Open Access Article
Song Rena,
Dengliang He*a,
Shishan Xue
*a,
Shuxin Liu
a and
Wei Zhangbc
aSchool of Chemistry and Material Engineering, Mianyang Teachers' College, Mianxing West Road No.166, Mianyang City, Sichuan Province 621000, CN. E-mail: 449011902@qq.com; xueshishancarol@163.com
bKey Laboratory of Solid Waste Treatment and Resource Recycle, Ministry of Education, Mianyang City, Sichuan Province 621000, CN
cAnalytical and Testing Center, Southwest University of Science and Technology, Mianyang, 621000, CN
First published on 11th December 2025
This study tackled the persistent challenges of low purity and limited diversity in recycled materials obtained from printed circuit board (PCB) acidic copper chloride etching waste solution (ACCEWS). High-purity Cu2(OH)2CO3 was first synthesized from purified ACCEWS (in contrast to raw waste solutions) using a Na2CO3–NaHCO3 buffer system. Subsequent alkaline treatment yielded crude CuO, which was then upgraded to high-purity CuO via calcination. Simultaneously, the effects of impurities on the purity, phase composition, and morphology of copper compounds were systematically investigated by XRD, SEM, TG, FTIR, ICP-OES, XPS and HRTEM, along with their transformation mechanisms and impurity behavior. The results demonstrated that purification markedly improved the purity of Cu2(OH)2CO3. Compared to untreated samples, the P-Cu2(OH)2CO3 derived from purified etching waste exhibited enhanced stability in copper content (55.40–55.50 wt% vs. 54.40–55.40 wt% in R-Cu2(OH)2CO3), reduced metal impurities (0.17–0.22 wt%), and notably lower chloride residues (consistently ≤0.014 wt%). Furthermore, purification effectively removed competitive interference from Cl− and other species during Cu2(OH)2CO3 crystallization, yielding more uniform particles with either flower-like spherical or spiky flake morphologies. The combined purification and calcination process significantly improved both the purity and crystallization behavior of nano-CuO. The nano P-CuO showed progressively increasing CuO purity: 80.24 wt% (300 °C/1 h), 92.24 wt% (400 °C/1 h), 98.54 wt% (500 °C/1 h), and 98.80 wt% (600 °C/1 h) – consistently higher than that of the corresponding R-CuO samples derived from untreated waste (68.48 wt%, 82.24 wt%, 94.48 wt%, and 97.90 wt%). Final optimization at 600 °C for 3 hours yielded ultra-pure P-CuO nanoparticles (≈110 nm) containing 99.04 wt% CuO with exceptionally low impurity levels: <0.12 wt% metallic impurities and <0.0015 wt% chloride content. This study demonstrated a “waste-to-wealth” approach through the simultaneous production of high-purity Cu2(OH)2CO3 and nano-CuO from the purification of ACCEWS. These findings offer important insights for both the sustainable utilization of PCB ACCEWS and the development of high-purity copper-based materials.
000 metric tons of copper.4 PCB etching solutions, as hazardous waste, contain elevated amounts of copper ions demonstrating bioaccumulation characteristics, which would present serious ecotoxicological hazards if released untreated.5 Additionally, the exceptional copper grade within waste solution (typically >5% compared to 0.5–2% in natural ores) makes direct disposal economically wasteful and environmentally unsound.6 Systematic copper recovery consequently would deliver valuable metal reclamation and crucial pollution prevention.
Currently, conventional approaches for PCB etching solution recycling comprise solvent extraction,7 neutralization precipitation,8 electrolysis,9 and ion adsorption,10 among others. For example, Nguyen et al. utilized Cyanex 272 to isolate Au(III) from a leaching solution of cemented Cu.11 Liu et al.12 proposed direct electrolysis to recover Cu from waste PCBs. The recovery rate of Cu was up to 97.32% with a purity of 99.86%.
These methods have demonstrated advantages in recovering precious metals, while the neutralization precipitation technique has garnered significant attention due to its straightforward process and low cost. Dou et al.13 exploited an advanced approach of decomplexation and neutralization and precipitation by NH3·H2O coupled with oxidation by O2, to separate Cu(II) and Cu(I) to produce Cu2(OH)3Cl. Guo14 and coworkers employed ammonia (NH3·H2O) and sodium hydroxide (NaOH) as neutralizers to reclaim Cu to produce Cu2Cl(OH)3, which can be used as a precursor for producing Cu(OH)2 and CuSO4·5H2O with higher purity.
