Elsevier

Powder Technology

Volume 363, 1 March 2020, Pages 286-299
Powder Technology

Study on the influence of solids volume fraction on filter cake structures using micro tomography

https://doi.org/10.1016/j.powtec.2019.12.054Get rights and content

Highlights

  • A downscale of lab nutsch according to VDI 2762 allows in-situ x-ray measurements.

  • Particle properties along the filter cake height are analysed by micro tomography.

  • Sedimentation effect in filtration is detected by top layer formation.

  • Further increase in feed solid fraction reduces particle property deviation.

  • Feed solid fraction influences cake structure and so filter cake resistance.

Abstract

Prediction of micro processes, filter cake build-up and porous media flow is a key challenge to describe macroscopic parameters like filter cake resistance. This is based on a precise description, not only of the disperse solid fraction, but the distributed properties of the voids between the particles. Lab-experiments are carried out with alumina and limestone, which differ in particle size distribution (PSD) and resulting filter cake structure. Filter cakes of both materials are characterized by standardized lab tests and additionally, alumina cakes are measured with X-ray microscopy (XRM). Focusing on distributed process key parameters, the data gives a deeper understanding of the laboratory experiments.

The solid volume fraction inside the feed strongly influences the particle sedimentation and leads typically to a top layer formation of fine particles in the final filter cake, which has a negative influence on subsequent process steps. The top layers seal the filter cake for washing liquid and increase the capillary entry pressure for gas differential pressure de-watering. The influence on cake structure can be seen in a change of porosity, particle size and shape distribution over the height of the filter cake. In all measurements, homogenous filter cake structures could only be achieved by increasing the solid volume fraction inside the suspension above a certain percentage, at which particle size related sedimentation effects could be neglected and only zone sedimentation occurred. XRM offers the chance to quantify these effects, which previously could only be described qualitatively.

Introduction

By cake filtration, highly concentrated suspensions with solid volume fraction of around 20 to 25 vol.-% are lead through the filter medium, where the particles are retained and form a water filled voids structure, mainly described by the void to total volume fraction, the porosity.

As an important step, filter cake de-watering can only sufficiently be described by understanding the interconnected pore network. Results in [1,2] are usually based on homogenous filter cakes with constant porosity and therefore globally estimated permeability related to Darcy's law and the established channel model. These estimations only include one-dimensional liquid flow through an incompressible filter cake. In reality, particle properties like shape, size, and wetting behaviour are distributed and they highly influence the porous network build-up with possible local deviation in vertical or horizontal alignment. Contrary, in practice on the macroscopic scale only integral properties are used – understanding of microscopic effects becomes very difficult. Wakeman [3] proved that the consolidation of filter cakes is both, a time and a pressure function. The velocity of consolidation depends on particle size and shape distribution. The balance between particle and liquid pressure reaches the equilibrium state for complete consolidation [4]. Wyckoff and Botset [5] detected a fluctuating liquid flow rate through sand, if it was not completely saturated. A restructuring of the layers took place due to increasing or decreasing saturation. Tiller and Cooper [6] observed differences in pressure at different locations within the bed, Comiti [7] traced it back to the fact of a strong wall effect. Tiller [8] and Alles [9] give proof of an instability by showing the influence of the cake pressure on the filter cake resistance. For differential pressure filtration, Bothe et al. [10] found that due to a widely distributed particle size distribution, segregation occurred within the feed, which subsequently negatively influenced the filter cake structure for subsequent dewatering. Hwang found similar results for filtration in the centrifugal field and attributed this to a heterogeneous cake structure. The results were all the worse when mixtures of several particle systems were used [11].

In contrast to the findings above, in filtration dominated theory and in simplified models for apparatus design, homogenous structures are assume and preferred, e.g. described in the established Kozeny-Carman equation [12] and Darcy's law [13]. Therefore, the combined development of experimental and theoretical techniques is essential to develop a better understanding of cake filtration and prove the findings of several authors above. By combining an in-situ XRM filtration setup with validation of experiments at laboratory scale, it becomes possible to gain an insight into network structure after filtration. Structure analysis with an achievable resolution of 5 μm enables to visualize porous network structures enhanced by single particle analysis.

In the area of the measuring method and the field of micro tomography, the reader is referred to the work of Miller et al. [[14], [15], [16]] and Lin et al. [[17], [18], [19], [20], [21]] for particulate systems. In the field of analysis of micro-tomography measurements of porous media, many works have emerged in recent years [18,[22], [23], [24], [25], [26]]. The authors deal with the permeability and pore size distributions on which many modeling approaches are based.

