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Introduction to
Mineral ProcessingDesignand Operation
PREFACE
In nature minerals of interest exist physically and chemically combined with the host rock.
Removal of the unwanted gangue to increase the concentration of mineral in an economically
viable manner is the basis of mineralprocessing operations. This book treats the strategy of
beneficiation as a combination of unit operations. Each unit process and its operation is
therefore treated separately. Integration of these units leading to the development of viable
flow sheets that meets the final objective, is then indicated.
The greatest challenge to a mineral processor is to produce high grade concentrates
consistently at maximum recovery from the ore body. To quantify recovery a reasonable idea
of the initial concentration of mineral in a lode is required. Proper sampling representing the
ore body is therefore essential. The book therefore commences with the techniques of
sampling of ore followed by the designandoperation of unit processes of comminution that
help to release the mineral from the associated rocks. Separation and concentration processes
using techniques involving screening, classification, solid-liquid separations, gravity
separation and flotation then follow. In the book some early methods of operation have been
included and the modern methods highlighted.
The designandoperation of each unit process is a study by
itself.
Over the years,
improvements in the understanding of the complexities of these processes have resulted in
increased efficiency, sustained higher productivity and grades. Mathematical modeling has
helped in this direction and hence its use is emphasized. However, the models at best serve as
guides to most processes operations that invariably involve complex interdependent variables
which are not always easily assessed or manipulated. To solve the dilemma, plants are
increasingly being equipped with instruments and gadgets that respond to changes much
faster than humans can detect. Dynamic mathematical models are the basis of operations of
these gadgets which are usually well developed, sophisticated, electronic equipment. In this
book therefore, the basics of instrumental process control is introduced the details of which
belong to the province of instrument engineers.
This book is written after several years on plant operationand teaching. The book is biased
towards practical aspects of mineral processing. It is expected to be of use to plant
metallurgist, mineral processors, chemical engineers and electronics engineers who are
engaged in the beneficiation of minerals. It is pitched at a level that serves as an introduction
to the subject to graduate students taking a course in mineralprocessingand extractive
metallurgy. For a better understanding of the subject solved examples are cited and typical
problems are set. Most problems may be solved by hand-held calculators. However most
plants are now equipped with reasonable numbers of computers hence solution to problems
are relatively simple with the help of spreadsheets.
The authors are grateful for the help received from numerous friends active in the field of
mineral processing who have discussed the book from time to time. Particular thanks are due
vi
to Dr Lutz Elber and Dr H. Eren who painfully went through the chapter on process control.
Authors are also grateful for permission received from various publishers who own material
that we have used and acknowledged in the text. And lastly and more importantly to our
respective families who have helped in various ways and being patient and co-operative.
A.Gupta and D.S.Yan
Perth, Australia, January 2006
Symbols and Units
A general convention used in this text is to use a subscript to describe the state of the quantity, e.g. S
for solid, L for liquid, A for air, SL or P for slurry or pulp, M for mass and V for volume. A subscript
in brackets generally refers to the stream, e.g. (O) for overflow, (U) for underflow, (F) for feed, (C) for
concentrate and (T) for tailing. There are a number of additions to this convention which are listed
below.
a a
constan t
a amplitud e
m
ap particl e acceleratio n
m/s
2
A
a
constan t
A apertur e micron s
A are a
m
2
Ac cross-sectiona l are a
m
2
Ai abrasio n inde x
Ay assa y
of
particle s
in the i
th
.
size
and
j
th
.