Basic copper carbonate (BCC; Cu2(OH)2CO3), another normal copper-containing compound, can also be fabricated through neutralization precipitation, which has been widely applied in various fields including pyrotechnics, pigments, insecticides, organic synthesis catalysts, and others.15–20 A typical process involved either reacting metallic copper with concentrated HNO3 to prepare Cu(NO3)2 or directly using Cu(NO3)2 as the raw material, with ammonium bicarbonate serving as the precipitating agent to afford Cu2(OH)2CO3.21 Alternative approaches have been reported, such as directly precipitating Cu2(OH)2CO3 crystals (5.0–6.5 µm) from a CuCl2 solution and Na2CO3 solution at 50 °C and pH 6.5–9.22 Additionally, Candal et al.23 employed a copper-containing solution with ammonia water as a pH regulator to prepare amorphous Cu2(OH)2CO3.
Despite BCC being widely applied in many fields, the economic efficiency is hardly attractive. However, BCC always works as a precursor to produce CuO, for which the high specific capacity, surface energy, and large surface area lead to promising applications in advanced fields, including electrochemical devices, optoelectronics, energy systems, catalysis, and biomedicine. The fabrication of CuO nanoparticles is generally achieved through physical, chemical, and biogenic techniques. Chemical precipitation combined with thermal decomposition is one of the most simple, low-cost and scalable techniques to produce CuO. Luna et al.24 synthesized CuO using cupric acetate as a precursor at 400 °C for 1 h under an air flow. Benhammada et al.25 utilized nitrate trihydrate, copper(II) chloride dehydrate, and copper(II) sulfate pentahydrate as precursors, respectively, which were further precipitated by NaOH solution. The obtained precipitates were annealed at 550 °C for 4 h to produce CuO. Kida et al.26 developed 5–10 nm CuO-NPs via ethanol-based solution-phase synthesis at 78 °C using Cu(CH3COO)2 in a CH3COOH/NaOH system. Chang et al.27 produced 40–50 nm CuO-NPs through 500 °C calcination of CuSO4/Na2CO3 precursors. Gan et al.28 achieved 20 nm crystalline CuO-NPs via chloride-based precipitation with ultrasonic purification.
Inspired by these published works, herein, we propose a coupling technique of neutralization precipitation and thermal decomposition to fabricate high-purity CuO using acidic copper chloride etching waste solutions (ACCEWS) as copper sources. The production technology of Cu2(OH)2CO3 was studied in detail, including the Na2CO3/NaHCO3 ratio and reaction temperature during the neutralization precipitation process. The low-temperature hydrothermal conversion and calcination parameters were also researched in depth to synthesize CuO. The as-prepared CuO obtained using the optimal parameters exhibited high purity (>99.04 wt%), low metallic impurities (<0.12 wt%) and low chloride content (<0.0015 wt%). This innovative strategy resolved the single-product constraint of traditional recovery processes, accomplishing coupled production of two valuable copper compounds and establishing an efficient hazardous waste upcycling paradigm.
:
2, 1
:
1, 2
:
1). As shown in Fig. 1A, all the products displayed well-defined diffraction peaks at 14.8°, 17.6°, 24.1°, and 31.2°, precisely corresponding to the (020), (120), (220), and (20–1) crystal planes of monoclinic Cu2(OH)2CO3 (JCPDS no. 41-1390), respectively, indicating their high crystallinity. The XRD patterns confirmed that P-ACCEWS consistently produced well-crystallized, high-purity Cu2(OH)2CO3 across different alkali ratios. This enhanced crystallization was mainly due to the effective elimination of interfering impurities (e.g., Cl− and metal ions), which created an optimized growth environment for monoclinic Cu2(OH)2CO3 crystals. In contrast, the products derived from R-ACCEWS at a 1
:
1 Na2CO3/NaHCO3 ratio exhibited monoclinic CuCl(OH)3 (JCPDS no. 87-0679) as the dominant phase, suggesting that competitive coordination of chloride suppressed the formation of Cu2(OH)2CO3 at low alkalinity. At a 1
:
2 Na2CO3/NaHCO3 ratio, monoclinic Cu2(OH)2CO3 from R-ACCEWS became the major phase. However, an unidentified impurity peak emerged at 22.2°, likely due to metallic impurity compounds. When the Na2CO3/NaHCO3 ratio was further increased to 2
:
1, monoclinic Cu2(OH)2CO3 formed as the exclusive phase, demonstrating that higher CO32−/OH− concentrations effectively overcame the interference from chloride.
