flow and filtration: the physics of brewing

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Flow and Filtration: Flow and Filtration: The Physics of The Physics of Brewing Brewing Dr. Alex Speers Department of Food Science and Technology <[email protected]>

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Flow and Filtration: The Physics of Brewing. Dr. Alex Speers Department of Food Science and Technology . Outline. Introduction Brewing gums shearing Methods Rheometry Filtration Summary. Why study  -glucans?. Cause processing problems in brewing: - PowerPoint PPT Presentation

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Page 1: Flow and Filtration: The Physics of Brewing

Flow and Filtration: The Flow and Filtration: The Physics of BrewingPhysics of Brewing

Dr. Alex Speers

Department of Food Science and Technology

<[email protected]>

Page 2: Flow and Filtration: The Physics of Brewing

OutlineOutline

Introduction– Brewing gums– shearing

Methods– Rheometry– Filtration

Summary

Page 3: Flow and Filtration: The Physics of Brewing

Why study -glucans?

Cause processing problems in brewing:

• Under-modification of barley endosperm

• High viscosity of wort and beer

• Slow runoff of wort and beer

• Haze formation in packaged beer

• Clogging of membranes

• Increased production cost

Page 4: Flow and Filtration: The Physics of Brewing

Localization of barley -glucans

Structure of a barley kernel

Page 5: Flow and Filtration: The Physics of Brewing

Brewer Product Type B-Glucan Arabinoxylan

A/USA Popular Priced Lager(PPL)

29.4 1968

B/USA 23.6 1031C/USA 20.4 1684A/USA Premium Lager (PL) 24.2 1657B/USA 23.6 2094B/USA 32.7 1292D/USA 0.4 1386E/USA 149.7 2368F/USA 79.9 3347G/Germany 247.7 2598H/Germany 145.1 3131B/USA Light 0.3 514F/USA Wheat 29.3 3103H/Germany 21.4 4211G/Germany 57.2 3174LSD 4.5 524

Beta-Glucan and Arabinoxylan Content of Selected Beers (ug / ml)

Page 6: Flow and Filtration: The Physics of Brewing

Chemical structure of barley -glucans

Unbranched chains of -D-glucopyranose residues

-(14)- linkage -(13)- linkage

O OO

OO O

Page 7: Flow and Filtration: The Physics of Brewing

Chemical structure of arabinoxylans

Page 8: Flow and Filtration: The Physics of Brewing

Localization of gums

• Deposited mainly in in endosperm cell walls

• Barley endosperm cell walls contain

20% arabinoxylans

70% -glucans

• Barley aleurone cell walls contain

65-67% arabinoxylans

26-29% -glucans

• Beta-glucan content

barley: 0.14 - 8.9 %

wort/beer: 12 - 940 mg/L

Page 9: Flow and Filtration: The Physics of Brewing

Non-Fermentable Brewing Gums

Defined as Non Starch Polysaccharides Gums - warm water extractable

Tend to viscosify wort and beerThus, add body/foam stabilityIn the distant past - not ‘a problem’With advent of membrane filters, tight

production schedules & lighter beerPose problems in some breweries some

times

Page 10: Flow and Filtration: The Physics of Brewing

Beta-Glucan fringed micelles

A

D

>70°C20°C

C

B

Page 11: Flow and Filtration: The Physics of Brewing

Micelle-like Aggregation

Page 12: Flow and Filtration: The Physics of Brewing

MethodsMethods

Page 13: Flow and Filtration: The Physics of Brewing

Rheological DefinitionsRheological Definitions

Science of deformation and flow Three important terms are shear rate (), shear

stress () and viscosity () - note different symbols used.

h={

V, F

V/h, = F/A

Page 14: Flow and Filtration: The Physics of Brewing

Calculation ExampleCalculation Example

Shear rate if dV= 1 cm/s and h = 1 cm? Shear rate = 1cm/s ÷ 1 cm =1 /s Shear rate units /s or s-1

Shear stress if F= 0.001 N and A= 1 m2 ? Shear stress = 0.001 N/ m2 = 1 mPa

Viscosity = 1 mPa s

Page 15: Flow and Filtration: The Physics of Brewing

Shear stress/shear rate Shear stress/shear rate measurement: rotationalmeasurement: rotational

RPM -> shear rate Torque -> shear stress Viscosity = shear stress/shear rate

Page 16: Flow and Filtration: The Physics of Brewing

Rheometry

Cone and plate and coaxial fixtures

Page 17: Flow and Filtration: The Physics of Brewing

Shear stress/shear rate Shear stress/shear rate measurement: pipe flowmeasurement: pipe flow

Flow rate -> shear rate Pressure loss -> shear stress Viscosity = shear stress/shear rate

Best suited for measuring Newtonian flow behaviour.

Page 18: Flow and Filtration: The Physics of Brewing

Rheometry

Capillary viscometer

Page 19: Flow and Filtration: The Physics of Brewing

Rheometry

Viscomat

Page 20: Flow and Filtration: The Physics of Brewing

Viscosity Dependence Viscosity Dependence

Temperature = A e E/RT

Concentration (gums,oP, Etoh)

Shear rate

Shear history

Page 21: Flow and Filtration: The Physics of Brewing

Shear effectsShear effectsShear effectsShear effects

Newtonian Flow

0

500

1000

1500

2000

2500

0 500 1000 1500

Shear Rate (/s)

Sh

ear

Str

ess

(mP

a)

Page 22: Flow and Filtration: The Physics of Brewing

Shear effectsShear effectsShear effectsShear effects

Newtonian Flow

0

0.5

1

1.5

2

2.5

0 500 1000 1500

Shear Rate (/s)

