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258                Polymer-based Nanocomposites for Energy and Environmental Applications


          Table 9.3 Comparison table among selected electrochemical energy
          storage technologies [177]

          Characteristics         Capacitor      Supercapacitors    Battery
                            1
          Specific energy (Wh kg )  <0.1         1–10               10–100
                           1
          Specific power (Wkg )   ≫10,000        500–10,000         <1000
          Discharge time          10  6  to 10  3  Seconds to minutes  0.3–3h
          Charge time             10  6  to 10  3  Seconds to minutes  1–5h
          Coulombic efficiency (%)  About 100    85–98              70–85
          Cycle life              Almost infinite  >500,000         About 1000
























         Fig. 9.4 Working principle of (A) electrochemical double-layer capacitance and
         (B) pseudocapacitance [180].

         the porous structure such as high porosity, high accessible surface area, and pore size
         distribution between 0.5 and 2 nm of the electrode material. Activated carbon has been
         used commercially as an electrode for EDLCs because of their industrial production,
         low cost, high conductivity, and thermal and mechanical stability [32,182]. Kondrat
         et al. concluded after experimental and theoretical studies that optimum pore size, for
         maximum energy density, depends on the voltage and pore size distribution and ion
         size [183]. It is generally stabled that the optimum pore diameter is around 2.5 nm
         in the case of liquid electrolyte [184] and the pore diameter should be equal to
         the ion size of the electrolyte [185]. Activated carbon shows very high surface area
                  2  1
         (>1000 m g ) but displays large pore size distribution with high percentage of
         microspores (<2 nm) and few mesopores (2–50 nm). These micropores in activated
         carbon are inaccessible by the liquid electrolytes and, therefore, cannot contribute
                                                                            1
         toward electric double-layer formation leading to low capacitance (100–120 F g )
                                              1
         and hence low energy density (4–5Whkg ) [186,187]. Therefore, several forms
         of nanocarbonaceous materials have been explored as electrode materials for the
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