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In this study, a circuitry model of the coupling of a qubit to reservoir modes is defined to clearly determine the effect of the reservoir modes on the qubit decay and dephasing rates. The main goal is to theoretically calculate the dephasing and decay rate of a qubit, particularly due to the circuitry effect. Firstly, the Hamiltonian of the system (coupling of a qubit to the reservoir modes) is defined and used to derive the time evolution of the density matrix for the qubit energy levels. By calculating the qubit level density evolutions, one can estimate at which frequency the maximum coupling occurs and, in addition, knows about the role of the electromagnetic bias in the qubit. Secondly, the qubit decay rate is theoretically derived. The results show that the decay rate is strongly affected by circuitry elements such as the qubit capacitor and, more importantly, the coupling capacitor between the qubit and the reservoir modes. As the main result, it is shown that the slight decrease in the coupling capacitors significantly affects the relaxation time even more than the qubit capacitor. Consequently, the dephasing rate, which is the effect of the reservoir modes on the transition frequency of the qubit, is theoretically examined using the Heisenberg-Langevin equation. Finally, by transforming the Heisenberg-Langevin equations into the Fourier domain, the number of photons of the qubit due to coupling to reservoir modes are calculated. This is considered to be the photons generated in the qubit owing to the noise effect. This term significantly influences the qubit coherence time.