Here, we present a protocol to synthesize two metal chalcogenides (Cu1.8S and SnSe) suitable for thermoelectrics via an ultrafast (second-range), solvent-free, and one-step mechanochemical synthesis using elemental precursors. Simultaneously, we demonstrate the monitoring of the temperature in the jar during planetary ball milling in situ by the newly developed device.
Mechanochemical synthesis is an extremely useful strategy to reach thermoelectric materials due to its solvent-free one-step character, as the targeted thermoelectricity (TE) materials in a nanocrystalline format can be prepared by mere high-energy milling of elemental precursors. Nevertheless, the subsequent densification method (e.g., spark plasma sintering or hot pressing) is required afterward, similarly to other synthetic methodologies. In this study, the simplicity of mechanochemical synthesis is presented for two selected metal chalcogenides, namely copper sulfide (Cu1.8S, digenite) and tin selenide (SnSe, svetlanaite), which are known for high ZT values. These compounds can be prepared via a mechanically induced self-propagating reaction (MSR), which is a combustion-like process instantly yielding the products in a very short timeframe (within 1 min). The occurrence of MSR can be well-tracked by in situ temperature monitoring since an abrupt temperature increase occurs at the moment of MSR. We have developed a device which is capable of monitoring the temperature inside the milling jar every 80 ms during planetary ball milling, and it is therefore possible to very precisely track the moment of MSR ignition. The developed device presents an improvement in the monitoring capabilities in comparison with commercially available analogs. This contribution aims to provide a visual insight into all steps, with simple high-energy ball milling of elements to reach TE materials and in situ temperature monitoring being the central points.
Statistically, more than 60% of energy in the world is lost, mostly as waste heat. Utilizing the waste heat for thermoelectricity (TE) applications has a great potential. TE offers a suitable method to convert waste heat into electrical energy. Special applications, like electrical energy sources in radioactive thermoelectric generators for space research and/or replacing the old Hg-Zn batteries in cardiac pacemakers, can be mentioned1.
Among various TE materials, chalcogenides belong among the favorites, especially if they are composed of abundant and non-toxic elements. Chalcogenides with tellurium, lead, and germanium content were reported as perspective TE materials in the past, with Bi2Te3 and (Bi,Sb)2Te3 being among the most prominent examples. However, both Bi and Te are rare and/or toxic, making the mass production of TE materials with this composition challenging2. Looking forward to selection among chalcogenides, the new alternatives that bear in mind non-toxicity, earth-abundancy, and TE efficiency are considered. Two systems that fulfill these criteria are copper sulfides Cu2-xS and tin selenide SnSe.
Copper sulfides are present frequently in nature as minerals in several compositions, with chalcocite Cu2S and covellite CuS as border members. In between, several non-stoichiometric compounds exist3. Among them, Cu1.97S and Cu1.98S, with interesting properties, were already synthesized by directly melting the elements Cu and S4,5. Also, digenite Cu1.8S is particularly interesting for thermoelectrics.
Tin selenide SnSe represents a high TE figure among chalcogenides. The synthesis at 1223 K for over 9.5 h led to its ultralow thermal conductivity and subsequent high thermoelectric efficiency6. Accompanying phenomena were not studied.
Synthesis routes of copper sulfides and tin selenides encompass mostly high-temperature treatment of reaction precursors4,7,8,9,10. However, there are also alternative, more environmentally sound synthesis routes such as mechanochemical synthesis3,11,12,13. The mechanochemical synthesis of chalcogenides from elements can, under some circumstances, occur as a mechanically induced self-propagating reaction (MSR), which is a combustion-like process instantly yielding the products in a very short timeframe14,15,16. For both systems reported in this study, the MSR was reported- for Cu1.8S, it was done instantly, albeit the Cu:S ratio 1.6 needed to be used due to the volatility of sulfur16,17, and for SnSe, it occurred in about 15 s16.
