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Influence of humidity on the tribo-electric charging and segregation in shaken granular media

We study the effect of humidity on the charge accumulation of polymer granulates shaken vertically in a stainless steel container. The setup allows to control the humidity level from 5 % to 100 %RH while performing automated charge measurements in a Faraday cup directly connected to the shaking container. We find that samples of approximately 2000 polymer spheres become highly charged at low humidity levels (<30 %RH), but acquire almost no charge for humidity levels above 80 %RH. The transition between these two regimes does depend on the material, as does the sign of the charge. For the latter we find a correlation with the contact angle of the polymer with only very hydrophilic particles attaining positive charges. We show that this humidity dependence of tribo-charging can be used to control segregation in shaken binary mixtures.


Introduction
Granular materials are among the most significant forms of matter in technology as well as in everyday life. Their production and handling, which account for about ten percent of the global energy consumption, 1 are hampered by a number of fundamental problems which are often not well understood. One of them is the effect of tribologic charging, which can occur whenever the grains are composed of a material different from the container, if two different grain materials are involved [2][3][4][5][6][7][8] or even if grains differ in size. [9][10][11] Tribo-electric charges can change the spatial composition of granular materials by inducing mixing, 12,13 de-mixing, 14,15 clustering 16,17 or even the formation of granular structures [18][19][20][21][22] and crystals, [23][24][25] cf. Fig. 1. Strong tribo-electric charging, which is capable of creating small sparks, 26 becomes even hazardous in the presence of flammable materials. [27][28][29] However, if charging is controlled it might provide a remedy for another well-known granular problem: segregation. We show that indeed electrostatic attraction between particles of different size counteracts the mechanisms which normally make them separate when the sample is mechanically excited. [30][31][32] Hence it is of great importance to understand, predict, and control tribo-electric charging in granular materials, in particular granular mixtures.
Tribo-electric charging describes the ability of two bodies to exchange charges when getting into contact. The description of this phenomenon dates back to the ancient Greece, 33 but even nowadays it is an open debate whether electrons, ions or the exchange of surface materials causes the net charge transfer from one contacting body to the other. 7,[34][35][36][37][38][39][40][41][42][43][44][45] This complicates the attempt to sort materials by their ability to accumulate charge when rubbed against each other. 46 These so-called triboelectric series are often mutually inconsistent and depend on hard to control details of the charge acquisition procedure. 5,47,48 Fig. 1 Crystalline structures formed by shaking PA and PTFE beads of 2 mm size in a PTFE container at 50 Hz and 2 g for 1 h. A body centered square lattice (cesium chloride crystal structure) is visible in the upper part of the image. The inset shows a 3D reconstruction of the particle positions, obtained by X-ray tomography.
A number of experimental and theoretical studies suggest that water molecules adhered to the surface of the materials play an important role in charge transfer. [3][4][5]16,34,41,44,45,47,[49][50][51][52][53][54][55][56][57][58][59] Such water layers are ubiquitous; however, their thickness is limited to the order of a few nm 3,59 as long as the ambient humidity is below 100%RH. 60,61 Already in 1902, Knoblauch hypothesized that the H + and OH À ions dissolved in the water adsorbed to the surface of polar solids would be reasonable charge carriers. 62 Subsequent experimental observations confirmed the idea of the importance of surface water; however, a consistent picture of its role still has to emerge. For instance, it was found that humidity strongly alters the charges that are generated via tribo-electricity. 45,47,49,51,63 This is attributed to the effect that higher air humidities will increase the air conductivity 64 and hence increase the leakage of charges from the surfaces to the ambient air. 4,34,47,57 An increased charging rate for increasing humidity was found by Wiles et al. who studied the charge transfer of a rolling metal sphere on a flat polystyrene surface. 51 Németh and coworkers concluded from their study of fluidized beds filled with polymer particles that the charge transfer mechanism is dominated by electrons at low humidity; at a higher humidity adhered water and ions contribute to electrostatic charging. 3 In other work, it was pointed out that water is not a necessity for the charge exchange 65 or that even small patches of water together with large electric fields can lead to the charge transfer between solid, hydrophobic objects and walls. 59,66,67 Another mechanism of tribo-electric charging might be the exchange of functional groups of the polymers, which are transferred to the surface of the beads when they are swelling at high humidities. 3,57 To summarize, there is as yet no complete picture of the role of humidity on the tribo-electric charging. In the present study, we therefore concentrate on phenomenological parameters which can be determined experimentally, such as the wettability of the materials by water (i.e., the contact angle 61 ) and the relative humidity (RH). We control the humidity of ambient air in a range from 5 to 100%RH to test the influence of this parameter on the charge accumulation of polymer spheres shaken vertically in a stainless steel container.

