So I'm solving some problems on filters and came up with an apparent contradiction that I would like to get clear. Considering a low-pass biquadratic section:
$$T(s)=\frac{V_o(s)}{V_i(s)}=\frac{K_0\omega_0^2}{s^2+\frac{\omega_0}{Q_0}s+\omega_0^2}$$
So in the first problem that this appeared I was expected to calculate the group-delay at pole frequency.
I considered the phase being given by (because in this exercise the gain is negative)
$$\phi(\omega)=\pi-\arctan(\frac{\frac{\omega\omega_0}{Q_0}}{\omega_0^2-\omega^2})$$
and the group delay calculated with $$\tau_g(\omega)=-\frac{d\phi}{d\omega}$$
I come up with $$\tau_g(\omega)=\frac{Q_0\omega_0(\omega_0^2+\omega^2)}{Q_0^2(\omega_0^2-\omega^2)^2+\omega_0^2\omega^2}$$
Finally at \$ \omega_0 \$: $$\tau_g(\omega_0)=\frac{2Q_0}{\omega_0}$$
Done!
Now off with the second exercise, I have to consider the same biquadratic section but now it is a Bessel filter with constant group delay \$\tau_0 \$. Now the author calculates the group delay as a function of the pole frequency and the quality factor and comes up with.
$$\tau_0=\frac{1}{Q_0\omega_0}$$
I have no idea where this expression comes from and why it contradicts my answer of the previous exercise. Is this because this a Bessel filter now? How do we arrive with this new expression? What are the math steps? Thank you in advance