Microfluidic fuel cells (MFCs) are potential micro power sources for portable electronics. MFCs utilize the co-laminar flowing of the solutions in the microchannel and remove the membranes in the traditional fuel cells. Flow-through electrodes exploit the internal electrode surfaces and improve the MFC performance. Carbon paper (CP) has been widely used as a flow-through electrode with a limited specific surface area. We have also used graphite felt (GF) with a high specific surface area as the electrode and then compared the performance of the MFCs with the CP and GF as the electrodes, respectively. Firstly, we showed the SEM surface morphologies of the two electrodes with or without the Pd catalysts. Secondly, we compared the electrochemical activities of the two electrodes in the solutions, respectively. The GF electrode always showed higher electrochemical activities than the CP electrode, since the GF electrode owned its larger accessible electrochemical surface area and less electrode resistance than the CP electrode. Thirdly, we compared the performance of the MFCs with the two electrodes. The results showed that the performance of the MFC with the GF electrodes electrodes was optimum, with the peak power density of 175.60 mW cm À 2 and limiting current density of 616.53 mA cm À 2 . Finally, we conducted the discharge performance of the MFCs with the two electrodes. There existed a minor variation in the discharge current densities of the MFCs with the CP cathodes.
Conventional Al‐air batteries are not suitable as portable power devices due to their complicated water management and bulky system. To resolve this issue, the fiber paper‐ and cotton cloth‐based Al‐air batteries were proposed, which exploited the capillary force from the paper (FP) and cotton cloth (CC) to deliver the solutions and eliminated the external pump. The physical features of the FP and CC were gained including the surface morphologies, surface elementary analysis, liquid absorption and flow rates. CC owned larger liquid absorption and faster flow rate due to its hierarchically woven‐spun fiber structure, compared to the randomly oriented fibers of the FP, although the surface of the CC demonstrated lower O/C ratio than that of the FP. So, the performance of the CC‐based Al‐air battery was largely higher than that of the FP‐based battery. The performance of the CC‐based Al‐air battery was optimal at 1.0 M NaOH electrolyte and the anode‐to‐cathode surface area ratio of 1 : 4, with the peak power density of 14.95±0.28 mW cm−2, and the maximum current density of 36.61±0.54 mA cm−2. To apply the CC‐based Al‐air battery, the two‐battery pack connected in series was assembled to drive a timer and light 9 LEDs.
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