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Chapter 3
Screen Analysis and separation
of Particles
Dr. Bilha Eshton
3.1 Analysis of Solid particles
3.1.1 Characterization of solid particles
• Individual solid particles are characterized by their
size, shape and density.
• Particles of homogeneous solids have the same
density as the bulky material.
• Particles obtained by breaking up a composite solid
(e.g metal-bearing ore) have various densities usually
different from the density of the bulk material.
Dr. Bilha Eshton
Why measure particle properties?
1. Better control of product quality (cement, urea,
cosmetics etc.)
In an increasingly competitive global economy, better
control of product quality delivers real economic benefits
such as:
• ability to charge a higher premium for your product;
• reduce customer rejection rates.
Dr. Bilha Eshton
2. Better understanding of products, ingredients
and processes
• improve product performance.
• troubleshoot manufacturing and supply issues
• optimize the efficiency of manufacturing processes
• increase output or improve yield
• stay ahead of the competition
3. Designing of equipment for different
operations
• For example equipment for crushing, grinding,
conveying, separation, storage etc.
Dr. Bilha Eshton
Which particle properties are important to
measure?
From a manufacturing and development perspective,
some of the most important physical properties to
measure are:
• particle size
• particle shape
• surface properties
• mechanical properties
• Microstructure
• Density
Dr. Bilha Eshton
3.1.2 Particle shape
• The shape of individual particles is best expressed in terms of
sphericity (Φs) which is independent of particle size.
• For spherical particle of diameter Dp, Φs=1; for non-spherical
particle, the sphericity is defined by this relation:
Φ𝑠 ≡
6𝑉
𝑝
𝐷𝑝𝑠𝑝
… … … … … … … … … … … … (3.1)
• Where:
Dp = equivalent or nominal diameter of particle
sp = surface area of one particle
Vp = volume of one particle
Dr. Bilha Eshton
• The equivalent diameter is sometimes defined as
the diameter of a sphere of equal volume.
• For fine particles, Dp is usually taken to be the
nominal size based on screen analysis or
microscopic analysis.
• The surface area is found from adsorption
measurements or from the pressure drop in a
bed of particles.
• For many crushed materials, Sphericity is
between 0.6 and 0.8. For particles rounded by
abrasion, their sphericity may be as high as 0.95.
Dr. Bilha Eshton
For many crushed materials, Φs is between 0.6 and 0.8 as
shown in the Table below.
Dr. Bilha Eshton
Table 28.1 in Unit operations of
Chemical Eng. Vol 5
Some materials with their images
Dr. Bilha Eshton
3.1.3 Particle Size
• The most important physical property of particulate
samples is particle size.
• Particle size measurement is routinely carried out across
a wide range of industries and is often a critical
parameter in the manufacturing of many products.
• Particle size has a direct influence on material
properties such as:
– Reactivity or dissolution rate e.g. catalysts, tablets
Dr. Bilha Eshton
– Stability in suspension e.g. sediments, paints
– Efficacy of delivery e.g. asthma inhalers
– Texture and feel e.g. food ingredients
– Appearance e.g. powder coatings and inks
– Flowability and handling e.g. granules
– Viscosity e.g. nasal sprays
– Packing density and porosity e.g. ceramics.
Dr. Bilha Eshton
• In general particle diameters may be specified for any
equi-dimensional particle. However, most particles
used in industries are not equi-dimensional i.e. that
are longer in one direction than in others.
• In order to simplify the measurement process, it is
often convenient to define the particle size using the
concept of equivalent spheres.
• In this case the particle size is defined by the diameter
of an equivalent sphere having the same property as
the actual particle such as volume or mass for
example.
Dr. Bilha Eshton
• The equivalent sphere concept works very well for
regular shaped particles.
• However, it may not always be appropriate for
irregular shaped particles, such as needles or plates,
where the size in at least one dimension can differ
significantly from that of the other dimensions.
• Such particles are often characterized by the second
longest major dimension. For example needle like
particles, Dp would refer to the thickness of the
particle, not their length.
Dr. Bilha Eshton
Some common diameters used in microscope analysis
are statistical diameters such as:
• Martin’s diameter (length of the line which bisects
the particle),
• Feret’s diameter (distance between two tangents on
opposite sides of the particle) and
• shear diameter (particle width obtained using an
image shearing device).
• Some of these diameters are described in the next
slide
Dr. Bilha Eshton
Dr. Bilha Eshton
• If a sieve is used to measure the particle size, an
equivalent sphere diameter will be obtained. This is
the diameter of a sphere passing through the same
sieve aperture.
