Order
Derive an expression to calculate the order of Inverse Chebyshev low pass filter
The attenuation is given by
\[
\alpha = -20 \log_{10}\left(|T(j\omega)|\right)
\]
We know,
\[
|T_n(j\omega)|^2 = \frac{\varepsilon^2 C_n^2(\omega)}{1 + \varepsilon^2 C_n^2(\omega)}
\]
Hence,
\[
\alpha = -20 \log_{10}\left(|T(j\omega)|\right)
\]
\[
\alpha = -10 \log_{10}\left(\frac{\varepsilon^2 C_n^2(\omega)}{1 + \varepsilon^2 C_n^2(\omega)}\right)
\]
\[
\alpha = 10 \log_{10}\left(1 + \frac{1}{\varepsilon^2 C_n^2(\omega)}\right)
\]
We know that at
\[
\omega = \omega_p, \quad \alpha = \alpha_p = \alpha_{\max}
\]
\[
\alpha_{\max} = 10 \log_{10}\left(1 + \frac{1}{\varepsilon^2 C_n^2(\omega_p)}\right)
\]
\[
10^{\frac{\alpha_{\max}}{10}} = 1 + \frac{1}{\varepsilon^2 C_n^2(\omega_p)}
\]
\[
\frac{1}{\varepsilon^2 C_n^2(\omega_p)} = 10^{\frac{\alpha_{\max}}{10}} - 1
\]
\[
C_n^2(\omega_p) = \frac{1}{\varepsilon^2 \left(10^{\frac{\alpha_{\max}}{10}} - 1\right)}
\]
Where,
\[
\varepsilon = \sqrt{10^{\frac{\alpha_{\min}}{10}} - 1}
\]
Thus,
\[
C_n^2(\omega_p) = \frac{10^{\frac{\alpha_{\min}}{10}} - 1}{10^{\frac{\alpha_{\max}}{10}} - 1}
\]
\[
C_n(\omega_p) = \sqrt{\frac{10^{\frac{\alpha_{\min}}{10}} - 1}{10^{\frac{\alpha_{\max}}{10}} - 1}}
\]
---
### Chebyshev Functions
For Chebyshev filters:
\[
C_n(\omega) = \cosh\left(n \cosh^{-1}(\omega)\right), \quad \omega > 1
\]
For **Inverse Chebyshev**:
\[
C_n\!\left(\frac{1}{\omega_p}\right) = \cosh\left(n \cosh^{-1}\!\left(\frac{1}{\omega_p}\right)\right), \quad \frac{1}{\omega_p} > 1 \; \text{or} \; \omega_p < 1
\]
Since \(\frac{1}{\omega_p} > 1\), we can write:
\[
\cosh\left(n \cosh^{-1}\!\left(\frac{1}{\omega_p}\right)\right) =
\sqrt{\frac{10^{\frac{\alpha_{\min}}{10}} - 1}{10^{\frac{\alpha_{\max}}{10}} - 1}}
\]
Taking inverse hyperbolic cosine:
\[
n \cosh^{-1}\!\left(\frac{1}{\omega_p}\right) =
\cosh^{-1}\!\left(\sqrt{\frac{10^{\frac{\alpha_{\min}}{10}} - 1}{10^{\frac{\alpha_{\max}}{10}} - 1}}\right)
\]
\[
n = \frac{
\cosh^{-1}\!\left(\sqrt{\dfrac{10^{\frac{\alpha_{\min}}{10}} - 1}{10^{\frac{\alpha_{\max}}{10}} - 1}}\right)
}{
\cosh^{-1}\!\left(\dfrac{1}{\omega_p}\right)
}
\]
If \(\omega_s\) is given, then:
\[
n = \frac{
\cosh^{-1}\!\left(\sqrt{\dfrac{10^{\frac{\alpha_{\min}}{10}} - 1}{10^{\frac{\alpha_{\max}}{10}} - 1}}\right)
}{
\cosh^{-1}\!\left(\dfrac{\omega_s}{\omega_p}\right)
}
\]
This gives the **order of the Inverse Chebyshev filter**.