Next Article in Journal
Optimization of Fracture Spacing and Well Spacing in Utica Shale Play Using Fast Analytical Flow-Cell Model (FCM) Calibrated with Numerical Reservoir Simulator
Next Article in Special Issue
Process Monitoring in Heavy Duty Drilling Rigs—Data Acquisition System and Cycle Identification Algorithms
Previous Article in Journal
Improvement of Strength Parameters of Cement Matrix with the Addition of Siliceous Fly Ash by Using Nanometric C-S-H Seeds
Previous Article in Special Issue
A Portable Environmental Data-Monitoring System for Air Hazard Evaluation in Deep Underground Mines

Increasing Energy Efficiency and Productivity of the Comminution Process in Tumbling Mills by Indirect Measurements of Internal Dynamics—An Overview

Faculty of Geoengineering, Mining and Geology, Wroclaw University of Science and Technology, Na Grobli 15, 50-421 Wrocław, Poland
Faculty of Automatic Control, Electronics and Computer Science, Silesian University of Technology, Akademicka 16, 44-100 Gliwice, Poland
Authors to whom correspondence should be addressed.
Energies 2020, 13(24), 6735;
Received: 15 November 2020 / Revised: 9 December 2020 / Accepted: 10 December 2020 / Published: 21 December 2020
(This article belongs to the Special Issue Mining Technologies Innovative Development)


Tumbling mills have been widely implemented in many industrial sectors for the grinding of bulk materials. They have been used for decades in the production of fines and in the final stages of ore comminution, where optimal levels for the enrichment particles’ sizes are obtained. Even though these ubiquitous machines of relatively simple construction have been subjected to extensive studies, the industry still struggles with very low energy efficiency of the comminution process. Moreover, obtaining an optimal size for the grinding product particles is crucial for the effectiveness of the following processes and waste production reduction. New, innovative processing methods and machines are being developed to tackle the problem; however, tumbling mills are still most commonly used in all ranges of the industry. Since heavy equipment retrofitting is the most costly approach, process optimization with dedicated models and control systems is the most preferable solution for energy consumption reduction. While the classic technological measurements in mineral processing are well adopted by the industry, nowadays research focuses on new methods of the mill’s internal dynamics analysis and control. This paper presents a retrospective overview of the existing models of internal load motion, an overview of the innovations in process control, and some recent research and industrial approaches from the energy consumption reduction point of view.
Keywords: ball mills; energy efficiency; internal dynamics; DEM model; resonance oscillations; measurements ball mills; energy efficiency; internal dynamics; DEM model; resonance oscillations; measurements

1. Introduction

Up to 70% of the costs of materials size-reduction operations fall on the rock particle’s size reduction from 30–50 mm to 20–50 microns [1,2]. This operation is performed by the most common type of milling comminution equipment—ball milling. The design of ball mills was described back in the 18th century—and the principle of their operation has not changed; the only significant changes are the increased diameter and some new solutions for the mill’s drives introduced. Energy consumption in ball and rod mills reaches up to 10–20 kWh per ton of rock. According to the study prepared by the U.S. Department of Energy [3] the biggest potential for energy savings in all of the energy-intensive ore and coal mining-related operations is to be found in grinding optimization (see Figure 1). To increase efficiency, designers of mining equipment tried to improve all the elements of ball mills, such as the geared mechanical drives, bearings, their lubrication systems, and electric motors. Moreover, efforts have been made to optimize the size of the grinding bodies, control the filling level of the drum with the material, and stabilize the rotation speed. However, the main problem of dramatically low energy efficiency is still unresolved—about 30% of grinding bodies are not involved in the dynamical process—they remain in a boundary dead zone. A large portion of the impacts of grinding bodies appears on the internal liners. There are several approaches to the activated material and grinding bodies’ motion inside the mill.
First, new designs of energy-saving mills have been introduced in the market. For example, vertical (tower) Vertimill (Metso) and horizontal Isamill (Glencore Technology), which use, respectively, gravitation forces or several subsequent rotating disks inside to intensify the milling process. However, ball mills of the traditional design process the main portion of bulk materials in the world.
The next solution is the installation of so-called lifters, situated along the mill shell over the perimeter to promote higher trajectories of the balls falling down and to better mix the media treated. However, these additional elements quickly deteriorate due to the intensive wear and shock impacts on them. Hence, they may have an effect only within a short period of time after replacement.
A promising approach is to utilize the dynamic phenomena inside the mill. Namely, when the central part of bulk media moves in oscillatory (synchronous or resonance) mode against the mill shell, and the rest is passive part of the load. This approach is more attractive from the viewpoint of implementation because it does not require any additional modernization of mechanical equipment. Only the instrumentation for signals’ measurement and processing, in combination with process parameters’ control—based on existing automation systems—is needed in such cases. However, such control needs in-depth knowledge of intra-mill load dynamics and its stages estimation by the different channels—electric motors current or power, vibration, and acoustic emission inside the equipment, or spatial sounds and mechanical torques of multi-motor drives. The realization of such an approach can only be based on advanced instrumentation—including wireless sensors, and dynamical models (both analytical and discrete elements) and signal processing techniques. These methods should account for the gradual changing of treated material properties (input variations and reduced-by-time-fractions) simultaneously with the wear of grinding balls and internal protective liners of the mill itself. Additionally, the influences of such intentionally produced oscillations on the torsional dynamics of mill drives need estimation.
This paper intends to represent a comprehensive retrospective overview of existing methods and recent trends in ball mills modeling and control aimed at increasing their energy efficiency and productivity by indirect measurements of internal dynamics with signals of different physical nature.

