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Mechaniccal Operations slides IIT Kharagpur CHemical Engineering.
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Mechanical Operations (CH 31007)
Unit operations
There are many physical operations that are common to a number
of the individual industries, and may be regarded as unit
operations
Some of these operations involve particulate solids
many of them are aimed at achieving a separation of the
components of a mixture
03-09-2015 CH 31007 2
Mechanical operations
Chemical Engineering unit operations :
Fluid flow processes: fluids transportation, filtration, and solids
fluidization
Heat transfer processes: evaporation, condensation, and heat
exchange
Mass transfer processes: gas absorption, distillation, extraction,
adsorption, and drying
Thermodynamic processes: gas liquefaction, and refrigeration
Mechanical processes: solids transportation, crushing and
pulverization, and screening and sieving
03-09-2015 CH 31007 3
Why mechanical operations!
Foundation of designs of chemical plants, factories, and equipment used
03-09-2015 CH 31007 4
Particulate Solids
Solids are difficult than Fluids !
complex geometrical arrangements
basic problem of defining completely the physical state of the
material
The most important characteristics of an individual
particle
its composition, properties as density and conductivity [provided
the particle is completely uniform]
size and shape
03-09-2015 CH 31007 5
Particulate Solids
Particle size affects properties such as the surface per unit volume
and the rate at which a particle will settle in a fluid
Particle shape ?
Industrial scale: Large quantities of particles are handled and it is
frequently necessary to define the system as a whole
Not the particle size
But the particle size distribution
Mean size
03-09-2015 CH 31007 6
Particulate Solids
To reduce the size of particles
To enlarge the size of particles or form them into
aggregates or sinters
03-09-2015 CH 31007 7
What will I cover?
Crushing and grinding
Mean particle size
Size distribution
Crushers and mills
Screening
Sieve or membrane: Screen of filter
Settling: different rate of sedimentation of particles or drops as they move through gas or
liquid
Special cases: Electrostatic, magnetic etc.
Slurry Transport
Mixing and Segregation
03-09-2015 CH 31007 8
Few things to remember!
Mid-Sem 30 Sep 14 - 22, 2015End-Sem 50 Nov 18, 2015 onwardTA 20 ??
03-09-2015 CH 31007 9
Coulson & Richardsons Chemical Engineering Vol. 2: Particle
Technology and Separation Processes: Richardson, J. F., Harker, J. H., and
Backhurst, J. R.) [Butterworth-Heinemann]
Unit Operations of Chemical Engineering: McCABE, W. L., SMITH, J. C. and
HARRIOTT, P. [McGraw-Hill]
Particle Size ReductionMechanical Operations (CH 31007)
Background
3-Sep-15 CH 31007 2
Materials are rarely found in the size range required
Often necessary either to decrease or to increase the size
While decreasing in size
particle size will have to be progressively reduced in stages
Most appropriate type of machine at each stage depends
size of the feed and of the product
properties as compressive strength, brittleness and stickiness
Background
Sometimes very fine powders are too difficult to handle
Hazardous dust clouds during transportation
Size enlargement processes include
granulation for the preparation of fertilisers
compaction using compressive forces to form the tablets
in pharmaceuticals
3-Sep-15 CH 31007 3
Single particles
The sphere of the same volume as the particle.
The sphere of the same surface area as the particle.
The sphere of the same surface area per unit volume as the particle.
The sphere of the same area as the particle when projected on to a plane
perpendicular to its direction of motion.
The sphere of the same projected area as the particle, as viewed from above, when
lying in its position of maximum stability such as on a microscope slide for example.
The sphere which will just pass through the same size of square aperture as the
particle, such as on a screen for example.
The sphere with the same settling velocity as the particle in a specified fluid.