• If sedimentation technique is used to measure
particle size then, the particle diameter is expressed
as the diameter of a sphere having the same
sedimentation velocity under the same conditions.
• Other examples of the properties of particles
measured and the resulting equivalent sphere
diameters are given in the next slide.
Dr. Bilha Eshton
Dr. Bilha Eshton
UNITS FOR PARTICLE SIZE
Depending on convention, particle sizes are expressed in
different units depending on the size range involved.
• Coarse particles: inches or millimeters,
• very fine particles: micrometers or nanometers.
• Ultrafine particles: surface area per unit mass, i.e.
m2/g
Dr. Bilha Eshton
3.1.4 Mixed particle sizes and size analysis
• In a sample of uniform particles of diameter Dp the total
volume of the particles is:
𝑉
𝑝 =
𝑚
𝜌𝑝
……………………………………………………..3.2
Where: m = total mass of the sample
ρp = density of particles
• The number of particles in a sample is then:
𝑁 =
𝑚
𝜌𝑝𝑉𝑝
……………………………………………………….3.3
• Total surface area of the particles is:
𝐴 = 𝑁𝑠𝑝 =
6𝑚
Φ𝑠𝜌𝑝𝐷𝑝
………………………………….3.4
Dr. Bilha Eshton
Particle Size Analysis
• To analyse the particle size for a mixtures of particles
having various sizes and densities, the mixture is sorted
into fractions, each of constant density and approximately
constant size.
• Each fraction can then be weighed, or the individual
particles in can be counted or measured by any method.
Equations 3.3 and 3.4 can then be applied to each fraction.
• Information from such particle size analysis is tabulated to
show the mass or number fraction in each size increment
as a function of the average particle size (size range).
Dr. Bilha Eshton
• An analysis tabulated based on size increment as a
function of average particle size is called a
differential analysis.
• An analysis which is obtained by adding,
consecutively, the individual increments, starting
with that containing smallest particles is called the
cumulative analysis.
• Both method are shown in a Figure (next slide)
Dr. Bilha Eshton
Differential Analysis
Cumulative Analysis
Dr. Bilha Eshton
Mass Quantities of sample of particles (Differential
Analysis)
Dr. Bilha Eshton
Cumulative mass fraction plot of data from previous
figure.
Dr. Bilha Eshton
3.1.5 Specific Surface Area of Mixture
• If the particle density ρp and sphericity Φs are known, the
surface area of the particles in each fraction may be
calculated from eqn. 3.4 and the results for all fractions
added to give Aw, the specific surface area (i.e. the total
surface area per unit mass of particles).
• If ρp and Φs are constants, Aw is given by:
Dr. Bilha Eshton
• Hence, Aw ……………………………………3.5
Where subscript = individual increments
xi = mass fraction in a given increment
n = number of increments
ഥ
𝐷𝑝𝑖 = Average particle diameter, taken
as arithmetic average of smallest and
largest particle diameters in
increment.
Dr. Bilha Eshton
3.1.6 Average Particle Size
The average particle size for a mixture of particles is defined by
the volume-surface mean diameter ഥ
𝐷𝑠 which is related to the
specific surface area Aw.
It is defined as:
ഥ
𝐷s ≡
6
Φ𝑠𝐴𝑤𝜌𝑝
…………………………………3.6
Substituting Aw (eq. 3.5) gives:
………………………………………3.7
Dr. Bilha Eshton
• If the number of particles in each fraction Ni is known
instead of the mass fraction, ഥ
𝐷𝑠 , is given by:
…………………………………..3.8
• And the arithmetic mean diameter ഥ
𝐷𝑁 is calculated by:
………………………………..3.9
Where:
NT = the number of particles in the entire sample.
Dr. Bilha Eshton
• The mass mean diameter ഥ
𝐷𝑤 is calculated from:
………………………………..3.10
• Dividing the total volume of the sample by the
number of particles in the mixture gives the average
volume of a particle. The diameter of such a particle
is a volume mean diameter calculated from:
………………………………..3.11
Dr. Bilha Eshton
• For samples consisting of uniform particles these
average diameters are all the same.
• For mixtures containing particles of various sizes,
average diameters may differ from one another.
Dr. Bilha Eshton
3.1.7 Number of Particles in a Mixture
• Equation 3.3 is used to calculate the number of particles in
fraction and Nw, the total population in one mass unit of
sample is obtained by summation over all the fractions.