It was found that the morphology and dispersity of Cu2(OH)2CO3 were significantly influenced by the type of ACCEWS. Compared to Cu2(OH)2CO3 obtained from R-ACCEWS, Cu2(OH)2CO3 derived from P-ACCEWS exhibited superior dispersity and more regular morphology (Fig. 1B). Additionally, the alkali ratio of Na2CO3/NaHCO3 also affected the morphology of Cu2(OH)2CO3. In the R-ACCEWS system, increasing the Na2CO3 ratio caused R-Cu2(OH)2CO3 to evolve from irregular fine particles (∼40 nm) with severe agglomeration at 1
:
2 and 1
:
1 Na2CO3/NaHCO3 ratios to irregular flaky particles forming 5–6 µm flower-like clusters at 2
:
1 Na2CO3/NaHCO3. By contrast, the P-ACCEWS system showed distinctly different morphological evolution: well-dispersed 6–8 µm flaky particle clusters formed at a 1
:
2 Na2CO3/NaHCO3 ratio, transforming into densely packed ∼10 µm spherical aggregates at a 1
:
1 Na2CO3/NaHCO3 ratio, and finally yielding mixed spherical/thorny-flake morphologies (∼1 µm) at a 2
:
1 Na2CO3/NaHCO3 ratio. The findings confirmed that purification successfully eliminated etching solution-derived impurities, which was critical for achieving controlled nucleation and subsequent growth of Cu2(OH)2CO3 crystals (Fig. 1B).
The functional groups of Cu2(OH)2CO3 were investigated by FTIR. The characteristic absorption peaks at 460 cm−1 and 530 cm−1 assigned to Cu–O stretching vibrations are observed in Fig. 1C. Additionally, the spectral features observed at 1100 cm−1 and 1550 cm−1 were attributed to the symmetric and asymmetric stretching modes of carbonate (CO32−) groups, respectively. Comparative FTIR spectra demonstrated that the purification process substantially influenced the characteristic infrared absorption profiles of the synthesized products. The characteristic CO32− vibration modes at 1100 cm−1 and 1550 cm−1 exhibited significantly greater intensity for R-Cu2(OH)2CO3. This enhancement likely originated from carbonate impurities derived from metal ion leaching in the R-ACCEWS system during precipitation. Subsequent purification effectively eliminated these interfering ionic species, resulting in phase-pure Cu2(OH)2CO3. The variation in the Na2CO3 ratio notably influenced the hydroxyl group vibrational characteristics. With the Na2CO3 ratio increasing, all samples exhibited enhanced –OH peak intensities near 3400 cm−1, particularly prominent for P-Cu2(OH)2CO3 and R-Cu2(OH)2CO3 samples at a 1
:
1 Na2CO3/NaHCO3 ratio. These spectroscopic changes indicated that alkalinity facilitates Cu2(OH)2CO3 crystallization, while simultaneously enhancing hydrogen-bonding networks through increased hydroxyl group density in the precipitated phases.
As shown in Fig. 1D, R-Cu2(OH)2CO3 contained 54.40 wt%, 54.48 wt%, and 55.40 wt% copper for Na2CO3/NaHCO3 ratios of 1
:
2, 1
:
1, and 2
:
1 respectively, with corresponding metallic impurity contents of 0.26 wt%, 0.24 wt%, and 0.27 wt%, and chloride contents of 0.044 wt%, 0.090 wt%, and 0.042 wt%, respectively. In comparison, P-Cu2(OH)2CO3 from P-ACCEWS demonstrated copper contents of 55.40 wt%, 55.50 wt%, and 55.40 wt% at the same Na2CO3/NaHCO3 ratios, with metallic impurities measuring 0.21 wt%, 0.22 wt%, and 0.17 wt%, and chloride contents of 0.012 wt%, 0.014 wt% and 0.012 wt% respectively. The experimental results demonstrated that the purification treatment significantly improved the purity of Cu2(OH)2CO3. The copper content in P-Cu2(OH)2CO3 (55.40–55.50%) showed better consistency across different Na2CO3/NaHCO3 ratios and closer approximation to the theoretical value (55.42 wt%) compared to R-Cu2(OH)2CO3 (54.40–55.40 wt%). Furthermore, purification effectively reduced metallic impurities (0.17–0.22 wt% in P-Cu2(OH)2CO3 versus 0.24–0.27 wt% in R-Cu2(OH)2CO3) and substantially suppressed chloride residues (all ≤0.014 wt% in P-Cu2(OH)2CO3, with certain batches showing over 50 wt% reduction). Notably, iron content fell below the detection limit after purification, indicating particularly outstanding removal efficiency for specific metals. When evaluated against Chinese industrial standards for BBC, the copper content and chloride levels for P-Cu2(OH)2CO3 satisfied Class I product requirements, while Fe, Pb, Zn, Cr, Cd, and As contents complied with Class II standards. In contrast, the products prepared from R-ACCEWS contained excessive metallic impurities and failed to meet standard requirements.