Vis

cosi

ty (

mP

a.s)

Page 23: Flow and Filtration: The Physics of Brewing

Non-Newtonian FlowNon-Newtonian FlowNon-Newtonian FlowNon-Newtonian Flow

Found at high gum concentrations

Pseudoplastic Flow

020406080

100120

0 500 1000 1500

Shear Rate (/s)

Vis

cosi

ty (

mP

a.s)

Page 24: Flow and Filtration: The Physics of Brewing

Rheological NotesRheological Notes

Normally viscosity properly defined as apparent viscosity - mPa s (= cP),

Kinematic viscosity is apparent viscosity divided by density (Stokes)

– (Misleading terms in literature),

1 mPa s is = 1 cP ~ viscosity of water at 20oC,

Apparent viscosty depends on density, temperature, shear rate and shear history.

Page 25: Flow and Filtration: The Physics of Brewing

Rheological NotesRheological Notes

Intrinsic Viscosity [

Based on extrapolated Specific viscosity (/ s -1)/c ->0

Can be used to determine shape of polymer based on molecular weight:

[

Page 26: Flow and Filtration: The Physics of Brewing

Determination of C* with 327 kDa -glucan in a control buffer

0

0.5

1

1.5

2

2.5

3

0 2 4 6 8 10

-glucan concentration (g/L)

C*= 3.11 g/L

1/

log

(

rel

)

Effect of ConcentrationEffect of Concentration

Page 27: Flow and Filtration: The Physics of Brewing

Early ResultsEarly Results

Using 327 kDa -glucan at 50 g/L, ethanol (0-7%), maltose (0-15%) and pH (3.6-5.2)

Viscosities were significantly different (P<0.05).

Page 28: Flow and Filtration: The Physics of Brewing

Variation of [] and C* of -glucan solutions

High ethanol 4.1 0.5 6.0 464 6.47

Low ethanol 4.1 0.5 4.0 812 2.72

Control 4.1 0.5 5.0 815 3.11

High maltose 4.1 0.8 5.0 806 2.13

Low maltose 4.1 0.1 5.0 862 3.05

Low pH 3.6 0.5 5.0 741 3.95

High pH 4.5 0.5 5.0 827 3.05

Treatment pH maltose ethanol [] C* (%) (%) (mL/g) (g/L)

Page 29: Flow and Filtration: The Physics of Brewing

Why Sporadic?

Depends on crop year

Stressed plant tends to more -glucan (Kendall)

Page 30: Flow and Filtration: The Physics of Brewing

Why Some Breweries?

Depends plant equipment

Depends on process

Possibly due to differences in shearing of wort & beer

Page 31: Flow and Filtration: The Physics of Brewing

Brewing Shear Rates?

Turbulent or laminar?

NRE =V L/

= density, V = velocity L= diameter = viscosity

Average shear rate in turbulence

= [(/)3 / ]1/4

= average power dissipation per unit mass

Page 32: Flow and Filtration: The Physics of Brewing

Brewing Shear Rates?

Turbulent or laminar? Turbulent flow cascades to

laminar flow at small distance scales

Page 33: Flow and Filtration: The Physics of Brewing

Brewing Shear Rates

Defined by Reynolds number of 2000-3000

Note Re= DV/ Also note V is the average pipe velocity

Generally get turbulent flow

Page 34: Flow and Filtration: The Physics of Brewing

Brewing Shear Rates

Shear in Kettle 8600 s-1

– (Speers et al. 2002) Shear in Fermenter 20-60 s-1

(Speers & Ritcey, 1995) Shear in Yeast brink tank <15 s-1

(Kawamura et al. 1999) Average shear rate in pipe flow

– High 915 s-1

– Mean 500 s -1

– Low 175 s -1

Page 35: Flow and Filtration: The Physics of Brewing

Membrane filtration

Theory developed in 30’sBased on capillary plugging due to gradual

restriction in diameter

Surdarmana et al. 1996 Tech Quarterly

t/V = t/Vmax + 1/Qinit

Vmax maximum filtrate volume

Qinit intial flow rate

Page 36: Flow and Filtration: The Physics of Brewing

Membrane filtration

Theory developed in 30’sBased on capillary plugging due to gradual

restriction in diameter

Surdarmana et al. 1996 Tech Quarterly

t/V = t/Vmax + 1/Qinit

Vmax maximum filtrate volume

Qinit intial flow rate

Page 37: Flow and Filtration: The Physics of Brewing

Filtration Filtration ApparatusApparatus

Page 38: Flow and Filtration: The Physics of Brewing

Example Sudarmana TransformExample Sudarmana Transform

Medium viscosity arabinoxlyan in model beer

Page 39: Flow and Filtration: The Physics of Brewing

Relation of Intrinsic Viscosity Relation of Intrinsic Viscosity and Filtrationand Filtration

1/Vmax [] for membrane test

Filterability negatively correlated with [] for commercial (DE) filtration

Membrane filtration more suited for detection of -glucan problems

Page 40: Flow and Filtration: The Physics of Brewing

ConclusionsConclusions

Ethanol, pH and maltose effect viscosityShear strong effect on filtration

Shear within brewery typically turbulent average 40-1250 s-1

Sudarmana fit ‘works’ (Tech. Quart 33:63)

Page 41: Flow and Filtration: The Physics of Brewing

Students !NSERC

Labatt Brewing R&D

NSDAMWestcan MaltingCanada MaltingPfeuffer GmbH and Profamo Inc

(Viscomat automated capillary rheometer)

Acknowledgments