Consider a signal with a sample rate $f_s = 44.1$ kHz. Let us upsample the signal by a factor of $L = 2$ and interpolate the zeros.
An ideal lowpass interpolator would have a gain of $L$ and a cutoff frequency of:
$$f_c = \frac{f_s}{L}$$
An ideal lowpass filter has an infinitesimally small transition band.
In practice I see real lowpass interpolators have a small transition band centred around $f_c$.
The transition band can be quite large, say, $0.45 f_s$ to $0.55 f_s$.
My question is: why do we centre the transition band of a practical lowpass interpolator around the ideal cutoff frequency? By doing that the practical lowpass stopband is above the ideal cutoff which does not make sense to me as that will allow a small unwanted spectral image from the $0.45 f_s$ to $0.50 f_s$ region to creep into the new signal. The obvious alternative is to make the stopband of the practical lowpass $0.5 f_s$ and put up with a passband starting at $0.4 f_s$ assuming we can't make the transition band steeper. There must be some reason this isn't the way it's done.