The thermal behavior of as-prepared Cu2(OH)2CO3 was investigated by TGA in this work (Fig. 1E). The TGA curve of R-Cu2(OH)2CO3 exhibited multiple weight loss steps between 30 and 450 °C with a total weight loss of 48% attributed to the decomposition of Cu2(OH)2CO3 (eqn (1) and (2)) and impurities (eqn (4) and (5)). An additional 10% weight loss occurred between 480 and 980 °C, probably resulting from further decomposition of Cu2(OH)2CO3 (eqn (3)) and impurities with hydroxyl and carbonate groups. In contrast, the TGA curve of P-Cu2(OH)2CO3 displayed only one distinct weight loss step (25%) in the 30–320 °C range, mainly due to Cu2(OH)2CO3 decomposition (eqn (1) and (2)), followed by a gradual 9% weight loss between 400 and 1000 °C that may be caused by eqn (3).29,30
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The analytical results demonstrated that the purification pretreatment effectively removed Cl− and other impurities from the etching solution, thereby eliminating competitive interference during Cu2(OH)2CO3 crystallization and enabling consistent production of phase-pure, highly crystalline Cu2(OH)2CO3 across all Na2CO3/NaHCO3 ratios. The reduced impurity content promoted regular crystal growth, yielding better particle dispersion and more uniform morphologies (e.g., spherical clusters or thorny flakes), along with copper content substantially closer to theoretical values and fewer metallic impurities.
:
1) according to the process flow in Scheme 1, with reaction temperatures systematically varied at 50 °C, 70 °C, and 90 °C. As shown in Fig. 2A, temperature-dependent color evolution was observed: the 50 °C product formed fine blue powders, whereas both 70 °C and 90 °C conditions yielded distinct emerald-green particulate products. The SEM images (Fig. 2B) clearly revealed a significant morphological transition correlated with synthesis temperature: products obtained at 50 °C display uniformly shaped prismatic rods with well-developed facets (20–40 µm in length), contrasting sharply with the 70 °C product's nanostructure-assembled spherical secondary particles (approximately 10 µm in diameter). Most remarkably, elevated temperature (90 °C) processing led to the formation of defective spherical aggregates showing pronounced structural fragmentation.
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| Fig. 2 (A) Digital photograph, (B) SEM images, (C) XRD patterns, and (D) FTIR spectra of Cu2(OH)2CO3. (E) Cu contents and impurity contents of Cu2(OH)2CO3 obtained at different temperatures. | ||
Moreover, the precipitates obtained at 50 °C showed main diffraction peaks at 13.8°, 23.8°, 25.1°, 22.4°, 28.7° and 29.0°, corresponding to monoclinic Na2Cu(CO3)2(H2O)3 phase (JCPDS no. 87-0679) (Fig. 2C). In contrast, precipitates obtained at 70 °C and 90 °C displayed characteristic peaks at 14.8°, 17.6°, 25.1° and 31.2°, matching the monoclinic Cu2(OH)2CO3 phase (JCPDS no. 41-1390). These results illustrated that the reaction temperature significantly influenced both the phase composition and morphology of the products.
FTIR spectra of precipitates obtained at different temperatures showed characteristic peak variations with increasing temperature from 50 °C to 90 °C (Fig. 2D). The peaks at 3400 cm−1, 477–530 cm−1 and 1600 cm−1 assigned to –OH stretching vibration, Cu–O stretching vibration and CO32− absorption, respectively, were observed to be apparently enhanced, indicating complete conversion to Cu2(OH)2CO3 with increased intermolecular bonding. The spectral shift of coordinated CO32− asymmetric stretching (from 1550–1510 cm−1 to 1450–1500 cm−1) confirmed this structural evolution. Interestingly, the 70 °C products showed stronger CO32− signals than the 90 °C sample, suggesting temperature-induced morphological changes (particle fracturing) reduced functional group availability, this being consistent with the SEM results.
Fig. 2E demonstrates the temperature-dependent variations in copper content, metallic impurities, and chloride level of the synthesized products. Notably, the 50 °C product showed markedly reduced copper content (40.40 wt%, primarily Na2Cu(CO3)2(H2O)3 phase) compared to the 70 °C (55.44%) and 90 °C (55.48 wt%) products. Importantly, all synthesized products maintained chloride concentrations <0.015 wt% and acceptable metal impurity levels, validating the purification process's effectiveness. The characterization (XRD, SEM, FTIR and elemental analysis) conclusively established reaction temperature as the critical parameter governing both crystalline phase and morphological features. Optimal synthesis of phase-pure, morphologically uniform Cu2(OH)2CO3 required precise temperature regulation at 70 °C.
