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Journal of the Southern African Institute of Mining and Metallurgy

versión On-line ISSN 2411-9717
versión impresa ISSN 2225-6253

J. S. Afr. Inst. Min. Metall. vol.119 no.10 Johannesburg oct. 2019

http://dx.doi.org/10.17159/2411-9717/707/2019 

GENERAL PAPERS

 

Ventilation friction factor determination and comparison: Two case studies of potash mining

 

 

M. Bascompta; L. Sanmiquel; H.F. Anticoi; J. Oliva

Department of Mining, Industrial and ICT Engineering, Polytechnic University of Catalonia, Spain

Correspondence

 

 


SYNOPSIS

Friction factor is a crucial parameter in assessing and modelling ventilation systems in underground mining. However, the development of a mine along its life-cycle can complicate the airflow supply required at the working faces, creating setbacks in terms of productivity and production. Hence, it is very important to determine all the ventilation parameters, including roughness and the friction factor. In this paper we examine the data from several surveys that were carried out in two potash mines (both using the room-and-pillar method) with the aim of determining the friction factors through the Von Kármán equation, which connects the Atkinson friction factor with airway roughness. Comparison of the two mines provided consistent results, despite some differences in the mining methods, and we were able to establish standard values for this type of mining. Furthermore, a roughness variation over a year in this type of evaporitic mining has been determined, indicating that the specific climate characteristics of the zone affect the walls and roofs of the tunnels and therefore their roughness. Friction factor values have also been validated by means of several ventilation simulations and contrasted with values in the literature.

Keywords: mine ventilation, friction factor, potash mining, roughness.


 

 

Introduction

Knowing the ventilation characteristics is crucial for determining the most effective ventilation circuit and for enhancing the efficiency ratios and saving energy, especially with the trend toward deeper ore deposits and gradually decreasing ore grades (Kazakov, Shalimov, and Kiryakov, 2013; Sasmito et aí., 2013; du Plessis, Marx, and Nell, 2014; Hurtado et aí., 2014; Develo, Pillalamarry, and Garab, 2016). Airway characteristics and obstacles (e.^., conveyors, machines, or other equipment) determine the airflow behaviour and the resistance the mine presents to airflow. Therefore, knowing these is crucial for modelling ventilation circuits (Shalimov, 2011) and for planning long-term airflow requrements. One of the most important aspects to consider is the friction factor, which is dependent on the geometrical characteristics of the tunnels, the mining method, and the physical condition of the mine (Duckworth and Prosser, 1997; Alymenko, 2012). This friction factor is also a function of the roughness of the airways which, together with obstacles in the ventilation circuit (e.g., conveyor belts or doors), will create resistance to airflow.

The currently available information is mainly focused on coal and metal mines. McElroy (1935) published one of the first studies in this field based on pressure loss values collected from several mines. These values have been used for a long time, with only some changes in the case of coal mining by Kharkar, Stefanko, and Ramani (1974), who pointed out the influence of support and lining on the friction factors. The problem with these values is that current mine openings are much larger and the equipment used is completely different. Therefore, several studies have extended this information, taking into account the evolution of the sector over time (Wala, 1991; Hartman, 1997; Prosser and Wallace, 1999, 2002; Fytas and Gagnon, 2008; Jase and Sastry, 2008; Duckworth, Loomis, and Prosser, 2012), establishing an important database, but without specific values for potash mining.

In this paper we determine the friction factors for two underground mines using continuous mining machines and the room-and-pillar method. As will be seen in the following sections, this type of mining has intrinsic characteristics that influence the roughness of the drifts and consequently the ventilation system. Once the friction factors have been determined, a model of the ventilation circuit in each mine is formulated in order to verify the results by means of ventilation software.

 

Theoretical background

The square law (Equation [1]) is the basic expression used to investigate the airflow behaviour in underground mines (Hall, 1981; Meyer, 1998; McPherson, 1993; Diego et al., 2011), which relates the concepts of pressure, airflow, and resistance to the passage of air through an airway.

where:

ΔΡ is pressure difference (Pa)

R is Atkinson's resistance (Ns2/m8)

Q is amount of airflow (m3/s)

n is a value that varies from unity in laminar regimes to 2.05 in fully turbulent conditions (dimensionless).