• For a given particle shape, the volume of any particle is
proportional to cube of its diameter.
• i.e. 𝑉
𝑝 = 𝑎𝐷𝑝
3……….……………………………………..3.12
Where a is the volume shape factor.
From equation 3.3 assume a is independent of size, then:
……………………….……….3.13
Dr. Bilha Eshton
3.1.8 Screen (sieve) Analysis and Standard
screen series
• Standard screens are used to measure the size (and
size distribution) of particles in the range between 3
and 0.0015 in. (76 mm and 38μm).
• Testing sieves are made of woven wire screens, the
mesh and dimensions (openings) of which are
carefully standardized.
• The openings are square and each screen is identified
in meshes per inch. e.g. 10 mesh, Dpi = 1/10 = 0.1 in.
Dr. Bilha Eshton
Mesh No. is the numbers
of opening per linear
inch.
• Area of opening in any screen = 2 times the
area of opening in next smaller screen.
• Mesh dimension of any screen = 1.41 times
Mesh dimension of next smaller screen.
Dr. Bilha Eshton
• The actual openings are however smaller than those
corresponding to the mesh number, because of
thickness of wire.
• The common screen series is the Tyler standard screen
series. The area of the openings in any one screen in
this series is exactly twice to that of the openings in
the next smaller screen.
• The ratio of the actual mesh dimension of any screen
to that of the next smaller screen is √2 =1.41.
Dr. Bilha Eshton
• For close sizing, intermediate screen are available, each of
which has a mesh dimension = 1.189 times that of next smaller
standard screen.
• Analysis using standard screen: Screens are arranged serially in
a stack, with the smallest mesh at the bottom and the largest at
the top. Materials are loaded at top and then shacked for a
period of time (e.g. 20 minutes).
• The particles retained of each screen are removed, weighed
and masses of individual screen increments are converted into
mass fraction of total sample.
• Any particle that passed the finest screen are caught in the pan
at the bottom of stack. Results of screen analysis are then
tabulated.
Dr. Bilha Eshton
Table 1. Tyler standard screen series (Appendix 20)
Dr. Bilha Eshton
Dr. Bilha Eshton
Dr. Bilha Eshton
Table 2. Other standard screen series
A typical screen analysis is shown in Table 3 (next slide)
• First column: mesh size,
• second column: width of opening of screen,
• third column: mass fraction of total sample that is retained
on that screen xi (where i is the number starting from the
bottom of the stack),
• fourth column: averaged particle size Dpi (since the particle
on any screen are passed immediately by the screen ahead
of it, the averaged of these two screen are needed to specify
the averaged size in that increment).
• Fifth column: cumulative fraction smaller than Dpi.
Dr. Bilha Eshton
Table 3: Screen Analysis
Dr. Bilha Eshton
Example 1
The screen analysis shown in Table 3 applies to a
sample of crushed quartz. The density of particles is
2650 kg/m3 and the shape factor are a=2 and Φs =
0.571. For material between 4-mesh and 200-mesh in
particle size, calculate:
(a) Aw in square millimeters per gram and Nw in
particles per gram.
(b)ഥ
Dv, ഥ
Ds , ഥ
Dw and Ni for the 150/200- mesh increment.
(c) What fraction of the total number of particles is in
the 150/200- mesh increment?
Dr. Bilha Eshton
3.2 SCREENING
• Screening is a method of separating particles
according to size alone by a semipermeable
membrane (or screening surface).
Dr. Bilha Eshton
• In screening, the solids are dropped on, or through a
screening surface.
• The under size or fines particles pass through the
screen openings; the oversize or tails do not.
• Material passed through a series of screens of
different sizes is separated into sized fractions, i.e.
fractions in which both the maximum and minimum
particle sizes are known.
• The final portions consist of particles of more uniform
size than those of the original mixture.
Dr. Bilha Eshton
The screening surface may consist of:
(i) woven-wire (ii) perforated plastic cloth
Dr. Bilha Eshton
(iii) grizzly bars and wedge wire sections
3.2.1 Material balance over a screen
• Simple material balance can be written over a
screen which is useful in calculating the ratios
of feed, oversize and undersize from the
screen.
• Consider a feed which contains material A and
B to be separated.
• Let F, D and B be the mass flow rates of feed,
overflow and underflow, respectively.
Dr. Bilha Eshton
• and let xF, xD and xB be the mass fractions of
the material A in these three streams.
• The mass fractions of material B in the feed,
overflow and underflow are: 1-xF, 1-xD and 1-xB
respectively.