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1. Crude R-CuO exhibited main diffraction peaks at 14.8°, 16.1°, 17.5°, 24.0°, 31°, 32.5°, 32.6°, 35.5°, and 35.9°. According to the Powder Diffraction Database, the main characteristic peaks of rhombohedral Cu2Cl(OH)3 appeared at 16.1° (011) and 17.6° (101), while monoclinic Cu2(OH)2CO3 showed primary peaks at 14.7° (020), 24.0° (220), and 31.3° (20–1). The diffraction peaks of monoclinic CuO were at 32.6° (110), 35.4° (−111), and 38.8° (111). The phase composition analysis conducted using Jade 9.0 software confirmed the presence of three predominant crystalline phases in crude R-CuO: rhombohedral Cu2Cl(OH)3 (JCPDS no. 78-0372), monoclinic Cu2(OH)2CO3 (JCPDS no. 41-1390), and monoclinic CuO (JCPDS no. 89-5897).
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| Fig. 3 (A) XRD patterns; (B) SEM images; (C) FTIR spectra; (D) CuO contents and impurity contents; (E) TGA curves of R-CuO and P-CuO. | ||
The primary phases identified in crude P-CuO include monoclinic Cu2(OH)2CO3 (JCPDS no. 41-1390), monoclinic CuO (JCPDS no. 89-5897), and rhombohedral Cu2Cl(OH)3 (JCPDS no. 78-0372), with characteristic diffraction peaks observed at 12.4°, 14.8°, 16.1°, 17.5°, 24.0°, 31.5°, 32.5°, 32.6°, 35.5°, and 35.9°. Notably, the peak intensities of crude P-CuO at 16.1° (011) and 17.5° (101), corresponding to Cu2Cl(OH)3, were significantly weaker compared to those of crude R-CuO, indicating a substantial reduction in Cu2Cl(OH)3 content in crude P-CuO.
The XRD patterns demonstrated that CuO constitutes the dominant phase in both R-CuO and P-CuO, accounting for approximately 60% of the total diffraction peak intensity. The presence of Cu2Cl(OH)3 impurities originated from chloride ions (Cl−) in the raw etching solutions, whose complexation with Cu2+ ions inhibited complete hydrolysis. However, the purification effectively reduced the Cu2Cl(OH)3 content in crude P-CuO. The presence of residual Cu2(OH)2CO3 indicated incomplete precursor decomposition, caused by an insufficient hydrothermal temperature (95 °C).
The crude P-CuO and R-CuO exhibited significant particle agglomeration (30–40 nm) (Fig. 3B), ascribed to the 95 °C hydrothermal reaction temperature, which favors smaller nanoparticle formation. Additionally, incomplete decomposition of Cu2(OH)2CO3 during the process might result in residual CO32− or OH− adsorbed on particle surfaces. These species could form bridging bonds (e.g., Cu–O–CO3–Cu), thereby connecting individual particles into aggregates.
FTIR spectra demonstrated that crude P-CuO exhibited stronger absorption peaks at 1110 cm−1 (CO32−) and 530 cm−1 (Cu–O), possibly due to its higher crystallinity and larger particle size leading to more incomplete thermal decomposition, which enhanced the vibrational signals of Cu–O bonds and CO32− groups (Fig. 3C). In contrast, crude R-CuO showed significantly weaker signals near 3400 cm−1 (–OH) and 1400 cm−1 (H–O–H), possibly caused by its higher content of hydroxyl impurities.
Furthermore, crude R-CuO contained 50.4 wt% CuO, with 0.42 wt% metallic impurities and 0.0052 wt% chloride. In comparison, crude P-CuO demonstrated significantly improved purity with 58.42 wt% CuO content, along with reduced metallic impurities (0.23 wt%) and lower chloride content (0.0022 wt%) (Fig. 3D). These results confirmed that the purification treatment effectively enhanced the CuO content while simultaneously decreasing both metallic and chloride impurity levels in the crude CuO.