2. State-of-the-Art in Mill Control

Being the main equipment used for fine-grinding in the raw materials industry and an element of the most energy-consuming stage in mineral processing, responsible for roughly half of the mining companies’ energy consumption [4,5], tumbling mills were subjected to legitimate and intensive studies in the search for improving the efficiency of ore processing. Depending on the industry’s nature, dedicated open and close grinding circuits are designed to perform comminution in a dry or wet environment [6,7]. Depending on the stage of the process and the requirement of the product grain size distribution (coarse, fine, or ultra-fine grinding) the specific energy rises exponentially with the final grains’ size reduction [8]. In many applications, comminution is performed in order to achieve the desired degree of minerals liberation, that is, the percentage of the valuable mineral in the free form in relation to the valuable injected in the gangue (locked form) [9]. Thus, improved control over the comminution process has significant influences on the concentration processes, such as flotation [10,11] and bio-leaching [12]. Obtaining high efficiency from the energy and material consumption points of view, has a significant potential to contribute to decreasing the environmental impact of this very burdensome process. Due to the difficulty of balancing the large ore particle supply with the optimal feed rate, the autogenous (AG) and semi-autogenous (SAG) mills operate in a meta-stable state, which creates a demand for accurate and real-time assessments of a mill’s load and its behavior [13].
Circuit retrofitting is the most difficult and costly approach to the grinding process optimization; thus, after initial circuit design, further optimization is achieved through the process control. In most cases it requires, however, process parameters’ measurement for the feedback approach or accurate process models for the feed-forward approach [14]. Taking into account the complexity and the dynamics of the close grinding circuits (most popular in the mineral processing industry) the most suitable solution would be to measure or model the mill’s output itself. The necessity of robustness and complexity of multivariate nonlinear predictive control of SAG ball mills is underlined in [15].
Direct observation of internal load motion is practically impossible; however, the knowledge about its trajectory plays the main role in the optimization of the disintegration of bulk material into smaller particles. Therefore, many scientists and engineers devoted their efforts to developing and improving indirect methods of studying the differences in operating conditions of ball mills. Some of the flagship examples of these types of measurements are the passive inertial measurements on the surface of a SAG mill, which have been used by Campbell et al. [16] to study the operating conditions of the machine, namely, to specify variations of the volumetric filling and motion characteristics. The vibrations of the machine’s shell taking place as a result of the collisions of the grinding media’ and ground ore with each other and with liners have been proven to provide informative data for condition surveillance when subjected to appropriate signal processing techniques. The usage of polar contour plots and spectrogram analysis has been presented as appropriate for deriving signals’ characteristics that respond well to changes in operating conditions, such as frequency band power. Such indirect methods can be based on various signals—on vibration signature: [17,18,19,20,21,22,23,24,25,26,27]; acoustic data: [28,29,30,31]; using both—acoustic and vibration data together: [24,32,33,34,35,36]. The weight of the mill’s charge has been also successfully evaluated by measuring strain changes in the mill’s shell, together with obtaining some information about the dynamic behavior of grinding media [37]. Another possibility for monitoring the mill filling level is the measurement of the motor: power draw [38], torque [39] and other signals from the motor control units [18,24,40]. Since the engine’s electrical signals’ characteristics are dependent on the process of elevation of the particles inside the drum—their collisions and impacts [41]—they allow one to observe the intra-mill material dynamic behavior as well [42]. Another important set of issues to be taken into consideration includes the accelerated wear of lifters and liners, and the destruction of discharge grates emerging when the feed rate deviates from a desirable value. The identification of the regions where direct shell impact takes place, leading to the damage of liners and accelerated wear, by means of vibration data analysis, has been demonstrated in [43].
Physical variables describing the performance of ball mill have been successfully measured with an instrumented ball, equipped with a data storage module, a power supply, communications electronics, and inertial sensors connected to a small micro-controller [44,45,46].
A wide range of scientific research in that area led to various industrial applications of the automatic stabilization of the mill’s motor power and the design of technical solutions for the control of its maximum level. Such solutions are becoming the standard in the raw materials industry worldwide, representing trends of Industry 4.0. Some of the most popular industrial solutions are StarCS from Mintek [47,48], MilSense from Outotek [49], and LoadIQ from FLSmidth [50]. Such systems usually measure a set of technological parameters, e.g., feed mass or volume flow rate, density, particle size distribution (PSD), and power drawn by the mill’s engines. Most recently, on top of classic direct measurements, industrial solutions use indirect measurements based on vibration, strain, and acoustic or vision signals. Such systems allow for a 1–2% increase of efficiency, without reducing specific energy consumption. Taking into account that the largest mills have electrical power of about 20–30 MW, even a tenth of a percent reduction in energy consumption gives tremendous annual savings for plants usually having several mills.
Circuit control systems are being implemented widely in order to control the feed rate and run the mill at the optimum efficiency level, which means, depending on the specific objective function: maximizing output, minimizing energy consumption, or providing an accurate particle size distribution for the further stages of mineral processing. Examples of such systems are: Grinding Circuit Control (GCC) solutions, used in Canadian processing plants [51] (e.g., Strathcona Mill, Raglan Mill, Eland Mill), MillVis system [52] developed by AMEplus and KGHM Polska Miedź S.A. for all of the Polish milling sections, where rod-primary-mills and ball-mills for regrinding are used in Divisions of Concentrators (O/ZWR Lubin, O/ZWR Polkowice, O/ZWR Rudna), or an intelligent optimal-setting control (IOSC) applied in the Chinese iron ore concentration plants’ grinding circuits [53]. While the systems operating in Canadian mines focus on accurate observation of the ore stream in multiple points of the circuit and reacting to the variations—in order to provide the stability of the milling process, the Polish process control and optimization system includes inertial and acoustic measurements aimed at the mill itself. More precisely speaking, in the case of MillVis, monitoring of the mill’s performance and its technical state is based on inertial data, acquired by accelerometers distributed on the machine’s shell—to diagnose liners and lifters; acoustic signal recorded in the direct neighborhood of the machine—for indirect assessment of grinding media and rotational speed; and additionally—video recording of the feed—to control feeds’ granulation variability and lithological compound [54]. In the case of the Chinese processing plant, the developed approach includes a loop controller using case-based reasoning and a soft sensor for particle size distribution control based on a neural network, together with the fuzzy inference adjusting method [55]. The goal function of the IOSC is to provide an optimal rate of production, maintaining appropriate particle size distribution for further enrichment processes.
Increased control over the comminution process may be beneficial since it allows one to take advantage of the phenomenon occurring in the grinding chamber, which can improve the efficiency of the particles’ size reduction. It was proven in the laboratory and industrial-scale studies of the internal mechanics of tumbling mills, that there is a resonant oscillation mode of the central part of the mill’s charge, occurring at a certain value of the feed and rotational speed [56].
Such an oscillation of the material in the low-frequency range (1–3 Hz), if maintained, may lead to an increase of the mill’s efficiency by 6–8% and a decrease of its energy consumption by 8–10% as it was discovered by industrial investigations in [57]. Some studies conducted on laboratory mills with different types of building materials give available energy savings up to 50% [58].
It was found in the experimental research that the resonant mode of oscillation can be preserved by changing the load factor in all the types of ball mills: ball mills using grinding media, semi-autogenous, and autogenous mills. Moreover, the granulometric characteristics of intra-chamber fill can affect the self-oscillatory effect, and thus the power intensity of the milling process [59]. Since many mills nowadays are still equipped with synchronous AC motors with not modifiable drive speeds, control of the operating mode (maintaining the resonance of intra-chamber material) in their case is possible only through changing the mill’s filling level, or the slurry density—by supplying different amounts of process water to the mill’s chamber.
Considering a complex system ’ore mill—magnetic separator’, it is found in [60] that mill filling level with ore can be determined by the sign of the first derivative signal of the active power of the electric motor of the magnetic separator by the active power signal of the mill motor. For wet, autogenous grinding mills positive sign means under-loading, while for ball mills this parameter has the opposite meaning.
For many years most motors driving SAG, AG and ball mills were of fixed speed. As more accurate and faster controllers emerged, together with a decrease of costs and dimensions of the hardware, control of drive’s operation became possible on an industrial scale. In order to optimize the material flow rate, decrease power draw, maintain maximized impact zone of cascading material, control the breakage rate function (in case of SAG mills), and to increase the availability of the comminution machines, more and more often mining companies decide to implement tumbling mills driven by the engines with modifiable speeds. There are two main solutions to make operating at variable rotation speed possible for tumbling mills [61]: cycloconverters—for the ones of high power and low speed, and multilevel voltage source inverters—appropriate for the mills demanding less power, operating at higher speeds.
The original method of ball mill control was proposed by the authors of the patent [62]. Their SmartMill uses a magnetic field created by electric magnets installed on the mill shell to keep the grinding media coupled with balls and prevent them from slipping in the “dead zone”. In addition, the magnetic field helps to direct the grinding media to an optimal trajectory, resulting in increased drop height and impact energy. Researchers also carried out mathematical modeling of processes in a mill with electromagnets, which made it possible to determine the range of the optimal number of electromagnets located in each section of the mill and reduce the time of their activation (less energy consumption). The SmartMill technology will be the most energy-efficient for grinding magnetic ores due to the direct effect of the magnetic field on the material. This technology—as declared by authors—can reduce energy consumption up to 50% that has also been achieved in the new types of mills like Vertimill (Metso) [63] and Isamill (Glencore Technology) [64].