densit y fraction s
A
E
effectiv e are a
m
2
A
EFF
area l efficienc y facto r
Ao ope n are a
%
A
0
E effectiv e ope n are a
%
A
M
assa y
of
minera l
% , g/t, ppm
Ay underflo w are a
m
2
b
a
constan t
b Rosin-Rammle r distributio n paramete r
By breakag e distributio n functio n
c
a
constan t
C
a
constan t
C circulatio n rati o
or
load
C concentration , (mas s solid/volum e
of
slurry ) kg/m
3
C
A
concentratio n
of air
kg/m
3
Cc averag e concentratio n
of
solid s
in the
compressio n zon e kg/m
3
C
D
dra g coefficien t
Ci concentratio n
of
specie s
i
kg/m
3
Co initia l concentratio n (mas s
of
solid/volum e
of
slurry ) kg/m
3
CMA X
maximu m concentratio n (mas s
of
solid/volum e
of
slurry ) kg/m
3
C
t
concentratio n
at
time
t
(mas s
of
solid/volum e
of
slurry ) kg/m
3
C
S
(c) concentratio n
of
solid
(C =
concentrate ,
F =
feed ,
T =
tail
f
=
froth ,
P =
pulp )
Cu,
C
F
concentration s
of the
underflo w
and
feed respectively , kg/m
3
(mas s
of
solid/volum e
of
slurry )
CCRI T
critica l concentratio n kg/m
3
C
F
correctio n facto r
CI confidenc e interva l
CR confidenc e rang e
C
S
(u) solid s concentratio n
in the
underflo w
(O =
overflow, F
=
feed )
%
concentratio n
by
mas s
of
solid s
in the
feed
%
xvi
CvS(F)
cc
cv
Coo
d
d
d
32
dN
dso,
dsoc
d
B
d
F
d
L
dMAX
dMIN
d\iiD
dcutter
dc
d
w
D
D
D*
D
c
D,
Do
Du
e
Ei
E
c
E
Ec
E
B
Eo
Eo
E
P
Eu
E
T
/
/(JB)
As)
/P,/F
fi
F
microns
F
F
F
Fi
concentration by volume of solids in the feed
concentration criterion
coefficient of variation
concentration at infinite time
a constant
particle size, diameter
Sauter mean diameter
nominal diameter
cut or separation size, corrected cut size
ball diameter
63.2%
passing size in the feed
liberation size
largest dimension
smallest dimension
mid-range dimension
cutter opening
cylpeb diameter
wire diameter
discharge mass ratio (liquid/solid)
displacement, distance, diameter
dimensionless parameter
cyclone diameter
inlet diameter
overflow diameter
underflow diameter
a constant
partition coefficient of size i = recovery of size i in the U/F
corrected partition coefficient
energy
corrected partition coefficient
energy of rebound
specific grinding energy
efficiency based on oversize
Ecart probability, probable error of separation
efficiency based on undersize
total energy
a constant
ball wear rate
ball load-power function
suspensoid factor
function relating to the order of kinetics for pulp and froth
mass fraction of size i in the circuit feed
feed size
floats at SG
froth stability factor
feed mass ratio (liquid/solid)
settling factor
%
-
-
kg/m
3
-
m
m
m
microns
cm, m
m
m
m
m
m
m
mm
m
-
m
-
m
m
m
m
-
-
-
kWh
-
Wh
kWh/t
-
-
-
kW
-
kg/h
-
-
-
-
cm,
-
-
-
xvii
Fgo
F
B
FB
Fc
Fc
F
D
Fg
FG
Fos
FR
F
s
Fs
g
G
G,G
bp
G'
AG
h
huh,*
H
H
H
t
H
B
H
B
He
He
HOF
HR
H
s
Hu
I
I
JB
Jc
JG
JR
Jp
k
k
A
,k
A
k
F
, k
s
ki
kc,
k
C5
o
ks,
k
S5
o
K
KDO
KE
80%
passing size of feed
Rowland ball size factor
buoyancy force
Bond mill factor
centrifugal force
drag force
gravitational force
correction factor for extra fineness of grind
correction factor for oversized feed
correction factor for low reduction ratio
mass flow rate
Bond slurry or slump factor
gravitational constant (9.81)
grade (assay)
net grams of undersize per revolution
grinding parameter of circulating load
free energy
parameter =
X/C T
diatances within the conical section of a mill
hindrance factor
height
height at time t
height of rebound pendulum
height of bed
height of ball charge
height of the start of the critical zone in sedimentation
height of the clarification zone (overflow)
height of rest
hindered settling factor