The ignition of an MSR is accompanied by a sudden increase in temperature and pressure. Upon monitoring these characteristics via specifically engineered milling jars, it is possible to determine the MSR onset. However, the commercially available devices for planetary ball milling monitoring offer only the data collection every 2 s, and due to the location of the sensors, MSR can be detected only via pressure monitoring, neither by temperature one16,18. Moreover, the mentioned system is not transferrable and can only be both purchased and used together with the specifically engineered milling jar, which is both limiting and costly. We have recently developed a transferrable device capable of collecting temperature data every 80 ms19. This advanced measuring system developed for in situ temperature monitoring during mechanochemical synthesis significantly enhances the capabilities over existing commercial solutions. This system employs an NRBG104F3435B2F NTC thermistor, featuring a resistance tolerance of ±1% at 25 °C and a beta value tolerance of ±1%, ensuring high-precision temperature measurements. With a data capture frequency of every 80 milliseconds, the system provides a high-resolution monitoring crucial for detecting the initiation of MSRs. The thermistor's high sensitivity to temperature changes, indicated by a steep resistance-temperature relationship, ensures accurate detection of rapid temperature spikes. The temperature sensor is strategically placed within an existing screw mechanism used for pressure release and gas addition, located in the hole of a massive cap. This placement protects the sensor from mechanical collisions and signal noise caused by the milling balls, ensuring stable and reliable temperature readings. The limitation is that the ball diameter needs to be larger than the hole diameter. With 10 mm balls, there is no problem. The system's wireless communication capability and robust sealing mechanism prevent material or heat leakage, thereby enhancing the reliability and accuracy of the temperature data collected during the milling process. Designed to be cost-effective and portable, this system represents a significant advancement in the real-time temperature monitoring of chemical reactions during planetary ball milling, offering critical insights for the optimization of materials synthesis.
This study aims to demonstrate the performance of this newly developed device by monitoring temperature during the mechanochemical synthesis of two selected metal chalcogenides that are interesting for TE applications. Another objective is to show the sustainable, simple, and time-saving character of the mechanochemical synthesis, which is boosted when the reaction occurs as an MSR.
1. Preparation of CuS mixture with the stoichiometry 1.6:1
2. Preparation of SnSe mixture with the stoichiometry 1:1
3. Sensor setup
4. Performing milling with in situ temperature monitoring
NOTE: The necessary equipment, including the scheme of the temperature monitoring device, is shown in Figure 1.
5. Collecting samples
6. Transferring the powders
7. Labeling the glass vials
8. Cleaning the jar and sensor
9. Processing data from in situ temperature monitoring
10. Powder X-ray diffraction (XRD) measurement
11. Rietveld refinement
The temperature during milling was recorded using Project SAV 1.0 software and plotted accordingly. Figure 3 demonstrates the changes in temperature with milling time. For the Cu1.8S samples (Figure 3A), the ignition times fall within the range of 0-0.6 s. In the sample Cu1.8S-1, the MSR occurred before temperature data collection began. Therefore, when performing the two next experiments (Cu1.8S-2 and 4), data collection was started prior to milling (therefore, the negative time values are present for the two curves in the figure). The ignition of MSR for samples Cu1.8S-1 and Cu1.8S-3 resulted in the maximum temperatures of 45.8 °C and 42.7 °C, respectively. In the latter case, the temperature increased by more than 15 °C at the moment of MSR. In contrast, small temperature increases were observed in samples Cu1.8S-2 and Cu1.8S-4, namely 3.8 °C and 1.0 °C. In Figure 3B, the temperature-time plots for the SnSe samples showing the occurrence of the MSR after 87 s, 89 s, and 97 s, accompanied by temperature increases of about 3.8 °C, 1.5 °C, and 8.0 °C respectively, are shown.
The XRD patterns of 1.6Cu+S and Sn+Se mixtures obtained immediately after the temperature change event, together with the mixed elemental mixtures, are shown in Figure 4. The as-prepared mixed elemental mixtures do not contain any sulfides, just elemental precursors. This means that the energy supplied by a mere mixing with a spatula is not sufficient. Milling the Cu:S mixture with a stoichiometric ratio of 1.6:1 results in the formation of rhombohedral and cubic polymorphs of digenite (Cu1.8S) and hexagonal covellite (CuS) (Figure 4A), in alignment with previous findings3. However, the obtained XRD patterns differ; they either contain sharp diffraction peaks of rhombohedral digenite with marginal amounts of cubic digenite and covellite (sample Cu1.8S-3), or the diffraction peaks are of lower intensity, and the presence of covellite is much more significant (sample Cu1.8S-1 and Cu1.8S-2). The sample Cu1.8S-4 represents a hybrid of these two scenarios, resembling more Cu1.8S-3 sample. In Figure 4B, the three similar XRD patterns of the Sn+Se mixture are shown. The distinct peaks corresponding to the (201), (011), (111), and (221) planes, characteristic of the orthorhombic svetlanaite (SnSe) phase, were identified16. Trace amounts of berndtite (SnSe2), as demonstrated, e.g., by the diffraction peak at 15°, were also formed in all the cases.
