Open Access Article
Meng Tian
and
Xianglan Zhang*
School of Chemical and Environmental Engineering, China University of Mining and Technology (Beijing), No. Ding 11, Xueyuan Road, Haidian District, Beijing 100083, PR China. E-mail: zhxl@cumtb.edu.cn; Tel: +86-135-2170-3609
First published on 8th December 2025
Recycling metal materials from waste copper clad laminate (WCCL) in a pollution-free and efficient way holds significance for the comprehensive utilization of resources. This study used waste paper-laminated copper clad laminate (PL-WCCL) as a raw material and conducted pyrolysis in a rotary furnace. The variations of the functional groups in PL-WCCL and the non-metallic part of PL-WCCL under different conditions were analyzed by thermogravimetric coupled Fourier transform infrared spectroscopy (TG-FTIR). The liquid-phase products were analyzed using gas chromatography-mass spectroscopy (GC-MS), and the morphology of the solid-phase products and the contact surfaces of the metal and non-metal parts of PL-WCCL were determined by photography and scanning electron microscopy-energy dispersive X-ray spectroscopy (SEM-EDS). The results indicate that the maximum weight loss rate of PL-WCCL is 62.48%, and the activation energy (E) is 29.84 kJ mol−1. During the pyrolysis, copper can lower the beginning reaction temperature, facilitate the release of bromine and chlorine, accelerate the synthesis of lighter hydrocarbons, and increase the release of CO2. The optimal conditions are as follows: a retention time of 60 min at 150 °C and a filling capacity of 51.95 g L−1, resulting in a 100% separation rate of metal, without requiring crushing. The liquid organic products obtained were merely phenol and o-cresol. This research introduced a comprehensive green processing method utilizing a rotary furnace as the reactor to effectively extract metallic copper from PL-WCCL.
Various technologies, including physical method,7 organic solvent swelling method,8 hybrid processes9 and pyrolysis method,10 have been employed to recycle copper from waste copper clad laminate (WCCL). Both the organic solvent swelling method and the hybrid process method are confined to laboratory studies and have not been utilized for large-scale recycling activities. It is the physical method that is widely adopted in industries for the recovery of copper. However, the recovery of the metal via the physical method typically involves shattering the sheet material into smaller pieces or even powder,11,12 and the metal is separated from non-metals under shear forces during this process, achieving a metal-recovery efficiency ranging from merely 65% to 90%.13 However, the recovery of the metal via the physical method involves a relatively large number of subsequent steps. Besides, if the reinforcing materials of the WCCL are wood pulp papers, it tends to adhere to the crushing machinery, which complicates the separation process of metals from non-metals and hinders the efficient recycling of metals from waste paper-laminated copper clad laminate (PL-WCCL).14
Pyrolysis, which is a potential technology and commonly used in recovering metals from WCCL, breaks down high-molecular polymers and destroys the bonding force between metals and non-metals of WCCL through heating, facilitating the separation of the metal and improving the metal recovery rate.15 Further, while generating high-value hydrocarbons, this technology significantly reduces the volume and recovers more energy.16 However, the halogen flame retardants contained in non-metal materials in WCCL commence decomposition at 280 °C,17 potentially generating persistent organic pollutants (POPs), such as poly-brominated diphenyl ethers (PBDEs), presenting health and safety hazards to humans and the environment.18 The inadequate handling of POPs may severely contaminate the ecological environment.19,20 Therefore, investigating effective approaches to separate and recover metals from PL-WCCL, as well as mitigating the environmental impact associated with non-metal parts, holds considerable practical value for the resourceful utilization of PL-WCCL.