mudline height at the underflow concentration
height after infinite time
impact crushing strength
imperfection
fraction of mill volume occupied by bulk ball charge
fraction of mill volume in cylindrical section occupied by balls
and coarse ore
superficial gas velocity
fraction of mill volume occupied by bulk rock charge
fraction of mill volume filled by the pulp/slurry
constant
rate constant for air removal via froth and tailings respectively
rate constant for fast and slow component respectively
comminution coefficient of fraction coarser that i
th
screen
screening rate constant, crowded condition, normal and half size
screening rate constant, separated condition, normal and half size
constant
material constant
kinetic energy
microns
-
N
-
N
N
N
-
-
-
kg/s,t/h
-
m/s
2
%, g/t, ppm
g/rev
-
J
-
m
-
m, cm
m
m
m
m
m
m
m
-
m
m
kg.m/mm
-
-
-
m/s
-
-
-
-
min"
1
-
t/h/m
2
m
1
-
-
kW
xviii
L
L
A
LAE
LEFF
Lc
LcYL,
LcONE
L
F
LMW ,
LMAX
LT
I_I
LVF
m
m
muo o
m
k
mu(O)
m(r)
m
T
mu(o>
m
i(U)
M
Mi
M
oi
My
M
B
M
B
M
c
Me
M
F
M
F
M
FT
M
F
MMIN
MR
MR
Mr
M
s
M
s
length
aperture size
effective aperture
effective grinding length
length of cyclone
length of cylindrical and cone sections
Nordberg loading factor
minimum and maximum crusher set
crusher throw
length of vortex finder
length from end of vortex finder to apex of a cyclone
moisture (wet mass/dry mass)
mineralogical factor
mass fraction of undersize in the feed
mass fraction of makeup balls of size k
mass fraction of undersize in the oversize
cumulative mass fraction of balls less than size r
mass rate of ball replacement per unit mass of balls
mass fraction of undersize in the undersize
mass of size i in the underflow (F = feed)
mass
mass
mass/mass fraction of i* increment
cumulative mass fraction retained on i* screen at zero time
mass percent of the i* size fraction and
j *
density fraction
mass of block
mass of balls
mill capacity
mass of crushing weight
mass of feed
mass of fluid
mass of floats
Nordberg mill factor
minimum mass of sample required
mass of rock
mass fraction of rock to total charge (rock + water)
cumulative mass fraction of balls of size r in the charge
mass of striking pendulum
mass of solid
m
m
m
m
m
m
-
m
m
m
m
-
kg/m
3
-
-
-
kg/h.t
-
kg
g
kg,t
kg,t
%
kg
kg
t/h
kg
t
kg
kg,t
-
kg,t
kg
-
kg
ke,t
. sec),
SO D
n^
5
of solid feed, concentrate and tailing respectively kg, t
mass of solid in froth
MS K
mass of sinks kg , t
M
S
{p) mas s
of
solid
in the
pulp
kg , t
AM(t) mas s
of top
size particl e
kg , t
Mj mas s
of new
feed
g
Mw mas s
of
water
kg , t
n numbe r
of
revolutions/mi n
min"
1
n numbe r
of
increments , measurement s
xix
n
n(r)
ns
N
N
N
N
L
N'
Oi
P
Pi
P
Pso
p
p
p
p
p
p
PA, PC, PE, PF
PcON
PCYL
PD
PG
P«
PL
PM
PM
PNET
PNL
Pos
PR
Ps
Ps
PE
AP
q
Q
QB
QH
Qo
Qu
QMSOT
QMSCQ
QM(F)
Qv(C),
(T), (F)
QvL(O)
order of rate equation
cumulative number fraction of balls of size less than r
number of sub-lots
number of mill revolutions
number of strokes/min
number
number of presentations per unit length
number of particles/gram
mass fraction of size i in the overflow
binomial probability of being selected in a sample
mass fraction of size i in the new feed
product size
80%
passing size of product
proportion of particles
pressure
Powers roundness factor
Jig power
JKSimFloat ore fioatability parameter
probability
probability of adherence, collision, emergence, froth recovery
power of the conical part of a mill
power for the cylindrical part of a mill
particle distribution factor
proportion of gangue particles
proportion of particles in the i . size and
j*.