In order to get information about the exact phase composition and crystallite size, Rietveld refinements were performed on two XRD patterns from each system (Figure 5). The identified phase composition is provided in Table 2. For both Cu1.8S samples, rhombohedral digenite was identified as the major phase with the content of around 90%. The residual 10% was either split in between covellite, CuS, and cubic Cu1.8S in the case of sample Cu1.8S-4 or belonged to covellite as a whole (sample Cu1.8S-1). The estimated crystallite size of rhombohedral Cu1.8S was 63 ± 1 nm and 39 ± 1 nm for Cu1.8S-4 and Cu1.8S-1 samples, respectively. In the case of Cu1.8S-1, the estimated crystallite size of CuS was 25 ± 1 nm (Table 2).
Regarding the SnSe system, the major desired svetlanaite SnSe phase was present in 84% and 94% of SnSe-1 and -2 samples, respectively. The rest was assigned to the berndtite SnSe2. The estimated crystallite size of SnSe product is 92 ± 2 nm and 80 ± 1 nm for SnSe-3 and SnSe-2 samples, respectively. In the case of SnSe-3, the crystallite size of SnSe2 admixture was 53 ± 5 nm (Table 2).
Figure 1: Necessary equipment and scheme of the temperature monitoring device to ignite MSR. The photographs of (A) Pulverisette 7 premium line planetary micro mill, (B) milling jar made from tungsten carbide with a volume of 80 mL, 25 pieces of 10 mm of tungsten carbide balls, rubber sealing and the lid of tungsten carbide jar, (C) device used for the in situ temperature monitoring including electronics and temperature NTC sensor, and (D) the schematic diagram of the working principle of the device. The sensor is equipped with a Li-ion battery. The temperature sensor NTC is supported by microcontroller STM 32 for the operation, and the recorded data is transferred to the PC by using Bluetooth module HC-O5. Please click here to view a larger version of this figure.
Figure 2: Appearance of the sample. Photographs of (A) Cu-S mixture before milling, (B) extracted Cu1.8S-1 (Cu1.8S-2 looks the same), (C) extracted Cu1.8S-3 (Cu1.8S-4 looks the same), (D) Sn-Se mixture before milling, and (E) extracted SnSe (all the products SnSe-1-3 look the same). Please click here to view a larger version of this figure.
Figure 3: Temperature changes during milling. (A) Cu-S system: Cu1.8S-1 with the ignition time of 0 s (black), Cu1.8S-2 with the ignition time of 0.08 s (red), Cu1.8S-3 with the ignition time of 0.43 s (magenta), Cu1.8S-4 with the ignition time of 0.6 s (blue). (B) Sn-Se system: SnSe-1 with an ignition time of 87 s (black), SnSe-2 with an ignition time of 89 s (green), and SnSe-3 with an ignition time of 97 s (red). The negative values in part a are due to the fact that the device was started prior to milling in order to catch the very fast reaction occurring immediately after milling initiation. Please click here to view a larger version of this figure.
Figure 4: XRD patterns. (A) Cu-S system, Cu1.8S-1 with the ignition time of 0 s (black) and Cu1.8S-2 with the ignition time of 0.08 s (red), Cu1.8S-3 with the ignition time of 0.43 s (navy), Cu1.8S-4 with the ignition time of 0.6 s (blue), mixture of Cu:S (1.6:1) before milling (magenta). (B) Sn-Se system, SnSe-1 was recorded with an ignition time of 87 s (black), SnSe recorded with an ignition time of 89 s (blue), SnSe-3 with an ignition time of 97 s (red), and mixtures of Sn:Se (1:1) (magenta). The identified crystallographic phases together with their ICDD-PDF2 card numbers, are presented in the figure. Please click here to view a larger version of this figure.
Figure 5: Rietveld refinement plots. (A) Cu1.8S-1 with the ignition time of 0.08 s. (B) Cu1.8S-4 with the ignition time of 0.6 s. The scattered black bullets are the experimental data, the red and blue lines are calculated, and full difference X-ray diffraction profiles, respectively. The Bragg diffraction of hexagonal CuS, rhombohedral Cu1.8S, and cubic Cu1.8S are depicted by the magenta, light green, and dark green lines, respectively. (C) SnSe-3 with the ignition time of 97 s. (D) SnSe-2 with the ignition time of 89 s. The scattered black bullet depicts the experimental data, the red and blue lines are calculated, and full difference X-ray diffraction profiles, respectively. The Bragg diffraction of SnSe and SnSe2 are depicted by the magenta and dark green lines, respectively. The fitting factors are also provided in the figure. Please click here to view a larger version of this figure.
Material | Milling chamber volume (mL) | Milling balls (pieces x diameter in mm) | Milling speed (rpm) | |
Tungsten carbide (WC) | 80 | 25 x 10 | 400 |
Table 1: The milling parameters for the synthesis of Cu1.8S and SnSe through the MSR and the photograph of the in situ monitoring device mounted on the milling jar.
