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Halton, P. and Blair, G. W. S. 1936. A study of some physical properties
of flour doughs in relation to their breadmaking qualities. Journal of
Physical Chemistry (1952). 40 (5), pp. 561-580.
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A STUDY OF SOME PHYSICAL PROPERTIES OF FLOUR DOUGHS IN RELATION TO THEIR
BREAD-MAKING
QUALITIES
P. HALTON1
ResearchAssociation ofBritish Flour Millers,St. Albans, England
AND
G. W. SCOTT BLAIR
Departmentof Physics, RothamstedExperimental Station, Harpenden, England
ReceivedAprilS, 1935
INTRODUCTION
Attempts tomeasure the physical propertiesofflourdoughswere made by Kosutány (4) as early as 1907. This author pulled out a cylinder
of flour dough at a constant rate, and measured tjhe stress build-up.2
Although not clearly distinguishingbetween viscous and elasticproperties, the author’sinterpretation ofhis data points clearly to a number of the conclusions reached inthe presentwork.
It iscurious that this valuable work,in which Kosutánycame so near
to separating and measuring specificphysicalproperties, should havelain fallow for so many years. From 1907 to 1932 work on the physical
properties of flour doughswas confined almost entirely to the production
ofinstrumentsmeasuringacomplexmixtureof properties,which,although in some cases ofrealvalue in the bread-making industry, threwlittle or
no light on the physical nature of the problem. In 1932-33 threepapers were published by Schofield and Scott Blair (8), in which certain of the physical properties ofdoughswere separated andindependentlymeasured. Forthesakeofconvenience these paperswillbereferredtoas
I,
II,
andIII.In paper I it was emphasized that flourdough belongs to a group of
materialsinwhicha highdegreeofplasticityiscombinedwithconsiderable elasticity. When under stress the relative amounts of plastic
(non-1
By mutual agreement the authors’ names are in alphabetical order and no
seniorityisimplied.
8
Terzaghi(9)developsvery similarideas. The constant whichhecalls “degree of elasticity” (p. 79) is closely connected with relaxation time (vide infra). Terzaghi’sworkrefers to soils and clays,but their behavior isin some ways
strik-ingly similartothatofflourdoughs. Seealsoarecentpaper by . P.Wolarowitsch andK. I. Samarina (10) dealingwith some physical properties of flour doughs.
561
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recoverable) and elastic (recoverable) deformation depend on the time
ofdurationof thestress. Anextended significancewas givento Maxwell’s
relaxation time,sothattheequation
tr —
ii/n
in which tr = relaxation time, = viscosity, and n = shear (rigidity)
modulus,3 could be applied to a material such as flour dough, in which
neither nor n isaconstant.
It was foundthat and tr decreasewith increasing stress and increase with increasing deformation. Fall in viscosity with increasing stress is a phenomenonwell knowninmany colloidalsystems, andhasbeencalled “structuralviscosity” (6). Increaseinviscositywithincreasingstrainis
a common characteristic of metals, andis called“work-hardening.” In paper
II,
thesetwo propertieswere morefully
studiedbyobservingthe rate of shear of cylinders of dough hung vertically, and allowed to elongateunder theactionofgravity (themethodof rheograms).
TheMaxwell equationcouldonlybetestedsatisfactorily after the most suitable valueofmodulusto use in calculatingviscositiesfrom relaxation times was known. Experiments to decide this point were described in paper
III,
and agreement was found to be as satisfactory as could be expected whenthe best value for the modulus was used. These experi-ments also made it clear that doughshows two other properties charac-teristicof metals, namely, elastic hysteresis and elastic after-effect.The formercauses the
rigidity
modulusto fallslowlyas stress israised, andalsoas stressislowered,butatthe point at which the sign of dS/d< changes,4themodulus increases abruptly. The latter means that elastic deformations are not recoveredinstantly, so thatunlesstimeisgivenfor slow recovery to take place, certain deformations will be regarded aspermanent which are in reality recoverable. This would lead to
con-siderable errors in determining viscosity and modulus (see experimental section). In viewofthe partialunderstanding which this treatment had already given, it seemed advisableto investigate furtherthe relationship between thesefundamental physicalproperties, and thosequalities of the dough which are of importancein the bread-making industry. For this purposethePhysicsDepartmentof theRothamsted Experimental Station and the ResearchAssociationofBritishFlour Millers decidedtocooperate in thefurtherstudyofthe problem.