3. Methods of Measurements and Optimization of Tumbling Mills

The measurements aimed at the evaluation of operating conditions and optimization of comminution, mentioned in previous section, are listed in Table 1 and Table 2 below. They have been divided according to the signal measured and the main criteria of optimization. The possible sources of informative data to be acquired on a tumbling mill or in its direct neighborhood, which were used by scientists and constitute an input for the process control systems used in the raw materials industry are acoustic emission in the surrounding of the mill, vibrations measured on the shell (possibly other parts of the machine), digital records of the output ore stream, current and other signals to be acquired from the motor control unit. A scheme showing the methods of measurement and the variables to be adjusted on the basis of multi-channel data acquisition is presented in Figure 2. Mill’s performance, monitored based on vision, acoustic, inertial data and motor signals can be optimized by the input of grinding media, changing of the slurry density (by adding process water), adjusting of the speed (expressed as a % of the critical speed) or increasing/decreasing of the mill’s load. All the mentioned adjustments influence the throughput and PSD of the product. Some of the crucial process parameters with their corresponding informative signals are presented in the Table 3.
Following Table 1, one can notice that the majority of studies are based on vibration and acoustic emission measurements, which seem to be caused by three main reasons:
  • Data acquisition methods and instrumentation for such signals are well proven in the industry;
  • The price of the equipment is relatively low;
  • Probably most importantly—it does not require direct contact of the sensor with the processed, highly abrasive material.
Acoustic emission technique is preferable for shock impacts sensing on the mill shell but requires wireless communication to record data. The same telemetry circuits are needed for strain gauges implementation on the rotating shafts of mechanical drives [65]. Therefore, it is important the measurement of angular backlashes in gear coupling [66] and to include in dynamical models of ball mills their drive-lines as the systems with non-linear parameters of stiffness [67].
The multi-motor drives of heavy ball mills with open couplings of the peripheral tire and pinion gears are subjected to intensive wear and excessive angular and radial clearances. The different kinds of dynamical processes occurring in the drives of ball mills are investigated in [70,71]. One of the effects occurring in such kind of drives are out-of-phase torsional vibrations in parallel lines [72] having high amplitudes, which may interfere with internal load dynamics and significantly affect mill speed control. The most difficult mode for mill drives is to start under load especially for synchronous AC motors. Control methods of soft start are implemented for such cases [73].
Although electric motor parameters are quite easy to register and use for process stability estimation in the existing automation systems of industrial plants [74], a surprisingly small number of works in the domain of ball mills is discovered. This is most likely related to the simplicity of the signal processing methods used, which are not allowing to recognize multivariate correlations in material properties in the motor current data, which is reacting only to the integral load inside the mill.
Therefore, as it follows from Table 2 and Table 3, the main efforts are undertaken in bulk media properties detection and related working conditions of the mill. Only a few studies are noted on the wear diagnostics of the grinding balls and protective liners, although this is very important for mills maintenance and balls replacement planning. Method of liners diagnostics is proposed in [69] based on analysis of infra-low frequencies (up to 0.01 Hz) of components in the active power spectrum. Another way to detect the wear of internal protective liners is to analyze self-excited torsional vibrations at the natural frequencies of the drive-line of the mill [75].
Application of the above-mentioned methods can be well described based on the MillVis system example [52]. As described in [54] the system uses vibration, acoustic, and vision measurements. Depending on the application (first or second stage grinding) it uses also other technological parameters like pulp density or average particle size. The latter are, however, accessible for mixed product streams from several mills sections and are used for global optimization purposes rather than individual mills performance improvement.
The system measures the mill’s vibrations with wireless DataLogger using accelerometers installed on the mill’s shell (see Figure 3A). Sensors and DataLogger rotate together with the mill, so wireless data transmission is required and device energy consumption optimization, since it operates using battery packages, rotating with the mill shell as well. According to the kinetics of grinding [76]—the vibration amplitude will rise while more of the kinetic energy of the grinding medium (e.g., steel balls) is transferred directly to the mill shell. The amplitude will be maximal when the balls hit the mill shell and the lowest when the balls sink in the processed material. Naturally, desired levels of the vibration amplitude will vary depending on the actual sensors position following from the rotation of the mill. Thus, quite important is to correlate the amplitude measurements with the mill position. It is quite straightforward using the vibration signal from the individual sensor rotating together with the mill shell and low-pass filtering in frequency domain [77].
Figure 3B shows exemplary data from two full convolutions of the mill represented by blue and red parts of the chart. Black parts represent the final stages of the previous convolution and initial stages of the following convolution. The yellow sine-wave-shaped chart is the filtration result, representing the position of one of the sensors rotating with the mill shell. Binding the angular position of the sensor with the vibration signal values allows one to perform easy-to-understand signal analysis using e.g., polar plots.
Figure 4 shows the comparison of the vibration signal for rod and ball mills. Each point on the polar plot represents the vibration amplitude (represented as a distance from the plot center) registered by the sensor in the given position during the mill rotation (represented by the angle value). One can easily observe the maximum amplitude angle changes with the process parameters variation (e.g., pulp density, throughput, grinding media charge).
The difference in the maximum amplitude angle for two compared mills is obvious and follows from different grinding media behaviour inside the mill’s working chamber. The visual representation of the mill’s behavior on the polar plots is useful for the operators to determine the state of the grinding process and the technical condition of the mill itself. Constant analysis of the above-mentioned parameters allows predictive maintenance and increases machinery availability.
Vibration signal amplitude analysis is only one of the system components. Values of technological process parameters, together with vibration signals’ other parameters (e.g., dedicated indexes calculated at the frequency domain) and vision system measurements for the feed particles size distribution estimation are finally used by the dedicated software in the supervisory control layer to calculate optimal control set-points hints for the operator [78].

4. Analytical Models of Grinding Process Dynamics

4.1. Mathematical Modelling

Scientists tried to develop methods for controlling the process of grinding in ball mills with mathematical modeling methods. Basic semi-empirical relationships between mechanical work needed in the comminution process and the size of particles subjected to grinding, are the well known Kick’s, Bond’s and, Von Rittinger’s equations applying to different thresholds of grain sizes [79].
  • Kick’s equation—for d > 50 mm
    W K = c K ( ln ( d S ) ln ( d G ) )
  • Bond’s equation—for 50 mm > d > 0.05 mm
    W B = c B ( 1 d G 1 d S )
  • Von Rittinger’s equation—for d < 0.05 mm
    W R = c R ( 1 d G 1 d S )
    where W K , W B , W R is the grinding work in kWh/t, c K , c B , c R are the work indexes, usually given in kWh/t, d S denotes pre-ground particle size, and d G —the size of the particle after comminution (the values of d S and d G are usually taken as d 8 0 from a granulometric curve, which describes the grain’s size, below which the cumulative sum of smaller ones gives 80 percent of material’s mass). However, it should be noted that energy consumption in the comminution processes still has not been theorized to a satisfactory degree [80].
In order to define different modes of operation depending on the geometry and rotational speed of a tumbling mill, the Froude number—a dimensionless ratio can be used to characterize bed dynamics and motion of the material during comminution [81,82]:
F r = ω 2 R g
where ω is the rotational speed in revolutions per second, R—the radius of rotation in meters and g—the gravitational acceleration in (m/s 2 ).
Figure 5A shows experimentally determined regions of different motion modes of steel balls inside the laboratory drum, which is visually represented in Figure 6. The vertical axis corresponds to the number of particles converted to the height of bulk media h counting from the bottom of the drum.
To account for the nonlinear nature of the phenomenon and friction-induced self-oscillations, a Froude pendulum dynamics model was proposed in [83]. It contributed some theoretical considerations on friction dynamics, having strong potential to be a foundation for the analysis of energy-transferring mechanisms from the working tool (mill shell) to the treated media (bulk internal load)—including ore mills. The author represented internal load motion as the parametric oscillations using the Mathieu differential equation with periodically changing parameters, solutions of which are comprehensively represented as an Ince–Strutt diagram. The fragment of this diagram is shown below—Figure 5B, enabling the identification of stable regions in the mentioned model. A detailed formulation of the analytical functions for stable (shown shaded) and unstable regions boundaries on the Ince–Strutt diagram can be found in [84]. Briefly— a 0 , b 2 and a 1 , b 1 are boundary lines separating unstable (I) and stable (II) regions of the oscillations for π and 2 π periodic solutions respectively; N 1 , N 2 , N 3 —the transition from unstable ( N 1 , N 2 ) to stable ( N 3 ) oscillations by the decreasing angular velocity of the rotation. The horizontal axis on this diagram corresponds to the excitation parameter and the vertical axis encompasses the relation of frequencies.
The shaded regions (II) determine the synchronization or out-of-synchronization in other regions (I) of the natural frequency and parametric excitation. The source of parametric oscillations can be any variable affecting the natural frequency: the moment of inertia, friction coefficient, filling level (mass of the internal load), etc. If these variables do not change, synchronization control can be achieved by the angular speed of mill rotation in case of regulated electric drives availability.
The optimal modes of ore milling are controlled by the processing of the electric motor current or power signal. Conditions of synchronization are estimated based on the signal after band-pass filtering and high-resolution spectral density obtained online. Crossing the unstable regions by internal load motion is detected by an increase in spectrum amplitudes at the frequencies pre-calculated by the dynamical model.
It is known from the general theory of Mathieu equations in application to the physical systems that viscous damping—proportional to the momentary value of the angular velocity of contacting bodies motion (ore load and mill shell), can only narrow the regions of instability but not eliminate the unlimited increase of the amplitude of parametric oscillations. In other words, for the same relation of natural to exciting frequencies, e.g., for principal resonance in Figure 5B, higher amplitudes of periodical disturbance are required, but when its certain level is achieved, the amplitude of oscillations can develop to unlimited values. However, in real systems like ball mills, some non-linearity in energy dissipation always exists, and this is the reason for parametric oscillation attenuation.
Based on this approach, the mechanism of friction-induced oscillations is proposed in ball ore mills—including their journal bearings diagnostics and different types of other industrial machines [57], e.g., steel rolling mills [86,87,88], where the effect of synchronization is also observed, like in ball mills.
Regardless of applied models for frictional interaction investigation, this dynamic phenomenon has shown the following common features observed in many experimental studies [89]:
  • Quick relative displacements observed at low speeds of mutual sliding of surfaces disappear with increasing speed;
  • The amplitude and frequency of the separate displacements depend on the sliding speed, the mass of the moving body and the rigidity of the system;
  • The first displacement of contacted bodies is much larger than the subsequent ones.
The appearance of abrupt displacements is explained either by the presence of a negative (falling) section of the friction force (moment) characteristic by sliding velocity or by an increase in the static friction force, which depends on the duration of the motionless contact.
Aiming to form an accurate mathematical description of the mill behavior, compromising between extreme operational states (Figure 6), a semi-phenomenological model extending the torque-arm-based equations [90], taking into account centrifugal mode of the load occurring at high rotational speed values, was developed by [91].
The author has shown that in the case of high-speed mills the Bond model is inadequate for describing their behavior and highlighted the need for investigation of the liners’ design and model parameters. Models allowing for a better description of the material flow, including the influence of the mill’s operating conditions and physical parameters of the ground ore, were presented by [92]. The authors used a geometric approach to investigate particles breakage process, obtaining equations describing the grinding media’s motion and the slippage relationships of mill’s charge In [93] mathematical models linking external signals (bearing pressure, power draw, and acoustic emission) with internal parameters of the mill, that can be utilized for optimization of the comminution process were presented.
A specific energy model and power consumption mathematical models derived with the use of the operational data from 4 industrial grinding circuits in Chilean Cu beneficiation plants were proposed by [94]. Despite having the potential to be used for predictive optimization of comminution processes, the model—referring to the authors’ words—can be useful for the SAG mills’ design purposes. In addition to the standard design variables (size of the mills, grinding media charge level, the concentration of solids in feed, rotation speed—expressed as a percentage of critical speed), an additional granulometric variable was included to account for PSD.

