The goal of the reported protocols is to create rechargeable zinc-sponge electrodes that suppress dendrites and shape change in zinc batteries, such as nickel–zinc or zinc–air.
We report two methods to create zinc-sponge electrodes that suppress dendrite formation and shape change for rechargeable zinc batteries. Both methods are characterized by creating a paste made of zinc particles, organic porogen, and viscosity-enhancing agent that is heated under an inert gas and then air. During heating under the inert gas, the zinc particles anneal together, and the porogen decomposes; under air, the zinc fuses and residual organic burns out, yielding an open-cell metal foam or sponge. We tune the mechanical and electrochemical properties of the zinc sponges by varying zinc-to-porogen mass ratio, heating time under inert gas and air, and size and shape of the zinc and porogen particles. An advantage of the reported methods is their ability to finely tune zinc-sponge architecture. The selected size and shape of the zinc and porogen particles influence the morphology of the pore structure. A limitation is that resulting sponges have disordered pore structures that result in low mechanical strength at low volume fractions of zinc (<30%). Applications for these zinc-sponge electrodes include batteries for grid-storage, personal electronics, electric vehicles, and electric aviation. Users can expect zinc-sponge electrodes to cycle up to 40% depth of discharge at technologically relevant rates and areal capacities without the formation of separator-piercing dendrites.
The purpose of the reported fabrication methods is to create zinc (Zn) sponge electrodes that suppress dendrite formation and shape change. Historically, these problems have limited the cycle life of Zn batteries. Zinc-sponge electrodes have resolved these issues, enabling Zn batteries with longer cycle lives1,2,3,4,5,6. The sponge structure suppresses dendrite formation and shape change because (1) the fused Zn framework electrically wires the entire volume of the sponge; (2) the pores hold zincate near the Zn-sponge surface; and (3) the sponge has a high surface area that decreases local current density below values identified to sprout dendrites in alkaline electrolytes7. However, if sponge surface area is too high, substantial corrosion occurs5. If the sponge pores are too large, the sponge will have a low volumetric capacity5. Also, if the sponge pores are too small, the Zn electrode will have insufficient electrolyte to access Zn during discharge, resulting in low power and capacity5,6.
The rationale behind the reported fabrication methods is to create Zn sponges with appropriate sponge porosities and pore diameters. Experimentally, we find that Zn sponges with porosities from 50 to 70% and pore diameters near 10 µm cycle well in full-cell batteries and display low corrosion rates5. We note that existing methods to manufacture commercial metal foams fail to achieve similar morphologies on these length scales8, so the reported fabrication methods are needed.
The advantages of the methods reported here over alternatives are characterized by fine control of sponge features and by the ability to fabricate large, dense Zn sponges with technologically relevant areal-capacity values5,6,9,10. Alternative methods to create Zn foams may be unable to create comparable 10 µm pores with sponge porosities near 50%. Such alternatives may, however, require less energy to fabricate because they avoid high-temperature processing steps. Alternative processes include the following strategies: cold sintering Zn particles11, depositing Zn on three-dimensional host structures12,13,14,15,16,17, cutting Zn foil into two-dimensional foams18, and creating Zn foams via spinodal decomposition19 or percolation dissolution20.
The context of the reported methods in the wider body of the published literature is primarily established by work from Drillet et al.21. They adapted methods of fabricating porous ceramics to create one of the earliest reported three-dimensional, albeit fragile, Zn foams for batteries. These authors, however, failed to demonstrate rechargeability, likely because of the poor connectivity between the Zn particles. Prior to rechargeable Zn-sponge electrodes, the best alternative to a Zn foil electrode was a Zn-powder electrode, wherein Zn powder is mixed with a gel electrolyte. Zinc-powder electrodes are commercially used in primary alkaline batteries (Zn–MnO2) but have poor rechargeability because Zn particles become passivated by Zn oxide (ZnO), which can increase local current density that spurs dendrite growth3,22. We note that there are other dendrite-suppression strategies that do not involve foam or sponge architectures23,24.