The design and selection of the reactor, along with the control and modulation of experiment conditions, exert a significant influence on the separation efficiency of metals and non-metals in PL-WCCL via pyrolysis. There are relatively few studies that explicitly use large-sized PL-WCCL as the experimental material and conduct research on metal separation via pyrolysis. For example, Liu et al. conducted pyrolysis of PL-WCCL at 300 °C in a fixed-bed reactor. After that, the metal separation rate reached 100%, indicating that intact copper foil sheets could be manually stripped.21 CCL is the fundamental component in the production of PCBs. From the perspective of composition, WCCL can almost be regarded as the same material as WPCBs without electronic components. Thus, the research regarding the separation of metals and non-metals of WPCBs through pyrolysis can be referenced.
Researchers have employed the fixed-bed reactor to conduct the pyrolysis of large-sized WPCB without electronic components and investigated the variation of the metal separation rate by controlling the temperature, reacting atmosphere and retention time.
Yan G. et al.22 conducted pyrolysis treatment on waste printed circuit boards (WPCBs). At 200 °C, the copper separation rate reached 85.66%. Kim B. et al.23 performed pyrolysis treatment on WPCBs and found that copper was enriched in the raw materials, with large particle sizes obtained at 300 °C. Chen Y. et al.13 carried out pyrolysis treatment on WPCBs and obtained a copper recovery rate of 92.38% at 330 °C. Guo X. et al.24 conducted pyrolysis treatment on WPCBs and found that at 500 °C, the metal and non-metal parts could be manually peeled apart. Long L. et al.25 performed pyrolysis treatment on WPCBs and found that at 550 °C, copper was enriched in the raw material particles with particle sizes larger than 0.45 mm, and the separation rate was approximately 99%. However, Ma H. et al.26 found that when performing pyrolysis treatment on WPCBs at 800 °C in a fixed-bed reactor equipped with a stirring function, the copper foil and non-metal parts could be automatically separated after the pyrolysis process was completed.
Current studies on the separation the metals and non-metals of WPCBs reveal that conducting the pyrolysis process under a fixed temperature range of 200 to 550 °C for 30 to 120 min in a fixed-bed reactor, whether in an air atmosphere, nitrogen atmosphere, or vacuum, enables easier separation of metals and non-metals and increases the metal recovery rate. However, after the pyrolysis process, further crushing, screening, sorting, or manual peeling is necessary. The addition of the stirring function to the fixed-bed reactor is conducive to the separation of the copper foil and non-metals, eliminating the need for further crushing and manual peeling. However, the above-mentioned literature studies did not address the release of non-metallic pollutants during the pyrolysis process. Currently, studies on the separation of metals and non-metals from WPCB or WCCL are mainly carried out in fixed-bed reactors, and there are no public reports on rotary furnaces.
The rotary furnace is a common type of industrial furnace. The materials within it rotate along with the furnace body under the drive of the blades. After rising to the highest point, the materials return to the bottom of the rotary furnace along the furnace bed.27 In a rotary furnace, the materials not only rotate but also undergo translation and collision,28 and these vigorous movement enhances the flow and heat transfer of the materials, ensuring thorough mixing.29 Moreover, rotary furnaces have a simple structure and wide adaptability to different types and sizes of raw materials while being convenient to operate. In pyrolysis experiments using the rotary furnace, most researchers adjust the parameters, such as the temperature, rotation speed, inclination angle of the reactor, particle size of the raw materials, and gas flow rate. The aim is to make the yield and composition of the final pyrolysis products comparable to those obtained when using a fluidized-bed reactor.28 Zhu Y. et al.30 designed a pilot-scale rotary kiln pyrolysis furnace featuring a hierarchical condensation function. By applying the method of controlling variables, they analyzed the impacts of temperature, moisture content of materials, and condensate water flow rate on the distribution of three-phase pyrolysis products of waste printed circuit boards (WPCBs).
Therefore, this study aims to capitalize on the prominent advantages of the rotary furnace to explore the optimal conditions for the automatic separation of metals and non-metal parts of PL-WCCL during the pyrolysis. Additionally, it endeavors to recycle metals with lower energy consumption by streamlining the technological process. Meanwhile, through the analysis of the distributions of gas, liquid, and solid-phase products at different pyrolysis temperatures and the composition of the liquid-phase products, secondary pollution resulting from the decomposition of halogen-containing flame retardants can be circumvented. In comparison with conventional physical methods for metal separation and recovery, the proposed method can ensure a relatively high separation efficiency while significantly reducing the number of subsequent separation process steps. It thus lays the foundation for the “green recycling”31 industry of metals and non-metals in PL-WCCL.