3-Sep-15 CH 31007 4
Sphericity
3-Sep-15 CH 31007 5
3-Sep-15 CH 31007 6
3-Sep-15 CH 31007 7
Size Reduction of Solids (Comminution)
To increase the surface area
most reactions involving solid particles, the rate of reactions is
directly proportional to the area of contact with a second
phase
drying of porous solids, where reduction in size causes both an
increase in area and a reduction in the distance the
moisture must travel within the particles in order to reach the
surface
3-Sep-15 CH 31007 8
Size Reduction of Solids (Comminution)
Necessary to break a material into very small particles in
order to separate two constituents, especially where
one is dispersed in small isolated pockets
Colour and covering power of a pigment is considerably
affected by the size of the particles
More intimate mixing of solids can be achieved if the
particle size is small
3-Sep-15 CH 31007 9
Mechanism of Size Reduction
3-Sep-15 CH 31007 10
A single lump of material is subjected to a sudden impact/blow
few relatively large particles
a number of fine particles
relatively few particles of intermediate size
Energy in the blow is increased
the larger particles will be of a rather smaller size & more
numerous
the number of fine particles will be appreciably increased, but
their size will not be much altered
Mechanism of Size Reduction
Size of the fine particles: closely connected with the
internal structure of the material
Size of the larger particles: more closely connected
with the process by which the size reduction is effected
Grind limit: After some time there seems to be little
change in particle size but may result in a change
in shape rather than in size
3-Sep-15 CH 31007 11
Effect of progressive grinding on size distribution
3-Sep-15 CH 31007 12
persistent mode
transitory mode
Method of Application of the Force
Impact: particle concussion by a single rigid force
Compression: particle disintegration by two rigid forces
Cutting or Shear: produced by a fluid or by particle
particle interaction
Attrition or Rubbing: arising from particles scraping
against one another or against a rigid surface
3-Sep-15 CH 31007 13
Method of Application of the Force
3-Sep-15 CH 31007 14
Impact: Coarse, medium, or fine particles
Compression: Coarse and relatively few fine particles
Cutting / Shear: definite particle size & shape, no fines
Attrition / Rubbing: very fine particles
Crushing + Attrition
Stress applied between two surfaces (either surfaceparticle or particleparticle) at low velocity, 0.0110 m/s
3-Sep-15 CH 31007 15
Jaw Crusher
3-Sep-15 CH 31007 16
Gyratory Crusher
3-Sep-15 CH 31007 17
Crushing Rolls
3-Sep-15 CH 31007 18
Impact + Attrition
Stress applied at a single solid surface (surfaceparticle or particleparticle) at high velocity, 10200 m/s
3-Sep-15 CH 31007 19
Hammer Mill
3-Sep-15 CH 31007 20
Fluid Energy Mill
3-Sep-15 CH 31007 21
Shear + Attrition
Stress applied by carrier mediumusually in wet grinding to bring about disagglomeration
3-Sep-15 CH 31007 22
Sand Mill
3-Sep-15 CH 31007 23
Colloid Mill
3-Sep-15 CH 31007 24
Ball Mill
3-Sep-15 CH 31007 25
Ball mill
May be used wet or dry although wet grinding facilitates
the removal of the product.
The costs of installation and power are low.
May be used with an inert atmosphere and therefore can
be used for the grinding of explosive materials.
The grinding medium is cheap.
Suitable for materials of all degrees of hardness.
May be used for batch or continuous operation.
3-Sep-15 CH 31007 26
Hammer Mill
3-Sep-15 CH 31007 27
Hardinge conical ball
3-Sep-15 CH 31007 28
Question!
If a ball mill, 1.2 m in diameter, is operating at 0.80 Hz, suggest the
modification in operating condition to achieve its improved
efficiency.
3-Sep-15 CH 31007 29
Ideal Crusher or Grinder !!
