J.Obiri - Yeboah and S. Arthur The Use of Statistical ...€¦ · hydrocyclones. The cluster of...
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J.Obiri- Yeboah and S. Arthur
The Use of Statistical Analysis for Hydrocyclone
Efficiency
for publication
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The Use of Statistical Analysis for Hydrocyclone Efficiency Estimation –
A Case Study
J. Obiri Yeboah and S. Arthur
Gold Fields Ghana Limited
P. O. Box 26
Tarkwa
Ghana
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ABSTRACT
In order to optimize gold liberation, an investigation was carried out to determine the particle
classification efficiency with respect to target set (i.e. 80 % - 75 µm) for the cluster of
hydrocyclones. The cluster of hydrocyclones, consist of eight cyclones of which seven are being
operated. A series of wet size analysis was performed over a period of one week, on the
cyclone overflow slurry, under cyclone vortex finder diameter of 10 inches and spigot diameter
of 6 inches.
Results indicate that operating at a cyclone pressure of 110 kPa – 120 kPa with 51 % - 60 %
solids feed density generates an overflow slurry density of 21 % - 31 % solids.
The cyclones had efficiencies between 65.38 % - 90.91 % with percentage passing 75 µm per
percentage solids of cyclone feed density as 0.6538 - 0.9091 respectively. Additionally, the
gradient establishes the extent of classification in relation to the set target and standard unit of
performance as percentage passing per percentage solids of cyclone feed density.
Feed density related linearly to percentage passing 75 µm, even at 1 % critical level of
significance. The prevailing parameters of cyclone pressure, feed rate, circulating load and fixed
parameters of Vortex finder and spigot diameters do not necessarily need to appear in the
formula for calculating or estimating efficiency since their resultant input and output
parameters are used.
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Key words:
hydrocyclones, Vortex finder, spigot diameters, percentage passing, of classification, test for
lineality and critical level
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1 INTRODUCTION
This study was carried out at Yosaj Goldfields Limited, Tarkwa, to optimize leaching in Carbon In
Leach (CIL) tanks of the company’s gold processing plant.
Generally , performance measurement indicates the level of resource usage or/ and a set target
achievement. The level of resource usage to achieve a set target is called efficiency and the
extent of target achievement depicts effectiveness.(Foulks Lynch Ltd, 2002).
Conventionally, the efficiency of a Hydrocyclone can be measured by estimating the probability
of the desired particle size appearing in a classified product (e.g. estimation of cyclone d 50 ). It
relates the weight fraction or percentage of each particle size in the feed which reports at the
apex or underflow to the particle size. The cut point or separation size refers to 50 % of particle
in the feed of d 50 size reporting to the underflow.
However, the Mineral Engineer is usually interested in knowing the fineness of grind reporting
at the overflow and the parameters to control to achieve a set target of fineness than cyclone
d 50 (B.A. Wills 1992). This makes it more important to provide this method of assessment. The
work assesses the use of statistical analysis to measure the level of efficiency of a hydrocyclone
as classification unit of a gold processing plant.
Invariably, at Yosaj Goldfields Limited, the needed grinding size of 80 % passing 75 µm, for the
effective liberation of gold, place important on the efficiency of the classification unit to
enhance leaching. The cluster of hydroclone unit currently in operation, had justification from
the increment in volume of slurry as a result of recent plant upgrade.
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Consequently, this investigation of the performance of hydrocyclones under their operating
conditions is to achieve optimum classification for thickening and leaching. This paper looks at
the relation between cyclone efficiency and cyclone feed density in order to enhance effective
operational control to achieve 80 % - 75 µm grind size, at the cyclone overflow product.
2 THE HYDROCYCLONE
Hydrocyclone is a classifying device that makes use of centrifugal force to increase the settling
rate of particles. It is made up of a cylindrical section connected to a conical shaped vessel with
an opening at the apex. The cylindrical section is closed off at the top with a pipe protruding
into the body of the cyclone. This is called the vortex finder.