4.2. Discrete Element Method

The recent rapid increase of computational power allowed researchers and technicians to use numerical methods that reflect the granular nature of the feed better, applying discontinuous simulations. The most widely utilized technique of such type is a discrete element method (DEM) [95]. Discrete numerical models were already found to be valid for the study of granular assemblies’ dynamics in 1979 [96]; however, for more than a decade DEM’s practical applications remained restrained to 2D analyses because even when the problem was simplified to two dimensions, it still took “hours of super-computer time” to solve it [97]. Despite the fact that the computational abilities of that day’s supercomputers were incomparable even to those of current smartphone devices, the authors of [98] have already managed to obtain some valuable information about the energy distribution, which occurs when ball-shape-represented particles collide. In a further study, the same authors found a potential of DEM to be employed for predictions of a real mill’s power draw [97]. The method was later extended to three-dimensions and applied to assess the mill’s power draw in a broad range of working conditions. Moreover, it could correctly model the motion of grinding media, what was confirmed by comparison with mill power consumption’s torque-based measurement and with video recordings of the charge’s behavior [99]. In [100] previously developed models were compared, to show their usefulness in describing different issues related to the charge movement. The model proposed in [101] was presented as an appropriate one for the definition of charge’s outer boundary behavior [102]—was found a valuable contribution, properly describing the movement of individual balls, whereas the advantage of the one presented in [103] was the ability of a quick charge profile’s computation. In [104] some constructive criticism about the definitions of significant parameters describing the behavior of intra-mill material has appeared. What is more, the authors presented how, and with which parameters as an input, the severity and incidence of impacting can be calculated, which is undoubtedly valuable from the mill’s design point of view. In a work devoted to the modeling of mill’s power draw with use of 3D discrete element method [105], the author proposes a method for decreasing the computational demand by assigning the mass of finer fractions, which require shorter timesteps, to the next coarser fraction classes. In this way, due to the increased timestep of the calculation, its speed was successfully reduced, allowing the modeling of the power consumption with the use of DEM—similarly accurately as in the case of empirical models however with higher flexibility. Another important contribution to the development of DEM as a tool for optimization and description of the comminution process in ball mills was the introduction of Smoothed Particle Hydrodynamics (SPH) [106,107]. It significantly improved the modeling of mill charge’s dynamic behavior, enabling additional predictions related to the fluid slurry flow, as a result providing more realistic simulations. Examples of such simulations are presented in Figure 7 and Figure 8 below.
There is a significant simplification used in DEM modeling, however, which is the representation of intra-mill material in the form of spheres. Most of the raw materials subjected to comminution comprise irregular particles, the interactions of which can not be accurately described when they are not represented with realistic, complex shapes. Some researchers extended DEM models, replacing circular particle representations in 2D with:
  • Polygons [108];
  • Ellipses [109].
In the case of 3D models, they used:
  • Polyhedrons [110,111];
  • Ellipsoids [112];
  • Super quadratic functions [113].
As an example of a compromise between the realistic representation of ground material particles and the computational complexity of the used model, the so-called “stacked spheres approach” or “glued spheres approach” can be given. In the models based on such an approach, a real particle is represented using particles of various sizes, which can overlap to create a surface resembling natural material [114]. An exhaustive review of DEM modeling of non-spherical particle systems can be found in [115].
The above-mentioned methods undoubtedly have advantages in describing the material’s dynamic behavior in a more realistic way; however, some significant problems appear for the detection of contact between particles. Moreover, the computational power in the case of industrial scale-models limits their practical implementation.

5. Discussion and Conclusions

To provide optimal control of the comminution process under non-stationary properties of input raw materials, advanced measurement techniques are necessary. Despite the advanced design of modern ball mills’ automation systems, the existing controllers can only stabilize the deviations at a certain level of motor power without a significant reduction of overall energy consumption.
Having enormous power and rotating inertia, ball mills need in-depth research of their internal load dynamics by different tools. Using mathematical models, both analytical and DEM simulations can improve the understanding of the processed material flow, not available for direct observation. Nevertheless, 3D modeling of the grinding media and intra-mill material behavior is still being done with significant simplifications regarding particle shape, which are done due to the limited computational power, not sufficient to withstand industrial-scale simulations, and due to the fact that basic semi-empirical formulas do not account for the complex structure of raw material.
The most profitable mode of mill operation is when the central part oscillates up and down over the rest of the media treated, which corresponds to the synchronous mode of mill operation. This mode of parametric resonance can be achieved by regulation of input feeding rate, water supply (friction factor), or mill rotation speed (for variable speed motors).
The most reliable mill control is by electric motor current or power. These signals are easy for monitoring in the existing automation systems, but their capability is restricted to the diagnostics of the filling levels and wear rates of balls and protective liners.
Using vibration and acoustic signals from outside surfaces of the mill shell or other parts of the machine is a promising approach. However, its successful implementation for process control requires advanced signal processing methods and verification under non-stationary mill loading, and gradual wear of grinding bodies and internal protective liners, which affect the external measured signals. The neighboring mills’ noise and vibrations can also interfere with measured signals. Therefore some methods of shielding or direct fitting of wireless sensors to the mill shell surface should be used. In the latter case, algorithms of data processing should account for the instantaneous sensor position depending on the mill rotation speed.
Optimal control of technological parameters in the ball mills should be combined with the simultaneous online monitoring and diagnostics of balls’ and internal liners’ wear, as their condition greatly affects the measured sound and vibration signals.
Further research is planned for both laboratory mills and industrial plants in order to achieve a resonance mode of operation and its control by the different signals available for measurement and control.