Large capacity
Product of single size or size distribution
Requirement of small power input per unit of product
Size reduction is a very inefficient process and only between 0.1 and
2.0 per cent of the energy supplied to the machine appears as
increased surface energy in the solids
3-Sep-15 CH 31007 30
Energy Requirements
3-Sep-15 CH 31007 31
for p = -2
Rittingers law
fc is the crushing strength of the materialThe energy required for size reduction the increase in surface
Energy Requirements
3-Sep-15 CH 31007 32
for p = -1
Kicks law
The energy required for size reduction the reduction ratio
Energy Requirements
Neither of these two laws permits an accurate calculation of the energy
requirements
Rittingers law is applicable mainly to that part of the process where
new surface is being created and holds most accurately for fine
grinding where the increase in surface per unit mass of material is large
Kicks law, more closely relates to the energy required to effect elastic
deformation before fracture occurs
Kicks law is more accurate than Rittingers law for coarse crushing
where the amount of surface produced is considerably less
3-Sep-15 CH 31007 33
Energy Requirements
3-Sep-15 CH 31007 34
for p = -3/2
Work index: the amount of energy required to reduce unit mass of material from an infinite particle size to a size L2 of 100 m
Bonds law
Problem
3-Sep-15 CH 31007 35
3-Sep-15 CH 31007 36
Classification of size reduction equipment
3-Sep-15 CH 31007 37
Nature of the material to be crushed
Hardness The hardness of the material affects the power consumption and the wear on the machine.
With hard and abrasive materials it is necessary to use a low-speed machine and to protect
the bearings from the abrasive dusts that are produced.
Structure Normal granular materials such as coal, ores and rocks can be effectively crushed employing
the normal forces of compression, impact, and so on. With fibrous materials a tearing action
is required
Moisture content It is found that materials do not flow well if they contain between about 5 and 50 per cent
of moisture. In general, grinding can be carried out satisfactorily outside these limits.
3-Sep-15 CH 31007 38
Nature of the material to be crushed
Crushing strength The power required for crushing is almost directly proportional to the
crushing strength of the material.
Friability The friability of the material is its tendency to fracture during normal
handling. In general, a crystalline material will break along well-defined planes and the power required for crushing will increase as the particle size is reduced.
Stickiness A sticky material will tend to clog the grinding equipment and it should
therefore be ground in a plant that can be cleaned easily.
3-Sep-15 CH 31007 39
Nature of the material to be crushed
Soapiness
In general, this is a measure of the coefficient of friction of the
surface of the material. If the coefficient of friction is low, the
crushing may be more difficult.
Explosive materials
must be ground wet or in the presence of an inert atmosphere.
Hazardous materials
Materials yielding dusts that are harmful to the health must be
ground under conditions where the dust is not allowed to escape.
3-Sep-15 CH 31007 40
Types of Crushing Equipment
3-Sep-15 CH 31007 41
Crushers (coarse & fine)
Grinders (intermediate & fine) Ultrafine grinders Cutting machines
Jaw crushers Hammer millsHammer mills with internal classification
Knife cutters
Gyratory crusher Bowl mills, Roller mills Fluid-energy mills Dicers
Crushing rolls Attrition mills Agitated mills Slitters
Tumbling mills(Ball mill, Rod mill, pebble mill, Tube mill)
Methods of operating crushers
Free crushing
feeding the material at a comparatively low rate so that the
product can readily escape
short residence time prevents the production of appreciable
quantities of undersize material
Choke feeding
the machine is kept full of material
discharge of the product is blocked so that the material remains
in the crusher for a longer period
3-Sep-15 CH 31007 42
Methods of operating crushers
Open circuit grinding choke feeding
Closed circuit grinding free crushing
3-Sep-15 CH 31007 43
Recap
3-Sep-15 CH 31007 44
Particle Size Distribution
Single particle size !!
3-Sep-15 CH 31007 46
It is important to use the method of size measurement
which directly gives the particle size which is relevant to
the situation or process of interest.
3-Sep-15 CH 31007 47
3-Sep-15
Why!
Quantitative indication of the mean size and of the spread of sizes
Results of a size analysis can most conveniently be represented by
means of a cumulative mass fraction curve
3-Sep-15 CH 31007 49
Size frequency curve
Size frequency curve
3-Sep-15 CH 31007 50
Cumulative distribution
3-Sep-15
Differential frequency distribution
3-Sep-15
Different distributions
3-Sep-15
Conversion between distributions
Many modern instruments actually measure a number
distribution, which is rarely needed in practice
3-Sep-15
Conversion between distributions
If N is the total number of particles in the population,
the number of particles in the size range
the surface area of these particles
aS is the factor relating the linear dimension of the particle
to its surface area
3-Sep-15
Conversion between distributions
3-Sep-15
S is the total surface area of the population of particles
For a given population of particles, the total number of
particles, N, and the total surface area, S are constant.
