  We consider continuous quantum measurement of a superconducting qubit in the
circuit QED setup with a moderate bandwidth of the measurement resonator, i.e.,
when the "bad cavity" limit is not applicable. The goal is a simple description
of the quantum evolution due to measurement, i.e., the measurement back-action.
Extending the quantum Bayesian approach previously developed for the "bad
cavity" regime, we show that the evolution equations remain the same, but now
they should be applied to the entangled qubit-resonator state, instead of the
qubit state alone. The derivation uses only elementary quantum mechanics and
basic properties of coherent states, thus being accessible to non-experts.