Experimental
Most charge measurements involving granular materials use a Faraday cup, which implies that the sample has to be transferred from the point where it acquires its charge to the point where this charge is being measured. 3,6,50,68 Because this transfer process can influence the charge in an uncontrolled way, we have designed a setup where the Faraday cup is directly connected to the shaking container; the transfer of the beads is then initiated by rotating this assembly with a stepper motor, cf. Fig. 2. Both the Faraday cup and the shaking container are made from stainless steel (alloy 4301) and have an inner diameter of 5.75 cm. The whole setup is mounted on an electromagnetic shaker (TIRAvib TV 5880/LS) and shaken sinusoidally in vertical direction. The granular samples used for charge measurements consist of different types of polymer beads with a diameter of 3 mm. Table 1 lists the materials studied, together with the polydispersity of the beads and the literature values of the equilibrium contact angle Y Y for water. Except for the PTFE beads, which were obtained from TIS Wälzkörpertechnologie, 69 all beads were ordered from Spherotech. 70

Measurement protocol
Prior to every measurement series, the particles were cleaned with de-ionized water and ethanol, and the Faraday cup and the shaking container were wiped with ethanol. Subsequently, the shaking container was filled with either a single bead or with 2000 AE 17 particles. The latter corresponds to a filling height of approximately 2 cm, which is one fifth of the container's height. The Faraday cup (orange) is mechanically connected to the shaking container but electrically isolated by a 1 mm PTFE ring (white). This assembly can be rotated around a common axis (red) using a toothed belt (brown) and a stepper motor (black). The shaking container (green) has 40 1 mm pin holes which allow an exchange of humidity with the outer hull (yellow). The outer hull itself can be flushed with air of controlled humidity via external valves; it also contains a temperature sensor and a humidity sensor. The whole setup is mounted on top of an electromagnetic shaker operated in the vertical direction. The charge measurement position is shown. The beads were shaken for at least 8 min at an amplitude of 1.4 mm and a frequency of 30 Hz, which corresponds to an acceleration of 2.5 g (g = 9.81 m s À2 ). Then the Faraday cup and the container are rotated by 1801 around a horizontal axis. After the rotation, an additional short shaking pulse of 1 s ensures that even beads which are still sticking to the walls of the container fall into the Faraday cup.
The charge of the granular sample is measured using a Keithley 6514 electrometer connected to the Faraday cup. The shaking container is grounded and the charge is measured as the average over 50 s. An additional drift correction of the electrometer was applied to all measurements. Uncertainty for the single bead measurements was 6.7 Â 10 À11 C. After finishing the charge measurement, both the Faraday cup and the shaking container are grounded. Then, the system is rotated back to its original position and a new shaking and measurement cycle begins.

Humidity control
In order to tune the humidity within the setup, the shaking container is embedded in an outer hull. Forty pin holes in the container (diameter: 1 mm) enable the exchange of air between the inside of the rotating cup setup and the space in the outer hull. To adjust the humidity in the range between 20 and 100%RH, the outer hull was flushed with preconditioned air from a self-built climate chamber which uses an ultrasonic transducer and a cold trap to control the humidity level. Measurements at a humidity level of 3-5%RH were performed by fixing a bag filled with 12 g of dry silica gel inside the outer hull.
For monitoring purposes the outer hull is equipped with a humidity sensor (HIH-5030/5031 with an accuracy of AE3%RH in the range of 11-89%RH and AE7%RH otherwise) and a temperature sensor (TMP102, with an accuracy of AE0.5 1C); both sensors were purchased from Tinkerforge. 75 Before starting the experiments, all air connections between the setup and the climate chamber were closed in order to maintain a closed atmosphere. The time scale for equilibration between the inner part of the sample chamber and the volume in the outer hull was found to be on the order of 80 min. Additionally, the shaker produces heat during operation, which increases the temperature in the sample chamber until it reaches an equilibrium at T = 28 AE 1 1C after approximately an hour. To account for both these effects, we have only considered charge measurements where the inner and outer parts of the setup can be considered to be equilibrated. Finally, a drift of E0.3%RH per hour was found for a humidity difference of 55%RH between the lab and the interior of the container. However, all measurements are attributed to the present humidity level determined with the humidity sensor.