Author Contributions

Conceptualization, P.K. and R.Z.; methodology, M.G.; formal analysis, S.O.; investigation, M.G.; resources, R.Z.; data curation, S.O.; writing—original draft preparation, P.K., M.G. and S.O.; writing—review and editing, M.G.; supervision, P.K.; project administration, R.Z.; funding acquisition, R.Z. All authors have read and agreed to the published version of the manuscript.


This research has received funding from European Institute of Innovation and Technology (EIT), a body of the European Union, under the Horizon 2020, the EU Framework Programme for Research and Innovation. This work is supported by EIT RawMaterials GmbH under framework partnership agreement number 18253 (OPMO—Operational Monitoring of Mineral Crushing Machinery).

Conflicts of Interest

The authors declare no conflict of interest.


  1. Walkiewicz, J.; Clark, A.; McGill, S. Microwave-assisted grinding. IEEE Trans. Ind. Appl. 1991, 27, 239–243. [Google Scholar] [CrossRef]
  2. Musa, F.; Morrison, R. A more sustainable approach to assessing comminution efficiency. Miner. Eng. 2009, 22, 593–601. [Google Scholar] [CrossRef]
  3. BCS Incoprorated for the U.S. Department of Energy: U.S. Mining Industry Energy Bandwidth Study. Available online: (accessed on 5 December 2020).
  4. Jeswiet, J.; Szekeres, A. Energy consumption in mining comminution. Procedia CIRP 2016, 48, 140–145. [Google Scholar] [CrossRef]
  5. Fuerstenau, D.; Abouzeid, A.Z. The energy efficiency of ball milling in comminution. Int. J. Miner. Process. 2002, 67, 161–185. [Google Scholar] [CrossRef]
  6. Mular, A. Mineral Processing Plant Design, Practice, and Control Proceedings; Society for Mining, Metallurgy, and Exploration: New York, NY, USA, 2002. [Google Scholar]
  7. Chelgani, S.C.; Parian, M.; Parapari, P.S.; Ghorbani, Y.; Rosenkranz, J. A comparative study on the effects of dry and wet grinding on mineral flotation separation—A review. J. Mater. Res. Technol. 2019, 8, 5004–5011. [Google Scholar] [CrossRef]
  8. Wang, Y.; Forssberg, E. Enhancement of energy efficiency for mechanical production of fine and ultra-fine particles in comminution. China Particuol. 2007, 5, 193–201. [Google Scholar] [CrossRef]
  9. Wills, B.A.; Napier-Munn, T. Comminution. In Wills’ Mineral Processing Technology; Butterworth-Heinemann: Oxford, UK, 2005; Chapter 5; pp. 108–117. [Google Scholar] [CrossRef]
  10. Sosa-Blanco, C.; Hodouin, D.; Bazin, C.; Lara-Valenzuela, C.; Salazar, J. Economic optimization of a flotation plant through grinding circuit tuning. Miner. Eng. 2000, 13, 999–1018. [Google Scholar] [CrossRef]
  11. Gao, P.; Zhou, W.; Han, Y.; Li, Y.; Ren, W. Enhancing the capacity of large-scale ball mill through process and equipment optimization: An industrial test verification. Adv. Powder Technol. 2020, 31, 2079–2091. [Google Scholar] [CrossRef]
  12. Nagar, N.; Garg, H.; Sharma, H.; Angadi, S.; Gahan, C. Influence of Grinding Time on The Bioleaching of Copper from Copper Slag. Biosci. Biotechnol. Res. Commun. 2019, 12, 512–522. [Google Scholar] [CrossRef]
  13. Jonsen, P.; Palsson, B.; Haggblad, H.A.; Tano, K.; Berggren, A. Simulation of charge and structure behaviour in a tumbling mill. In Proceedings of the European LS-DYNA Users Conference, Strasbourg, France, 23–24 May 2011. [Google Scholar]
  14. Astrom, K.; Wittenmark, B. Computer-Controlled Systems: Theory and Design; Prentice Hall: Upper Saddle River, NJ, USA, 1997. [Google Scholar]
  15. Craig, I. Grinding mill modeling and control: Past, present and future. In Proceedings of the 31st Chinese Control Conference, Anchui, China, 25–27 July 2012; pp. 16–21. [Google Scholar]
  16. Campbell, J.; Spencer, S.; Sutherland, D.; Rowlands, T.; Weller, K.; Cleary, P.; Hinde, A. SAG mill monitoring using surface vibrations. In Proceedings of the Third International Conference on Autogenous and Semiautogenous Grinding Technology (SAG2001), Vancouver, BC, Canada, 30 September–3 October 2001; Volume 2, pp. 373–385. [Google Scholar]
  17. Su, Z.; Wang, P.; Yu, X.; Lv, Z. Experimental investigation of vibration signal of an industrial tubular ball mill: Monitoring and diagnosing. Miner. Eng. 2008, 21, 699–710. [Google Scholar] [CrossRef]
  18. Bai, R.; Chai, T. Optimization control of ball mill load in blending process with data fusion and case-based reasoning. Huagong Xuebao/CIESC J. 2009, 60, 1746–1752. [Google Scholar]
  19. Tang, J.; Chai, T.; Zhao, L.; Yu, W.; Yue, H. Soft sensor for parameters of mill load based on multi-spectral segments PLS sub-models and on-line adaptive weighted fusion algorithm. Neurocomputing 2012, 78, 38–47. [Google Scholar] [CrossRef]
  20. Tang, J.; Zhao, L.; Yu, W.; Yue, H.; Chai, T. Soft Sensor Modeling of Ball Mill Load via Principal Component Analysis and Support Vector Machines. In Lecture Notes in Electrical Engineering; Springer: Berlin, Germany, 2010; pp. 803–810. [Google Scholar] [CrossRef]
  21. Tang, J.; Zhao, L.-j.; Zhou, J.-w.; Yue, H.; Chai, T.-y. Experimental analysis of wet mill load based on vibration signals of laboratory-scale ball mill shell. Miner. Eng. 2010, 23, 720–730. [Google Scholar] [CrossRef]
  22. Tang, J.; Zhao, L.; Yue, H.; Yu, W.; Chai, T. Vibration Analysis Based on Empirical Mode Decomposition and Partial Least Square. Procedia Eng. 2011, 16, 646–652. [Google Scholar] [CrossRef]
  23. Das, S.P.; Das, D.P.; Behera, S.K.; Mishra, B.K. Interpretation of mill vibration signal via wireless sensing. Miner. Eng. 2011, 24, 245–251. [Google Scholar] [CrossRef]
  24. Tang, J.; Chai, T.; Yu, W.; Zhao, L. Modeling Load Parameters of Ball Mill in Grinding Process Based on Selective Ensemble Multisensor Information. IEEE Trans. Autom. Sci. Eng. 2013, 10, 726–740. [Google Scholar] [CrossRef]
  25. Mohanty, S.; Gupta, K.K.; Raju, K.S. Vibration Feature Extraction and Analysis of Industrial Ball Mill Using MEMS Accelerometer Sensor and Synchronized Data Analysis Technique. Procedia Comput. Sci. 2015, 58, 217–224. [Google Scholar] [CrossRef]
  26. Nayak, D.K.; Das, D.P.; Behera, S.K.; Das, S.P. Monitoring the fill level of a ball mill using vibration sensing and artificial neural network. Neural Comput. Appl. 2019, 32, 1501–1511. [Google Scholar] [CrossRef]
  27. Behera, B.; Mishra, B.; Murty, C. Experimental analysis of charge dynamics in tumbling mills by vibration signature technique. Miner. Eng. 2007, 20, 84–91. [Google Scholar] [CrossRef]
  28. Cho, K.S.; Kim, S.H.; Lee, Y.H. Correlation between Acoustic Intensity and Ground Particle Size in Alumina Ball Mill Process. J. Korean Ceram. Soc. 2018, 55, 275–284. [Google Scholar] [CrossRef]
  29. Aldrich, C.; Theron, D. Acoustic estimation of the particle size distributions of sulphide ores in a laboratory ball mill. J. S. Afr. Inst. Min. Metall. 2000, 100, 243–248. [Google Scholar]
  30. Pax, R.; Djordjevic, N.; Hocking, R. Non contact acoustics measurement and validation of SAG mill operation. In Proceedings of the XXII International Mineral Processing Congress, Cape Town, South Africa, 29 September–3 October 2003; SAIMM: Cape Town, South Africa, 2003; Volume 1, pp. 371–377. [Google Scholar]