The feed is introduced under pressure through the feed inlet, tangential to the cylindrical
section of the cyclone. This produces a spiral motion, which generates a vortex in the cyclone
with a low pressure zone along the vertical axis of the cyclone.
Particles in the pulp stream are subjected to an outward centrifugal force and inward drag force
or centripetal force. The coarsest or Heaviest particles are pulled by centrifugal force to the
inner walls of the cyclone displacing the finer, lighter particle and excess water towards the
center.Thus particles are graded by size and mass from outside to inside of the spinning
mixture. The coarsest or heaviest particles spiral down the walls and discharges through the
apex as underflow.
The split of particles is dependent on the balance between the centrifugal and drag forces and
hence the overall performance of a cyclone depends on the relative values of the radial and
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tangential velocities at all positions. For different solids and liquids, the values of fluid viscosity,
solids and fluids densities and effective values of diameter contribute to the overall cyclone
performance. Fig. 1 shows a sketch diagram of a hydrocyclone (Department of Minerals
Engineering and Extractive Metallurgy, 1988).
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Fig.1 HYDROCYCLONE
Vortex Finder
Feed Inlet
Feed Chamber
Spigot
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3 EXPERIMENTAL CONDITIONS AND SIZE ANALYSIS RESULTS
One liter of overflow samples were taken at a sampling frequency of one hour interval. The
respective overflow densities were measured and their corresponding cyclone feed densities ,
cyclone pressure and mill feed rate were tabulated in table 1 – 7. The samples were taken over
a period of seven days with twelve samples each day.
Each overflow sample was taken through wet sizing analysis using a screen with aperture of 75
µm. The respective +75 µm density was measured by the use of Marcy scale to deduce
corresponding percentage -75 µm from wet sizing log table for percentage passing 75µm of ore
with Specific gravity (SG) of 2.7 shown in fig. 2. Feed density, Mill feed rate and Cyclone
pressure were taken from the scada automatic digital recorded reports.
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Table 1 Test work Results and experimental condition for day 1
Time (hrs)
Feed
density
(% solids)
Overflow
density
(% solids)
Overflow
Density of
+75 µm
(% solids)
Mill Feed
Rate (t/hr)
Cyclone
Pressure
(kPa)
Overflow
Percentage
Passing
75 µm (%)
800 60 30 12 671 111 68
900 58 28 7 617 111 75
1000 57 23 5 669 110 78
1100 56 25 5 655 112 80
1200 58 28 8 618 110 71
1300 58 29 6 645 110 79
1400 60 28 9 655 115 68
1500 56 30 6 669 110 80
1600 57 25 7 671 111 72
1700 56 26 7 684 113 73
1800 59 28 5 615 110 82
1900 55 27 8 605 114 70
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Table 2 Test work Results and experimental condition for day 2
Time (hrs)
Feed
density
(% solids)
Overflow
density
(% solids)
Overflow
Density of
+75 µm
(% solids)
Mill Feed
Rate (t/hr)
Cyclone
Pressure
(kPa)
Overflow
Percentage
Passing
75 µm (%)
800 60 30 5 498 118 83
900 59 25 6 645 110 76
1000 59 31 12 603 116 61
1100 60 31 10 687 120 68