30.000 g of PL-WCCL was taken, and the copper foil and non-metal parts were separated manually and weighed separately. The contents of metals and non-metals contained in the PL-WCCL are 3.2056 g and 26.7964 g. The content of Cu in PL-WCCL was calculated to be 11%.
Elemental analysis and X-ray fluorescence (XRF) analysis were conducted on the non-metallic part of waste paper laminated-copper clad laminate (PL-NMWCCL), and the experimental results are listed in Tables 1 and 2, respectively. Table 1 shows that the content of carbon in PL-NMWCCL is 46.22%, indicating a high content of organic matter. In Table 2, the contents of chlorine and bromine in PL-NMWCCL account for 80% of all the elements measured, and the content of chlorine is about twice that of bromine.
| C/wt% | H/wt% | O/wt% | N/wt% | S/wt% |
|---|---|---|---|---|
| 46.22 | 4.02 | 22.48 | 4.95 | 0.13 |
| Element | Relative content % | Element | Relative content % |
|---|---|---|---|
| Br | 29.837 | Fe | 1.222 |
| P | 2.815 | Ca | 0.552 |
| Cr | 2.241 | S | 0.249 |
| Al | 1.971 | Na | 0.225 |
| Si | 1.715 | Zn | 0.025 |
| Cl | 49.497 |
(1) The influence of the pyrolysis temperature and time: about 30 g of PL-WCCL with a particle size of 4 cm × 2 cm (the corresponding number of filling blocks is denoted as Q0) was placed in the rotary furnace. N2 gas (99.9%) was injected into the rotary furnace at a flow rate of 100 mL min−1, and the rotation speed was 2.44 rpm. The pyrolysis temperature was raised at a rate of 5 °C min−1 to varying final temperatures (150, 200, 250, 300, and 350 °C), and the retention time was set to 30 min or 60 min.
(2) The influence of the varying amounts of PL-WCCL added: with the pyrolysis temperature fixed at the temperature required to achieve the above-mentioned optimal metal separation rate and a retention time of 60 min, the separation status of metal and non-metal under the conditions of varying raw material amounts of 50 g, 100 g, and 150 g was investigated.
(3) Comparison between rotary furnaces and fixed furnaces: at the temperature corresponding to the aforementioned optimal metal separation rate, 50 g of PL-WCCL was put into a rotary furnace and a fixed furnace, separately, and the retention time was 60 min.
Through statistically counting the quantity Q1 of metals after complete separation, the metal separation rate was obtained using eqn (1). The yields of the solid and liquid products are calculated by eqn (2) and (3), respectively, and the yield of gas products was obtained using the mass balance eqn (4).
![]() | (1) |
![]() | (2) |
![]() | (3) |
| Yg = 100% − Ys − Yl | (4) |
Among them, Sm represents the metal separation rate; M0 is the mass of the raw materials added, Ma is the mass of the non-metallic product from pyrolysis, and Mb is the mass of the liquid-phase product from pyrolysis.
The name of the pyrolysis products was designated as “raw material + furnace type + temperature + product form” (The first letter of the word represents itself, like G for gas, S for solid, L for liquid, SI for solid interface between metal part and non-metal part). Regarding the short expression of the raw material, PW is waste paper laminated copper clad laminate (PL-WCCL), MPW represents the metal part of PL-WCCL and NPW is the non-metallic part of waste paper laminated copper clad laminate (PL-NMWCCL). For instance, PW-F-150-L indicates the liquid product of PL-WCCL after pyrolysis at 150 °C in a fixed furnace; NPW-R-300-S represents the solid product of PL-NMWCCL after pyrolysis at 300 °C in a rotary furnace. When cross-sectional characterization of the solid product is necessary, “CS” is added to the end, like NPW-R-300-S-CS.
