episode 38 : bin and hopper design

76
SAJJAD KHUDHUR ABBAS Ceo , Founder & Head of SHacademy Chemical Engineering , Al-Muthanna University, Iraq Oil & Gas Safety and Health Professional – OSHACADEMY Trainer of Trainers (TOT) - Canadian Center of Episode 38 : Bin and Hopper Design

Upload: sajjad-khudhur-abbas

Post on 15-Apr-2017

615 views

Category:

Engineering


7 download

TRANSCRIPT

Page 1: Episode 38 :  Bin and Hopper Design

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

Page 2: 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.

Page 3: Episode 38 :  Bin and Hopper Design

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

Page 4: Episode 38 :  Bin and Hopper Design

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?

Page 5: Episode 38 :  Bin and Hopper Design

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

Page 6: Episode 38 :  Bin and Hopper Design

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

Page 7: Episode 38 :  Bin and Hopper Design

Funnel Flow

“Dead” or non-flowing region

Act

ive

Flow

C

hann

el

Page 8: Episode 38 :  Bin and Hopper Design

Expanded Flow

Funnel Flow upper section

Mass Flow bottom section

Page 9: Episode 38 :  Bin and Hopper Design

Problems with Hoppers

Ratholing/Piping

Page 10: Episode 38 :  Bin and Hopper Design

Ratholing/Piping

Stable Annular Region

Voi

d

Page 11: Episode 38 :  Bin and Hopper Design

Problems with Hoppers

Ratholing/Piping Funnel Flow

Page 12: Episode 38 :  Bin and Hopper Design

Funnel Flow-Segregation

-Inadequate Emptying

-Structural Issues

Coa

rse

Coa

rse

Fine

Page 13: Episode 38 :  Bin and Hopper Design

Problems with Hoppers

Ratholing/Piping Funnel Flow Arching/Doming

Page 14: Episode 38 :  Bin and Hopper Design

Arching/Doming

Cohesive Arch preventing material from exiting hopper

Page 15: Episode 38 :  Bin and Hopper Design

Problems with Hoppers

Ratholing/Piping Funnel Flow Arching/Doming Insufficient Flow

Page 16: Episode 38 :  Bin and Hopper Design

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

Page 17: Episode 38 :  Bin and Hopper Design

Problems with Hoppers

Ratholing/Piping Funnel Flow Arching/Doming Insufficient Flow Flushing

Page 18: Episode 38 :  Bin and Hopper Design

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

Page 19: Episode 38 :  Bin and Hopper Design

Problems with Hoppers

Ratholing/Piping Funnel Flow Arching/Doming Insufficient Flow Flushing Inadequate Emptying

Page 20: Episode 38 :  Bin and Hopper Design

Inadequate emptyingUsually occurs in funnel flow silos where the cone angle is insufficient to allow self draining of the bulk solid.

Remaining bulk solid

Page 21: Episode 38 :  Bin and Hopper Design

Problems with Hoppers

Ratholing/Piping Funnel Flow Arching/Doming Insufficient Flow Flushing Inadequate Emptying Mechanical Arching

Page 22: Episode 38 :  Bin and Hopper Design

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

Page 23: Episode 38 :  Bin and Hopper Design

Problems with Hoppers

Ratholing/Piping Funnel Flow Arching/Doming Insufficient Flow Flushing Inadequate Emptying Mechanical Arching Time Consolidation - Caking

Page 24: Episode 38 :  Bin and Hopper Design

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

Page 25: Episode 38 :  Bin and Hopper Design

Segregation

Mechanisms- Momentum or velocity- Fluidization- Trajectory- Air current- Fines

Page 26: Episode 38 :  Bin and Hopper Design

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

Page 27: Episode 38 :  Bin and Hopper Design

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

Page 28: Episode 38 :  Bin and Hopper Design

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

Page 29: Episode 38 :  Bin and Hopper Design

How is a hopper designed?

Measure- powder cohesion/interparticle friction- wall friction- compressibility/permeability

Calculate- outlet size- hopper angle for mass flow- discharge rates

Page 30: Episode 38 :  Bin and Hopper Design

What about angle of repose?

Pile of bulk solids

Page 31: Episode 38 :  Bin and Hopper Design

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!