Sample | Time until MSR (s) | Rhombohedral digenite, Cu1.8S | Cubic digenite, Cu1.8S | Hexagonal covellite, CuS |
Cu-S system | ||||
Cu1.8S-1 | 0 | 90 ± 1 | – | 10 ± 1 |
Cu1.8S-4 | 0.6 | 92 ± 2 | 3 ± 1 | 5 ± 1 |
Sn-Se system | Time until MSR (s) | Orthorhombic svetlanaite, SnSe | Hexagonal berndtite, SnSe2 | |
SnSe-3 | 98 | 84 ± 2 | 16 ± 2 | |
SnSe-2 | 89 | 94 ± 2 | 6 ± 2 |
Table 2: MSR ignition time and phase composition (%) of the four selected samples according to Rietveld refinement.
Mechanically induced self-propagating reactions (MSR) are an immediate transformation of precursors into products via an exothermic combustion-like process activated by mechanical action (similar to self-heat sustaining reactions where similar processes are activated by heat). The occurrence of MSR can often be identified by changes in the physical appearance of the product, a distinct smell at the moment of the reaction, or a scratching sound from the milling jar. However, empirical evidence suggests that these sensory indicators are not always reliable, and in many cases, the MSR event may not have occurred despite the presence of these signs16.
Gas temperature and pressure sensors have been developed and mounted into milling jar lids in the past to address these limitations, and numerous studies on the MSR events in chemical synthesis have been reported20,21,22. However, the valuable equipment is expensive and not interchangeable between jars. Therefore, we developed an economical temperature sensor for observing MSR during planetary ball milling. This sensor provides a cost-effective and practical alternative to a more expensive and less sensitive sensor system since, in the present case, the sensor is directly in contact with the gas and sometimes also powder. The sensor, placed inside a small hole in the jar's lid close to the powder and milling balls, transfers the heat generated inside the jar into a readable temperature measurement. This principle allows for real-time monitoring of the MSR through the conversion of heat into an electrical signal, enabling precise and continuous temperature tracking. The fastest scan rate of the temperature is 80 ms. The sensor demonstrated high sensitivity to local temperature changes inside the jar, as evidenced by the real-time monitoring of temperature fluctuations during steps 4.7 and 4.8 in the protocol.
The MSR occurred much faster in the Cu-S system than in the case of Sn-Se. This is in agreement with our previous works14,19. The difference between the repeated experiments in the case of ignition time is not large and is within an experimental error. Notably, the transformation to the SnSe phase was rapid, occurring within the range between 87 and 97 seconds for all three experiments, respectively. In the case of Cu1.8S synthesis, the MSR event was observed consistently in all four trials, always within the first second of milling. However, there were big differences in terms of the temperature increase in both systems. This is most probably related to the fact that the hot particles will get close to the sensor or not, which might always be different. Thus, the temperature increase cannot be considered as a relevant parameter, at least with the current setup. Nevertheless, it seems that the temperature increase is milder in the Cu-S system. The obtained products exhibit distinct physical characteristics compared to the precursors. Cu1.8S, appearing blue and agglomerated (Figure 2A,B), suggests the occurrence of the MSR. The dark blue color is typical for covellite, CuS and the photograph was taken for the sample Cu1.8S-1 where, according to XRD, the content of covellite was around 10 %. For the samples where the amount of covellite was lower, the color of the product was black,e.g., Cu1.8S-4. The SnSe products were always gray.