| Raw materials | Initial temperature/°C | Peak temperature/°C | Final temperature °C | Weight loss/% |
|---|---|---|---|---|
| PL-WCCL | 250 | 278 | 484 | 62.48% |
| PL-NMWCCL | 252 | 277 | 473 | 66.51% |
As shown in Fig. 3, there is no significant difference in the TG curves of PL-WCCL and PL-NMWCCL. The initial decomposition temperature of PL-WCCL is 250 °C and that of PL-NMWCCL is 252 °C (Fig. 3b). Regarding the termination decomposition temperature, it is 484 °C for PL-WCCL and 473 °C for PL-NMWCCL. The maximum weight loss rate of PL-WCCL is 62.48% and that of PL-NMWCCL is 66.51%. During the pyrolysis, the temperature range of the thermal weight loss of PL-WCCL is broader than that of PL-NMWCCL, suggesting that the metal Cu contained in PL-WCCL has a certain influence on the pyrolysis, although the influence is relatively minor.20,32–34
The PL-WCCL pyrolysis is a relatively complex solid-state thermal decomposition process,35 which can be represented by the following reaction function in eqn (5):
| A(solid) → B(solid) + C(volatile) | (5) |
Consequently, the reaction rate equation during the pyrolysis process is eqn (6):
![]() | (6) |
. f(α) is the reaction mechanism function, α is the conversion rate and can be calculated byIf f(α) = (1 − α)n, dt = dT/β (β is the heating rate, K s−1), eqn (6) can be converted into eqn (7):
![]() | (7) |
Eqn (7) and (8) are integrated to obtain the following:
![]() | (8) |
The Coats–Redfern integration model method is employed to fit and solve eqn (8), which can calculate the kinetic parameters for PL-WCCL pyrolysis in different stages of pyrolysis using a TG curve. The Coats–Redfern integration model method can be expressed as eqn (9):
![]() | (9) |
After performing integration on eqn (8), if n = 1, the Coats–Redfern function is converted into eqn (10):
![]() | (10) |
If n ≠ 1, the Coats–Redfern function is converted into eqn (11):
![]() | (11) |
, and eqn (10) and (11) can be simplified as eqn (12) and (13), respectively:
![]() | (12) |
![]() | (13) |
can then be achieved by solving a univariate quadratic equation (y = kx + b). Therefore, the pyrolysis activation energy and pre-exponential factor can be derived. The correlation coefficient r2, pyrolysis activation energy, and pre-exponential factor calculated by adopting different n values are listed in Table S1.
By employing the C–R method, it was calculated that when the kinetics n of PL-NMWCCL was 1.5, R2 was 0.98, the activation energy E was 31.95 kJ mol−1, and the pre-exponential factor A was 1.303 × 103 min−1. When the kinetics n of PL-WCCL was 1.5,36 R2 was 0.97, the activation energy E was 29.84 kJ mol−1, and the pre-exponential factor A was 5.035 × 102 min−1. The activation energy required for the pyrolysis of PL-WCCL with insulating paper as the substrate was lower than that of FR4-WCCL, with the glass fibres as the substrate (144.11 kJ mol−1).29
![]() | ||
| Fig. 4 3D-FTIR spectra of the volatile products at 30–850 °C: (a) PL-NMWCCL and (b) PL-WCCL. FTIR curves of the C–Cl bond and C–Br bond at various temperatures: (c) PL-NMWCCL and (d) PL-WCCL. | ||
Fig. 5 presents the FTIR curves of the volatile products resulting from the pyrolysis at various temperatures. From Fig. 5a and b, the infrared peak intensities of both PL-NMWCCL and PL-WCCL reach the maxima at 300 °C. The peaks at 750 cm−1 and 2933 cm−1 are likely attributed to the presence of –(CH2)n–, with n ≤ 3. When combined with the peaks at 1195 cm−1, 1364 cm−1, and 1394 cm−1, it can be deduced that there exists an isopropyl structure, –CH(CH3)2.39 The peaks at 1512 cm−1, 1542 cm−1, and 1554 cm−1 are characteristic of the C
C bond vibration of the benzene ring. The C–H bond vibration wave peaks of the benzene ring, –C6H5, at 1700–1769 cm−1 and 795 cm−1 could highlight that the substitution on the benzene ring is of the 1, 3, 5, 6 type.40 The peak at 1233 cm−1 corresponds to the C–O bond stretching vibration of the fatty ether, while the peak at 1064 cm−1 is the C–O bond stretching of the benzyl ether molecular skeleton.
