Figures & data
Figure 6. This graph corresponds to the impulse response g(t) with respect to the different order when . Method1 corresponds to the complex path integral method and method2 corresponds to Mittag–Leffler function series method.
![Figure 6. This graph corresponds to the impulse response g(t) with respect to the different order when R=1Ω,C=1F. Method1 corresponds to the complex path integral method and method2 corresponds to Mittag–Leffler function series method.](/cms/asset/dedb965e-5e91-4551-8777-bc7684fca89c/gipe_a_2228986_f0006_oc.jpg)
Figure 8. The dotted line corresponds to the solution using the inverse integral formula, chain line is for the solution using the Mittag–Leffler function.
![Figure 8. The dotted line corresponds to the solution using the inverse integral formula, chain line is for the solution using the Mittag–Leffler function.](/cms/asset/8af2a1fa-ecd5-420f-83cb-baee74107c49/gipe_a_2228986_f0008_oc.jpg)
Figure 9. The critical damping phenomena of different order α with corresponding R when L=1000000H, C=0.01F, E=1V.
![Figure 9. The critical damping phenomena of different order α with corresponding R when L=1000000H, C=0.01F, E=1V.](/cms/asset/8677f369-d9f7-4bbe-9a32-9a75ca74057c/gipe_a_2228986_f0009_oc.jpg)
Figure 10. The critical damping phenomena of different order α with corresponding R when L=1000000H, C=0.001F, E=1V.
![Figure 10. The critical damping phenomena of different order α with corresponding R when L=1000000H, C=0.001F, E=1V.](/cms/asset/5eb3cc50-a97f-45d6-84f9-158b535ba3a7/gipe_a_2228986_f0010_oc.jpg)
Figure 11. The critical damping phenomena of different order α with corresponding R when L=1000H, C=0.1F, E=1V.
![Figure 11. The critical damping phenomena of different order α with corresponding R when L=1000H, C=0.1F, E=1V.](/cms/asset/dde07fc8-a6a4-4db5-91d2-919c1a37fbc4/gipe_a_2228986_f0011_oc.jpg)
Table 1. The experimental data.
Table 2. The values of λ with respect to different fractional orders α.