Page 32: Episode 38 :  Bin and Hopper Design

Bulk Solids Testing

Wall Friction Testing Powder Shear Testing - measures both powder

internal friction and cohesion Compressibility Permeability

Page 33: Episode 38 :  Bin and Hopper Design

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

Page 34: Episode 38 :  Bin and Hopper Design

Testing Considerations

Must consider the following variables- time- temperature- humidity- other process conditions

Page 35: Episode 38 :  Bin and Hopper Design

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

Page 36: Episode 38 :  Bin and Hopper Design

Wall Friction TestingJenike Shear Tester

Wall Test Sample

Ring

CoverW x A

S x A

Bracket

Bulk Solid

Page 37: Episode 38 :  Bin and Hopper Design

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

Page 38: Episode 38 :  Bin and Hopper Design

Jenike Shear Tester

Ring

CoverW x A

S x A

Bracket

Bulk SolidBulk Solid

Shear plane

Page 39: Episode 38 :  Bin and Hopper Design

Other Shear Testers

Peschl shear tester Biaxial shear tester Uniaxial compaction cell Annular (ring) shear testers

Page 40: Episode 38 :  Bin and Hopper Design

Ring Shear Testers

W x ABottom cell rotates slowly

Arm connected to load cells, S x A

Bulk solid

Page 41: Episode 38 :  Bin and Hopper Design

Shear test data analysis

C fc 1

Page 42: Episode 38 :  Bin and Hopper Design

Stresses in Hoppers/Silos

Cylindrical section - Janssen equation Conical section - radial stress field

Stresses = Pressures

Page 43: Episode 38 :  Bin and Hopper Design

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

Page 44: Episode 38 :  Bin and Hopper Design

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.

Page 45: Episode 38 :  Bin and Hopper Design

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.

Page 46: Episode 38 :  Bin and Hopper Design

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.

Page 47: Episode 38 :  Bin and Hopper Design

Silo Stresses - Overall

hydrostatic

Bulk solidNotice that there is essentially no stress at the outlet. This is good for discharge devices!

Page 48: Episode 38 :  Bin and Hopper Design

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

Page 49: Episode 38 :  Bin and Hopper Design

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!

Page 50: Episode 38 :  Bin and Hopper Design

Types of BinsConical Pyramidal

Watch for in-flowing valleys in these bins!

Page 51: Episode 38 :  Bin and Hopper Design

Types of BinsWedge/Plane Flow

B

L

L>3B

Chisel

Page 52: Episode 38 :  Bin and Hopper Design

A thought experiment1 c

Page 53: Episode 38 :  Bin and Hopper Design

The Flow Function

1

c

Flow function

Time flow function

Page 54: Episode 38 :  Bin and Hopper Design

Determination of Outlet Size

1

c

Flow function

Time flow function

Flow factor

c,i

c,t

Page 55: Episode 38 :  Bin and Hopper Design

Determination of Outlet Size

B = c,i H()/

H() is a constant which is a function of hopper angle

Page 56: Episode 38 :  Bin and Hopper Design

H() Function

Cone angle from vertical10 20 30 40 50 60

1

2

3

H(

)

Rectangular outlets (L > 3B)

Square

Circular

Page 57: Episode 38 :  Bin and Hopper Design

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

Page 58: Episode 38 :  Bin and Hopper Design

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

Page 59: Episode 38 :  Bin and Hopper Design

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?

Page 60: Episode 38 :  Bin and Hopper Design

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?

Page 61: Episode 38 :  Bin and Hopper Design

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?

Page 62: Episode 38 :  Bin and Hopper Design

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

Page 63: Episode 38 :  Bin and Hopper Design

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

Page 64: Episode 38 :  Bin and Hopper Design

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!

Page 65: Episode 38 :  Bin and Hopper Design

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.

Page 66: Episode 38 :  Bin and Hopper Design

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.

Page 67: Episode 38 :  Bin and Hopper Design

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.

Page 68: Episode 38 :  Bin and Hopper Design

Limiting Flow Rates

Vertical stress

Bulk

density

Interstitial gas pressure

Note that gas pressure is less than ambient pressure

Page 69: Episode 38 :  Bin and Hopper Design

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.

Page 70: Episode 38 :  Bin and Hopper Design

Limiting Flow Rates - Carleton Equation

gd

vB

v

ps

ff 3/5

3/40

3/23/120 15sin4

Page 71: Episode 38 :  Bin and Hopper Design

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

Page 72: Episode 38 :  Bin and Hopper Design

Silo Discharging Devices

Slide valve/Slide gate Rotary valve Vibrating Bin Bottoms Vibrating Grates others

Page 73: Episode 38 :  Bin and Hopper Design

Rotary Valves

Quite commonly used to discharge materials from bins.

Page 74: Episode 38 :  Bin and Hopper Design

Screw FeedersDead Region

Better Solution

Page 75: Episode 38 :  Bin and Hopper Design

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.

Page 76: Episode 38 :  Bin and Hopper Design

Thanks for Watching Please follow me / SAJJAD KHUDHUR ABBAS