X-ray micro-tomography
We studied segregation in binary mixtures using X-ray computed tomography. The setup (Nanotom, General Electrics) uses a tungsten target and was operated at 130 kV acceleration voltage and 90 mA current to produce X-rays. The data sets consist of 900 Â 900 Â 800 voxels where each voxel has a size of 60 mm 3 . Air was removed prior to bead detection using a threshold determined via the Ostu method. 76 The same approach was used to discriminate the beads of different materials. After an image erosion step 77,78 and binarization, the center of the beads was detected with an accuracy of 1% of the small bead diameters, which is smaller than the polydispersity of the grains.

Results
The aim of our work is to quantify the influence of humidity on the generation of charges in granular media. Section 3.1 describes the influence of humidity on shaken samples of four different granular materials. A possible relationship between tribo-charging and the wetting behavior of the polymer materials is discussed in Section 3.2. Section 3.3 compares the different impact of humidity on bead-wall and bead-bead contacts. Finally, the role of humidity in the segregation of binary mixtures is highlighted in Section 3.4. (I) All materials are strongly charged at low humidities. At a material-specific critical humidity RH crit there is a crossover into a low charge regime. We determine RH crit by modeling the data in Fig. 3 with a 5th order polynomial and then computing the point where the negative slope has a maximum. RH crit values of all four materials are listed in Table 2.

Impact of the humidity level on the charge
(II) The hydrophilic PA and POM beads are positively charged and the hydrophobic PS and PTFE beads are negatively charged. We will return to the sign of the charge in Section 3.2. Fig. 3 Magnitude of charge as a function of humidity for each 2000 PA, POM, PS, or PTFE spheres shaken in a steel container. Up to moderate humidities, all fillings are highly charged. Then, at a material specific humidity, a crossover to a low-charged regime is found. At very high humidities, only the hydrophobic materials PS and PTFE are able to accumulate charges. The data points correspond to bins of 3%RH width, each containing at least three individual measurements.

Soft Matter Paper
Open Access Article. Published on 05 December 2016. Downloaded on 9/25/2020 9:50:54 AM. This article is licensed under a Creative Commons Attribution 3.0 Unported Licence.

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(III) The hydrophobic materials are still charged up to a few tens of nC even at very high humidities (480%RH).
Several authors observed changes in the magnitude of charge upon altering the ambient humidity with the general trend being that charging is suppressed at high humidity. 3,45,49,50,63 However, there exists no unified ab initio model that directly relates tribo-charging to the thickness h of the adsorbed water film. The exact value of h depends on the effective interface potential of the surface and it increases in a nonlinear way with the relative humidity. For the case of incomplete wetted materials such as polymers the range of h is between fractions to several tens of monolayers of water. 3,59-61 An interpretation of our data has therefore to rely on a combination of the following mechanisms: First, if charging is due to the presence of water on the surface of the particles, free charge carriers are either supplied due to the dissociation of water molecules present in the ambient air 44,55-57 or it could be ions transferred via ''water bridges'' from one body to the other upon contact. 41,45,48,49,53,59 Second, charging could be completely independent of water 36,39,40,65 and third, discharging can occur whenever the presence of surface water decreases the surface resistivity. 3,49,63 A possible fourth mechanism is the charge loss due to the increased conductivity of humid air. 64,79 However, this mechanism can at best explain differences between positively and negatively charged surfaces, 57 but not the observed material-dependent variations. We therefore exclude it from our further considerations.
The fact that we observe the strongest charge accumulation at the lowest humidity levels does not contradict the relevance of water for charging as suggested by the first mechanism, since charging will require only a small amount of water molecules to be present at the surfaces. However, it does also not exclude the possibility that other charge transfer mechanisms related to the second argument are responsible for the observed charging.
The crossover to smaller or even zero charge at RH crit can be explained by the third mechanism, an increased charge loss due to surface water. 4,63 Table 2 lists some literature values for the formation of the first monolayer on polymer surfaces, which corresponds to a conducting hull around each particle; these values are in reasonable agreement with our measured values of RH crit . Moreover, Nemeth et al. 3 measured the surface resistivity r of PA (PA-12), POM and PS particles. For PA particles they found an approximately sevenfold decrease of r between 30 and 50%RH. For PS particles there is a twentyfold decrease between 50 and 70%RH whereas the surface resistivity values of PS do not decrease up to a humidity level of 70%RH. All three of these results are in good agreement with our measured RH crit .
Finally, observation III, the finite charge on PS and PTFE beads at high humidity levels, supports the idea that this charge is related to water adhered to the surface.