• Since the total material fed to the screen must
leave it either as underflow (B)or as overflow
(D), then:
Dr. Bilha Eshton
𝐹 = 𝐷 + 𝐵……………………………………3.14
• The material A in the feed must also leave in
these two streams, then
𝐹𝑥𝐹=𝐷𝑥𝐷+𝐵𝑥𝐵…………………………….3.15
• Eliminating B from equations 3.14 and 3.15 gives
𝐷
𝐹
=
𝑥𝐹−𝑥𝐵
𝑥𝐷−𝑥𝐵
…………………………………………3.16
Dr. Bilha Eshton
Eliminating D from equation 3.15 gives:
𝑩
𝑭
=
𝒙𝑫−𝒙𝑭
𝒙𝑫−𝒙𝑩
…………………………………….3.17
Dr. Bilha Eshton
3.2.2 Effectiveness of screens
• The effectiveness of a screen (or screen efficiency) is a
measure of the success of a screen in separating
materials A and B.
• If the screen functioned properly, all material A would
be in the overflow and all material B would be in the
underflow.
Dr. Bilha Eshton
• A common measure of screen effectiveness is the ratio
of oversize material A that is actually in the overflow
to the amount of A entering with the feed.
• Screen effectiveness with respect to material A is
therefore:
𝐸𝐴=
𝐷𝑥𝐷
𝐹𝑥𝐹
………………………………………...3.18
• Where EA is the screen effectiveness based on the
oversize.
Dr. Bilha Eshton
• Similarly an effectiveness based on the undersized
material is given by:
𝐸𝐵=
𝐵(1−𝑥𝐵)
𝐹(1−𝑥𝐹)
…………………………………………..3.19
A combined overall effectiveness can be defined as the
product of the two individuals and if the product is
denoted by E, we get:
……........…………………………….3.20
Dr. Bilha Eshton
• Substituting D/F and B/F from equation 3.16 and
3.17 into equation 3.20 gives
……….………….3.21
Example 2
A quartz mixture having the screen analysis shown in Table 3
(next slide) is screened through a standard 10-mesh screen.
The cumulative screen analysis of overflow and underflow are
given in the Table. Calculate the mass ratios of the overflow
and underflow to feed and the overall effectiveness of the
screen.
Dr. Bilha Eshton
Dr. Bilha Eshton
3.2.3 Capacity of screens
• The capacity of screens is measured by the mass of material
that can be fed per unit time to a unit area of the screen.
• The probability of passage of a particle through a screen
depends on the fraction of the total surface represented by
openings, on the ratio of the diameter of the particle to the
width of an opening in the screen, and on the number of
contacts between the particle and the screen surface.
• For a series of screens of different mesh sizes, the number of
openings per unit screen area is proportional to 1/Dpc
2 where
Dpc = width of screen opening.
Dr. Bilha Eshton
3.3 Screening equipment
• Varieties of screen are available for different
purposes.
• In most screen particles drop through openings by
gravity.
• Some of screening equipment include: Stationary
screens and grizzlies; Gyrating screens; Vibrating
screens; Centrifugal sitter.
Dr. Bilha Eshton
3.3.1 Grizzly Screens
• consist of a set of parallel bars held apart by spacers
at some predetermined opening.
• Bars are frequently made of manganese steel to
reduce wear.
• A grizzly is widely used before a primary crusher in
rock- or ore-crushing plants to remove the fines
before the ore or rock enters the crusher.
• It can be a stationary set of bars or a vibrating screen.
• Types: (i) stationary grizzly (ii) flat grizzlies (iii)
vibrating grizzlies.
Dr. Bilha Eshton
Grizzly Screens
Vibrating Grizzlies
Stationary Grizzlies
Dr. Bilha Eshton
3.3.2 Vibrating Screens
• They are used as standard practice when large
capacity and high efficiency are desired.
• The capacity, especially in the finer sizes, is so much
greater than that of any of the other screens that they
have practically replaced all other types when
efficiency of the screen is an important factor.
• Advantages include accuracy of sizing, increased
capacity per unit area, low maintenance cost per ton
of material handled, and a saving in installation space
and weight.