The TGA curves of crude R-CuO and P-CuO showed distinct differences (Fig. 3E). For crude R-CuO, the weight loss was 15% at 30–240 °C, 10% at 240–300 °C, 8% at 300–450 °C, and 4% at 450–600 °C, with a total weight loss of 37%. In comparison, crude P-CuO exhibited weight losses of 2% (30–230 °C), 4% (230–270 °C), 15% (270–300 °C), and 2% (300–600 °C), resulting in a significantly lower total weight loss of 23%. The thermogravimetric results confirmed the significant differences in thermal behavior between crude R-CuO and crude P-CuO. Crude P-CuO exhibited only a 3% weight loss in the 30–230 °C range, primarily attributed to adsorbed water removal, whereas crude R-CuO showed substantially higher weight loss (15%) due to combined water desorption and thermal decomposition of impurity compounds (Fe, Ca) (eqn (1), (4) and (6)).31 The subsequent weight losses of crude P-CuO at 230–270 °C and 270–300 °C correspond to the decomposition of Cu2(OH)2CO3 (eqn (1) and (2)) and Cu(OH)2 pyrolysis (eqn (3)), respectively, with a total weight loss of 23% – markedly lower than crude R-CuO weight loss of 34%. This discrepancy confirmed that crude P-CuO contains significantly reduced chloride and impurity content, as evidenced by the absence of substantial weight loss contributions from Cu2Cl(OH)3 decomposition (eqn (7) and (8)) that account for 22% of crude R-CuO's total weight loss between 240 and 600 °C. Ultimately, crude P-CuO achieves higher CuO content (58.42% vs. 50.4% in crude R-CuO), validating that purification effectively removed Fe/Ca impurities and chlorides, minimized thermal decomposition losses, and enhanced both product purity and effective CuO yield.
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| Fig. 4 (A) XRD patterns, (B) SEM images, and (C) FTIR spectra of products calcined at different temperatures. CuO contents and impurity contents of (D) R-CuO and (E) P-CuO. | ||
As shown in Fig. 4B, both R-CuO (300 °C) and R-CuO (400 °C) consisted of irregularly shaped fine particles. The particle size of R-CuO (500 °C) was approximately 100 nm with severe agglomeration, while R-CuO (600 °C) displayed particles of around 110 nm in size, accompanied by significant particle aggregation. In contrast, P-CuO (300 °C) presented well-defined nanoparticles. P-CuO (400 °C) clearly displayed porous structures, forming aggregated morphologies composed of sheet-like, needle-like, and fine particulate components. Both P-CuO (500 °C) and P-CuO (600 °C) demonstrated regular morphologies with uniform particle sizes ranging from 110 to 120 nm.
The morphological differences between R-CuO and P-CuO reflected the crucial influence of precursor composition and calcination temperature on crystallization behavior and particle growth kinetics.32 In the R-CuO series, both 300 °C and 400 °C calcined products consisted of irregular fine particles without significant morphological differences, indicating weak temperature effects on nucleation processes below 400 °C. When the temperature increased to 500 °C, the particle size grew to approximately 100 nm with severe agglomeration. In contrast, the P-CuO series exhibited distinct growth characteristics. Obviously, the 300 °C product formed extremely small-sized particles, while at 400 °C, distinct pore structures appeared along with complex aggregates composed of sheet-like, needle-like, and fine particulate morphologies. When the temperature reached 500–600 °C, the products transformed into uniform nanoparticles (110–120 nm) with well-defined shapes, suggesting that the purified precursor favors the formation of size-controlled nanostructures at high temperatures. This divergence likely originated from altered thermal decomposition pathways due to impurity removal during the etching purification process, which subsequently modified the anisotropic growth behavior of CuO crystals.
As shown in Fig. 4C, all CuO calcined below 500 °C exhibited –OH stretching (3400 cm−1) and bending (1600 cm−1) peaks, indicating incomplete decomposition of Cu(OH)2. When the temperature rose to 600 °C, the –OH peaks weakened significantly, showing complete hydroxyl removal and formation of a perfect CuO crystal structure. Meanwhile, the Cu–O characteristic peaks at 460–530 cm−1 become sharper and stronger with increasing temperature, illustrating CuO grain growth and improved crystallinity. Additionally, all products below 500 °C showed a CO32− peak near 1200 cm−1 from residual Cu2(OH)3CO3, which disappeared completely after 600 °C calcination, confirming its full decomposition.
