Chapter 2 Multiple Particle Systems · 2007. 10. 9. · interface, h B-Emin Variation in heights of...

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C h a p t e r 2 M u l t i p l e P a r t i c l e S y s t e m s 2 . 1 S e t t l i n g o f a S u s p e n s i o n o f P a r t i c l e s H i n d e r e d S e t t l i n g . . E f f e c t i v e v i s c o s i t y o f s u s p e n s i o n μ e = μ f ( ε ) E f f e c t i v e d e n s i t y o f s u s p e n s i o n ρ ave = ερ f +(1- ε ) ρ p U p , U f : a c t u a l ( i n t e r s t i t i a l ) v e l o c i t y o f p a r t i c l e s a n d f l u i d , r e s p e c t i v e l y U ps , U fs : s u p e r f i c i a l v e l o c i t y U ps = U p (1- ε ) U fs = U f ε w h e r e ε : v o i d a g e o r v o i d f r a c t i o n ∴1- ε = particle volume suspension volume = volume concentration of particles = c v = v o l u m e U ps a n d U fs : v o l u m e f l u x o f p a r t i c l e s a n d f l u i d ( m / s m 3 fluid or particles m 3 suspension ) U ps U fs s u p e r f i c i a l v e l o c i t y f l u x ! C o r r e c t e d t e r m i n a l s e t t l i n g v e l o c i t y U rel T U p - U f U T U T ε f ( ε ) B e c a u s e o f n o n e t f l o w U ps + U fs =0

Transcript of Chapter 2 Multiple Particle Systems · 2007. 10. 9. · interface, h B-Emin Variation in heights of...

Page 1: Chapter 2 Multiple Particle Systems · 2007. 10. 9. · interface, h B-Emin Variation in heights of interfaces with respect to time CA=0 CB CE,min CS Ups Velocity of A-B interface

Chapter 2 Multiple Particle Systems

2.1 Settling of a Suspension of Particles

Hindered Settling

입자가 모여 있으면 서로의 향이 침강에 미친다. 이를 간섭침강이라

한다.

Effective viscosity of suspension

μe=

μ

f ( ε )

Effective density of suspension

ρave= ερ f+ (1- ε)ρ p

U p , U f

: actual(interstitial) velocity of particles and fluid,

respectively

U ps , U fs

:superficial velocity

U ps= U p ( 1- ε )

U fs= U fε

where ε : voidage or void fraction

∴1-ε=particle volumesuspension volume

= volume concentration of particles= c v = volume

∴ U ps and U fs

: volume flux of particles and fluid

( m/s⋅m 3 fluid or particles

m 3 suspension)

☞ U ps와 U fs

는 superficial velocity임과 동시에 부피 flux 임!

Corrected terminal settling velocity

U relT≡U p-U f

≠UT

≡U Tεf ( ε )

Because of no net flow

U ps+ U fs= 0

Page 2: Chapter 2 Multiple Particle Systems · 2007. 10. 9. · interface, h B-Emin Variation in heights of interfaces with respect to time CA=0 CB CE,min CS Ups Velocity of A-B interface

2.2 Batch Settling

(1) Settling Flux as a Function of Suspension Concnetration

U p(1- ε)+U fε= 0

∴ U p( 1- ε)+ [U p-U Tεf ( ε ) ]ε= 0

∴ U p= U Tε 2f(ε)

e.g. Richardson and Zaki(1954)

U p= U Tεn

where

4.8- nn- 2.4

= 0.043Ar 0.57 [ 1- 2.4(d pD )

0.27

]

Superficial solid velocity or volumetric solid flux(m/s)

U ps= U p ( 1- ε )= U Tε 2f( ε ) ( 1- ε )

= U T ( 1- ε)εn

Settling flux curve ( U ps vs. C v): Figure 2.1

(2) Sharp Interfaces in Sedimentation

C2

C1

Up1

Up2

Uint

Material Balance over the interface

(U p1- U int)C 1 = (U p2- U int)C 2

where C=1- ε, solids fraction

∴ U int=U ps 1

- U ps2

C 1- C 2

As ΔC→0,

Page 3: Chapter 2 Multiple Particle Systems · 2007. 10. 9. · interface, h B-Emin Variation in heights of interfaces with respect to time CA=0 CB CE,min CS Ups Velocity of A-B interface

U=dU psdC

The velocity of layer of concentration C

C1=0 C2 C3C4

Ups

Slope=velocity of layer ofconcentration C4

Slope=Uint, 12

Slope=Uint, 23

(3) Batch Settling

Supplying information for the design of a thickener

Type I Settling

B

A

B

SS

A

CB CA =0CBCS CSCA =0

A-B

B-S

A-S

Time, t

Height ofinterface,

h

Variation of heights of interfaces with

respect to time

CA=0 CB2 CSCB

Ups Velocity ofA-Binterface

Velocity ofB-Sinterface

Flux vs. concentration

Type II Settling

Page 4: Chapter 2 Multiple Particle Systems · 2007. 10. 9. · interface, h B-Emin Variation in heights of interfaces with respect to time CA=0 CB CE,min CS Ups Velocity of A-B interface

