episode 38 : bin and hopper design
TRANSCRIPT
SAJJAD KHUDHUR ABBASCeo , Founder & Head of SHacademyChemical Engineering , Al-Muthanna University, IraqOil & Gas Safety and Health Professional – OSHACADEMYTrainer of Trainers (TOT) - Canadian Center of Human Development
Episode 38 : Bin and Hopper Design
Introduction
< 1960s storage bins were designed by guessing Then in 1960s A.W. Jenike changed all.- He
developed theory, methods to apply, inc. the eqns. And measurement of necessary particles properties.
WHY HOPPER?
For protection and storage of powdered materials It must be designed so that they are easy to load and
more importantly easy to unload
The Four Big Questions
What is the appropriate flow mode? What is the hopper angle? How large is the outlet for reliable flow? What type of discharger is required and what is the
discharge rate?
Hopper Flow Modes
Mass Flow - all the material in the hopper is in motion, but not necessarily at the same velocity
Funnel Flow - centrally moving core, dead or non-moving annular region
Expanded Flow - mass flow cone with funnel flow above it
Mass Flow
Typically need 0.75 D to 1D to
enforce mass flow
D
Material in motion
along the walls
Does not imply plug flow with equal velocity
Funnel Flow
“Dead” or non-flowing region
Act
ive
Flow
C
hann
el
Expanded Flow
Funnel Flow upper section
Mass Flow bottom section
Problems with Hoppers
Ratholing/Piping
Ratholing/Piping
Stable Annular Region
Voi
d
Problems with Hoppers
Ratholing/Piping Funnel Flow
Funnel Flow-Segregation
-Inadequate Emptying
-Structural Issues
Coa
rse
Coa
rse
Fine
Problems with Hoppers
Ratholing/Piping Funnel Flow Arching/Doming
Arching/Doming
Cohesive Arch preventing material from exiting hopper
Problems with Hoppers
Ratholing/Piping Funnel Flow Arching/Doming Insufficient Flow
Insufficient Flow- Outlet size too small
- Material not sufficiently permeable to permit dilation in conical section -> “plop-plop” flow
Material needs to dilate here
Material under compression in
the cylinder section
Problems with Hoppers
Ratholing/Piping Funnel Flow Arching/Doming Insufficient Flow Flushing
Flushing
Uncontrolled flow from a hopper due to powder being in an aerated state- occurs only in fine powders (rough rule of thumb - Geldart group A and smaller)- causes --> improper use of aeration devices, collapse of a rathole
Problems with Hoppers
Ratholing/Piping Funnel Flow Arching/Doming Insufficient Flow Flushing Inadequate Emptying
Inadequate emptyingUsually occurs in funnel flow silos where the cone angle is insufficient to allow self draining of the bulk solid.
Remaining bulk solid
Problems with Hoppers
Ratholing/Piping Funnel Flow Arching/Doming Insufficient Flow Flushing Inadequate Emptying Mechanical Arching
Mechanical Arching
Akin to a “traffic jam” at the outlet of bin - too many large particle competing for the small outlet
6 x dp,large is the minimum outlet size to prevent mechanical arching, 8-12 x is preferred
Problems with Hoppers
Ratholing/Piping Funnel Flow Arching/Doming Insufficient Flow Flushing Inadequate Emptying Mechanical Arching Time Consolidation - Caking
Time Consolidation - Caking
Many powders will tend to cake as a function of time, humidity, pressure, temperature
Particularly a problem for funnel flow silos which are infrequently emptied completely
Segregation
Mechanisms- Momentum or velocity- Fluidization- Trajectory- Air current- Fines
What the chances for mass flow?
Cone Angle Cumulative % of from horizontal hoppers with mass flow
45 060 2570 5075 70
*data from Ter Borg at Bayer
Mass Flow (+/-)
+ flow is more consistent+ reduces effects of radial segregation+ stress field is more predictable+ full bin capacity is utilized+ first in/first out- wall wear is higher (esp. for abrasives)- higher stresses on walls- more height is required
Funnel flow (+/-)
+ less height required- ratholing- a problem for segregating solids- first in/last out- time consolidation effects can be severe- silo collapse- flooding- reduction of effective storage capacity
How is a hopper designed?
Measure- powder cohesion/interparticle friction- wall friction- compressibility/permeability
Calculate- outlet size- hopper angle for mass flow- discharge rates
What about angle of repose?
Pile of bulk solids
Angle of Repose
Angle of repose is not an adequate indicator of bin design parameters
“… In fact, it (the angle of repose) is only useful in the determination of the contour of a pile, and its popularity among engineers and investigators is due not to its usefulness but to the ease with which it is measured.” - Andrew W. Jenike
Do not use angle of repose to design the angle on a hopper!