Contact angle and wetting behavior
The data in Fig. 3 seem to imply that hydrophobic surfaces, i.e. with a contact angle Y Y 4 901, charge negatively while hydrophilic materials charge positively. However, this picture is oversimplified as the inclusion of a larger variety of polymer materials in Fig. 4 demonstrates: already for Y Y 4 701, all samples are negatively charged. Only the two most hydrophilic polymers, PA and POM, charge positively.
This more complicated dependence can be expected from the fact that there is no simple relation between the thickness h of the adsorbed water film and Y Y . 61 Still there seems to be a correlation between cos(Y Y ) and the sign of the accumulated charge. This raises the question of the nature of the charge carriers that cause tribo-charging. Numerical results imply that hydrophobic graphene surfaces favor the adsorption of negatively charged hydroxide ions OH À from ambient air. 53 Experimental support for this interpretation comes from experiments where water is flowing through PS and PTFE tubes and charges them negatively. 48 Clint and Dunstan 80 directly relate the wetting properties of materials with the capability of a surface to donate electrons and their position in the triboelectric series. However, this does not exclude ions as charge carriers due to adhered surface water: it was observed that for instance metals tend to provide free charge carriers via ion partitioning at the solid-gas interface 56 and that the tribocharge does depend on the details of the surface chemistry 3,41 with an H + adsorption on basic surfaces and an OH À adsorption on acidic surfaces. 44 45 To summarize, there is evidence that the surface chemistry links both the wetting properties and the charging behaviour of granular materials.
3.3 Comparing particle-wall and particle-particle contacts When shaking 2000 polymer beads in our steel container, a bead-bead collision is approximately nine times more likely than a bead container collision (based on the ratio of the total bead surface area of 565.5 cm 2 to the inner container area of 62.1 cm 2 ). Hence the charges presented in the last two subsections will be strongly affected by polymer-polymer collisions. However, due to charge conservation within the bed, the main source of charge is due to collisions with the container wall. Now to probe exclusively these polymer-steel collisions we have repeated the experiments with a single polymer sphere shaken in the steel container.
The inset of Fig. 4 shows that the correlation between the sign of the charge and Y Y does not change for the polymersteel collisions. However, the amount of accumulated charge does. Fig. 5 displays the ratio R between the charge acquired by a single shaken bead and the charge acquired by a bead shaken within a sample of 2000 beads. Or, in other words, it describes how an increased number of polymer-polymer collisions alter the charge on a bead. Fig. 5 shows that R decreases with decreasing contact angle. In general, metal-insulator contacts can result either in electron 3,54 or ion transfer processes. 41,47,51,82 Without a microscopic understanding of our charging mechanism it is difficult to explain the trend in Fig. 5. However, the presence of water seems to be crucial for our observation as the observed hierarchy of charging is not compatible with measurements performed at polymer-metal contacts under vacuum conditions i.e. in the absence of surface water. 47 Moreover, the contact angle of stainless steel with water is roughly 661. 83 Therefore the more hydrophobic a polymer is, the stronger will be the contrast in Y Y and consequentially the exchange of water when the polymer gets into contact with steel.
Collisions between the charged polymer particles can cause nonlinear effects 25,84 , diffusion of charges along the grain surface and contact de-electrification. 68 The latter mechanism according to Soh et al. 68 implies that charges are transferred to the atmosphere upon contact. We can only say that contact de-electrification seems to be a stronger effect for smaller water surface layer thickness and higher contact angles. This could be related to the Paschen-breakdown mechanism in the vicinity of the contact area between beads. 68,85