The cases studied were always in turbulent conditions, as explained in the subsequent paragraphs. The pressure difference in an airway is a function of the resistance, characteristics of the tunnel, obstacles, and quantity of air flowing through that airway. This difference can be calculated directly, by carrying out a survey with a gauge-tube system or a barometer, or indirectly, by measuring the airflow and the characteristics of the airways, such as roughness (McPherson, 1993). This study is based on the indirect method.

Friction factors, which are determined by the roughness of the tunnels, produce a pressure drop that influences the airflow quantity. These values can be obtained using Equation [2], which is a form of the Chézy-Darcy expression:

where

f is coefficient of friction (dimensionless)

Per is airway perimeter (m)

A is the cross-sectional area (m2)

ρ is air density (kg/m3)

u is air velocity (m/s)

L is length of the airway (m).

Subsequently, Equation [2] was adapted to yield the well-known Atkinson equation (Equation [3]), expressed as frictional pressure drop . The equivalent length is used to take into account any permanent obstacle found in the airway.

where

k is the Atkinson friction factor (kg/m3)

Leqis equivalent length (m).

The same equation can also be expressed in terms of resistance using the square law (Equation [4]), and considering any variation in air density inside the mine due to pressure or temperature factors (Montecinos and Wallace, 2010).

The Atkinson friction factor is not a constant value; it varies depending on the Reynolds number. However, the airflow in the vast majority of underground places is turbulent in nature, except in a few cases such as behind stoppings or some leakages (McPherson, 1993). Thus, it has been considered as always turbulent in this paper.

Von Kármán's equation provides a relationship between the coefficient of friction and the friction factor from Atkinson's expression for turbulent flows by means of the drift characteristics. Equation [5] is applicable to circular and non-circular airways by means of the hydraulic mean diameter and is expressed as follows: Dh= 4A /Per, where A is the cross-sectional area (m2) and Per the perimeter (m).

where

Dh is the hydraulic mean diameter of the tunnel (m) e is the height of the roughening (m).

 

Data collection and methodology

Determination of the friction factors requires a database of the characteristics of the airways (Meyer, 1998). Thus, several points from the ventilation circuits in both mines have been selected to represent the airways and ventilation conditions. For this purpose, some friction factors in potash mines from the literature have been used (Bascompta, Sanmiquel, and Oliva, 2014), as well as a database system that was created with additional data collected in situ (Bascompta, Sanmiquel, and Oliva, 2015).

Once the points were chosen, all of them were given an identification number with the date and coordinates inside the mine. Five measurements of roughness were performed at each point every time, using a tape measure. Afterwards, the mean roughness values were classified according to the four seasons of the year. Overall, the drift characteristics have been measured over five years.

In addition, the cross-section and air velocity at each point were also measured to model the ventilation circuit. A rotating vane anemometer was used to obtain the mean velocity, and the cross-section was acquired by means of a laser distance measurement. Drift information such as length, obstacles, shape of the airway, and directional variations were also recorded.

Apart from the parameters collected, the mean values of perimeter, hydraulic diameter, and coefficient of friction at each control point were determined. The nomenclature used to identify the points is based on the information provided by the mines, and their number varies depending on the different ventilation layouts.

In order to facilitate the understanding and processing of the data, the mines are distinguished as Mine1 and Mine2 from here on.

 

Results

All data from both mines (Mine1 and Mine2) was processed separately, and then the outcomes were compared both between Mine1 and Mine2 and with other types of mining. The results for both mines are displayed by season and globally, with their corresponding standard deviations. Finally, the results were validated by means of modelling the ventilation system using the VnetPro software (SRK Consulting, Fresno, USA).

Mine1

Table I shows the mean values used to calculate the friction factors, with special focus on the coefficient of friction (f), which is a function of the other parameters in the table. These values were measured in situ or calculated using the data collected and the equations previously detailed. Airway features were adopted from Bascompta, Sanmiquel, and Oliva (2015).

 

 

The values displayed in Table II correspond to the mean friction factors per season and average values per point, considering the four-season values at each key point and their standard deviations (Box et al., 2005 ).

It should be pointed out that there are no results for points A and D in the summer, because the ventilation circuit was partially modified and there is insufficient representative data for these points.