Dr. Bilha Eshton
• They are divided into two main classes:
(i) mechanically vibrated screens (ii) electrically vibrated screens
Dr. Bilha Eshton
3.3.3 Gyrating Screens
• the machine gyrates in a circular motion at a near level
plane at low angles. The drive is an eccentric gear box
or eccentric weights
Dr. Bilha Eshton
On your own, read:
3.3.4 Revolving screens
3.3.5 Centrifugal sifters
END OF CHAPTER
Dr. Bilha Eshton

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EMCQ-2242- Chapter 3-Screen analysis- Revised.pdf

  • 1. Chapter 3 Screen Analysis and separation of Particles Dr. Bilha Eshton
  • 2. 3.1 Analysis of Solid particles 3.1.1 Characterization of solid particles • Individual solid particles are characterized by their size, shape and density. • Particles of homogeneous solids have the same density as the bulky material. • Particles obtained by breaking up a composite solid (e.g metal-bearing ore) have various densities usually different from the density of the bulk material. Dr. Bilha Eshton
  • 3. Why measure particle properties? 1. Better control of product quality (cement, urea, cosmetics etc.) In an increasingly competitive global economy, better control of product quality delivers real economic benefits such as: • ability to charge a higher premium for your product; • reduce customer rejection rates. Dr. Bilha Eshton
  • 4. 2. Better understanding of products, ingredients and processes • improve product performance. • troubleshoot manufacturing and supply issues • optimize the efficiency of manufacturing processes • increase output or improve yield • stay ahead of the competition 3. Designing of equipment for different operations • For example equipment for crushing, grinding, conveying, separation, storage etc. Dr. Bilha Eshton
  • 5. Which particle properties are important to measure? From a manufacturing and development perspective, some of the most important physical properties to measure are: • particle size • particle shape • surface properties • mechanical properties • Microstructure • Density Dr. Bilha Eshton
  • 6. 3.1.2 Particle shape • The shape of individual particles is best expressed in terms of sphericity (Φs) which is independent of particle size. • For spherical particle of diameter Dp, Φs=1; for non-spherical particle, the sphericity is defined by this relation: Φ𝑠 ≡ 6𝑉 𝑝 𝐷𝑝𝑠𝑝 … … … … … … … … … … … … (3.1) • Where: Dp = equivalent or nominal diameter of particle sp = surface area of one particle Vp = volume of one particle Dr. Bilha Eshton
  • 7. • The equivalent diameter is sometimes defined as the diameter of a sphere of equal volume. • For fine particles, Dp is usually taken to be the nominal size based on screen analysis or microscopic analysis. • The surface area is found from adsorption measurements or from the pressure drop in a bed of particles. • For many crushed materials, Sphericity is between 0.6 and 0.8. For particles rounded by abrasion, their sphericity may be as high as 0.95. Dr. Bilha Eshton
  • 8. For many crushed materials, Φs is between 0.6 and 0.8 as shown in the Table below. Dr. Bilha Eshton Table 28.1 in Unit operations of Chemical Eng. Vol 5
  • 9. Some materials with their images Dr. Bilha Eshton
  • 10. 3.1.3 Particle Size • The most important physical property of particulate samples is particle size. • Particle size measurement is routinely carried out across a wide range of industries and is often a critical parameter in the manufacturing of many products. • Particle size has a direct influence on material properties such as: – Reactivity or dissolution rate e.g. catalysts, tablets Dr. Bilha Eshton
  • 11. – Stability in suspension e.g. sediments, paints – Efficacy of delivery e.g. asthma inhalers – Texture and feel e.g. food ingredients – Appearance e.g. powder coatings and inks – Flowability and handling e.g. granules – Viscosity e.g. nasal sprays – Packing density and porosity e.g. ceramics. Dr. Bilha Eshton
  • 12. • In general particle diameters may be specified for any equi-dimensional particle. However, most particles used in industries are not equi-dimensional i.e. that are longer in one direction than in others. • In order to simplify the measurement process, it is often convenient to define the particle size using the concept of equivalent spheres. • In this case the particle size is defined by the diameter of an equivalent sphere having the same property as the actual particle such as volume or mass for example. Dr. Bilha Eshton