Using humidity to control segregation in binary mixtures
The fact that the ambient humidity determines the charge on the particles allows for some control of segregation in vertically shaken samples. To demonstrate this point we have mixed equal volumes of large (3 mm) and small (1.59 mm) PTFE beads and shaken them in a PA container (diameter 50 mm) for one hour and at 100 Hz and 2 g. We then obtained X-ray tomographies of the samples and detected the particle positions. Fig. 6(a) and (b) depict the difference between samples shaken at ambient humidities of 50%RH and 100%RH. For 50%RH, small and large particles are well-mixed within the sample. Fig. 1 shows that even crystalline mixtures may result when same-sized grains are shaken. This is most readily interpreted as being due to attractive electrostatic interactions between the beads. In contrast, at 100%RH the sample displays horizontal and radial segregation, cf. Fig. 6(c). This so called Brazil nut segregation pattern can be explained by the two segregation mechanisms of void filling and convection rolls. [86][87][88] To study the degree of segregation in our binary mixtures, we define the dimensionless segregation parameter P segr as with n L,i being the normalized volume density of large (L) particles and n s,i being the normalized density of small (s) particles at bin i. The pre-factor 1/2 ensures the normalization of P segr and h max is the maximum height of the sample. A higher value of P segr indicates a higher degree of segregation. For the mixtures depicted in Fig. 6 we obtain P segr = 0.06 for 50%RH and 0.32 at 100%RH. To investigate the impact of charging on segregation in more detail, we conducted segregation experiments in a PTFE cup (diameter 50 mm) at low (o30%RH), medium (30-70%RH) While hydrophobic particles charge stronger in polymer-steel collisions than in polymer-polymer collisions, this ratio decreases with decreasing Y Y . Error bars were computed using error propagation and the data in Fig. 4. The dashed line is a guide for the eye. and high (470%RH) humidity using equal-volume mixtures of PA and PTFE grains which differ in their composition. Beads were again shaken for one hour at 100 Hz and 2 g. Subsequently, the reconstructed bead positions allow us to compute the vertical volume densities. The experiments were performed three times in each humidity range using the climate chamber described in Section 2.2.
Different models account for beds consisting of tribo-charged particles by assuming either homogeneous 12,13 or heterogeneous 89 charge distribution along the surface of grains. The latter will have an impact on the interaction of the particles that goes beyond simplistic Coulomb-like interactions. 25,84 However, since we only access the total charge of individual grains, we aim at qualitatively linking segregation to the impact of charge by computing the product Q L Q s . Q L and Q s are the mean charge values of the large and small beads, respectively, in the binary mixture. The charges were measured by extracting ten large and small beads from each bed after shaking using an anti-static tweezer and depositing them individually in a self-made Faraday cup.
The impact of tribo-charging on granular segregation is shown in Fig. 7 where Q L Q s is plotted against P segr . The equal volume mixture consisting of large and small PA particles does not charge when shaken in the PTFE cup. However, the other mixtures do. Even though the data is quite noisy, we can put two statements: first, all products Q L Q s are negative indicating that -to the lowest order -large and small particles attract each other. Second, more negative values of Q L Q s always correspond to a lower degree of segregation. Thus, we have shown that electrostatic interactions can not only suppress segregation but also open an avenue to create packings by design, cf.

Conclusion
When samples of polymer particles are shaken vertically in a steel container they do tribo-charge. The sign of the accumulated charge shows some correlation with the water contact angle of the material. The amount can be controlled by the relative humidity of ambient air. At low humidity levels we observe a plateau of approximately constant charge. Above a materialspecific threshold the magnitude of charge decreases to zero or a small level. All these results point to the importance of the water film adsorbed at the surface of the beads for understanding their tribo-electric charge accumulation. Finally, tribo-generated charges can suppress segregation by providing attractive interactions between beads which are strong enough to counteract segregation during shaking.