![]() | ||
| Fig. 5 FTIR of the volatile products at 30–850 °C: (a) PL-NMWCCL and (b) PL-WCCL. Variations of three functional groups at 30–850 °C: (c) PL-NMWCCL and (d) PL-WCCL. | ||
The variations of the above-mentioned three functional groups within the temperature range of 30–850 °C are depicted in Fig. 5c and d. It can be observed that for PL-NMWCCL, the release intensity of the functional groups reaches the maximum at 285 °C, with that for –C6H5 being 0.0049 a.u., –CH(CH3)2 being 0.0036 a.u., and –O– being 0.0029 a.u. For PL-WCCL, the release intensity of the functional groups also peaks at 285 °C, with that for –C6H5 being 0.0046 a.u., –CH(CH3)2 being 0.0043 a.u., and –O– being 0.0043 a.u. The release amounts of –CH(CH3)2 and –O– bond in PL-WCCL are more than those in PL-NMWCCL, which indicates that the Cu contained in 1 mm2 of the blocky material can also accelerate the generation of lighter hydrocarbons.41
Fig. 6 presents the gaseous products at various pyrolysis temperatures. The range of 2327–2364 cm−1 is the characteristic spectrum of the CO2 gas;42,43 the 3015 cm−1 band represents CH4 gas, and the peak at 3742 cm−1 is the stretching vibration of the –OH bond; thus, the range of 3855–3901 cm−1 corresponds to H2O.44
![]() | ||
| Fig. 6 FTIR of the gaseous products of pyrolysis at various temperatures: (a) PL-NMWCCL and (b) PL-WCCL. | ||
Fig. 6 describes that when PL-NMWCCL and PL-WCCL undergo pyrolysis at different temperatures, the release of CO2 and H2O reaches the maximum at approximately 300 °C. After experiencing a period of decline, from 700 °C, the release of CO2 continues to increase rapidly, and the release amount of PL-WCCL is slightly higher than that of PL-NMWCCL. The maximum absorbance of CO2 for PL-NMWCCL is 0.0301 a.u., while for PL-WCCL, it is 0.0357 a.u. The release of CH4 reaches the maximum at around 500 °C, but no peaks of HCl and HBr are present. The beginning pyrolysis temperatures of PL-WCCL and PL-NMWCCL are 135 °C and 167 °C, respectively, which means that the presence of Cu would decrease the beginning temperatures of pyrolysis and increase the amount of CO2 released.42,43,45 This is also consistent with the conclusion drawn from the thermogravimetric curves.
![]() | ||
| Fig. 7 Influence of the pyrolysis temperature and retention time on the metal separation rate of PL-WCCL. | ||
Fig. 8 depicts the influence of different furnace types and raw material dosages on the metal separation rate of PL-WCCL at a pyrolysis temperature of 150 °C and a retention time of 60 minutes. As illustrated in Fig. 10b, the metal separation rate in the fixed furnace is merely 16.7%, while it is 100% in the rotary furnace, suggesting that the rotation of the rotary furnace is the primary factor for the separation of metals from non-metals. When the dosage of PL-WCCL is 30 g and 100 g, the metal separation rate is 100%, and the loading capacity of the rotary furnace at this time is 51.95 g L−1. Conversely, when the dosage of PL-WCCL is increased to 150 g, the metal separation rate decreases to 74.57%.
