We assume that initially the current i = 0 and ω′ ≈ ω since b = R/2L is small.
Initially the energy of the capacitor = U = q2/2C and the energy of the capacitor after a time T is
The quantity ω/2b = ωL/R is called the Q of the circuit (for ‘quality’). A high-Q circuit has low resistance and a low fractional energy loss per cycle (=2π/Q).