Conversion between distributions
assuming particle shape is independent of size,
i.e. aS is constant
3-Sep-15
Conversion between distributions
Similarly, for the distribution by volume
3-Sep-15
Conversion between distributions
3-Sep-15
Describing the mixture by a single number
The mode
Most frequently occurring size in the sample
For the same sample, different modes would be obtained for
distributions by number, surface and volume
The median
Easily read from the cumulative distribution as the 50% size
The size which splits the distribution into two equal parts
Different means including arithmetic, geometric, quadratic,
harmonic, etc.
3-Sep-15
Different means
3-Sep-15
3-Sep-15
3-Sep-15
Mean sizes based on volume
3-Sep-15 CH 31007 64
Considering unit mass of particles consisting of n1 particles of
characteristic dimension d1, constituting a mass fraction x1
mean volume diameter
volume mean diameter
Different means
3-Sep-15
Problem
3-Sep-15
Solution
3-Sep-15
3-Sep-15
3-Sep-15
Problem
3-Sep-15
Solution
3-Sep-15
3-Sep-15
0
3-Sep-15
Quiz!
The size analysis of a powdered material on a mass basis is represented by
a straight line from 0% mass at 1 micron particle size to 100% mass at 101
micron particle size. What is the surface mean diameter of the particles
constituting the system?
3-Sep-15 CH 31007 74
3-Sep-15 CH 31007 75
Recap
Frequency distribution curves
Cumulative curves
Cumulative distribution is the integral of the frequency
distribution
Distributions can be by number, surface, mass or volume
3-Sep-15
Methods of particle size measurement
Sieving (>50 m)
dry sieving using woven wire sieves is a simple, cheap method
gives a mass distribution and a size known as the sieve diameter
sieve series are arranged so that the ratio of aperture sizes on
consecutive sieves is 2, 21/2 or 21/4 according to the closeness of
sizing
horizontal & vertical vibration
lower limit of size!!
3-Sep-15 CH 31007 77
3-Sep-15 CH 31007 78
Screen efficiency
F = feed, D = overflow, B = underflow
xF , xD , xB mass fraction of material A
(1-xF), (1-xD), (1-xB), mass fraction of material C
F = B + D
F xF = D xD + B xB
=
=
Screen efficiency
= ; based on oversize = (1)(1); based on undersize = = (1)(1); overall effectiveness = ()()(1)()2 1
Capacity and effectiveness of screens
The capacity of a screen is measured by the mass of
material that can be fed per unit time to a unit area of
the screen.
Capacity and effectiveness are opposing factors.
To obtain maximum effectiveness, the capacity must be
small, and large capacity is obtainable only at the
expense of a reduction in effectiveness.
3-Sep-15 CH 31007 81
3-Sep-15 CH 31007 82
3-Sep-15 CH 31007 83
3-Sep-15 CH 31007 84
3-Sep-15 CH 31007 85
For coarse crushing, Kicks law may be used
mean diameter of feed = 45 mm, mean diameter of product = 4 mm,
energy consumption = 13.0 kJ/kg, compressive strength = 22.5 N/m2
mean diameter of feed = 42.5 mm, mean diameter of product = 0.50 mm
compressive strength = 45 MN/m2
Methods of particle size measurement
Microscopic analysis (1100 m)
measurement of the projected area of the particle and also
enables an assessment to be made of its 2-D shape
3-Sep-15 CH 31007 86
Methods of particle size measurement
Sedimentation and elutriation methods (>1 m)
the rate of sedimentation of a sample of particles in a liquid
The suspension is dilute and so the particles are assumed to fall
at their single particle terminal velocity in the liquid (usually
water)
Stokes law is assumed to apply
the method using water is suitable only for particles typically less
than 50 mm in diameter
3-Sep-15 CH 31007 87
3-Sep-15 CH 31007 88
terminal falling velocity of a particle in a fluid increases with size
Assumptions
The suspension is sufficiently dilute for the particles to
settle as individuals (i.e. not hindered settling)
Motion of the particles in the liquid obeys Stokes law
(true for particles typically smaller than 50 mm)
Particles are assumed to accelerate rapidly to their
terminal free fall velocity UT so that the time for
acceleration is negligible
3-Sep-15 CH 31007 89
Sedimentation
3-Sep-15 CH 31007 90
Particles are assumed to accelerate rapidly to their terminal free fall velocity
UT so that the time for acceleration is negligible
3-Sep-15 CH 31007 91
Ergun Equation
3-Sep-15 CH 31007 92
Permeametry
This is a method of size analysis based on fluid flow
through a packed bed
The pressure gradient across a packed bed of known
voidage is measured as a function of flow rate
The diameter we calculate from the CarmanKozeny