Table S2 presents a summary of the published literature about the separation of the metal and non-metal components of PL-WCCL through pyrolysis, encompassing the processing conditions, reactor types, subsequent steps needed and the metal separation rate achieved. Obviously, when the conditions of the stirring function for the reactor and a high processing temperature of 800 °C are available, the subsequent steps, including crushing or peeling off manually, are not necessary to complete the separation of the metal from the non-metal. Moreover, compared to other emerging low-temperature processes (such as organic solvent methods and combined processes), the proposed method requires less time, exhibits lower energy consumption, and generates minimal pollution. Compared with the physical method46 in Fig. 9a, the pyrolysis in the rotary furnace is capable of not only automatically separating the metals and non-metals of PL-WCCL under 150 °C but also of reducing the number of processing steps from six to two (Fig. 9b). Furthermore, when compared to the physical method for separating metals and non-metals in WPCB, the low-temperature rotary process can reduce energy consumption by at least 70%.47,48
The morphology and the EDS spectrum analysis of the contact surfaces of both sides after manual delamination of the metal and non-metal in PL-WCCL are depicted in Fig. 13. As shown in Fig. 13a, the surface of the delaminated Cu foil consists of bright dots and lamellar structures. Through EDS analysis of the entire area, it can be observed that the granular bright dots in the figure are copper particles. The elements of bromine and chlorine are distributed densely and uniformly, with a bromine–chlorine ratio of 1
:
3, and 13.5% of the non-metal residue is present on the surface of the Cu foil in this area. It can be obtained from Fig. 13b that the non-metal is tightly bonded with a dense internal structure. The elements of bromine and chlorine are distributed evenly and densely. The bromine–chlorine ratio is consistent with that in the metal, and elements such as sodium, silicon, and iron are also detected.
Fig. 14 is the SEM images of the contact surfaces between the metal and non-metal parts of PL-WCCL after the pyrolysis for 60 min at various temperatures. Fig. 14a–e depict the SEM images of the contact surfaces of the metal part of PL-WCCL in the temperature range of 150 °C to 350 °C, and Fig. 14f–j represent the SEM images of the contact surfaces of the non-metal part at the same range of temperature. It can be observed from Fig. 14a–e that with the increase in the pyrolysis temperature, an increasing amount of the inner metal surface is exposed, and the adhesion of non-metal is gradually reduced, thereby weakening the bond between the metal and the non-metal in PL-WCCL.21,54 As shown in Fig. 14f and g, the surface of the non-metal is no longer densely adhered but assumes a honeycomb-like structure. The separation of the resin layer and the insulating paper layer is visible in Fig. 14h–14j. Further, even in the SEM images of the non-metal part at 250 °C and 300 °C, the fibrous structure within the insulating paper can be discerned after the epoxy resin layer has peeled off. This indicates that during the pyrolysis process, the non-metal undergoes decomposition and produces gas, which forms a number of bubbles at the contact surface of the metal and non-metal parts. Due to the malleability of the metal and the different properties of the metal and non-metal, the bubbles lead to a decline in the adhesive force at their contact surface. Further, under the influence of gravity and centrifugal force within the rotary furnace, separation can occur at a lower temperature during the pyrolysis process.
The SEM images of the cross-section of the non-metal part of PL-WCCL before and after pyrolysis at 150 °C in a rotary furnace are presented in Fig. 14k and l, respectively. The longitudinal section of the original non-metal part of PL-WCCL is compact and intact, while after being subjected to pyrolysis, its longitudinal section exhibits distinct stratification. This indicates that during the pyrolysis process, the cross-linking effect between the layers of epoxy resins is weakened due to the gas generated, resulting in the reduction of the adhesive force between the insulating paper layers and the macroscopic stratification phenomenon.
| This journal is © The Royal Society of Chemistry 2025 |