B

A

B

SS

A

CB CA =0CBCS CSCA =0

E

A

SCA =0CB

E

CE,max

CS

CE,max

Recommended web site :

http://www.aem.umn.edu/Solid-Liquid_Flows/video.html

A-B

Emax-S

A-S

Time, t

Height ofinterface,

hB-Emin

Variation in heights of interfaces with

respect to time

CA=0 CE,min CSCB

Ups Velocity ofA-Binterface

Velocity ofE-Sinterface

CE,max

Velocity ofB-Einterface

Flux vs. concentration for

particle slurry

즉 두 type의 침강은 기농도에 의존하는 것으로서 후자의 경우 하나의

층이 더 나타나는 것은 C B의 치에서 C S가 변곡 때문에 가려서 생기는

문제이다. 따라서 농도가 진하여 변곡 아주 가까이에 있을 때 type II의

침강이 생긴다.

2.3 Continuous Settling

(1) Settling of a Suspension in a Flowing Fluid

Thickener vs. Clarifier Figure 2.11

Downward flow

Page 5: Chapter 2 Multiple Particle Systems · 2007. 10. 9. · interface, h B-Emin Variation in heights of interfaces with respect to time CA=0 CB CE,min CS Ups Velocity of A-B interface

U ps = Q ( 1 - ε )

A + U T

ε 2f ( ε )

Total Flux Flux solid due to due to

flux bulk flow settling

Define C v≡1- ε, particle volume concentration

Figure 2.12:

Feed concentration,CF → bottom section concentration, CB

Upward flow

U ps = - Q ( 1 - ε )

A + U T

ε 2f ( ε )

Figure 2.13:

Feed concentration,CF → Top section concentration, CT

(2) Real Thickener

CT

CB

Underflow

L, CL

Feed

F, CF V, CV

Feed/ Under(down)flow/ up(over)flow:

F(CF) L(CL) V(CV)

Below feed

U ps = L ( 1 - ε )

A + U T

ε 2f ( ε )

Above feed

U ps = - V ( 1 - ε )

A + U T

ε 2f ( ε )

Page 6: Chapter 2 Multiple Particle Systems · 2007. 10. 9. · interface, h B-Emin Variation in heights of interfaces with respect to time CA=0 CB CE,min CS Ups Velocity of A-B interface

C

Ups

C

Ups

Underflow flux, slope=L/A

Overflow flux, slope=-V/A

Below feed

Above feed

Downward flux

Downward flux

Upward flux

Batch fluxCcrit

* Critical concentration: C crit≡ C atU p, upward=0

(3) Critically Loaded Thickener

C F=C crit

∴ U p, upward= 0, CB=CF , CT= CV=0 and

U ps, downflow=FCFA

=LCLA

Page 7: Chapter 2 Multiple Particle Systems · 2007. 10. 9. · interface, h B-Emin Variation in heights of interfaces with respect to time CA=0 CB CE,min CS Ups Velocity of A-B interface

C

Ups

Ups=FCF/A =LCL/A

CF=CB

Ccrit

C

Ups

Ups=VCv/A =0 CT and Cv

Underflow flux,L/A

Overflow flux, -V/A

Below feed

Above feed

Downward flux

Downward flux

Upward flux

Batch fluxCL

Feed flux, F/A

(4) Underloaded Thickener

C F < C crit

∴ U p, upward= 0, C B < C F and CT= CV=0

U ps, downflow=FCFA

=LCLA

(5) Overloaded Thickener

C F > C crit

∴ U p,upward=FCFA

-U ps, downflow, CB=CF and C T > C V≠0

U ps, downflow=LC LA

Page 8: Chapter 2 Multiple Particle Systems · 2007. 10. 9. · interface, h B-Emin Variation in heights of interfaces with respect to time CA=0 CB CE,min CS Ups Velocity of A-B interface

C

Ups

Ups=FCF/A =LCL/A

C

Ups

Ups=VCv/A =0 CT and Cv

Underflow flux,L/A

Overflow flux, -V/A

Below feed

Above feed

CL

Feed flux, F/A

CFCB Ccrit

Underloaded Thickener

C

Ups=LCL/A

CF=CB

CT C

Ups

Ups=VCv/A

Cv

Underflow flux,L/A

Overflow flux, -V/A

Below feed

Above feed

Downward flux

Downward flux

Upward flux

Batch fluxCL

Feed flux, F/AFCF/A

Overloaded thickener

* Centrifugal Sedimentation rω 2 instead of g

Worked Example 2.4