1200 58 27 8 620 117 70
1300 58 30 6 479 110 80
1400 57 27 4 510 111 85
1500 57 29 4 447 113 86
1600 51 21 6 505 110 76
1700 58 30 6 479 118 80
1800 58 25 5 480 110 80
1900 57 28 4 495 115 86
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Table 3 Test work Results and experimental condition for day 3
Time (hrs)
Feed
density
(% solids)
Overflow
density
(% solids)
Overflow
Density of
+75 µm
(% solids)
Mill Feed
Rate (t/hr)
Cyclone
Pressure
(kPa)
Overflow
Percentage
Passing
75 µm (%)
800 54 27 8 587 115 70
900 58 25 6 634 115 76
1000 59 30 9 600 110 70
1100 61 28 9 568 114 68
1200 60 27 8 630 118 70
1300 58 30 8 570 110 73
1400 56 24 6 529 113 75
1500 57 29 7 449 111 76
1600 56 25 6 507 120 76
1700 58 29 8 572 119 72
1800 58 29 9 498 116 69
1900 56 24 6 594 113 75
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Table 4 Test work Results and experimental condition for day 4
Time (hrs)
Feed
density
(% solids)
Overflow
density
(% solids)
Overflow
Density of
+75 µm
(% solids)
Mill Feed
Rate (t/hr)
Cyclone
Pressure
(kPa)
Overflow
Percentage
Passing
75 µm (%)
800 57 23 6 568 117 74
900 59 25 6 643 112 76
1000 58 26 9 602 115 65
1100 56 26 7 597 117 73
1200 58 27 8 595 117 70
1300 58 28 9 496 113 68
1400 57 29 7 573 120 76
1500 56 25 6 498 111 76
1600 53 21 5 572 112 78
1700 56 27 9 490 119 70
1800 57 24 6 585 111 75
1900 58 29 6 590 110 79
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Table 5 Test work Results and experimental condition for day 5
Time (hrs)
Feed
density
(% solids)
Overflow
density
(% solids)
Overflow
Density of
+75 µm
(% solids)
Mill Feed
Rate (t/hr)
Cyclone
Pressure
(kPa)
Overflow
Percentage
Passing
75 µm (%)
800 55 27 7 469 110 74
900 55 29 6 654 118 79
1000 57 25 6 604 115 76
1100 55 28 7 597 119 75
1200 57 27 6 623 120 78
1300 56 24 7 507 111 71
1400 57 24 6 582 113 75
1500 56 27 6 508 111 78
1600 57 25 7 512 115 72
1700 56 23 5 572 117 78
1800 55 25 5 459 112 80
1900 56 27 7 595 116 74
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Table 6 Test work Results and experimental condition for day 6
Time (hrs)
Feed
density
(% solids)
Overflow
density
(% solids)
Overflow
Density of
+75 µm
(% solids)
Mill Feed
Rate (t/hr)
Cyclone
Pressure
(kPa)
Overflow
Percentage
Passing
75 µm (%)
800 57 28 9 670 120 68
900 59 25 9 657 110 68
1000 59 26 8 681 118 69
1100 57 30 9 662 117 70
1200 59 27 8 598 115 70
1300 58 29 9 654 112 69
1400 57 30 9 625 114 70
1500 57 25 9 676 113 68
1600 58 25 6 717 110 76
1700 56 28 7 688 112 75
1800 55 23 6 598 114 74
1900 55 27 8 579 112 70
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Table 7 Test work Results and experimental condition for day 7
Time (hrs)
Feed
density
(% solids)
Overflow
density
(% solids)
Overflow
Density of
+75 µm
(% solids)
Mill Feed
Rate (t/hr)
Cyclone
Pressure
(kPa)
Overflow
Percentage
Passing
75 µm (%)
800 56 27 7 611 113 74
900 57 30 8 608 110 73
1000 57 25 7 663 111 72
1100 56 27 8 645 113 70
1200 58 29 9 617 115 69
1300 56 26 8 597 113 69
1400 57 25 9 615 114 68
1500 55 27 8 646 112 70
1600 55 29 8 617 114 72
1700 58 28 9 648 111 68
1800 57 27 8 651 112 70
1900 56 28 7 600 116 75
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4 STATISTICAL ANALYSIS OF TEST VALUES
Table 8 Analysis of day 1 experiment
Sample
No.