Section snippets

Material characterization

For all filtration experiments, crushed and classified α-Al2O3 particles (T60/64, Almatis, Germany, ρ = 3.82 g/cm3) in the size range of 55 to 200 μm are used. The particle system can be described with a lognormal distribution function, defined as the first derivation of the cumulative particle size distribution (PSD, x50.3 = 102 μm, σ3 = ln(x84.3/x50.3) = 0.43, laser diffraction, cf. Fig. 1).

As reference for laser diffraction (LD, Sympatec HELOS) the PSD was also measured by dynamic image

Experimental set-up

The filtration experiments are carried out at 0.3 bar in a lab-scale pressure nutsch filter set-up (cf. Fig. 2) according to VDI 2762–1 with an internal diameter of 5 cm and an effective filter area of A = 20 cm2. The filtration tests stop at complete saturation of the filter cakes. The filter cakes are subsequently dried at 40 °C for 48 h, so that rearrangement of particles can be neglected due to drying effects as seen from micro tomography scans before and after drying. The two datasets were

Sample preparation and tomography measurements

Tomography measurements offer the possibility to gain an insight into the differences of the packing structure without destroying the filter cake matrix. Compared to a conventional tomographic set-up, an XRM has a microscopy optic that allows an additional magnification by the factor of 10. Due to the non-destructive nature of X-ray tomography, the sample can be reused for other measuring principles besides X-ray tomography. Considering the internal dimensions of the XRM and the projected

Workflow for image processing

The reconstruction is done by using the filtered back projection algorithm implemented in the ZEISS Xradia reconstruction software (Xradia XMReconstructor 10.7). This includes an automatic centre shift and beam hardening correction with a factor of 0.05. A gauss filter with a kernel of 0.7 for smoothing is applied already at the raw data. The image data has to be further processed because of artefacts due to the XRM-measurement, low contrast and image noise. Filtering in ImageJ (Fiji 1.51n)

Detailed insight into filter cake structure

Comparing the PSD measured by image analysis from XRM, different size distributions over the whole height of filter cake are detected, proven by the cumulative PSD in Fig. 7, in which the distributions are calculated by the equivalent sphere diameter (EQPS, eq. (4)). Based on the binary image stack, the porosity as number of void voxels can be also determined along the depth of the built cake.xEQPS=6πV3

Even a solid volume fraction of cV = 0.25 within the suspension does not prevent

Discussion and comparison

In Table 1 the number of analysed particles of each scan offers an overview about the statistics behind each data point for cV = 0.10 to 0.40: All solid feed fractions are measured once, except cV = 0.25, for which three different experiments are carried out. The work of Koglin et al. [41] proved that with increasing number of particles the possible error related to the analysis can be neglected due to.f2=fA2+fP2

With f2 as total error, combining the errors fA2 for sampling and fP2 of the

Conclusions

With the obtained data from XRM measurements, many properties of both, the disperse particle system and filter cake characteristics can be determined by one single tomogram. By varying the solids volume fraction, it was found that with conventionally suggested volume fraction of cV = 0.25, superimposed separation of size and shape of the particles as a function of the filter cake height occurred. Only when cV was increased to >0.3, it was possible to prevent the formation of a top layer of fine

Notation

Symbol/abbr.Meaning (Unit)
Afilter area (m2)
APprojection area (m2)
ASsurface area (m2)
Bpermeability (m2)
cvsolid volume fraction (m3/m3)
ddiameter (m)
ftotal error (-)
fperror value of sampling (-)
faerror value of analysis (-)
hfilter cake height (m)
nnumber of particles (-)
P(t)tolerable error rate due to t-distribution (-)
ppressure (Pa)
Q3sum distribution (-)
rCspecific filter cake resistance (1/m2)
UPProjection perimeter (m)
uLvelocity of the liquid (m/s)
Vparticle volume (m3)
xparticle

Acknowledgement

We express our gratitude to the Deutsche Forschungsgemeinschaft (DFG), which supported this research, project number 1160/23-1. Additionally, we would like to thank Vietnam International Education Development (VIED) – Ministry of Education and Training for financial support through the 911 Project. Further, thanks to DAAD and WUS for their support in Germany. The Authors would like to thank colleagues in the department of Mechanical Process Engineering and Mineral Processing, TU Bergakademie

Declaration of Competing Interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

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