The CuO content and impurity level of R-CuO and P-CuO are shown in Fig. 4D and E. The test results showed that the CuO contents of R-CuO (300 °C, 400 °C, 500 °C, 600 °C) were 68.48 wt%, 82.24 wt%, 94.48 wt%, and 97.90 wt% respectively, with metal impurity contents of 0.29 wt%, 0.24 wt%, 0.22 wt%, and 0.20 wt%, and chloride contents of 0.0040 wt%, 0.0020 wt%, 0.0014 wt%, and 0.0014 wt%. In contrast, the CuO contents of P-CuO (300 °C, 400 °C, 500 °C, 600 °C) were 80.24 wt%, 92.24 wt%, 98.54 wt%, and 98.80 wt% respectively, with metal impurity contents of 0.22 wt%, 0.15 wt%, 0.15 wt%, and 0.11 wt%, and chloride contents of 0.0014 wt%, 0.0013 wt%, 0.0012 wt%, and 0.0012 wt%. The experimental results demonstrated that purification treatment and calcination had a synergistic optimization effect on the preparation process of CuO. At the same calcination temperature, P-CuO exhibited higher CuO content (e.g., 80.24 wt% purity at 300 °C compared to 68.48 wt% for R-CuO) and lower impurity levels (both metallic impurities and chlorides). Notably, R-CuO forms a Cu2Cl(OH)3 impurity phase at 300 °C due to residual chlorides, while this phenomenon was absent for P-CuO, confirming that purification effectively reduced chloride influence. As the calcination temperature increases (300–600 °C), the CuO content of the calcined products significantly improved and impurity levels gradually decreased. However, P-CuO maintains lower residual metallic impurities (0.11 wt% at 600 °C vs. 0.20 wt% for CuO–O) and chlorides (0.0012 wt% vs. 0.0014 wt%), demonstrating that purification treatment can synergistically enhance product purity with calcination.
The XPS spectra of R-CuO (600 °C) and P-CuO (600 °C) are shown in Fig. 5A and B, respectively. In the Cu(2p) spectra of both samples, the results revealed Cu 2p3/2 (933.5–934.5 eV) and Cu 2p1/2 (953.5–954.5 eV) peaks, confirming the presence of Cu in +2 oxidation state (Cu2+) with no detectable Cu+ or Cu0. The C 1s spectrum of R-CuO clearly showed a C
O peak (291.5 eV), suggesting that the precursor solution may contain incompletely removed organic additives (such as complexing agents, stabilizers or surfactants) that remained on the CuO surface. The purification process (including filtration, ion exchange and centrifugation) likely effectively removed these organic impurities, as evidenced by the absence of C
O peak in P-CuO's C1s spectrum. In the O 1s spectra, R-CuO exhibited significantly higher binding energy, indicating the precursor solution may contain oxidative impurities (such as residual H2O2, nitrates or sulfates) that formed high-valence oxygen species during preparation. This could also result from impurity doping or increased oxygen vacancies, causing lattice distortion, thereby elevating the O 1s binding energy. Meanwhile, the purification process removed these impurities, resulting in predominantly lattice oxygen in the product and consequently lower overall O 1s binding energy for P-CuO.
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| Fig. 5 XPS spectra of (A) R-CuO and (B) P-CuO. TEM images of (C) R-CuO and (D) P-CuO calcined at 600 °C. | ||
The TEM images showed that R-CuO particles (Fig. 5C) were nearly spherical with mixed rod-like flake particles, having sizes of 110–120 nm and exhibiting some agglomeration, likely due to high surface energy causing aggregation through van der Waals forces or –OH interactions. In contrast, P-CuO (Fig. 5D) displayed more uniform spherical particles of about 110 nm. HRTEM images in Fig. 5C and D revealed that both products have a lattice spacing of 0.23 nm, corresponding to the (200) plane of a CuO crystal.
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| Fig. 6 (A) XRD patterns, (B) SEM images, and (C) FTIR spectra of CuO. (D) CuO contents and impurity contents of CuO calcined for different times. | ||
The SEM images in Fig. 6B demonstrated that P-CuO (2 h) exhibited particle sizes of approximately 110–130 nm with noticeable particle agglomeration. With prolonged calcination time, P-CuO (3 h) and P-CuO (4 h) showed slightly increased particle sizes and expanded interparticle gaps, along with reduced agglomeration. This phenomenon primarily resulted from extended calcination, promoting tighter particle contact, where grain boundary migration led to coalescence into single crystals.33 Additionally, gas released during precursor decomposition created micropores at original sites, and prolonged calcination facilitates pore interconnection, forming more interparticle voids.
The FTIR spectra in Fig. 6C revealed that temperature significantly affects the –OH absorption near 3424 cm−1. When the calcination time reaches 4 h, the –OH absorption peak nearly disappears, primarily due to thermal decomposition of the basic copper carbonate precursor Cu2(OH)2CO3 during calcination, resulting in –OH group elimination. At the same time, the Cu–O stretching vibration peak at 530 cm−1 showed no significant changes.
The CuO contents and impurity contents of P-CuO prepared with different calcination durations are presented in Fig. 6D. The products calcined at 600 °C for 2 h, 3 h, and 4 h showed CuO contents of 98.98 wt%, 99.04 wt%, and 99.08 wt%, respectively, with total metal impurities below 0.12% and chloride content under 0.0015% in all cases. The results indicated that prolonged calcination time hardly altered the CuO contents of P-CuO, demonstrating complete thermal decomposition of CuO precursors (e.g., Cu2(OH)2CO3) and common impurity phases (e.g., Cu2Cl(OH)3), along with thorough oxidation of intermediate crude CuO products.