equation is the arithmetic mean of the surface
distribution
3-Sep-15 CH 31007 93
Electrozone Sensing
Particles are held in suspension in a dilute electrolyte which is drawn
through a tiny orifice with a voltage applied across it
As particles flow through the orifice a voltage pulse is recorded
The amplitude of the pulse can be related to the volume of the particle
passing the orifice
Thus, by electronically counting and classifying the pulses according to
amplitude this technique can give a number distribution of the
equivalent volume sphere diameter
The lower size limit is dictated by the smallest practical orifice and the
upper limit is governed by the need to maintain particles in suspension
3-Sep-15 CH 31007 94
3-Sep-15 CH 31007 95
Although liquids more viscous than water may be used to reduce
sedimentation, the practical range of size for this method is 0.31000 mm
SAMPLING
In practice, the size distribution of many tonnes of powder are often
assumed from an analysis performed on just a few grams or
milligrams of sample
The importance of that sample being representative of the bulk
powder cannot be overstated
The powder should be in motion when sampled
The whole of the moving stream should be taken for many short
time increments
3-Sep-15 CH 31007 96
Methods of particle size measurement
Microscopic analysis (1100 m)
measurement of the projected area of the particle and also
enables an assessment to be made of its 2-D shape
3-Sep-15 CH 31007 2
Methods of particle size measurement
Sedimentation and elutriation methods (>1 m)
the rate of sedimentation of a sample of particles in a liquid
The suspension is dilute and so the particles are assumed to fall
at their single particle terminal velocity in the liquid (usually
water)
Stokes law is assumed to apply
the method using water is suitable only for particles typically less
than 50 mm in diameter
3-Sep-15 CH 31007 3
3-Sep-15 CH 31007 4
terminal falling velocity of a particle in a fluid increases with size
Assumptions
The suspension is sufficiently dilute for the particles to
settle as individuals (i.e. not hindered settling)
Motion of the particles in the liquid obeys Stokes law
(true for particles typically smaller than 50 mm)
Particles are assumed to accelerate rapidly to their
terminal free fall velocity UT so that the time for
acceleration is negligible
3-Sep-15 CH 31007 5
Sedimentation
3-Sep-15 CH 31007 6
Particles are assumed to accelerate rapidly to their terminal free fall velocity
UT so that the time for acceleration is negligible
3-Sep-15 CH 31007 7
Ergun Equation
3-Sep-15 CH 31007 8
Permeametry
This is a method of size analysis based on fluid flow
through a packed bed
The pressure gradient across a packed bed of known
voidage is measured as a function of flow rate
The diameter we calculate from the CarmanKozeny
equation is the arithmetic mean of the surface
distribution
3-Sep-15 CH 31007 9
Electrozone Sensing
3-Sep-15 CH 31007 10
Although liquids more viscous than water may be used to reduce
sedimentation, the practical range of size for this method is 0.31000 mm
Electrozone Sensing
Particles are held in suspension in a dilute electrolyte which is drawn
through a tiny orifice with a voltage applied across it
As particles flow through the orifice a voltage pulse is recorded
The amplitude of the pulse can be related to the volume of the particle
passing the orifice
Thus, by electronically counting and classifying the pulses according to
amplitude this technique can give a number distribution of the
equivalent volume sphere diameter
The lower size limit is dictated by the smallest practical orifice and the
upper limit is governed by the need to maintain particles in suspension
3-Sep-15 CH 31007 11
SAMPLING
In practice, the size distribution of many tonnes of powder are often
assumed from an analysis performed on just a few grams or
milligrams of sample
The importance of that sample being representative of the bulk
powder cannot be overstated
The powder should be in motion when sampled
The whole of the moving stream should be taken for many short
time increments
3-Sep-15 CH 31007 12
Particle in a Fluid
To develop an understanding of the forces resisting the
motion of a single particle
To provide methods for the estimation of the steady
velocity of the particle relative to the fluid
3-Sep-15
Motion of Solid Particles in a Fluid
The drag force resisting very slow steady relative motion
(creeping motion) between a rigid sphere and a fluid of
infinite extent
where U is the relative velocity, x is the sphere dia.