density fractions
liberation factor
proportion of mineral particles
mill power
net mill power draw
no load power
period of oscillation
relative mill power
particle shape factor
power at the mill shaft
potential energy
pressure drop
alternate binomial probability = 1
—
p
capacity
makeup ball addition rate
basic feed rate (capacity)
tonnage of oversize material
capacity of the underflow
flowrate of solids by mass in the overflow (U = U/F, F = feed)
mass flow of solid in concentrate
capacity, of feed slurry by mass
flowrate by volume in concentrate, tailing and feed respectively
capacity (flowrate) of liquid by volume in the overflow
-
-
-
-
min'
1
-
nf
1
g"
1
-
-
-
microns
microns
-
Pa
-
W
-
-
kW
kW
-
-
-
-
-
kW
kW
kW
s
-
-
kW
kW
kPa
-
t/h
kg/day
t/h/m
t/h
t/h
t/h
t/h
t/h
m
3
/h
nrVh
(U=underflow, F=feed)
xx
QVOP(U ) flowrat e b y volum e o f entraine d overflo w pul p in th e U/ F
QVOL(U ) flowrat e b y volum e o f entraine d overflo w liqui d in th e U/ F m
3
/h
Qvos(u ) flowrat e b y volum e o f entraine d overflo w solid s i n th e U/ F m
3
/h
Qvs(O ) flowrat e b y volum e o f solid s i n th e overflo w ( U = U/F , F = feed )
Qv(f ) flowrat e b y volum e i n th e frot h
Qv(O ) flowrat e b y volum e o f overflo w (pulp ) ( U = underflow )
Q w bal l wea r rat e
r
0
fractio n o f tes t scree n oversiz e
r bal l radiu s
r rati o o f rat e constant s =
IC A
/(kA+kA )
ri ,
r 2 radiu s withi n th e conica l sectio n o f a mil l
R radiu s
R recover y
R reductio n rati o
Ri,R2,R 3 Dietric h coefficient s
R th e mea n radia l positio n o f th e activ e par t o f th e charg e
R ' fractiona l recovery , wit h respec t t o th e fee d t o th e first cel l
R ' mas s o f tes t scree n oversiz e afte r grindin g
R e radiu s o f con e a t a distanc e L j fro m cylindrica l sectio n
ReA , Re c Reynold s numbe r i n th e ape x an d con e sectio n respectivel y
Re
P
particl e Reynold s numbe r
R F
frot h recover y facto r
Ri radia l distanc e t o th e inne r surfac e o f th e activ e charg e
Ro mas s o f tes t scree n oversiz e befor e grindin g
R P
radia l distanc e o f particl e fro m th e centr e o f a mil l
RR O
optimu m reductio n rati o
R T
radiu s a t th e mil l trunnio n
R v recover y o f fee d volum e t o th e underflo w
Ro o recover y a t infinit e tim e
S spee d
S sink s a t S G
S surfac e are a
S B
surfac e are a o f bal l
S
B
bubbl e surfac e are a flu x
S; breakag e rat e functio n
S F
Nordber g spee d facto r
S spacing , distanc e
S dimensionles s paramete r
SG , SG s specifi c gravity , specifi c gravit y o f soli d
T perio d o f pulsatio n
T N
mas s percen t passin g 1/ N o f th e origina l siz e
t tim e
to detentio n o r residenc e tim e
t
R
effectiv e residenc e tim e
tu tim e fo r al l solid s t o settl e pas t a laye r o f concentratio n C
tio siz e tha t i s on e tent h th e siz e o f origina l particl e
t
A
mea n tim e take n fo r activ e par t o r charg e t o trave l fro m
th e to e t o th e shoulde r
m
3
/h
m
3
/h
m
3
/h
m
3
/h
mm/ h
m
m
m
m
m
m
g
m
m
m/ s
m
2
m
2
s"
1
min"
1
m
h, min , s
h
s
h
m m
s
xxi
U
Up
V
V*
V
c
Vc
VCONE
L(F )
Vo
VR
VB °
VB
1
vs°
Vs
1
var(d)
var(c)
var(pa)
var(t)
var(x)
w
w
W
W
WE
W;
W
s
x
x
x
Xj
X
mean time for free fall from the shoulder to the toe s
mass fraction of size i in the underflow
fraction of void space between balls at rest, filled by rock
fraction of the interstitial voids between the balls and rock charge -
in a SAG mill occupied by slurry of smaller particles
