{1}{s L_{e1} + \frac{1}{s C_{e1}}} [/tex]
That is, the ## L_{e1} ## and ## C_{e1} ## should be swapped around. When I asked about it, I was told that I was "definitely wrong", but I am struggling to see why.
Question 2:
If we wanted to transfer both the filter type (LPF --> Band stop) and the filter values (i.e. change from normalized values of 1 rad/s cut-off to arbitrary value), how would I transform the circuit values? For the inductors, would I:
1. Transform the inductor via ## L_{new} = \frac{R_0 L_n}{\omega_0} ##
2. Then transform ## L_{new} s_n ## as shown in the image above
or have I misunderstood this?
Any help would be greatly appreciated. I can provide more information if required to clarify the post.