  • 13. • The equivalent sphere concept works very well for regular shaped particles. • However, it may not always be appropriate for irregular shaped particles, such as needles or plates, where the size in at least one dimension can differ significantly from that of the other dimensions. • Such particles are often characterized by the second longest major dimension. For example needle like particles, Dp would refer to the thickness of the particle, not their length. Dr. Bilha Eshton
  • 14. Some common diameters used in microscope analysis are statistical diameters such as: • Martin’s diameter (length of the line which bisects the particle), • Feret’s diameter (distance between two tangents on opposite sides of the particle) and • shear diameter (particle width obtained using an image shearing device). • Some of these diameters are described in the next slide Dr. Bilha Eshton
  • 16. • If a sieve is used to measure the particle size, an equivalent sphere diameter will be obtained. This is the diameter of a sphere passing through the same sieve aperture. • If sedimentation technique is used to measure particle size then, the particle diameter is expressed as the diameter of a sphere having the same sedimentation velocity under the same conditions. • Other examples of the properties of particles measured and the resulting equivalent sphere diameters are given in the next slide. Dr. Bilha Eshton
  • 18. UNITS FOR PARTICLE SIZE Depending on convention, particle sizes are expressed in different units depending on the size range involved. • Coarse particles: inches or millimeters, • very fine particles: micrometers or nanometers. • Ultrafine particles: surface area per unit mass, i.e. m2/g Dr. Bilha Eshton
  • 19. 3.1.4 Mixed particle sizes and size analysis • In a sample of uniform particles of diameter Dp the total volume of the particles is: 𝑉 𝑝 = 𝑚 𝜌𝑝 ……………………………………………………..3.2 Where: m = total mass of the sample ρp = density of particles • The number of particles in a sample is then: 𝑁 = 𝑚 𝜌𝑝𝑉𝑝 ……………………………………………………….3.3 • Total surface area of the particles is: 𝐴 = 𝑁𝑠𝑝 = 6𝑚 Φ𝑠𝜌𝑝𝐷𝑝 ………………………………….3.4 Dr. Bilha Eshton
  • 20. Particle Size Analysis • To analyse the particle size for a mixtures of particles having various sizes and densities, the mixture is sorted into fractions, each of constant density and approximately constant size. • Each fraction can then be weighed, or the individual particles in can be counted or measured by any method. Equations 3.3 and 3.4 can then be applied to each fraction. • Information from such particle size analysis is tabulated to show the mass or number fraction in each size increment as a function of the average particle size (size range). Dr. Bilha Eshton
  • 21. • An analysis tabulated based on size increment as a function of average particle size is called a differential analysis. • An analysis which is obtained by adding, consecutively, the individual increments, starting with that containing smallest particles is called the cumulative analysis. • Both method are shown in a Figure (next slide) Dr. Bilha Eshton
  • 23. Mass Quantities of sample of particles (Differential Analysis) Dr. Bilha Eshton
  • 24. Cumulative mass fraction plot of data from previous figure. Dr. Bilha Eshton
  • 25. 3.1.5 Specific Surface Area of Mixture • If the particle density ρp and sphericity Φs are known, the surface area of the particles in each fraction may be calculated from eqn. 3.4 and the results for all fractions added to give Aw, the specific surface area (i.e. the total surface area per unit mass of particles). • If ρp and Φs are constants, Aw is given by: Dr. Bilha Eshton
  • 26. • Hence, Aw ……………………………………3.5 Where subscript = individual increments xi = mass fraction in a given increment n = number of increments ഥ 𝐷𝑝𝑖 = Average particle diameter, taken as arithmetic average of smallest and largest particle diameters in increment. Dr. Bilha Eshton
  • 27. 3.1.6 Average Particle Size The average particle size for a mixture of particles is defined by the volume-surface mean diameter ഥ 𝐷𝑠 which is related to the specific surface area Aw. It is defined as: ഥ 𝐷s ≡ 6 Φ𝑠𝐴𝑤𝜌𝑝 …………………………………3.6 Substituting Aw (eq. 3.5) gives: ………………………………………3.7 Dr. Bilha Eshton
  • 28. • If the number of particles in each fraction Ni is known instead of the mass fraction, ഥ 𝐷𝑠 , is given by: …………………………………..3.8 • And the arithmetic mean diameter ഥ 𝐷𝑁 is calculated by: ………………………………..3.9 Where: NT = the number of particles in the entire sample. Dr. Bilha Eshton
  • 29. • The mass mean diameter ഥ 𝐷𝑤 is calculated from: ………………………………..3.10 • Dividing the total volume of the sample by the number of particles in the mixture gives the average volume of a particle. The diameter of such a particle is a volume mean diameter calculated from: ………………………………..3.11 Dr. Bilha Eshton