volume fraction of solids in the overflow, (U=underflow, F=feed) -
volume fraction of solids finer than the d
50
in the feed (V
d
5o/V
S
(
F
)) -
volume m
3
dimensionless parameter
volume of the mill charge m
3
volume of the compression zone m
3
volume of conical section of mill m
3
volume of solids finer than the dso in the feed
percent of mill volume occupied by balls %
volume dilution in the feed =
VL(F/VS(F )
volume of liquid in the feed, (U=underflow, F=feed) m
3
volume of mill m
3
volume dilution in the overflow =
VL(O/VS(O >
or
QVL(O/QVS(O )
percent of mill volume occupied by rock %
volume of solids in the feed, (U = underflow, O = overflow) m
terminal velocity m/ s
unknown true value
velocity of block pendulum before impact m/s
velocity of block pendulum after impact m/s
velocity of striking pendulum before impact m/s
velocity of striking pendulum after impact m/s
distribution variance
composition variance
preparation and analysis variance
total variance
variance
thickness of slurry m
fraction of feed water in the underflow
width m
dimensionless parameter
effective width m
Bond Work Index kWh/ t
Bond Work Index, laboratory test kWh/ t
operating work index kWh/ t
corrected operating work index kWh/ t
water split =
QML(O)/QML<F )
deviation from the true assay
geometric mean of size interval micron s
Rosin-Rammler size parameter micron s
Sample mean
i* measurement
deviation from standard unit
xxii
a
a
a, a
0
ttr» «s
«TS
Y
T
YSA >
YSL >
TL A
£
e
A
K
9
-e-
<))
4>c
¥>¥»
Vw
VCRIT
(1
P
Pb
PC
PB
PF
Po
PL
PR
ps
PSL
Pw
PM> pG
U
0
A
CL
CTM
0p
Op
A
CT
S
0
T
e
fractional average mineral content
Lynch efficiency parameter
angle
toe and shoulder angles of the charge
the slurry toe angle
function of charge position and mill speed
volume fraction of active part of the charge to the total charge
surface energy, surface tension, interfacial tension
coefficient of restitution
void fraction
a ball wear parameter
a ball wear parameter, wear distance per unit time
porosity of a ball bed
ratio of experimental critical speed to theoretical critical speed
fraction with the slow rate constant
fraction of critical speed
settling or sedimentation flux
withdrawal flux
critical flux
coefficient of friction
specific gravity (dimensionless) or density
density or SG of balls
bulk density of the total charge, rock + balls + water
bulk density
density of fluid
density of ore
density of liquid
density of rock
density of solid
density of slurry
density of water
density of the mineraland the gangue respectively
standard deviation (where o
2
= var(x))
statistical error in assay
standard deviation of a primary increment
standard deviation on a mass basis
standard deviation of the proportion of particles in a sample
standard deviation of preparation and assay
statistical error during sampling
total error
nominal residence time
angle
-
-
radians
radians
radians
-
-
N/m
-
-
-
-
-
-
-
-
kg/m
2
/s
kg/m
2
/s
kg/m
2
/s
-
kg/m
3
, t/m
3
kg/m
3
,-
t/m
3
kg/m
3
kg/m
3
kg/m
3
kg/m
3
kg/m
3
kg/m
3
kg/m
3
kg/m
3
kg/m
3
, t/m
3
-
-
-
-
-
-
-
-
s
radians,
degree
viscosity
velocity
critical speed
mNm, Pa.s
m/s
rpm
