Figure 1 shows the X-ray diffraction (XRD) patterns revealed by the two LFP sample structure shapes and phase purities. Based on phase identification from the XRD pattern results, the two LFP sample’s crystalinity were analyzed. Both patterns show similar LiFePO4 main diffraction peaks and match the orthorhombic structure as well as Pnma space group. The sharp, narrow diffraction peaks without detectable phase impurities indicate the LFP sample has high crystalinity. For the sample calcined at 750oC, an olivine phase without detectable impurity phases was observed, while the 700oC sample showed a 97% pure olivine phase, and a phase impurity in the form of FeO11P4. The LFP sample calcined at 750oC had a sharper diffraction peak with narrower full width at half maximum (FWHM) and a higher intensity, compared to the 700oC counterpart. According to the peak FWHM, the crystal size of the samples prepared at 700°C and 750°C calculated by the Scherrer equation resulted in 99 nm and 100 nm, respectively.
The LFP/rGO nanocomposite particles’ morphological and microstructure are observable with SEM-EDX (Figure 2). Based on the images, LFP particles have spherical lumps and are firmly attached to rGO, resembling a thin flake (Figures 2a and b). LFP’s spherical lumps indicate agglomeration, where several particles are joined together to look larger, with a non-homogenous and unevenly distributed grain size in certain places. This agglomeration occurs because the LFP powder, rGO solution, and N-butanol are not evenly mixed in the slurry-making process, while, the black lumps indicate the cathode sheet has shafts. Figure 2b shows large LFP particles are scattered and firmly attached to each rGO layer side, thus, acting as a “bridge” among the particles surroundings. Lithium ion has a greater diffusion distance between the crystal grain’s boundary and center, due to the larger crystal size. Furthermore, the rGO bridge is quite effective in limiting the LFP’s grain growth and widening the surface area, thus shortening the lithium ion’s diffusion length. Therefore, the close relationship between LFP and rGO nanoparticles encourages maximum efficiency while implementing the framework. Also, the presence of Fe, P, O, and C were confirmed in EDX elemental analysis for the LFP/rGO nanocomposite.
Figure 3 shows the LFP/rGO nanocomposites’ electronic conductivity and stored energy, and these are much higher, compared to pure LFP. Mixing LiFePO4 particles with rGO by mechanical ultrasonification plays a significant role in enhancing the electronic conductivity and stored energy, and these properties increase with increase in rGO percentage. The optimum result of 7.84x10-4 S/cm was obtained for samples with a mass ratio of 70% LFP and 30% rGO, while the counterparts for pure LiFePO4 (theoretical), and LFP synthesized by the sol-gel method are ~ 10-9 S/cm and 2.09 x 10-7 S/cm, respectively.
Meanwhile, energy stored from LFP/rGO nanocomposites show a unique phenomenon, and the optimum value of 6.50x10-3 J was obtained by samples with a mass ratio of 85% LFP and 15% rGO. This explains the addition of rGO bridging LFP particles must be carried out within certain limits, and is reinforced by the LFP/rGO nanocomposite cathode material’s electrochemical properties. A lithium battery’s energy capacity depends on how many lithium ions are stored in the electrode structure, and how much the ions are able to move during charging and discharging, because the amount of electron current stored and distributed is proportional to the amount of lithium ions diffused. Further discussion is to refer to the two samples, for a comparative study.
Figure 4 shows the LFP/rGO nanocomposite’s cyclic voltammogram curve, with the addition of 15% and 30% rGO percentages in the first charge-discharge cycle. Both curves show sharp and symmetric anodic/cathodic peaks, indicating good electrochemical performance due to single electron transfer reaction during the cycle. In addition, both electrodes showed a Fe2+/Fe3+ redox peak at a 0.1 mVs-1 scan rate. Meanwhile, for LFP/rGO nanocomposites with a 85% - 15% mass ratio, the anodic peak was located at 3.46V, and this corresponds to the oxidation of Fe2+ to Fe3+, while the cathodic peak at 3.30V corresponds to the reduction of Fe3+ to Fe2+, with a 0.16V potential interval between the two redox peaks. The anodic and cathodic peaks voltage difference within the same cycle correlates with the redox reaction’s polarization and inverse, and this indicates the battery material’s reversibility. A reduction in voltage difference lowers the polarization and increases the battery material’s reversibility, resulting in greater cycle stability. This is consistent with the charge-discharge graph and accelerates the Li+ ions’ diffusion rate. The observed separation between the oxidation and reduction peaks is often used to distinguish electrochemical reversibility from electrode materials, with larger separations indicating lower reversibility. This narrow separation from the redox peak implies the LFP/rGO nanocomposite has excellent electrochemical kinetics.
Figure 5 shows the Nyquist plot, derived from the electrochemical impedance spectroscopies (EIS) of both LFP/rGO nanocomposite samples, measured to further prove the rGO thin-layers in LFP/rGO nanocomposites increase the material’s the electronic conductivity. According to the image, the nyquist plots obtained are in the form of semicircles and slopes. The semicircle pattern in moderate frequency region shows the lithium ion’s charge transfer process on the LFP/rGO and electrolyte surfaces. Meanwhile, the straight line pattern represents the lithium ion diffusion process into the electrode bulk material, commonly known as Warburg diffusion. This pattern shows the electrodes are capable of storing lithium ions, and are therefore suitable for use in lithium-ion batteries. The charge-transfer resistance width also determines the battery’s electrical conductivity of the battery. An increase in pattern narrowness leads to an increase in electrical conductivity.
A comparison of the EIS profile semicircle diameters shows the LFP/rGO nanocomposite cathode with a weight ratio of 70% - 30% (∼400 ohm) has a much smaller charge-transfer resistance, compared to the counterpart with a ratio of 85% - 15% (∼450 ohm). This much smaller solid-electrolyte interface resistance ought to be due to the rGO layers’ presence in the LFP/rGO nanocomposite, with a much better electronic conductivity.
The galvanostatic charge-discharge was measured with lithium cells at a current density of 0.1C (1C = 170 mAg-1), to evaluate the LFP/rGO nanocomposite’s electrochemical properties. The results obtained were as a graph of the relationship between the voltage and the charge-discharge capacity, provided with a constant current and a cut-off voltage of 2.5 - 4.2 volts, during the analysis. Furthermore, the cut off voltage is the initial voltage before treatment (charging and discharging). During charging, lithium ions move from anode to cathode until a maximum voltage of 4.2 volts is reached. Subsequently, the ions move from cathode to anode until a minimum voltage of 2.5 volts is reached (discharging). Figure 6 shows the initial cycle profile of the LFP/rGO nanocomposite electrode with a mass ratio of 85% -15% and 70% -30%, at room temperature. According to the image, the first cycle’s charge profile shows a stable voltage at 3.5V (versus Li+/Li), and this must correspond to the redox pair Fe2+/Fe3+. The discharge profile from the first cycle shows a stable voltage at 3.3V (versus Li+/Li), with a very small separation (0.2V) being stable at the charge profile. In the first cycle, the specific discharge capacity is 128 mAhg-1, and this is about 75% of LiFePO4’s theoretical specific capacity. This excellent electrochemical performance is attributed to the large specific surface area and a wide bridging layer, ensuring electrons pass through each LiFePO4 particle, shortening electronic transport pathways, and reducing interface resistance. The lithium ions easily intercalate into the LiFePO4 framework through the rGO layer, and this in turn avoids particle structure collapse during the charge shedding. Therefore, the LFP/rGO nanocomposite structure endures high current density charge/discharge.