Menne, D., 1983. the Slip Velocity Between Particulate Solids and an Interstitial Fluid...

2
?' I ~i I , '-I ~V-- S.~ 7, i ' I M V I i II 1/, ,/ 1/ --- V ~I The slip velocity between particulate solids and an interstitial fluid by D. MENNE*. B.Sc. (Ing. Chem). SYNOPSIS An empirical dimensionless correlation is presented that relates system variables to the superficial slip velocity between solid mineral products and an interstitial fluid. The correlation is valid within engineering accuracy for all solids and fluids at all concentrations. The particular usefulness of the correlation is that it provides explicit equations for both slip velocity and voidage. SAMEVATTING 'n Empiriese dimensielose verwantskap wat sisteem veranderlikes met die glipsnelheid tussen minerale vastestow- we en 'n omringende vloeistof verbind, word gegee. Die verwantskap het voldoende akkuraatheid vir ingenieurs- doeleindes vir alle vastestowwe en vloeistowwe teen alle konsentrasies. Die besondere nut van die verwantskap le in die explisiete oplossings wat dit bied vir beide glipsnelheid en vloeistof volume fraksie. Introduction The superficial slip velocity, Vc, between solids and interstitial fluid is a quantity needed for calculations in a wide range of applications in solid and fluid technology such as fluidization, vertical transport of solids, sizing of discharge orifices and downcomers, classification, sedi- mentation, thickening, and continuous crystallization. Relationship between Desi~n Quantities and Super- ficial Slip Velocity The mean suspension velocity, V rn, of a slurry in up- flow is related to Vc as follows: Urn - Vc(I-E)/(Ed-E), where E Ed - the in situ liquid fraction in the pulp, and = the volume fraction of the input and dis- charge liquid of the slurry. For a fluidized bed in which the solids flux is zero, Vc equals the superficial flowrate of liquid, i.e. the upflow rate of liquid above the interface of the fluidized bed. For sedimenting systems, the solids flux is Vc (I - E). For a discharge orifice or a downcomer feeding a closed receiver, this equals the displaced-liquid flux. A General Explicit Correlation for Superficial Slip Velocity Above the fluidizing limit (typically above E = 0,4), the superficial Reynolds number of particles being fluidized, Re = Vcd/v, can be related to their Archimedes number, Ar = gd3 (8 - 1)/V2, as follows: Re = a((1 + bEe Ar)i - I). The term Ec is an empirical correction to account for the effect of increased effective drag due to the momen- tum transfer between particles and the decreased cross- sectional area of fluid flow as the concentrations of par- ticles increase. For most mineral products that are much smaller than the spacings on the equipment, this equation is valid within an engineering accuracy that is acceptable, in view of the usual ignorance concerning corrections for variations in particle shapes, over the entire range of flow regimes if the constants a = 8,4, b = 0,10, and c = 4,7 are chosen. This is demonstrated in Figs. 1 and 2. For greater precision, the constants should be determined * Bateman Engineering Limited, P.D. Box 565, Boksburg 1460, Transvaal. @ 1983. 1000 VI "- E E )0- f- u g w > c ~ 100 u c w Cl: D.. 10 10 100 1000 MEASURED VELOCITY ","Is ~ Fig. I-Free settling velocities in water (measured velocities from Taggartl). SG = specific gravity or relative density. 100000 I 10000 .. ~ 1000 E >- I:: 100 u 0 ..J ~ 10-+ ! c W f- !:! c '" Cl: Q. 0,1 0.01 O,DI 10 1000 10000 100000 100 0,1 MEASURED VELOCITY mm Is ~ Fig.1-Free settling velocities in air (measured velocities from Taggart2). SG = specific gravity or relative density. JOURNAL OF THE SOUTH AFRICAN INSTITUTE OF MINING AND METALLURGY MAY 1983 103

description

Scientific paper

Transcript of Menne, D., 1983. the Slip Velocity Between Particulate Solids and an Interstitial Fluid...

Page 1: Menne, D., 1983. the Slip Velocity Between Particulate Solids and an Interstitial Fluid [v083n05p103]

?'I

~i I,

'-I ~V--S.~ 7,i'

I

M VI

i

II 1/,

,/ 1/---

V~I

p

The slip velocity between particulate solidsand an interstitial fluid

by D. MENNE*. B.Sc. (Ing. Chem).SYNOPSIS

An empirical dimensionless correlation is presented that relates system variables to the superficial slip velocitybetween solid mineral products and an interstitial fluid. The correlation is valid within engineering accuracy for allsolids and fluids at all concentrations. The particular usefulness of the correlation is that it provides explicit equationsfor both slip velocity and voidage.

SAMEVATTING'n Empiriese dimensielose verwantskap wat sisteem veranderlikes met die glipsnelheid tussen minerale vastestow-

we en 'n omringende vloeistof verbind, word gegee. Die verwantskap het voldoende akkuraatheid vir ingenieurs-doeleindes vir alle vastestowwe en vloeistowwe teen alle konsentrasies. Die besondere nut van die verwantskap lein die explisiete oplossings wat dit bied vir beide glipsnelheid en vloeistof volume fraksie.

Introduction

The superficial slip velocity, Vc, between solids andinterstitial fluid is a quantity needed for calculations ina wide range of applications in solid and fluid technologysuch as fluidization, vertical transport of solids, sizing ofdischarge orifices and downcomers, classification, sedi-mentation, thickening, and continuous crystallization.