  • 30. • For samples consisting of uniform particles these average diameters are all the same. • For mixtures containing particles of various sizes, average diameters may differ from one another. Dr. Bilha Eshton
  • 31. 3.1.7 Number of Particles in a Mixture • Equation 3.3 is used to calculate the number of particles in fraction and Nw, the total population in one mass unit of sample is obtained by summation over all the fractions. • For a given particle shape, the volume of any particle is proportional to cube of its diameter. • i.e. 𝑉 𝑝 = 𝑎𝐷𝑝 3……….……………………………………..3.12 Where a is the volume shape factor. From equation 3.3 assume a is independent of size, then: ……………………….……….3.13 Dr. Bilha Eshton
  • 32. 3.1.8 Screen (sieve) Analysis and Standard screen series • Standard screens are used to measure the size (and size distribution) of particles in the range between 3 and 0.0015 in. (76 mm and 38μm). • Testing sieves are made of woven wire screens, the mesh and dimensions (openings) of which are carefully standardized. • The openings are square and each screen is identified in meshes per inch. e.g. 10 mesh, Dpi = 1/10 = 0.1 in. Dr. Bilha Eshton
  • 33. Mesh No. is the numbers of opening per linear inch. • Area of opening in any screen = 2 times the area of opening in next smaller screen. • Mesh dimension of any screen = 1.41 times Mesh dimension of next smaller screen. Dr. Bilha Eshton
  • 34. • The actual openings are however smaller than those corresponding to the mesh number, because of thickness of wire. • The common screen series is the Tyler standard screen series. The area of the openings in any one screen in this series is exactly twice to that of the openings in the next smaller screen. • The ratio of the actual mesh dimension of any screen to that of the next smaller screen is √2 =1.41. Dr. Bilha Eshton
  • 35. • For close sizing, intermediate screen are available, each of which has a mesh dimension = 1.189 times that of next smaller standard screen. • Analysis using standard screen: Screens are arranged serially in a stack, with the smallest mesh at the bottom and the largest at the top. Materials are loaded at top and then shacked for a period of time (e.g. 20 minutes). • The particles retained of each screen are removed, weighed and masses of individual screen increments are converted into mass fraction of total sample. • Any particle that passed the finest screen are caught in the pan at the bottom of stack. Results of screen analysis are then tabulated. Dr. Bilha Eshton
  • 36. Table 1. Tyler standard screen series (Appendix 20) Dr. Bilha Eshton
  • 38. Dr. Bilha Eshton Table 2. Other standard screen series
  • 39. A typical screen analysis is shown in Table 3 (next slide) • First column: mesh size, • second column: width of opening of screen, • third column: mass fraction of total sample that is retained on that screen xi (where i is the number starting from the bottom of the stack), • fourth column: averaged particle size Dpi (since the particle on any screen are passed immediately by the screen ahead of it, the averaged of these two screen are needed to specify the averaged size in that increment). • Fifth column: cumulative fraction smaller than Dpi. Dr. Bilha Eshton
  • 40. Table 3: Screen Analysis Dr. Bilha Eshton
  • 41. Example 1 The screen analysis shown in Table 3 applies to a sample of crushed quartz. The density of particles is 2650 kg/m3 and the shape factor are a=2 and Φs = 0.571. For material between 4-mesh and 200-mesh in particle size, calculate: (a) Aw in square millimeters per gram and Nw in particles per gram. (b)ഥ Dv, ഥ Ds , ഥ Dw and Ni for the 150/200- mesh increment. (c) What fraction of the total number of particles is in the 150/200- mesh increment? Dr. Bilha Eshton
  • 42. 3.2 SCREENING • Screening is a method of separating particles according to size alone by a semipermeable membrane (or screening surface). Dr. Bilha Eshton
  • 43. • In screening, the solids are dropped on, or through a screening surface. • The under size or fines particles pass through the screen openings; the oversize or tails do not. • Material passed through a series of screens of different sizes is separated into sized fractions, i.e. fractions in which both the maximum and minimum particle sizes are known. • The final portions consist of particles of more uniform size than those of the original mixture. Dr. Bilha Eshton
  • 44. The screening surface may consist of: (i) woven-wire (ii) perforated plastic cloth Dr. Bilha Eshton (iii) grizzly bars and wedge wire sections