The reported Zn-sponge fabrication methods require a tube furnace, sources of air and nitrogen gas (N2), and a fume hood. All steps can be performed at a lab desk without environmental control, but exhaust from the tube furnace during heat treatment should be piped to a fume hood. Resulting electrodes are appropriate for those interested in creating rechargeable Zn electrodes capable of high areal capacity (> 10 mAh cmgeo–2)6.
The first reported fabrication method is an emulsion-based route to create Zn-sponge electrodes. The second, is an aqueous-based route. An advantage of the emulsion route is its ability to create Zn paste that, when dried, is easy to demold from a mold cavity. A disadvantage is its reliance on expensive materials. For the aqueous route, sponge preforms can be challenging to demold, but this process uses inexpensive and abundant materials.
Both methods involve mixing Zn particles with a porogen and viscosity-enhancing agent. The resulting mixture is heated under N2 and then breathing air (not synthetic air). During heating under N2, the Zn particles anneal and the porogen decomposes; under breathing air, the annealed Zn particles fuse and the porogen burns out. These processes yield metal foams or sponges. The mechanical and electrochemical properties of the Zn sponges can be tuned by varying Zn-to-porogen mass ratio, heating time under N2 and air, and size and shape of the Zn and porogen particles.
1. An emulsion-based method to create Zn-sponge electrodes
2. An aqueous-based method to create Zn-sponge electrodes
Resulting, fully heat-treated, emulsion-based Zn sponges have densities of 2.8 g∙cm–3 while aqueous-based sponges approach 3.3 g∙cm–3. During heating under air, a layer of ZnO forms on the Zn surfaces, which should have a thickness of 0.5–1.0 µm (observed using scanning electron microscopy)5. The solid in the resulting sponges should be 72% Zn (emulsion version) or 78% Zn (aqueous version) with the remainder being ZnO (measured by X-ray diffraction)6. Both sponges should have porosities near 50%, pore-diameter distributions centered on 10 µm, and specific surface areas of 4.0 m2∙g–1 (measured via mercury-intrusion porosimetry)6. The tensile strength of both sponges should be 1.1–1.2 MPa (measured with diametral compression)5,6. We note that the sponges should be rigid and brittle. Cross-sections of the Zn sponges should look similar to those shown in Figure 2A,B. If all the properties of the fabricated sponges fall within the provided ranges, the result is positive; if not, the result is negative.
With the stated properties, Zn sponges cycle well in properly constructed batteries. Their performance also depends on the counter electrode, electrolyte, separator, and cell construction; construction of reliable full cells is beyond the scope of this paper. To test the electrochemical validity of Zn sponges, we recommend harvesting commercial counter electrodes from nickel–metal hydride batteries5,6. Shape a Zn-sponge to have a 10 mm diameter and 0.5-mm thickness. Cycle this sponge at 20 mA∙cmgeo–2 (geometric area) for discharge and 10 mA∙cmgeo–2 for charge in a nickel–zinc cell as described in the literature5. Assuming appropriate construction, the Zn-sponge electrode should show cycling stability at a gravimetric capacity of 328 mA∙h∙gsponge-1 (per gram of ZnO@Zn-sponge electrode) as shown in Figure 2C, which maps to 43% depth of discharge (the quotient of gravimetric discharge capacity with respect to every atom of Zn in the electrode divided by the theoretical gravimetric capacity of Zn). After extensive cycling, no dendrites are observed by scanning electron microscopy (Figure 3). X-ray diffraction can be used to track the state of charge of the Zn-sponge electrode by monitoring Zn and ZnO reflections1. We note the surface of the Zn sponge undergoes restructuring during cycling. The deeper the level of discharge and the greater the cycle life, the greater the amount of restructuring5. These factors contribute to the difference in surface morphology shown in Figure 3A,B. If this rechargeable capacity is achieved, the result is positive; if not, the result is negative and could be caused by either the Zn sponge, poor cell construction, or failure of other cell components.
Figure 1: Zinc sponges before and after heat treatment using the aqueous-based method. (A) Photo of custom-machined molds made from Delrin or polyoxymethylene (POM) that is packed with Zn paste before heating occurs. (B) Photo of hand-made mesh casing, notched alumina holder, and resulting Zn sponge after heat treatment. Please click here to view a larger version of this figure.