Feed
Density
(% solids)
X
Overflow
Percentage
Passing
75 µm (%)Y
XY
X 2
Y 2
1 60 68 4 080 3 600 4 624
2 58 75 4 350 3 364 5 625
3 57 78 4 446 3 249 6 084
4 56 80 4 480 3 136 6 400
5 58 71 4 118 3 364 5 041
6 58 79 4 582 3 364 6 241
7 60 68 4 080 3 600 4 624
8 56 80 4 480 3 136 6 400
9 57 72 4 104 3 249 5 184
10 56 73 4 088 3 136 5 329
11 59 82 4 838 3 481 6 724
12 55 70 3 850 3 025 4 900
Sum 690 896 51 496 39 704 67 176
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TEST FOR LINEALITY AT 1% CRITICAL LEVEL
By formula: Sb 2 = Se 2 /SSX …………………………….(1)
Where Sb = standard error of the gradient of regression line on X and Y – axes
Se = standard error of the tested values, b = gradient, n = total number of tested samples and
SSX = X 2 - ( X) 2 /n …………………………………….(2)
Se 2 = {[ (Y 2 ) - ( X 2 )] - [b( XY - X Y/n)]}/n-2 ………………(3)
b = [n( XY) - X Y]/[n X 2 - ( X 2 )] ……………………………(4)
t = (b - B)/Sb …………………………………………………………………………………(5)
n = 12
X = 690, Y = 896, X 2 = 39704, Y 2 = 67176, XY = 51496
From (4)
b = [ 12(51496) – (690)(896)]/[ 12(39704) – (690) 2 ]
b = - 0.82759
From (2)
SSX = 39704 – (690) 2 /12
SSX = 29
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From (3)
Se 2 = {[67176 – (690) 2 /12] – [ -0.82759((51496) – (690)(896)/12]}/12-2
Se 2 = 2498.285
Sb 2 = (2498.285)/(29)
Sb 2 = 86.14777
Sb = 9.281582
Ho:B = 0, implies hypothesis of no gradient or no linear relation.
H 1 :B < 0, implies hypothesis of linear relation
By t-distribution, the following evaluation can be obtained
From (5)
t = (b-B)/Sb
t = (-0.82759-0)/9.281582
t calculated = -0.089165
From t-distribution statistical table at 1% critical level and 11 degree of freedom;
t 01.0 11 = 2.718
Since, -0.08916 < 2.718, Ho is rejected and H 1 is accepted.
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This means that, even at 1 % critical level of significant there is linear relation between Feed
density –X (i.e. % solids) and percentage passing 75 µm – Y (i.e.% solids).(S. Al-Hassan,2004)
Fig. 2 Regression of Percentage passing 75 µm on Cyclone feed density
Subjecting each of the day’s feed densities and overflow percentage passing 75 µm to statistical
linearity analysis as calculated for day 1, table 8 above, shows a linear relation at even 1%
critical level of significance. Also regression of Percentage passing 75 µm on Cyclone feed
density of day 2,3,4,5,6 and 7 experiments as in fig. 3, give graphs with linear equations; y = -
0.6538x + 115.29, y = -0.7699x + 116.83, y = -0.8793x + 123.38, y = -0.875x + 124.83, y = -
0.7079x + 111.11 and y = -0.9091x + 122.2 respectively.
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5 DISCUSSION
Basically, efficiency is given by the ratio of output to input and can be expressed as a
percentage. Hence from table 1-7, output represents percentage 75 µm (i.e. Y on the statistical
table) and input as feed density (i.e. X on the statistical table). This arrangement is in
conformity with the operational principle of hydrocyclone. Interestingly, using parameters
which are not related to input and output may defeat the aim of estimating efficiency.
Consequently, it is imperative to note that, the feed densities (input) and corresponding
percentage passing 75 µm (output) are resultant products of the prevailing parameters of
cyclone pressure, feed rate, circulating load and fix parameters of 10 inches Vortex finder and 6
inches spigot diameters. As in all calculation or estimation of efficiency, these two resultant
products are used to depict level of effect of the prevailing parameter on performance which
may be adjusted for efficiency improvement.
Therefore, the prevailing parameters of cyclone pressure, feed rate, circulating load and fixed
parameters of 10 inches Vortex finder and 6 inches spigot diameters are not necessarily
needed to appear in the formula for calculating or estimating efficiency when their resultant
input and output parameters are used.