Stokes law
3-Sep-15
Stokes law
Stokes law is found to hold for single particle Reynolds
number,
almost exactly for Rep 0.1
within 9% for Rep 0.3
3-Sep-15
Drag Coefficient
3-Sep-15
3-Sep-15
Particles falling under gravity through a fluid
3-Sep-15
A particle falling from rest in a fluid will initially experience a high
acceleration as the shear stress drag, which increases with relative
velocity, will be small.
As the particle accelerates the drag force increases, causing the
acceleration to reduce.
Eventually a force balance is achieved when the acceleration is zero and
a maximum or terminal relative velocity is reached. This is known as the
single particle terminal velocity.
Particle terminal velocity
3-Sep-15
where UT is the single particle terminal velocity
Particle terminal velocity
3-Sep-15
in the Stokes law region
terminal velocity is proportional to the square of the particle diameter
Particle terminal velocity
In the Newtons law region
terminal velocity is independent of the fluid viscosity and
proportional to the square root of the particle diameter
3-Sep-15
Particle terminal velocity
In the intermediate region no explicit expression
Generally, when calculating the terminal velocity for a
given particle or the particle diameter for a given
velocity, it is not known which region of operation is
relevant.
3-Sep-15
For a given particle size
3-Sep-15
Archimedes number
produce a straight line of slope 2 if plotted on the
logarithmic coordinates (log CD versus log Rep) of the
standard drag curve. The intersection of this straight line with
the drag curve gives the value of Rep.
For a given UT
3-Sep-15
Non-Spherical Particles
3-Sep-15
Shape affects drag coefficient far more in the intermediate
and Newtons law regions than in the Stokes law region.
In the Stokes law region particles fall with their longest surface
nearly parallel to the direction of motion, whereas, in the
Newtons law region particles present their maximum area to the
oncoming fluid.
3-Sep-15
Sand particles falling from rest in air
(particle density, 2600 kg/m3)
3-Sep-15 CH 31007 27
Effect of boundaries on terminal velocity
When a particle is falling through a fluid in the presence
of a solid boundary the terminal velocity reached by the
particle is less than that for an infinite fluid.
In practice, this is really only relevant to the falling
sphere method of measuring liquid viscosity, which is
restricted to the Stokes region.
3-Sep-15
Effect of boundaries on terminal velocity
In the case of a particle falling along the axis of a
vertical pipe this is described by a wall factor,
the ratio of the velocity in the pipe, UD to the velocity in an
infinite fluid, Ua.
3-Sep-15
A sphere of diameter 10 mm and density 7700 kg/m3 falls under gravity at terminal
conditions through a liquid of density 900 kg/m3 in a tube of diameter 12 mm. The
measured terminal velocity of the particle is 1.6 mm/s. Calculate the viscosity of the
fluid. Verify that Stokes law applies.
3-Sep-15 CH 31007 30
3-Sep-15 CH 31007 31
3-Sep-15 CH 31007 32
3-Sep-15 CH 31007 33
3-Sep-15 CH 31007 34
3-Sep-15 CH 31007 35
Separation
Separation can be divided into 2 classes:
Diffusional operations: transfer of material between phases
Mechanical separation: based on physical differences, e.g. size,
shape, density
Mechanical separation are applied to heterogeneous
mixtures, NOT to homogeneous mixtures
3-Sep-15
Mechanical Separation
Separation of solids from gases
liquid drops from gases
solids from solids
solids from liquids
Mechanical separation can be achieved by: Sieve or membrane: Screen of filter
Settling: different rate of sedimentation of particles or drops as they move through gas or liquid
Special cases: Electrostatic, magnetic etc.