  31. Wu, D.; Chen, W.; Yan, H.; Fischer, J.; Doolan, C. Identifying grinding mill dynamics using acoustic beamforming and numerical modelling. Powder Technol. 2020, 371, 231–243. [Google Scholar] [CrossRef]
  32. Zeng, Y.; Forssberg, E. Monitoring grinding parameters by signal measurements for an industrial ball mill. Int. J. Miner. Process. 1993, 40, 1–16. [Google Scholar] [CrossRef]
  33. Tang, J.; Liu, Z.; Wu, Y.J.; Zhao, L.J. Modeling Difficult-to-Measure Process Parameters Based on Intrinsic Mode Functions Frequency Spectral Features of Mechanical Vibration and Acoustical Signals. Adv. Mater. Res. 2014, 989–994, 3671–3674. [Google Scholar] [CrossRef]
  34. Tang, J.; Yu, W.; Chai, T.; Liu, Z.; Zhou, X. Selective ensemble modeling load parameters of ball mill based on multi-scale frequency spectral features and sphere criterion. Mech. Syst. Signal Process. 2016, 66–67, 485–504. [Google Scholar] [CrossRef]
  35. Tang, J.; Chai, T.; Yu, W.; Liu, Z.; Zhou, X. A Comparative Study That Measures Ball Mill Load Parameters Through Different Single-Scale and Multiscale Frequency Spectra-Based Approaches. IEEE Trans. Ind. Inform. 2016, 12, 2008–2019. [Google Scholar] [CrossRef]
  36. Tang, J.; Qiao, J.; Liu, Z.; Zhou, X.; Yu, G.; Zhao, J. Mechanism characteristic analysis and soft measuring method review for ball mill load based on mechanical vibration and acoustic signals in the grinding process. Miner. Eng. 2018, 128, 294–311. [Google Scholar] [CrossRef]
  37. Kolacz, J. Measurement system of the mill charge in grinding ball mill circuits. Miner. Eng. 1997, 10, 1329–1338. [Google Scholar] [CrossRef]
  38. Morrell, S. Power Draw of Grinding Mills—Its measurements and Prediction. In Proceedings of the 5th Mill Operators Conference, Roxby Downs, Australia, 16–20 October 1994. [Google Scholar]
  39. Melero, M.; Cano, J.; Norniella, J.; Pedrayes, F.; Cabanas, M.; Rojas, C.; Alonso, G.; Aguado, J.M.; Ardura, P. Electric motors monitoring: An alternative to increase the efficiency of ball mills. Renew. Energy Power Qual. J 2014, 849–854. [Google Scholar] [CrossRef]
  40. Pontt, J. MONSAG: A new monitoring system for measuring the load filling of a SAG mill. Miner. Eng. 2004, 17, 1143–1148. [Google Scholar] [CrossRef]
  41. Cleary, P. Predicting charge motion, power draw, segregation and wear in ball mills using discrete element methods. Miner. Eng. 1998, 11, 1061–1080. [Google Scholar] [CrossRef]
  42. Esteves, P.M.; Stopa, M.M.; Filho, B.J.C.; Galery, R. Charge behavior analysis in ball mill by using estimated torque. In Proceedings of the 2014 IEEE Industry Application Society Annual Meeting, Vancouver, BC, Canada, 5–9 October 2014. [Google Scholar] [CrossRef]
  43. Campbell, J.; Holmes, R.; Spencer, S.; Sharp, V.; Davey, K.; Barker, D.; Phillips, P. The collection and analysis of single sensor surface vibration data to estimate operating conditions in pilot-scale and production-scale AG/SAG mills. In Proceedings of the XXII International Mineral Processing Congress, Cape Town, South Africa, 29 September–3 October 2003; pp. 280–288. [Google Scholar]
  44. Martins, S.; Li, W.; Radziszewski, P.; Caron, S. Investigating the differences in charge dynamics due to a variation of the instrumented ball properties. IFAC Proc. Vol. 2007, 12, 463–468. [Google Scholar] [CrossRef]
  45. Martins, S.; Li, W.; Radziszewski, P.; Caron, S.; Aguanno, M.; Bakhos, M.; Petch, E.L. Validating the instrumented ball outputs with simple trajectories. Miner. Eng. 2008, 21, 782–788. [Google Scholar] [CrossRef]
  46. Martins, S.; Li, W.; Radziszewski, P.; Faucher, A.; Makni, S. Experimental and simulated instrumented ball in a tumbling mill—A comparison. Miner. Eng. 2013, 43–44, 79–84. [Google Scholar] [CrossRef]
  47. Coetzee, L. Stabilising and optimising a primary closed-loop milling circuit feeding a flotation circuit using StarCS RNMPC. In Proceedings of the 19th IFAC World Congress on International Federation of Automatic Controll Congress, Cape Town, South Africa, 24–29 August 2014; Volume 47, pp. 9786–9791. [Google Scholar] [CrossRef]
  48. Coetzee, L.; Ramonotsi, M. Applying StarCS RNMPC with Real-Time Optimiser to Pilanesberg Platinum Mines Primary UG2 Milling Circuit. IFAC-PapersOnLine 2016, 49, 78–83. [Google Scholar] [CrossRef]
  49. Outotec. Outotec Automation Solutions for Grinding Optimization. Available online: (accessed on 5 November 2020).
  50. FLSmidth. Maximize Grinding Efficiency with LoadIQ. Available online: (accessed on 5 November 2020).
  51. Thwaites, P. Developments in Process Control—Grinding Controls. 2015. Available online:—Grinding-Controls-by-P-Thwaites.pdf (accessed on 5 November 2020).
  52. AMEplus. MillVis: System for the Optimization of the Grinding Process Control. Available online: (accessed on 5 November 2020).
  53. Chai, T.; Ding, J. Integrated automation system for hematite ores processing and its applications. Meas. Control 2006, 39, 140–146. [Google Scholar]
  54. Kuzba, B.; Pawlos, W.; Konieczny, A.; Krzeminska, M. Optimisation Platform for copper ore processing at the Division of Concentrator of KGHM Polska Miedz SA. In Proceedings of the E3S Web of Conferences; EDP Sciences: Les Ulis, France, 2016; Volume 8, p. 01037. [Google Scholar]
  55. Zhou, P.; Chai, T.; Wang, H. Intelligent Optimal-Setting Control for Grinding Circuits of Mineral Processing Process. IEEE Trans. Autom. Sci. Eng. 2009, 6, 730–743. [Google Scholar] [CrossRef]
  56. Deineka, K.; Naumenko, Y. Revealing the effect of decreased energy intensity of grinding in a tumbling mill during selfexcitation of autooscillations of the intrachamber fill. Eastern-Eur. J. Enterp. Technol. 2019, 1, 6–15. [Google Scholar] [CrossRef]
  57. Maryuta, A. Frictional Oscillations in Mechanical Systems; Nedra: Moscow, Russia, 1993; p. 240. [Google Scholar]
  58. Naumenko, Y. Fundamentals of the Theory of Working Processes of Drum Mills; NUVGP: Rivne, Ukraine, 2014; p. 336. [Google Scholar]
  59. Deineka, K.; Naumenko, Y. Establishing the effect of a decrease in power intensity of self-oscillating grinding in a tumbling mill with a reduction in an intrachamber fill. Eastern-Eur. J. Enterp. Technol. 2019, 6, 43–52. [Google Scholar] [CrossRef]
  60. Alekseyev, M.; Alkhori, F. Automated control of ore-pebble mill charge by the signal of active power of magnetic separator electric motor. Sci. Bull. Natl. Min. Univ. Ukraine 2014, 3, 71–76. [Google Scholar]
  61. Atutxa, I.; Legarra, I. Stepping forward: Using variable speed drives for optimizing the grinding process in SAG and ball mills. In Proceedings of the Sixth International Conference on Semi-Autogenous High Pressure Grinding Technology, Vancouver, BC, Canada, 20–24 September 2015. [Google Scholar]
  62. Smotritskiy, A.; Smotritskiy, A.; Boriskov, F.; Chervyakov, S. Method for Grinding Materials in Rotating Drum Using Ferromagnetic Grinding Bodies. EU Patent EP3020483B1, 8 July 2013. [Google Scholar]
  63. Vertimill. Metso Mining. Available online: (accessed on 5 November 2020).
  64. Isamill. Glencore Technology. Available online: (accessed on 5 November 2020).