  • 45. 3.2.1 Material balance over a screen • Simple material balance can be written over a screen which is useful in calculating the ratios of feed, oversize and undersize from the screen. • Consider a feed which contains material A and B to be separated. • Let F, D and B be the mass flow rates of feed, overflow and underflow, respectively. Dr. Bilha Eshton
  • 46. • and let xF, xD and xB be the mass fractions of the material A in these three streams. • The mass fractions of material B in the feed, overflow and underflow are: 1-xF, 1-xD and 1-xB respectively. • Since the total material fed to the screen must leave it either as underflow (B)or as overflow (D), then: Dr. Bilha Eshton
  • 47. 𝐹 = 𝐷 + 𝐵……………………………………3.14 • The material A in the feed must also leave in these two streams, then 𝐹𝑥𝐹=𝐷𝑥𝐷+𝐵𝑥𝐵…………………………….3.15 • Eliminating B from equations 3.14 and 3.15 gives 𝐷 𝐹 = 𝑥𝐹−𝑥𝐵 𝑥𝐷−𝑥𝐵 …………………………………………3.16 Dr. Bilha Eshton
  • 48. Eliminating D from equation 3.15 gives: 𝑩 𝑭 = 𝒙𝑫−𝒙𝑭 𝒙𝑫−𝒙𝑩 …………………………………….3.17 Dr. Bilha Eshton
  • 49. 3.2.2 Effectiveness of screens • The effectiveness of a screen (or screen efficiency) is a measure of the success of a screen in separating materials A and B. • If the screen functioned properly, all material A would be in the overflow and all material B would be in the underflow. Dr. Bilha Eshton
  • 50. • A common measure of screen effectiveness is the ratio of oversize material A that is actually in the overflow to the amount of A entering with the feed. • Screen effectiveness with respect to material A is therefore: 𝐸𝐴= 𝐷𝑥𝐷 𝐹𝑥𝐹 ………………………………………...3.18 • Where EA is the screen effectiveness based on the oversize. Dr. Bilha Eshton
  • 51. • Similarly an effectiveness based on the undersized material is given by: 𝐸𝐵= 𝐵(1−𝑥𝐵) 𝐹(1−𝑥𝐹) …………………………………………..3.19 A combined overall effectiveness can be defined as the product of the two individuals and if the product is denoted by E, we get: ……........…………………………….3.20 Dr. Bilha Eshton
  • 52. • Substituting D/F and B/F from equation 3.16 and 3.17 into equation 3.20 gives ……….………….3.21 Example 2 A quartz mixture having the screen analysis shown in Table 3 (next slide) is screened through a standard 10-mesh screen. The cumulative screen analysis of overflow and underflow are given in the Table. Calculate the mass ratios of the overflow and underflow to feed and the overall effectiveness of the screen. Dr. Bilha Eshton
  • 54. 3.2.3 Capacity of screens • The capacity of screens is measured by the mass of material that can be fed per unit time to a unit area of the screen. • The probability of passage of a particle through a screen depends on the fraction of the total surface represented by openings, on the ratio of the diameter of the particle to the width of an opening in the screen, and on the number of contacts between the particle and the screen surface. • For a series of screens of different mesh sizes, the number of openings per unit screen area is proportional to 1/Dpc 2 where Dpc = width of screen opening. Dr. Bilha Eshton
  • 55. 3.3 Screening equipment • Varieties of screen are available for different purposes. • In most screen particles drop through openings by gravity. • Some of screening equipment include: Stationary screens and grizzlies; Gyrating screens; Vibrating screens; Centrifugal sitter. Dr. Bilha Eshton
  • 56. 3.3.1 Grizzly Screens • consist of a set of parallel bars held apart by spacers at some predetermined opening. • Bars are frequently made of manganese steel to reduce wear. • A grizzly is widely used before a primary crusher in rock- or ore-crushing plants to remove the fines before the ore or rock enters the crusher. • It can be a stationary set of bars or a vibrating screen. • Types: (i) stationary grizzly (ii) flat grizzlies (iii) vibrating grizzlies. Dr. Bilha Eshton
  • 58. 3.3.2 Vibrating Screens • They are used as standard practice when large capacity and high efficiency are desired. • The capacity, especially in the finer sizes, is so much greater than that of any of the other screens that they have practically replaced all other types when efficiency of the screen is an important factor. • Advantages include accuracy of sizing, increased capacity per unit area, low maintenance cost per ton of material handled, and a saving in installation space and weight. Dr. Bilha Eshton
  • 59. • They are divided into two main classes: (i) mechanically vibrated screens (ii) electrically vibrated screens Dr. Bilha Eshton
  • 60. 3.3.3 Gyrating Screens • the machine gyrates in a circular motion at a near level plane at low angles. The drive is an eccentric gear box or eccentric weights Dr. Bilha Eshton
  • 61. On your own, read: 3.3.4 Revolving screens 3.3.5 Centrifugal sifters END OF CHAPTER Dr. Bilha Eshton