3-Sep-15
Screening
Separating particles due to size ONLY
Single screen gives unsized fractions
Series of screens provides sized fractions
Commonly applied for large scale for the separation
Generally applicable for particles of a size as small as
about 50 m
3-Sep-15
Screening
For very fine materials
difficulty of producing accurately woven fine gauze of sufficient
strength
screens become clogged
other methods of separation are usually more economical
Woven wire cloth is generally used for fine sizes and
perforated plates for the larger meshes
3-Sep-15
Screening
Commonly done in dry mode, occasionally in wet mode
With coarse solids the screen surface may be
continuously washed by means of a flowing stream of
water
to keep the particles apart
to remove the finer particles from the surface of larger particles
to keep the screen free of adhering materials
3-Sep-15
Screening
Fine screens are normally operated wet, with the solids
fed continuously as a suspension
Concentrated suspensions have high effective viscosities
and frequently exhibit shear-thinning non-Newtonian
characteristics
By maintaining a high cross-flow velocity over the surface of the
screen, or by rapid vibration, the apparent viscosity of the
suspension may be reduced and the screening rate substantially
increased.
3-Sep-15
Multiphase systems
3-Sep-15
Dissolved or dispersed phase
Continuous medium
Solution Colloid Coarse dispersion
Gas GasGas mixture: air (oxygen and other gases in nitrogen)
None None
Liquid Gas NoneAerosols of liquid particles: fog, mist, vapor, hair sprays
Aerosol
Solid Gas NoneAerosols of solid particles: smoke, cloud, air particulates
Solid aerosol: dust
Gas Liquid Solution: oxygen in water Liquid foam: whipped cream, shaving cream Foam
Liquid Liquid Solution: alcoholic beverages Emulsion Emulsion: milk, mayonnaise, hand cream
Solid Liquid Solution: sugar in water Liquid sol: pigmented ink, bloodSuspension: mud (soil, clay or silt particles are suspended in water)
Gas Solid Solution: hydrogen in metals Solid foam: aerogel Foam: dry sponge
Liquid Solid Solution: amalgam Gel: agar, gelatin, silica gel, opal Wet sponge
Solid Solid Solution: alloys Solid sol: cranberry glass Gravel, granite
Source: Wikipedia
Non-Newtonian fluid
3-Sep-15
Non-Newtonian fluid
3-Sep-15
Time-dependent viscosity
RheopecticApparent viscosity increases with duration of stress
Printer ink
ThixotropicApparent viscosity decreases with duration of stress
Yogurt, aqueous iron oxide gels, gelatin gels, some clays, some drilling muds, many paints, colloidal suspensions
Time-independent viscosity
Shear thickening(dilatant)
Apparent viscosity increases with increased stress
Suspensions of corn starch in water, sand in water
Shear thinning(pseudoplastic)
Apparent viscosity decreases with increased stress
Nail polish, whipped cream, ketchup, molasses, syrups, paper pulp in water, latex paint, blood, some silicone oils, some silicone coatings
Generalized Newtonian fluids
Viscosity is constantStress depends on normal and shear strain rates and also the pressure applied on it
Custard, Water
Screening Equipment
In most cases, the particles drop through the openings
by gravity
Coarse particles drop through easily, but with fine
particles, screen must be agitated
Agitation can be done by
shaking
vibrating
mechanically or electrically
3-Sep-15
Stationary screen & Grizzly
Made of longitudinal bars up to 3 m long, fixed in a
rectangular framework
Space between bars is 2 8 in.