Bulk Solids Testing
Wall Friction Testing Powder Shear Testing - measures both powder
internal friction and cohesion Compressibility Permeability
Sources of Cohesion (Binding Mechanisms)
Solids Bridges-Mineral bridges-Chemical reaction-Partial melting-Binder hardening-Crystallization-Sublimation
Interlocking forces
Attraction Forces-van der Waal’s-Electrostatics-Magnetic
Interfacial forces-Liquid bridges-Capillary forces
Testing Considerations
Must consider the following variables- time- temperature- humidity- other process conditions
Wall Friction TestingWall friction test is simply Physics 101 - difference for bulk solids is that the friction coefficient, , is not constant.
P 101
N
FF = N
Wall Friction TestingJenike Shear Tester
Wall Test Sample
Ring
CoverW x A
S x A
Bracket
Bulk Solid
Wall Friction Testing Results
Wall Yield Locus, constant wall friction
’
Normal stress, W
all s
hear
stre
ss,
Wall Yield Locus (WYL), variable wall friction
Powder Technologists usually express as the “angle of wall friction”, ’
’ = arctan
Jenike Shear Tester
Ring
CoverW x A
S x A
Bracket
Bulk SolidBulk Solid
Shear plane
Other Shear Testers
Peschl shear tester Biaxial shear tester Uniaxial compaction cell Annular (ring) shear testers
Ring Shear Testers
W x ABottom cell rotates slowly
Arm connected to load cells, S x A
Bulk solid
Shear test data analysis
C fc 1
Stresses in Hoppers/Silos
Cylindrical section - Janssen equation Conical section - radial stress field
Stresses = Pressures
Stresses in a cylinder
h
dh
Pv A
D
(Pv + dPv) A
A g dh
D d
h
Consider the equilibrium of forces on a differential element, dh, in a straight-sided silo
Pv A = vertical pressure acting from above
A g dh = weight of material in element
(Pv + dPv) A = support of material from below
D dh = support from solid friction on the wall
(Pv + dPv) A + D dh = Pv A + A g dh
Stresses in a cylinder (cont’d)Two key substitutions
= Pw (friction equation)
Janssen’s key assumption: Pw = K Pv This is not strictly true but is good enough from an engineering view.
Substituting and rearranging,
A dPv = A g dh - K Pv D dh
Substituting A = (/4) D2 and integrating between h=0, Pv = 0 and h=H and Pv = Pv
Pv = ( g D/ 4 K) (1 - exp(-4H K/D))
This is the Janssen equation.
Stresses in a cylinder (cont’d)
hydrostatic
Bulk solids
Notice that the asymptotic pressure depends only on D, not on H, hence this is why silos are tall and skinny, rather than short and squat.
Stresses - Converging Section
r
Over 40 years ago, the pioneer in bulk solids flow, Andrew W. Jenike, postulated that the magnitude of the stress in the converging section of a hopper was proportional to the distance of the element from the hopper apex.
= ( r, )This is the radial stress field assumption.
Silo Stresses - Overall
hydrostatic
Bulk solidNotice that there is essentially no stress at the outlet. This is good for discharge devices!
Janssen Equation - ExampleA large welded steel silo 12 ft in diameter and 60 feet high is to be built. The silo has a central discharge on a flat bottom. Estimate the pressure of the wall at the bottom of the silo if the silo is filled with a) plastic pellets, and b) water. The plastic pellets have the following characteristics:
= 35 lb/cu ft ’ = 20º
The Janssen equation is
Pv = ( g D/ 4 K) (1 - exp(-4H K/D))
In this case: D = 12 ft = tan ’ = tan 20º = 0.364
H = 60 ft g = 32.2 ft/sec2
= 35 lb/cu ft
Janssen Equation - Example
K, the Janssen coefficient, is assumed to be 0.4. It can vary according to the material but it is not often measured.
Substituting we get Pv = 21,958 lbm/ft - sec2.
If we divide by gc, we get Pv = 681.9 lbf/ft2 or 681.9 psf
Remember that Pw = K Pv,, so Pw = 272.8 psf.
For water, P = g H and this results in P = 3744 psf, a factor of 14 greater!
Types of BinsConical Pyramidal
Watch for in-flowing valleys in these bins!