Relationship between Desi~n Quantities and Super-ficial Slip Velocity

The mean suspension velocity, V rn, of a slurry in up-flow is related to Vc as follows:

Urn - Vc(I-E)/(Ed-E),where

EEd

- the in situ liquid fraction in the pulp, and

= the volume fraction of the input and dis-charge liquid of the slurry.

For a fluidized bed in which the solids flux is zero, Vcequals the superficial flowrate of liquid, i.e. the upflowrate of liquid above the interface of the fluidized bed.For sedimenting systems, the solids flux is Vc (I - E).For a discharge orifice or a downcomer feeding a closedreceiver, this equals the displaced-liquid flux.

A General Explicit Correlation for Superficial SlipVelocity

Above the fluidizing limit (typically above E = 0,4), thesuperficial Reynolds number of particles being fluidized,Re = Vcd/v, can be related to their Archimedes number,Ar = gd3 (8 - 1)/V2, as follows:

Re = a((1 + bEe Ar)i - I).The term Ec is an empirical correction to account for

the effect of increased effective drag due to the momen-tum transfer between particles and the decreased cross-sectional area of fluid flow as the concentrations of par-ticles increase.

For most mineral products that are much smaller thanthe spacings on the equipment, this equation is validwithin an engineering accuracy that is acceptable, inview of the usual ignorance concerning corrections forvariations in particle shapes, over the entire range offlow regimes if the constants a = 8,4, b = 0,10, andc = 4,7 are chosen. This is demonstrated in Figs. 1 and 2.For greater precision, the constants should be determined

* Bateman Engineering Limited, P.D. Box 565, Boksburg 1460,Transvaal.

@ 1983.

1000

VI

"-EE

)0-

f-ugw>c~ 100ucwCl:D..

10

10 100 1000

MEASURED VELOCITY ","Is ~

Fig. I-Free settling velocities in water (measured velocitiesfrom Taggartl). SG = specific gravity or relative density.

100000 I

10000

..

~ 1000

E

>-I:: 100u0..J~ 10-+

!

cWf-!:!c

'"Cl:Q.

0,1

0.01O,DI 10 1000 10000 1000001000,1

MEASURED VELOCITY mm Is ~

Fig.1-Free settling velocities in air (measured velocitiesfrom Taggart2). SG = specific gravity or relative density.

JOURNAL OF THE SOUTH AFRICAN INSTITUTE OF MINING AND METALLURGY MAY 1983 103

Page 2: Menne, D., 1983. the Slip Velocity Between Particulate Solids and an Interstitial Fluid [v083n05p103]

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x~+ e

~~.~

1<11

I"~

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BEDEXPANSION

25 %50-%75%

100%125".

100

11 10

AMBIENT TEMP.5.C 35.C. (!)

+ $)C e0 .A ~

--MEASURED VELOCITY mm!.

Fig. 3-Hindered settling velocities of wetted activated car-bon (relative density 1,28) in water (measured velocities from

Edward L. Bateman).

by experiment for specific applications. An exampleis the fluidization of activated carbon for the recovery of

Precious MetalsMr Robert P. Paise, AMTEC Corporation, Gilroy,

California, Chairman of the IPMI International Con-ference on Precious Metals, released highlights of the7th Conference, to be held in San Francisco, California,from 13th to 16th June, 1983.

For the first time IPMI will conduct a mini-exhibit ofliterature and equipment of its member companies.Exhibit hours are scheduled on Tuesday, Wednesday,and Thursday during the conference.

The technical programme organized by David Reese,

104 MAY 1983

100

gold, for which the constants A = 5,47, B = 0,0335,and C = 4,7 give a good fit (see Fig. 3).

The particular usefulness of the above equation is thatUc or E can be solved explicitly. This gives directsolutions for systems with essentially uniform particle-size distributions such as typical sedimenting coagulatesor 'floes'. Fluidized beds can be considered to consist oflayers containing uniform particles if size ranges under1,414 : 1 are considered.

Symbols Used

Ar - Archimedes number (ratio of particle buoy-ancy to drag forces) = (gd3(S - 1)/v2)

d - Particle diameterE = Fraction of in situ fluid volumeEd = Fraction of inlet and discharge flui<fvolumeg - Gravitational constant = 9,81 m/sRe - Reynolds number (ratio of particle inertial to

viscous forces) = Ucd/v= Relative density of particle relative to the

density of the in situ suspensionUc - Superficial slip velocity between solids and the

interstitial fluidUm - Mean upflow velocity of a suspension (solids

plus fluid)- Kinematic viscosity of fluid

S

v

1.

2.

ReferencesTAGGART, ARTHUR F. Handbook of mineral dressing. JohnWiley & Sons. Inc. 1945. p. 8 - 04.TAGGART, ARTHUR F. Ibid., p. 9 - 03.

Micro MetalIics Corp., consists of ten sessions for a totalof 40 papers over the three-day period. The sessionsplanned are Economics and Trading, Recovery ofPrecious Metals from Mining Operations, Unique Proper-ties of Precious Metals, New Technology, Recovery andRefining, Precious Metal Applications, AnalyticalMethods, Mining and Metal Extraction, and Chemistry ofPrecious Metals.

For further information, contact IPMI, 2254 Barring-ton Rd., Bethlehem, PA 18018, V.S.A. (215/866-1211).

JOURNAL OF THE SOUTH AFRICAN INSTITUTE OF MINING AND METALLURGY