The X-ray diffraction, in combination with proper data treatment, is an extremely powerful tool to describe the phase composition of the products. Copper sulfides produced via the mechanochemical synthesis can possess different phase compositions, depending on the precursors used. For example in Godočíková et al.23, when the copper acetate (CH3COO)2Cu.4H2O and Na2S were milled, covellite and chalchantite (CuSO4.5H2O) were obtained. When the synthesis was performed on a larger scale in an eccentric vibratory mill, utilizing the Cu:S stoichiometric ratio 1:1 yielded the formation of CuS and Cu2S phases24. Our group was the first to report the MSR event for Cu-S system16, and it was found that CuS and Cu1.8S are formed as a result of MSR when treating 1:1 stoichiometry, with covellite becoming more pronounced with prolonged milling25. It has to be noted that copper has to have a specific needle-like morphology to react via a MSR14,16. As mentioned in the results part, there are differences in the phase composition of the XRD patterns of Cu1.8S samples. These differences are most probably caused by the time how fast we were able to stop the milling process after the MSR event. According to Baláž et al.3, almost pure digenite is formed after MSR, which is in accordance with the sample Cu1.8S-3. We most probably succeeded in stopping the mill quite early in this case. However, further milling leads to a partial transformation to covellite, and in the case of samples Cu1.8S-1 and Cu1.8S-2, we managed to stop the mill slightly later. According to the reports on the mechanochemical synthesis of SnSe from corresponding elements, the phase-pure orthorhombic SnSe phase was almost exclusively obtained16,26,27. In our case also the presence of SnSe2 phase was observed. Again, its amount differs among the three experiments, and thus, we are of the opinion that there is some interchange between the SnSe and SnSe2 depending on the time that elapsed from the MSR until the stopping of the mill. Nevertheless, the Sn-Se system seems to be more stable than Cu-S one with regards to the phase composition obtained after MSR, as the appearance of all three XRD patterns is very similar (Figure 3A), unlike in the Cu-S system (Figure 3B). The answers regarding phase compositions during milling could be provided by in situ X-ray monitoring28,29 and we are planning to study these reactions in this way in the future. However, only oscillation milling can be monitored in this way for now (in situ monitoring of planetary ball milling setup is not available yet). The Rietveld refinement of the two selected XRD patterns from both systems confirmed the nanocrystalline character of the products. Metal chalcogenides are usually prepared with the crystallites on the nanoscale via mechanochemistry16. However, MSR processes are specific, and due to combustion, the crystallite sizes are usually larger than when performing the reaction in a gradual manner, e.g., the ones in Baláž et al.16 are much larger than the ones in Tsuzuki et al.30. In the case of Cu1.8S, the determined crystallite size of the main digenite phase was either around 63 nm or 39 nm. In the former case, the product was analyzed sooner after the MSR, so the crystallite size is larger. The crystallite sizes reported in this study are larger than 15 nm reported for the CuS obtained after the MSR in25. The SnSe particles were larger than that of Cu1.8S, namely the values larger than 84 nm were observed. These values are significantly larger than 12 nm reported for SnSe synthesized by mechanical alloying for 1 h31. In general, continuing milling after the MSR seems to rapidly diminish the crystallite size. After the MSR event, the crystallite size decreases and can reach similar values to the ones obtained via gradual processes after some time.
The nanostructuring being brought about via the mechanochemical approach is very beneficial for the TE performance of the materials32. Despite the fact, that they are densified by a subsequent step (such as spark plasma sintering), the materials still keep the memory of their original synthetic procedure33. However, it is beyond the scope of this study to analyze and discuss the TE performance of the prepared products.
This protocol shows a simple, environmentally and user-friendly methodology to obtain nanocrystalline materials and even monitor temperature during the process. The critical steps in the protocol are to check if the monitoring device is working properly (step 3.2) and to stop the milling process as soon as possible after the MSR occurrence (step 4.8). The rest is just about characterization and data analysis. For now, there is a limitation about the quick destruction of the sensor, but this can be easily replaced with a new one, as these are very cheap. It would be great if the mill could automatically stop at the moment of MSR, but this has not been solved yet. The solution proposed in this study offers much more detailed temperature monitoring than is available on the market for now. From the synthesis point of view, by just introducing elements, we are capable of producing the powder suitable for TE applications within the second range. Utilizing mechanochemical synthesis to ignite MSRs for diverse materials preparation via simultaneous temperature monitoring might be an interesting topic for future research on a more general level.
The authors have nothing to disclose.
The present investigation was supported by the Grant Agency of the Ministry of Education, Science, Research and Sport of the Slovak Republic (project 2/0112/22). The present investigation was also supported by ERA-MIN3 POTASSIAL 27 project.
Copper | Pometon, Germany | 7440-50-8 | Red powder |
D8 Advance diffractometer | Bruker, Germany | M88-E03036 | X-ray instrument |
DiffracPlus Evaluation package release | Bruker, Germany | DOC-M85-EXX002 | Diffraction analysis software |
Etaben | Mikrochem, Slovakia | 64-17-5 | solution |
Jedit | Open Source software | Programmer's text editor | |
Project SAV 1.0 | Software developed to record data from in situ temeprature monitoring | ||
Pulverisette P7 planetary mill | Fritsch, Germany | 07.5000.00 | The milling device, utilized in the synthesis of Cu1.8S and SnSe |
Selenium | Acros Organic, Germany | 7782-49-2 | Gray powder |
Sulfur | Sigma Aldrich, Germany | 7704-34-9 | Yellow powder |
Tin | Merck, Germany | 7440-31-5 | Gray powder |
Topas Academic | Coelho Software | General non-linear least squares software driven by a scripting language. Its main focus is in crystallography, solid state chemistry and optimization. |
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