Types of BinsWedge/Plane Flow
B
L
L>3B
Chisel
A thought experiment1 c
The Flow Function
1
c
Flow function
Time flow function
Determination of Outlet Size
1
c
Flow function
Time flow function
Flow factor
c,i
c,t
Determination of Outlet Size
B = c,i H()/
H() is a constant which is a function of hopper angle
H() Function
Cone angle from vertical10 20 30 40 50 60
1
2
3
H(
)
Rectangular outlets (L > 3B)
Square
Circular
Example: Calculation of a Hopper Geometry for Mass Flow
An organic solid powder has a bulk density of 22 lb/cu ft. Jenike shear testing has determined the following characteristics given below. The hopper to be designed is conical.
Wall friction angle (against SS plate) = ’ = 25º
Bulk density = = 22 lb/cu ft
Angle of internal friction = = 50º
Flow function c = 0.3 1 + 4.3
Using the design chart for conical hoppers, at ’ = 25º
c = 17º with 3º safety factor
& ff = 1.27
Example: Calculation of a Hopper Geometry for Mass Flow
ff = /a or a = (1/ff)
Condition for no arching => a > c
(1/ff) = 0.3 1 + 4.3 (1/1.27) = 0.3 1 + 4.3
1 = 8.82 c = 8.82/1.27 = 6.95
B = 2.2 x 6.95/22 = 0.69 ft = 8.33 in
Material considerations for hopper design
Amount of moisture in product? Is the material typical of what is expected? Is it sticky or tacky? Is there chemical reaction? Does the material sublime? Does heat affect the material?
Material considerations for hopper design
Is it a fine powder (< 200 microns)? Is the material abrasive? Is the material elastic? Does the material deform under pressure?
Process Questions
How much is to be stored? For how long? Materials of construction Is batch integrity important? Is segregation important? What type of discharger will be used? How much room is there for the hopper?
Discharge Rates
Numerous methods to predict discharge rates from silos or hopper
For coarse particles (>500 microns)Beverloo equation - funnel flowJohanson equation - mass flow
For fine particles - one must consider influence of air upon discharge rate
Beverloo equation
W = 0.58 b g0.5 (B - kdp)2.5
where W is the discharge rate (kg/sec)b is the bulk density (kg/m3)
g is the gravitational constantB is the outlet size (m)k is a constant (typically 1.4)dp is the particle size (m)
Note: Units must be SI
Johanson Equation
Equation is derived from fundamental principles - not empirical
W = b (/4) B2 (gB/4 tan c)0.5
where c is the angle of hopper from verticalThis equation applies to circular outletsUnits can be any dimensionally consistent setNote that both Beverloo and Johanson show that W B2.5!
Discharge Rate - Example
An engineer wants to know how fast a compartment on a railcar will fill with polyethylene pellets if the hopper is designed with a 6” Sch. 10 outlet. The car has 4 compartments and can carry 180000 lbs. The bulk solid is being discharged from mass flow silo and has a 65° angle from horizontal. Polyethylene has a bulk density of 35 lb/cu ft.
Discharge Rate Example
One compartment = 180000/4 = 45000 lbs.Since silo is mass flow, use Johanson equation.6” Sch. 10 pipe is 6.36” in diameter = B
W = (35 lb/ft3)(/4)(6.36/12)2 (32.2x(6.36/12)/4 tan 25)0.5
W= 23.35 lb/secTime required is 45000/23.35 = 1926 secs or ~32 min.In practice, this is too long - 8” or 10 “ would be a better choice.
The Case of Limiting Flow Rates
When bulk solids (even those with little cohesion) are discharged from a hopper, the solids must dilate in the conical section of the hopper. This dilation forces air to flow from the outlet against the flow of bulk solids and in the case of fine materials either slows the flow or impedes it altogether.
Limiting Flow Rates
Vertical stress
Bulk
density
Interstitial gas pressure
Note that gas pressure is less than ambient pressure
Limiting Flow Rates
The rigorous calculation of limiting flow rates requires simultaneous solution of gas pressure and solids stresses subject to changing bulk density and permeability. Fortunately, in many cases the rate will be limited by some type of discharge device such as a rotary valve or screw feeder.
Limiting Flow Rates - Carleton Equation
gd
vB
v
ps
ff 3/5
3/40
3/23/120 15sin4
Carleton Equation (cont’d)
where v0 is the velocity of the bulk solid
is the hopper half angles is the absolute particle density
f is the density of the gas
f is the viscosity of the gas
Silo Discharging Devices
Slide valve/Slide gate Rotary valve Vibrating Bin Bottoms Vibrating Grates others
Rotary Valves
Quite commonly used to discharge materials from bins.
Screw FeedersDead Region
Better Solution
Discharge Aids
Air cannons Pneumatic Hammers VibratorsThese devices should not be used in place of a
properly designed hopper!They can be used to break up the effects of time consolidation.
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