Abstract

The practical implementation of supercapacitors is hindered by low utilization and poor structural stability of electrode materials. Herein, to surmount these critical challenges, a three-dimensional hierarchical α-Co(OH)2/α-Ni(OH)2 heterojunction nanorods are built in situ on Ni foam through a mild two-step growth reaction. The unique lamellar crystal structure and abundant intercalated anions of α-M(OH)2 (M = Co or Ni) and the ideal electronic conductivity of α-Co(OH)2 construct numerous cross-linked ion and electron transport paths in heterojunction nanorods. The deformation stresses exerted by α-Co(OH)2 and α-Ni(OH)2 on each other guarantee the excellent structural stability of this heterojunction nanorods. Using nickel foam with a three-dimensional network conductive framework as the template ensures the rapidly transfer of electrons between this heterojunction nanorods and current collector. Three-dimensional hierarchical structure of α-Co(OH)2/α-Ni(OH)2 heterojunction nanorods provides a large liquid interface area. These result together in the high utilization rate and excellent structure stability of the α-Co(OH)2/α-Ni(OH)2 heterojunction nanorods. And the capacitance retention rate is up to 93.4% at 1 A g−1 from three-electrode system to two-electrode system. The α-Co(OH)2/α-Ni(OH)2//AC device also present a long cycle life (the capacitance retention rate is 123.6% at 5 A g−1 for 10000 cycles), a high specific capacitance (207.2 F g−1 at 1 A g−1), and high energy density and power density (72.6 Wh kg−1 at 196.4 W kg−1 and 40.9 Wh kg−1 at 3491.8 W kg−1), exhibiting a fascinating potential for supercapacitor in large-scale applications.

Highlights

  • The rapid consumption of non-renewable energy resources and the booming development of mobile electronics and hybrid electric vehicle have aroused intensive attention on green and safe energy storage devices with high specific capacitance and excellent working life[1,2,3,4,5]

  • The researchers try to improve the comprehensive performance of electrode materials by building rich heterojunctions inside electrode materials and successfully prepared a series of heterojunction composites for supercapacitors (such as Ni3S2/Ni(OH)[221–23], NiS/ Ni(OH)[224,25], NiCo2S4/Ni(OH)[226–28] and CoS/Ni(OH)229), which combine the high ionic conductivity of Ni(OH)[2] electrode attributing to its two-dimensional layered crystal structure and the excellent electronic conductivity of nickel sulfide owing to its compact crystal structure and high metallicity of sulfur atoms

  • The strong peaks at 2025 cm−1 corresponds to the absorption peak of carbonyl group[46], and relative intensity of the peak in the heterojunction structure is much weaker, which illustrates that amount of NH2COO− anions have been reduced after second reaction

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Summary

Results and Discussion

Figure (5a,b) display the discharge curves of α-Co(OH)[2] nanowires and α-Co(OH)2/α-Ni(OH)[2] heterojunction nanorods from a potential of 0–0.5 V at 0.1 to 2 A g−1 of current densities in three-electrode system. For heterojunction α-Co(OH)2/α-Ni(OH)[2] nanorods, which show a specific capacitance with 981.5, 979.2, 964.7, 950.3, 887.3, 872.85 and 854.3 F g−1 at same current density with α-Co(OH)[2], respectively, yielding a 87% of initial capacitance-retention ratio, 95.2% capacitance retention is still kept when the material undergo rate cycle from high current density. Electrode material Ni(OH)2-Co(OH)[2] Co-Ni(OH)2/Ni3S2 NiCo2S3@Ni(OH)2@ppy Ni(OH)[2] Co3O4/CoS/Ni(OH)2@Co Ni(OH)2/Mn2O3 Ni3S2@ Co(OH)2@Ni Ni(OH)[2] NiCoP @C@Ni(OH)[2] (Ni-Co-S)/Co(OH)[2] CoMoO4@Ni(OH)[2] RGO/α-Ni(OH)[2] Ni-Co-S/G FeOF/Ni(OH)[2] Mg(OH)2/Ni(OH)[2] Co-α-Ni(OH)2/RGO MWCNT/amor-Ni(OH)2/PEDOT:PSS α-Co(OH)2@α-Ni(OH)[2]

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