Mine2

Tables III and IV detail the coefficients of friction, friction factors per season, and other parameters necessary to calculate the average friction factor at each point. The procedure followed was the same as that described in the previous subsection.

 

 

Comparison of outcomes

Initially, there was a significant difference (56.8%) between the mean roughness values in Mine1 and Mine2, 0.185 and 0.105 respectively. This fact is, among other factors explained below, because of the differences in the exploitation method.

A comparison of the friction factors between both mines and the values reported in the literature can be useful to know the variability and concordance of the results. Table V displays the mean friction factors from all the points in Mine1 and Mine2 according to the season.

Although the values are quite similar, the friction factors from Mine2 are lower in all seasons than those in Mine1, with an average difference of 23.4%. Thus, Mine2 offers better conditions for the air to flow in terms of friction within the drift. However, there are other features that could influence the flow, such as obstacles or directional changes.

Figure 1 compares the seasonal variations in the friction factors in each mine. As can be seen, the trends are quite similar, with higher values in the spring and autumn than in the winter and summer. This behaviour could be due to the important variations in temperature and humidity in the spring and autumn, even within the same day, which would affect the characteristics of the air and, therefore, the stability of the roofs and walls in the airways, changing the roughness and subsequently the friction factor values.

 

 

The difference in standard deviation between the two mines could be due to several factors, either intrinsic to the mines or related to operational characteristics such as airway maintenance, which is quite different in each mine.

Since there is no bibliographic information concerning underground potash mining, the values obtained were compared with the current parameters from coal and metal mines (Table VI). Comparison from the 'Mine ramp' airway type , in Table VI, has only been performed with values from Minel, because there is no ramp in Mine2. The other values were obtained using data from both mines. Table VI shows the percentage variation from values gathered by Bascompta et al. (2014) and from the current paper. As it can be seen, there is an important difference in some airway types, such as 'Mine ramp', but there is a significant correlation in most of the types of airways.

Validation

Tthe friction factors obtained for each season (Tables II and IV) were used to model both mines by means of the ventilation software VnetPro, and a comparison between the airflow modelled and the in situ measures was performed, either in Mine2 or Minel.

Mine1

Four different models, corresponding to the four seasons of the year, with their friction factors, have been constructed. Consistent results were achieved in all the cases, with the only appreciable variations in some leakages, in percentage terms. This is a standard behaviour in mine ventilation models, where leakages can cause high percentage differences. Hence, the airflow is within just a few cubic metres in these cases, without affecting the soundness of the model. Besides, a 10% difference can be considered acceptable in standard control points (Belle, 2013). Table VII displays the absolute and percentage variations between the measured and modelling control points. The comparison is done using the average variation in each mine.

Mine2

The same analysis is shown in Table VIII for Mine2. Once more, only airflows from leakages show considerable differences between the model and the real values.

 

Conclusions

Characteristic friction factors were determined in two potash mines using the room-and-pillar method. These values can be useful for mine ventilation planning, which usually relies on k-factor values to estimate the resistance of planned airways. The average and seasonal friction factor values have been assessed as suitable to create a ventilation model, depending on the climatic conditions where the mine is situated. However, more data from other similar operations is recommended to increase the accuracy.

Roughness of the airways varies slightly depending on the ventilation circuit zone and mine. Consistent differences in the friction factors over the year are found in Mine1 and Mine2, but these are too small to influence the model. In most cases in both mines, except for some leakages, the difference between the measured and modelled airflows is less than 10%.

After observing all the features from the case studies, it can be concluded that the roughness of the airways basically depends on three factors:

(1) The exploitation method and maintenance of the airways

(2) The nature of the deposit, which has certain deformable properties that affect the shape of the drifts

(3) The outside climatic conditions (temperature and humidity) have been proved to be significant factors in terms of roughness variations.

 

Acknowledgments

This work was supported by the ICL Chair in Mining Sustainability (UPC). The authors would like to thank the staff of both mines for their willingness and contributions to the results.

 

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Correspondence:
M. Bascompta
marc.bascompta@upc.edu

Received: 8 Apr. 2019
Revised: 7 Jul. 2019
Accepted: 29 Jul. 2019
Published: October 2019

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