Usually inclined at an angle to the horizontal
Greater the angle, the greater is the throughput BUT the
screening efficiency is reduced
Effective for very coarse free-flowing solids containing
few fine particles
3-Sep-15
Grizzlies
3-Sep-15 Source: Google Image
Electromagnetic screen
3-Sep-15The screen itself is vibrated
Mechanical screen
3-Sep-15The whole assembly is vibrated
Mechanical screen
As very rapid accelerations and retardations are produced, the
power consumption and the wear on the bearings are high
Generally mounted in a multi-deck fashion with the coarsest
screen on top, either horizontally or inclined at angles up to
45
With the horizontal machine, the vibratory motion fulfils the
additional function of moving the particles across the screen
3-Sep-15
Mechanical screen
The screen area which is required for a given operation
cannot be predicted without testing the material under
similar conditions on a small plant
In particular, the tendency of the material to clog the
screening surface can only be determined experimentally
3-Sep-15
Trommel
3-Sep-15
A very large mechanically operated screen
Electrostatic separator
3-Sep-15
3-Sep-15
Cyclone separator
1. IntroductionMechanical Operations (CH 31007)Unit operationsMechanical operationsWhy mechanical operations!Particulate SolidsParticulate SolidsParticulate SolidsWhat will I cover?Few things to remember!
2. Particle Size Reduction and EnlargementParticle Size ReductionMechanical Operations (CH 31007)BackgroundBackgroundSingle particlesSphericitySlide Number 6Slide Number 7Size Reduction of Solids (Comminution)Size Reduction of Solids (Comminution)Mechanism of Size ReductionMechanism of Size ReductionEffect of progressive grinding on size distributionMethod of Application of the ForceMethod of Application of the ForceCrushing + AttritionJaw CrusherGyratory CrusherCrushing RollsImpact + AttritionHammer MillFluid Energy MillShear + AttritionSand MillColloid MillBall MillBall millHammer MillHardinge conical ballQuestion!Ideal Crusher or Grinder !!Energy RequirementsEnergy RequirementsEnergy RequirementsEnergy RequirementsProblemSlide Number 36Classification of size reduction equipmentNature of the material to be crushedNature of the material to be crushedNature of the material to be crushedTypes of Crushing EquipmentMethods of operating crushersMethods of operating crushersRecapParticle Size DistributionSingle particle size !!Slide Number 47Slide Number 48Why!Size frequency curveCumulative distributionDifferential frequency distributionDifferent distributionsConversion between distributionsConversion between distributionsConversion between distributionsConversion between distributionsConversion between distributionsConversion between distributionsDescribing the mixture by a single numberDifferent meansSlide Number 62Slide Number 63Mean sizes based on volumeDifferent meansProblemSolutionSlide Number 68Slide Number 69ProblemSolutionSlide Number 72Slide Number 73Quiz!Slide Number 75RecapMethods of particle size measurementSlide Number 78Screen efficiencyScreen efficiencyCapacity and effectiveness of screensSlide Number 82Slide Number 83Slide Number 84Slide Number 85Methods of particle size measurementMethods of particle size measurementSlide Number 88AssumptionsSedimentationSlide Number 91Ergun EquationPermeametryElectrozone SensingSlide Number 95SAMPLING
3. Particle in fluidSlide Number 1Methods of particle size measurementMethods of particle size measurementSlide Number 4AssumptionsSedimentationSlide Number 7Ergun EquationPermeametryElectrozone SensingElectrozone SensingSAMPLINGParticle in a FluidMotion of Solid Particles in a FluidStokes lawDrag CoefficientSlide Number 17Particles falling under gravity through a fluidParticle terminal velocityParticle terminal velocityParticle terminal velocityParticle terminal velocityFor a given particle sizeFor a given UTNon-Spherical ParticlesSlide Number 26Sand particles falling from rest in air (particle density, 2600 kg/m3)Effect of boundaries on terminal velocityEffect of boundaries on terminal velocitySlide Number 30Slide Number 31Slide Number 32Slide Number 33Slide Number 34Slide Number 35SeparationMechanical SeparationScreeningScreeningScreeningScreeningMultiphase systemsNon-Newtonian fluidNon-Newtonian fluidScreening EquipmentStationary screen & GrizzlyGrizzliesElectromagnetic screenMechanical screenMechanical screenMechanical screenTrommelElectrostatic separatorSlide Number 54