Figure 2: Zinc-sponge morphology and electrochemical performance. Scanning electron micrographs of cross-sectioned (A) emulsion-based Zn sponge and (B) aqueous-based Zn sponge. (C) Voltage versus time of an emulsion-based sponge cycled in a nickel–zinc cell discharged at 20 mA∙cmgeo–2 and charged at 10 mA∙cmgeo–2 with a gravimetric capacity of 328 mA∙h∙gsponge–1. Data adapted from Hopkins et al.5,6. Please click here to view a larger version of this figure.
Figure 3: Zinc-sponge electrodes suppress dendrite formation. Emulsion-based Zn sponge (A) before and (B) after electrochemical cycling. Data adapted from Hopkins et al.5. Please click here to view a larger version of this figure.
Modifications and troubleshooting associated with these protocols include filling the freshly mixed Zn paste into a mold cavity. Care should be taken to avoid air pockets. Unwanted voids can be decreased by tapping the mold after filling or while filling. Because the aqueous Zn paste is dry, pressure can be applied directly to the Zn paste to push out air pockets while filling up the mold cavity.
A limitation of the methods is that Zn-sponge pore structure is disordered, but the Zn and porogen particle sizes can be used to alter pore morphology. A more ordered and potentially stronger and lighter Zn sponge may be fabricated using additive manufacturing. The mechanical and electrochemical properties of resulting Zn sponges, however, can be tuned by varying Zn-to-porogen mass ratio and the size and shape of the Zn and porogen particles5,6. Another potential limitation is that the dried Zn-paste can be fragile, so transferring it into a mesh casing may be challenging and limit Zn-sponge size.
The significance of these methods with respect to existing methods is that resulting Zn sponges achieve long cycle life with high volumetric and areal capacities5,6. Resulting Zn sponges are also mechanically robust5,6.
Future applications of the processes could, in principle, be adapted to create other metal foams for batteries or other applications. For example, iron, magnesium, or aluminum foams may be useful as anodes for metal–air batteries25,26,27. Zn-sponge electrodes, in particular, can be used to create batteries for a range of applications that include wearables, grid storage, personal electronics, electric vehicles, and electric aviation28.
A critical step, which may also require modification or troubleshooting, is the heating process. Furnace temperatures can vary. The heating time under N2, near but below the melting point of Zn, anneals the Zn particles together. The heating time under air burns out the residual porogen, fuses the Zn, and forms a ZnO layer. If the Zn particles appear to be fusing improperly, increase the heating time under N2. If the ZnO layer is too thick, decrease the heating time under air by 10 min or more until the desired thickness of thermal oxide is achieved.
We note that a thick layer of ZnO enhances the mechanical properties of the Zn sponge but also decreases the immediately useable capacity of the Zn electrode. The Zn electrode can be charged by electrochemically converting ZnO to metallic Zn. However, stable cycling at 40% depth of discharge can be achieved without any precharge5. If the ZnO layer is too thin, the Zn sponge can crumble during handling5.
The authors have nothing to disclose.
This research was funded by the United States Office of Naval Research.
Corn starch | Argo | Not applicable | This acts as a porogen and viscosity-enhancing agent. |
Decane | MilliporeSigma | D901 | |
Medium viscosity water-soluble carboxymethyl cellulose (CMC) sodium salt | MilliporeSigma | C4888-500G | This CMC acts primarily as a viscosity-enhancing agent. |
Overhead stirrer | Caframo Lab Solutions | BDC3030 | |
Small cylindrical models for Zn sponges | VWR | 66014-358 | The caps of the vials can be used as molds. |
Sodium dodecyl sulfate | MilliporeSigma | 436143 | |
Water-insoluble IonSep CMC 52 preswollen carboxymethyl cellulose resin | BIOpHORETICS | B45019.01 | This CMC acts as a porogen and viscosity-enhancing agent. |
Zn powder | EverZinc | Custom order |