  65. Krot, P. Telemetering systems for monitoring dynamic loads in drive lines of rolling mills. Vib. Mach. Meas. Reduct. Prot. 2008, 1, 46–53. [Google Scholar]
  66. Krot, P. Methods and instrumentation for measuring wear in drivelines of rolling mills. Metall. Process. Equip. 2003, 2, 45–53. [Google Scholar]
  67. Krot, P. Dynamics and diagnostics of the rolling mills drivelines with non-smooth stiffness characteristics. In Proceedings of the 3rd International Conference of Nonlinear Dynamic (ND-KhPI2010), Kharkov, Ukraine, 21–24 September 2012; pp. 115–120. [Google Scholar]
  68. Tang, J.; Chai, T.Y.; Cong, Q.M.; Liu, Z.; Yu, W. Modeling mill load parameters based on selective fusion of multi-scale shell vibration frequency spectra. Kongzhi Lilun Yu Yingyong/Control Theory Appl. 2015, 32, 1582–1591. [Google Scholar] [CrossRef]
  69. Meshcheryakov, L. Recognition of the operational state of the lining of drum mill. Sci. Bull. Natl. Min. Univ. Ukraine 2018, 53, 200–213. [Google Scholar]
  70. Vinogradov, B. Dynamics of Tumbling Mills; Economic Herald of State Higher Educational Institution, USUCT: Dnipro, Ukraine, 2004. [Google Scholar]
  71. Vinogradov, B.; Khristenko, A. The forced vibrations are in twin-engine synchronous drives of ball mills. Sci. Bull. Natl. Min. Univ. Ukraine 2012, 6, 72–76. [Google Scholar]
  72. Krot, P.V. Dynamical processes in a multi-motor gear drive of heavy slabbing mill. J. Vibroeng. 2019, 21, 2064–2081. [Google Scholar] [CrossRef]
  73. Borodai, V.; Borovyk, R.; Nesterova, O. Efficient transient modes of synchronous drive for mining and smelting mechanisms. Mech. Mater. Sci. Eng. J. 2017, 8. [Google Scholar] [CrossRef]
  74. Putnoki, A.; Klevtsov, O.; Ermolenko, A.; Verenev, V.; Krot, P. Evaluation of operation of equipment at the rolling mill. Stal 2003, 10, 56–58. [Google Scholar]
  75. Maryuta, A.; Kovalenko, A.; Meshcheryakov, L. Method for Determining Wear of Shaped Linings in Grinding Aggregate. Patent SU709173, 15 January 1980. [Google Scholar]
  76. Beke, B. The Process of Fine Grinding, 1st ed.; Springer: Dordrecht, The Netherlands, 1981; Volume 1. [Google Scholar] [CrossRef]
  77. Nussbaumer, H.J. Fast Fourier Transform and Convolution Algorithms; Springer: Berlin, Germany, 1982. [Google Scholar] [CrossRef]
  78. Konieczny, A.; Ogonowski, S.; Kurzydlo, M.; Foszcz, D. Vision systems in O/ZWR as a support tool for production management and optimization. In Proceedings of the Mineral Engineering Conference (MEC2014), Istebna, Poland, 15–18 September 2014. [Google Scholar]
  79. Thomas, A.; Filippov, L. Fractures, fractals and breakage energy of mineral particles. Int. J. Miner. Process. 1999, 57, 285–301. [Google Scholar] [CrossRef]
  80. Naziemiec, Z.; Saramak, D. Analiza energochłonności procesów rozdrabniania kruszyw mineralnych. Prace Naukowe Instytutu Górnictwa Politechniki Wrocławskiej. Studia i Materiały 2012, 134, 209–220. [Google Scholar]
  81. Weidenbaum, S.S. Mixing of solids. In Advances in Chemical Engineering; Elsevier: Amsterdam, The Netherlands, 1958; Volume 2, pp. 209–324. [Google Scholar]
  82. Heim, A.; Gluba, T.; Obraniak, A. Bed dynamics during drum granulation. Fizykochemiczne Problemy Mineralurgii/Physicochem. Probl. Miner. Process. 2004, 38, 167–176. [Google Scholar]
  83. Maryuta, A.N. Analysis of motion of mechanical systems with frictional interaction. Sov. Appl. Mech. 1989, 25, 1031–1040. [Google Scholar] [CrossRef]
  84. Butikov, E.I. Analytical expressions for stability regions in the Ince–Strutt diagram of Mathieu equation. Am. J. Phys. 2018, 86, 257–267. [Google Scholar] [CrossRef]
  85. Mardiansyah, Y.; Khotimah, S.; Viridi, S. Characterization of motion modes of pseudo-two dimensional granular materials in a vertical rotating drum. J. Phys. Conf. Ser. 2016, 739, 012148. [Google Scholar] [CrossRef]
  86. Marjuta, A.; Krot, P. High frequency rolling mills chatter–mathematical identification and simulation. In Proceedings of the 1st International Symposium on “Multi-Body Dynamics Monitoring and Simulation Techniques”, Bradford, UK, 25–27 March 1997; pp. 407–419. [Google Scholar]
  87. Krot, P. Parametrical vibrations in the rolling mills. Collect. Sci. Pap. Natl. Min. Acad. Ukraine 2002, 3, 15–21. [Google Scholar]
  88. Krot, P. Investigation of ’ribbing’ defect and high-frequency oscillations of mills for strip cold rolling. Proizvod. Prokata 2002, 3, 21–23. [Google Scholar]
  89. Kragelsky, I.; Dobychin, M.; Kombalov, V. Friction and Wear: Calculation Methods; Pergamon Press: Oxford, UK, 1982; p. 474. [Google Scholar]
  90. Arbiter, N.; Harris, C. Scale-up and dynamics of large grinding mills-a case study. In Design and Installation of Comminution Circuits; AIME: New York, NY, USA, 1982; pp. 491–508. [Google Scholar]
  91. Moys, M. A model of mill power as affected by mill speed, load volume, and liner design. J. S. Afr. Inst. Min. Metall. 1993, 93, 135–141. [Google Scholar]
  92. Abou, S.C.; Tarasiewicz, S.; Remy, M. Mathematical modelling of ball mill charge slippage: Geometric approach. In Proceedings of the 4e Conférence International sur l’Automatisation Industrielle, Montréal, QC, Canada, 9–11 June 2003; CIAI: Montreal, QC, Canada, 2003. [Google Scholar] [CrossRef]
  93. Wang, Z.H.; Han, Y.X.; Chen, B.C. A Mathematical Model for Predicting the Internal Parameters of Ball Mill. Adv. Mater. Res. 2012, 454, 151–156. [Google Scholar] [CrossRef]
  94. Silva, M.; Casali, A. Modelling SAG milling power and specific energy consumption including the feed percentage of intermediate size particles. Miner. Eng. 2015, 70, 156–161. [Google Scholar] [CrossRef]
  95. Kozicki, J.; Donze, F. YADE-OPEN DEM: An opensource software using a discrete element method to simulate granular material. Eng. Comput. 2008, 26. [Google Scholar] [CrossRef]
  96. Cundall, P.A.; Strack, O.D.L. A discrete numerical model for granular assemblies. Géotechnique 1979, 29, 47–65. [Google Scholar] [CrossRef]
  97. Mishra, B.; Rajamani, R.K. The discrete element method for the simulation of ball mills. Appl. Math. Model. 1992, 16, 598–604. [Google Scholar] [CrossRef]
  98. Mishra, B.K.; Rajamani, R.K. Motion Analysis in Tumbling Mills by the Discrete Element Method. KONA Powder Part. J. 1990, 8, 92–98. [Google Scholar] [CrossRef]
  99. Agrawala, S.; Rajamani, R.; Songfack, P.; Mishra, B. Mechanics of media motion in tumbling mills with 3d discrete element method. Miner. Eng. 1997, 10, 215–227. [Google Scholar] [CrossRef]
  100. Radiszewski, P. Comparing three DEM charge motion models. Miner. Eng. 1999, 12, 1501–1520. [Google Scholar] [CrossRef]
  101. Powell, M.; Nurick, G. A study of charge motion in rotary mills Part 1—Extension of the theory. Miner. Eng. 1996, 9, 259–268. [Google Scholar] [CrossRef]
  102. Mishra, B.; Rajamai, R.K. Simulation of charge motion in ball mills. Part 2: Numerical simulations. Int. J. Miner. Process. 1994, 40, 187–197. [Google Scholar] [CrossRef]
  103. Radziszewski, P.; Tarasiewicz, S. Ballmill simulation: Part II—Numerical solution to ballcharge model. Trans. Soc. Comput. Simul. 1989, 6, 75–88. [Google Scholar]
  104. Powell, M.; McBride, A. A three-dimensional analysis of media motion and grinding regions in mills. Miner. Eng. 2004, 17, 1099–1109. [Google Scholar] [CrossRef]