Purified ACCEWS (P-ACCEWS): a quantitative amount of R-ACCEWS was placed in a beaker with magnetic stirring at room temperature. NaOH solution and Na2CO3 solution of different concentrations were added to the beaker to adjust the pH of the solution to a specific value. After standing for 12 h to stabilize their pH value upon re-measurement, the solutions were filtered to obtain P-ACCEWS. The details of the purification procedure have been reported in our previous work.40
Other reagents: sodium hydroxide (AR, Chengdu Jinshan Chemical Reagent Co. Ltd), sodium carbonate (AR, Chengdu Kelong Chemical Reagent Factory), sodium bicarbonate (AR, Chengdu Kelong Chemical Reagent Factory), nitric acid (AR, Chengdu Kelong Chemical Co. Ltd), phosphoric acid (AR, Chengdu Jinshan Chemical Reagent Co. Ltd), sulfuric acid (AR, Chengdu Kelong Chemical Co. Ltd), potassium iodide (AR, Tianjin Beichen Fangzheng Reagent Factory), sodium thiosulfate (AR, Guangzhou Howei Pharmaceutical Technology Co. Ltd), starch indicator (Guangzhou Howei Pharmaceutical Technology Co. Ltd), silver nitrate (AR, Chengdu Kelong Chemical Co. Ltd), acetic acid (AR, Chengdu Jinshan Chemical Reagent Co. Ltd), sodium fluoride (AR, Ron Reagent), national standard reference material GSB 04-1767-2004 (Al, As, B, Ba, Be, Bi, Cd, Co, Cr, Cu, Fe, Ga, Li, Mg, Mn, Ni, Pb, Sb, Sn, Ti, V, Zn; National Analysis Center for Nonferrous Metals & Electronic Materials), national standard reference material GSB 04-1770-2004 (Cl; National Analysis Center for Nonferrous Metals & Electronic Materials), copper(II) carbonate basic reference standard (AR, Shandong Keyuan Biochemical Co. Ltd), copper(II) oxide reference standard (99%, Chengdu Jinshan Chemical Reagent Co. Ltd).
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1 liquid–solid ratio) to form a slurry. After preheating to 95 °C and adjusting the pH to 12 using 10 mol L−1 NaOH solution, the mixture was stirred for 120 min at 95 °C. The products were hot-filtered, ultrasonically washed 3 times with DI water, and dried at 105 °C for 2.5 h to obtain crude CuO (crude R-CuO or crude P-CuO). Final calcination at varying temperatures followed by furnace cooling produced high-purity R-CuO or P-CuO. The fabrication process is shown in Scheme 2.
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Firstly, Solution B (10 mL) was placed into a colorimetric tube (50 mL). Then 2 mL nitric acid solution was added to Solution B and then diluted to 40 mL with DI water. Finally, silver nitrate solution (1 mL) was added to the solution and diluted to the mark (50 mL). The as-prepared solution was allowed to stand for 10 min for turbidity comparison with the standard turbidity solution, which was prepared by mixing 10 mL of solution A and 5 mL chloride standard solution.
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(1) The purification process efficiently eliminated chloride ions and metallic impurities from the precursor materials, substantially enhancing the purity of both Cu2(OH)2CO3 and CuO products. Furthermore, it modified the crystallization kinetics and particle aggregation patterns, resulting in copper compounds with distinct phase compositions and morphological characteristics.
(2) Uniform spherical Cu2(OH)2CO3 was synthesized using purified ACCEWS as the copper source under optimized conditions: 1
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1 Na2CO3/NaHCO3 molar ratio, 70 °C reaction temperature, and 1 h duration. The resulting product exhibited high purity with 55.52 wt% copper content, while maintaining impurity levels below 0.24 wt% for total metals and 0.05 wt% for chloride. These specifications satisfied the Class I chloride standard (≤0.05 wt%) and Class II metal impurity standard (≤0.3 wt%) as specified in HG/T 4825-2015 for high-purity basic copper carbonate.
(3) High-purity Cu2(OH)2CO3 was hydrothermally converted to CuO using NaOH solution under low-temperature conditions. The intermediate product contained 58.42 wt% CuO, with total metallic impurities below 0.20 wt% and chloride content under 0.0015 wt%. Subsequent calcination at 600 °C for 3 hours produced high-purity CuO, achieving 99.04 wt% purity, metallic impurities below 0.12 wt%, residual chloride content under 0.0015 wt%, and a controlled average particle size of ∼110 nm.
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