8Note that forflourdoughs, Poisson’sratiobeing
0.5,we can assume therigidity modulus tobeequal toone-thirdof Young’s modulus. The shearingstresslikewise
isone-thirdof the loadingstress. Inthe present paper, the term“rigiditymodulus”
isoftenabbreviated to “modulus,”sinceno other modulus isdiscussed.
4Where£is
The general principles havenow beenelucidated, and although much detailrequires yet to be filled in, thepresent paper gives adescriptionof the conclusions to date.
EXPERIMENTAL
By far the most serious difficulties that have been encountered were
those associated with the reproducibility of measurements on different testpiecesfromthesame dough. Inpapers
I,
II,
andIII accurate replica-tion on different test pieces was not attempted, and although thephe-nomena described could be repeatedly observed, it was realized that no
fully
satisfactory technique existed for such replication. In the courseofthepresentinvestigation much time hasbeen spentindeveloping such
a technique, andthe methodfinallyadoptedhasprovedon thewholetobe satisfactory.
TABLE 1
Theeffectofmixingon theviscosityandmodulusofthe dough
TIME OF MIXING TIME OFRESTING
AFTER MIXING VISCOSITY* MODULUS*
minutes minutes
3 0 6.38 X 10s 4.29 X 10*
30 4.92 X 106 3.94 X 10* 60 4.04 X 10« 3.73 X 10*
12 0 2.92 X 106 3.02 X 10*
30 3.55 X 10= 3.41 X 10*
60 3.51 X 10« 3.50 X 10*
*All dataforviscosities (ij) and moduli
(re)in thispaperare givenino.o.s. units, but it mustbebornein mindthat theyrefer only to arbitraryfixed conditions of
stressandstrain.
It isnecessarytomakeashomogeneous a doughas possible, andit has beenfoundthatmachinemixing oftheflourandwatergivesthemost satis-factory results. The longerthe time of mixing, the more homogeneous
is the finished dough, but excessive mixinghas a very marked effect on
thedough’s physicalproperties.
Fromthe dataintable1itcan beseen thatexcessivemixing considerably lowers the viscosity and modulus of the dough, but that theseincrease againon resting. Suchtreatment,however,permanentlylowers the tensile strength ofthe dough.
It willbeshownlaterthat thegeneraltendencyon aginga doughisfor the viscosityandmodulusboth to fall. It isonly afterprolongedmixing that the opposite effect more than compensatesfor this fall, producing a
min-HALTON AND G. W. SCOTT BLAIR
utes mixing, the effect ofstandingisthe opposite ofthat producedby12 minutes mixing.
The sample of doughistransferredfrom the mixerto a “gun,” consist-ing of a hollow metal cylinder, 5 cm. long and2.5 cm. in diameter, fitted with a plunger. To the bottom of the cylinderis fitted a solidpiece of metaldrilledwitha hole3.5cm. long and0.5cm. indiameter. Thisfirst gun,into whichthe doughcan beplacedbymeans ofaspatula,thus
avoid-ing handling it, istoo big to fit conveniently on to the apparatus, and
therefore the extended dough cylinderis squeezed straight into a second smaller gun 15 cm. long and 1 cm. in diameter, "which is fitted with an
end piece similarto that ofthe firstgun. The dough isforcedfrom this secondgunstraighton to thesurfaceofa bathofmercury.
Statisticalanalysis5showedthattherewas no greatererror in comparing
testpiecesfrom differentdoughsthanincomparing piecesfromthesame
dough. It thusappearedthatthe chiefsource oferror lay in the method
of preparationofthe testpieces. It was foundthat theforceapplied to the guns very largely affected the physical properties of the prepared doughcylinder. A system ofpulleys and weightswas thereforeused for manipulation oftheguns, and, provided that theweightswere small, we
found very little alteration ofthe properties of the doughs. The impor-tanceofa carefullystandardizeduse ofthese guns cannotbetoo strongly emphasized.