[...]... heterogeneous (liberated) and see Table 1.3 for intermediate material) m = mineralogical factor The mineralogical factor, m, has been defined as: (1-7) where a is the fractional average mineral content and PM and po the specific gravity of the mineraland the gangue respectively The liberation factor, PL, is related to the top size, d A and to the liberation size, dL of the MX mineral in the sample space... fraction and j density fraction as MM and 3 Consider Ay and Py as the assay and the proportion of particles in the i size and j * density fractions For sampling a mixture of two components (mineral and gangue) the proportion of particles in the ij fraction would be; 12 12 ( Eh/-?) } And the assay of the mixture, Ay will be approximately equal to: A IPM(PB-PO)IOOJ = where PM = density of the mineral and. .. proportion of mineral particles proportion of gangue particles number of particles Then the standard deviation of the proportion of mineral particles in the sample, Gp; will be: 9 (1.9) aP = The standard deviation on a mass basis (CTM) can be written in terms of the percent mineral in the whole sample provided the densities (p) are known Thus if pM and PG are the densities of the mineraland gangue,... percent of mineral in the entire sample, consisting of mineraland gangue (the assay), will be: AM = 100 PM p M P (1-10) M P M + P G PG assuming the particles of mineraland gangue have the same shape and size dA The standard deviation of the entire sample is given by a T = —— a p or T _ I (10Q-AM)PM+AMPG I ,„„ / ' AM(100-AM) N Example 1.3 Regular samples were required of the feed to a copper processing. .. important role in defining the difference between random variations and systematic errors and in quantifying both 2 ASSAY Random error Systematic error True value, v SAMPLE Fig 1.1 Representation of a random and systematic error 1.1.1 Mean The most important parameter for a population is its average value In sampling and weighing the arithmetic mean and the weighted mean are most often used Other measures... (American Society for Testing and Materials) Cleaned Top Size in mm 1 Uncleaned Mass in kg Number Mass in kg Number 1 15 15 15 1 3 7 35 35 35 16 50 150 3 7 The overall standard deviation of sampling, sample preparation and assay is a function of the variability of the particulate material, the number and mass of the increments and the random errors associated with sample preparation and assay It can be expressed... particle in kg Experience and theory are embodied in a number of national and international standards on sampling of particulate materials where the sampling regimes are defined in terms of the total number of increments, and the average mass of a primary increment It is generally accepted that a primary increment should contain no less than one-thousand (1,000) particles In the standard on sampling of... infinite degrees of freedom and if the number of replicate results exceeds 8 then a factor of 1.0 is an acceptable approximation 1.2 Mineral particles differing in size - Gy's method Representing large bodies of minerals truly and accurately by a small sample that can be handled in a laboratory is a difficult task The difficulties arise chiefly in ascertaining a proper sample size and in determining the... as: ^ where (1.19) . Introduction to Mineral Processing Design and Operation PREFACE In nature minerals of interest exist physically and chemically combined with the host rock. Removal. material) m = mineralogical factor The mineralogical factor, m, has been defined as: (1-7) where a is the fractional average mineral content and PM and po the specific gravity of the mineral and the. separations, gravity separation and flotation then follow. In the book some early methods of operation have been included and the modern methods highlighted. The design and operation of each unit process