From fig 3 - 9 graphs, all the least square regression analysis equations (Y = a + bx) (S. Al-Hassan,
2004), have negative sense (i.e. Negative gradient). This negative gradient which is the
percentage passing 75 µm (grinding grade) per percentage solids of the cyclone feed density
(input), authenticates the fact that lower feed densities favour higher percentage of -75µm
particle size in the overflow product (output). a = the intercept on Y (percentage of -75 µm) axis
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and b = the gradient (Percentage of -75 µm of overflow per percentage solids of feed density).
The gradient is therefore equal to output divided by input which is efficiency by definition.
Therefore, fig 3-9 graphs had equations with gradients (efficiencies) which occurred under the
cyclone feed densities between 51 % to 60 % solids at pressures of 110 kPa to 120 kPa. This is a
quicker and a more convenient method of estimating efficiency as compared to conventional
method. The high linearity between cyclone feed density and percentage of -75 µm, is a proven
justification and accuracy of this statistical method.
When y = o, the x – intercept, shows the limit of percentage solids at which classification would
be practically impossible. That is at this point of feed density, there will not be enough water or
liquid to enhance differential settling among particles. Therefore classification is zero at this
point. Also when x = 0, the y – intercept depict a point where there is no solid flowing through
the cyclone. The zero feed density corresponds to a point on y – axis where virtually, only water
comes as overflow. Practically, that is 100 % - 75 µm. This means that all overflow discharge
may be only water or solid of size -75 µm.
The least square regression method makes use of all variables under consideration, giving it a
higher potential of low deviation as compared to forming composite samples and subsequently
dividing for size analysis. It also gives better account of the end result than using the average
value. That is all values are taken into consideration to overcome the effect of skewness on the
average value (i.e. mean).
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6 CONCLUSION
Using the conventional method of estimation (i.e. by computing the particle size probability of
appearing in a classified product, example estimation of cyclone d 50 ) has higher potential of
deviation. This is due to errors that may occur in numerous sequence of test works involved in
the method. It does not give direct relations for trouble shooting.
On the other hand, statistical methods of estimating hydrocyclone efficiency provides the
means of optimizing the extent of control of the cyclone feed density to achieve expected
target. This is due to the expression of efficiency as percentage of the cut off size per
percentage solid of cyclone feed density.
Additionally, statistical analysis of hydrocyclone efficiency, has higher accuracy due to fewer
sequential test work method as compared to others. The proven linearity between the
parameters used in the method at even 1 % critical level of significance is an indication of the
effectiveness of the method.
Graphically, regression of percentage passing 75 µm on cyclone feed density can be used for
quick estimation with gradient of the regression line, representing the efficiency of the cyclone
during the time of operation.
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REFERENCE
B. A. Wills (1992), Mineral Processing Technology, Cambonne School of Mines and Cornwall,
England, pp. 381-387
Department of Minerals Engineering and Extractive Metallurgy (1988), The Extraction and
Recovery of Gold, Western Australian School of Mines, Australia, pp. 4.1-4.5
Foulks Lynch (2004), Managing People, EPP Books Services, pp. 75&76
S. Al-Hassan (2004), “Lecture Notes on Statistical Models MSc. Modular Programme”, Western
University College, Tarkwa, pp. 11& 4
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James Obiri-Yeboah is a Metallurgical Superintendent at Gold Fields Ghana
Limited, Tarkwa. He has worked as a Metallurgist at Teberebe Gold Fields from
1997 to1999, AngloGold Ashanti from 2000 to 2005. He holds a PhD in
Management from Swiss Management Center University and MSc degree in
Mineral Engineering from the University of Mines and Technology, Tarkwa. He
is researching into the use of engineering and management (Strategic
Opportunity Management) principles to resolve production problems.
Sampson Arthur is a Unit Manager Technical Service at Gold Fields Ghana Limited,
Tarkwa. He has worked as a metallurgist at Teberebe Goldfields from 1994 to
1999, AngloGold Ashanti from 2000 to 2004. He holds an MSc degree in Mineral
Engineering from the University of Mines and Technology, UMaT. His research
area is Assessing the need for Knelson Concentrator in the CIL plant at Goldfields
Ghana Limited.