Some Simple Observations on the Failure of Particle Networks

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Peter Scales Particulate Fluids Processing Centre Department of Chemical and Biomolecular Engineering University of Melbourne Australia Some Simple Observations on the Failure of Particle Networks

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Peter Scales Particulate Fluids Processing Centre Department of Chemical and Biomolecular Engineering University of Melbourne Australia. Some Simple Observations on the Failure of Particle Networks. Suspending Medium.  <  gel.    gel. Particles. Network Characteristics. - PowerPoint PPT Presentation

Transcript of Some Simple Observations on the Failure of Particle Networks

Page 1: Some  Simple Observations  on the  Failure  of  Particle Networks

Peter ScalesParticulate Fluids Processing Centre

Department of Chemical and Biomolecular Engineering

University of MelbourneAustralia

Some Simple Observations on the Failure of Par-ticle Networks

Page 2: Some  Simple Observations  on the  Failure  of  Particle Networks

Network Characteristics

Particles

Suspending Medium

< gel gel

Flow properties typified by:

• Yielding• Shear thinning behaviour

at concentrations above gel

• Strain hardening in compression

• Strain softening in shear

Page 3: Some  Simple Observations  on the  Failure  of  Particle Networks

Yield Measurement

0

10000

20000

30000

40000

50000

60000

70000

80000

0 0.0005 0.001 0.0015 0.002

Tim

e, t

(s)

(Specific Filtrate Volume)2, V2 (m2)

S1 Py Run 2Pressure Step

10 kPa

20 kPa

40 kPa

80 kPa150 kPa

300 kPa

0.2 rpm

vaneslurry

Torq

ue

Time

Page 4: Some  Simple Observations  on the  Failure  of  Particle Networks

Shear and Uni-axial Compression

Volume Fraction 0.1 1

0.1

1

10

100

1000

AKP-15AKP-20AKP-30AKP-50

pH = 8.9

Z. Zhou

Shea

r Yie

ld S

tress

/d2

Volume Fraction 0.1 1

0.1

1

10

100

1000

AKP-15AKP-20AKP-30AKP-50

pH = 8.9

Z. Zhou

Shea

r Yie

ld S

tress

/d2

Volume fraction 0.2 0.3 0.4 0.5 0.6 0.8.0.1 1

1e-1

1e+0

1e+1

1e+2

1e+3

1e+4

1e+5 pH = 9.0

Compression

Shear

Z. Zhou

Yie

ld S

tress

/d2

Volume fraction 0.2 0.3 0.4 0.5 0.6 0.8.0.1 1

1e-1

1e+0

1e+1

1e+2

1e+3

1e+4

1e+5 pH = 9.0

Compression

Shear

Z. Zhou

Yie

ld S

tress

/d2

Zhou et al., CES, 56: 2901-2920 (2001)

Page 5: Some  Simple Observations  on the  Failure  of  Particle Networks

PROCESS SHEAR COMPRESSION MODELCoating ✔ ✔Mixing/pumping ✔ ✔Pipeline transport ✔ ✔ ✗Sedimentation ✔ ✔Thickening ✔ ✔ ✗Pressure filtration ✔ ✔Belt press filtration ✔ ✔ ✗Centrifuge (decanter) ✔ ✔ ✗Centrifuge (bowl) ✔ ✔Vacuum filtration ✔ ✔ ✗Drying ✔ ✔ ✗

MOTIVATION

Page 6: Some  Simple Observations  on the  Failure  of  Particle Networks
Page 7: Some  Simple Observations  on the  Failure  of  Particle Networks

Critical State Approach (von Mises) Supposes that the compressive and shear stresses co-operate to produce yield

Compressive stress

Max

imum

she

ar s

tress

Elastic

Plastic

Implication is that continuous stirring will cause the network to proceed to maximum density

pres

sure

Eq’m density

unstirredstirred

Page 8: Some  Simple Observations  on the  Failure  of  Particle Networks

Channell, White & Zukoski saw a family of curves of the type one would expect for a series of shear stresses

Shear rate 0 0.69 1.85 5.63 11.3

In other words, they saw that material undergoing shear flow could behave as if it were still a solid in compression.

At the right shear rate, the system almost becomes incompressible

Page 9: Some  Simple Observations  on the  Failure  of  Particle Networks

But how do we get the water out?

The rate of collapse is controlled by the rate of water escape

Page 10: Some  Simple Observations  on the  Failure  of  Particle Networks

SummaryThe challenge for hard to dewater materials is to find the right combination of shear and compression to exploit the material properties

Getting the water out in a reasonable time is still an issue and pathways are needed

The concept of a simple elasto-plastic transition (yield stress) for particle networks is too crude to be useful in multi-dimensional network yielding and we need a new fundamental description