  105. Djordjevic, N. Influence of charge size distribution on net-power draw of tumbling mill based on DEM modelling. Miner. Eng. 2005, 18, 375–378. [Google Scholar] [CrossRef]
  106. Cleary, P.W.; Morrison, R.D. Prediction of 3D slurry flow within the grinding chamber and discharge from a pilot scale SAG mill. Miner. Eng. 2012, 39, 184–195. [Google Scholar] [CrossRef]
  107. Jahani Chegeni, M. Combined DEM and SPH simulation of ball milling. J. Min. Environ. 2019, 10, 151–161. [Google Scholar] [CrossRef]
  108. Walton, O. Particle-Dynamics Calculations of Shear Flow. In Mechanics of Granular Materials—New Models and Constitutive Relations; Elsevier: Amsterdam, The Netherlands, 1983; pp. 327–338. [Google Scholar] [CrossRef]
  109. Ting, J.M.; Khwaja, M.; Meachum, L.R.; Rowell, J.D. An ellipse-based discrete element model for granular materials. Int. J. Numer. Anal. Methods Geomech. 1993, 17, 603–623. [Google Scholar] [CrossRef]
  110. Cundall, P. Formulation of a three-dimensional distinct element model—Part I. A scheme to detect and represent contacts in a system composed of many polyhedral blocks. Int. J. Rock Mech. Min. Sci. Geomech. Abstr. 1988, 25, 107–116. [Google Scholar] [CrossRef]
  111. Hocking, G. The discrete element method for analysis of fragmentation of discontinua. Eng. Comput. 1992, 9, 145–155. [Google Scholar] [CrossRef]
  112. Lin, X.; Ng, T.T. A three-dimensional discrete element model using arrays of ellipsoids. Geotechnique 1997, 47, 319–329. [Google Scholar] [CrossRef]
  113. Williams, J.R.; Pentland, A.P. Superquadrics and modal dynamics for discrete elements in interactive design. Eng. Comput. 1992, 9, 115–127. [Google Scholar] [CrossRef]
  114. Favier, J.; Fard, M.; Kremmer, M.; Raji, A. Shape representation of axi-symmetrical, non-spherical particles in discrete element simulation using multi-element model particles. Eng. Comput. Int. J. Comput.-Aided Eng. 1999, 16, 467–480. [Google Scholar] [CrossRef]
  115. Zhong, W.; Yu, A.; Liu, X.; Tong, Z.; Zhang, H. DEM/CFD-DEM modelling of non-spherical particulate systems: Theoretical developments and applications. Powder Technol. 2016, 302, 108–152. [Google Scholar] [CrossRef]
Figure 1. Energy saving potential for various energy-intensive processes in mining [3]. 1 Btu (British thermal unit) ≈ 1055 Joule.
Figure 1. Energy saving potential for various energy-intensive processes in mining [3]. 1 Btu (British thermal unit) ≈ 1055 Joule.
Energies 13 06735 g001
Figure 2. Schematic representation of the measured parameters and the parameters to be manipulated in order to obtain appropriate performance of the mill.
Figure 2. Schematic representation of the measured parameters and the parameters to be manipulated in order to obtain appropriate performance of the mill.
Energies 13 06735 g002
Figure 3. Location of the vibration sensors on the mill’s shell (A) and time series of the ball mill vibration measurements (black, blue, and red representing separate full convolutions) and a rotation signal reconstructed from the original (B).
Figure 3. Location of the vibration sensors on the mill’s shell (A) and time series of the ball mill vibration measurements (black, blue, and red representing separate full convolutions) and a rotation signal reconstructed from the original (B).
Energies 13 06735 g003
Figure 4. Ball mill (A) and rod mill (B) vibration signals presented on polar plots.
Figure 4. Ball mill (A) and rod mill (B) vibration signals presented on polar plots.
Energies 13 06735 g004
Figure 5. Characterization of steel granular materials’ motion modes for given drum geometries and rotational speeds (A) [85] and the fragment of the Ince–Strutt diagram for the Froude pendulum-based dynamics model (B) [83].
Figure 5. Characterization of steel granular materials’ motion modes for given drum geometries and rotational speeds (A) [85] and the fragment of the Ince–Strutt diagram for the Froude pendulum-based dynamics model (B) [83].
Energies 13 06735 g005
Figure 6. Internal load motion in the ball mill under different operational modes [85].
Figure 6. Internal load motion in the ball mill under different operational modes [85].
Energies 13 06735 g006
Figure 7. An example of typical mill flow pattern simulated with use of DEM. On the left-hand side (A) the particles are colored by diameter, dark blue being the finest and red the coarsest. On the right-hand side (B) the particles are colored by speed—blue being the slowest and red the fastest [106].
Figure 7. An example of typical mill flow pattern simulated with use of DEM. On the left-hand side (A) the particles are colored by diameter, dark blue being the finest and red the coarsest. On the right-hand side (B) the particles are colored by speed—blue being the slowest and red the fastest [106].
Energies 13 06735 g007
Figure 8. An example of a 3D DEM simulation of particle flow, based on (A) the only-solid-phase approach (basic DEM) and (B) combining DEM with SPH to take into account both phases: solid and liquid [107].
Figure 8. An example of a 3D DEM simulation of particle flow, based on (A) the only-solid-phase approach (basic DEM) and (B) combining DEM with SPH to take into account both phases: solid and liquid [107].
Energies 13 06735 g008
Table 1. Examples of scientific papers contributing to the optimization of comminution in tumbling mills by signal monitored.
Table 1. Examples of scientific papers contributing to the optimization of comminution in tumbling mills by signal monitored.
Signal MonitoredWork
Vibration [16,17,18,19,20,21,22,23,24,25,26,27,32,33,34,35,36,37,68] (with use of strain transducer), [43,51]
(estimated based on torque), [54]
Acoustic Emission [24,28,29,30,31,32,33,34,35,36,51,54]
Power Draw [38,51,69]
Instrumented Ball [44,45,46]
Vision [46,51,54]
Other [24]—motor current, [39]—torque, [40]—bearing pressure and motor vector control,  [42]—torque signal estimated on the basis of angular position and motor electric signals, [55]—product particle size (PPS) soft sensor
Table 2. Examples of scientific papers contributing to the optimization of comminution in tumbling mills by different criteria.
Table 2. Examples of scientific papers contributing to the optimization of comminution in tumbling mills by different criteria.
Purpose of MeasurementWork
Power draw reduction [32]
Wear reduction [31,43,54]
Particle size distribution optimization[25,28,29,32,51,54,55]
Detection of characteristic working conditions[17,23,27,51]
Fill level/behaviour[16,18,19,20,21,22,26,30,31,34,37,39,40,42,44,45,68]
Other [32]—pulp temperature, [51,55]—throughput maximization, [46]—DEM tuning, [69]—wear diagnostics of liners
Table 3. Examples of milling process parameters to be assessed by the measurement of particular signals.
Table 3. Examples of milling process parameters to be assessed by the measurement of particular signals.
Signal Measured/Process ParametersFill LevelBalls WearLiners WearParticle Size Distribution
Power draw
Other signals from electric motor
Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Back to TopTop