Duringextrusionthe doughcylinderswells,thisswellingbeingingeneral greaterforgoodthanforpoor qualityflours. The exact connection, how-ever,isnot clearlyunderstood.
The dough cylinders have been examined by the twogeneral methods described in papers I,
II,
andIII,
namely (a) rheograms, and (b) the mercury troughextensimeter, but the technique ofthelatter methodhas beenextended and developed.(a) The rheogram method. This method has been further developed and has now reached a stage at which theresults are excellently
repro-ducible, and, although not free from errors, it provides the most satis-factoryway at present availableforseparatingtheeffectsof work-harden-ing (rise in viscosity with rising strain) and structural viscosity (fall in viscositywithrisingstress).
In mostdoughs thesetwo propertiesappear,undertheconditionsofthe rheogram experiments, approximately to cancel out. Without commit-ting ourselvesto any assessment of the degreeof accuracy of individual samples, an examination ofthe data obtainedfrom a study of some sixty
doughs made from a series of twenty different flours, leads to the
con-clusion that certain flours tend to show higher or lowerdegrees of
work-6Our best thanksare due to Mr. F.Yates of theRothamsted Experimental
hardening than others, and that this property generally persists when differentamounts ofwaterand timesofagingare used. Suchdifferences do not, however, correlate directly with flour quality, and we conclude that weakness in a flourdue to an unsuitable degree of work-hardening istheexceptionrather than therule.
Certain practical difficulties are encountered in using the rheogram techniquein thecase ofstickydoughs, anddoughsofpoor tensilestrength.
Moreover, both viscosity and rigidity modulus can be calculated from
a single test on the extensimeter (vide infra); therefore the rheogram methodwas not employed further in this investigation.
(b) The extensimeter. This instrument, which is an improved model of the extensimeter described in papers I and
III,
is shown diagram-matically infigure 1.AdoughcylinderA, about10cm. longby0.7cm. indiameter, made as
described above,isfloatedon a mercury bath. Theendsof this cylinder
are connectedbymeans ofcork“chairs”and cottonthreadsto two small scales B, which are observed through low-power microscopes, C. The
IT
-<5> r
Fig. 1. The mercury bathextensimeter
smallest divisions on the scales are 0.013 cm. in length, and readings to
one-tenthofthiscan beestimatedwithafairdegreeof accuracy. Toone scaleis fastenedasteelspringD, the otherendofwhichissecurelyattached totheframework of the apparatus;theotherscale isconnectedby cotton to a smallwinch (E), which can bewound either byhand or bya small motor.
During experiments the dough is protected by a cover, the felt lining
ofwhichisdamped toprovideahumidatmosphereto prevent drying out
of the dough surface.
When thewinch (E)iswoundup,thedough andscalesare moved to the
left, and this extends the spring D. The dough is therefore subjected to astress,thevalueof whichisproportional tothe extensionofthe spring, and inversely proportional to the cross section of the dough cylinder. The spring iscalibrated by noting theextensioncausedbyhangingweights ofvarioussizesfrom it when placedina vertical position. Thediameter
W.
of shearingstresstovelocity gradient(i.e., rate ofchangeof non-recoverable strain),we can either fix therateof change.ofstrainandmeasure thestress, or fix the stress and measure the rate of change of strain. The latter has in practice been found to be byfar the simpler method to use, and has been the basis for most of the experiments described in this paper. Before doing an experiment, the necessary deflection ofthe spring to givethe desiredstress isfirstcalculatedfroma knowledge ofthe constant for the spring and the cross section of the dough cylinder. The winch
is then rapidly wound up until the shift in the scale attached to the spring corresponds to this required stress. For ordinary purposes we
worked with an arbitrary tensile stress of 1500 dynes per square centi-meter (shearing stress 500 dynes per square centimeter).
Understressthe doughcylinderextends, andforfiveminutesthis exten-sionistakenupby slowly winding the winchso that thedeflection of the
right-handscaleiskeptconstant. Bythismeans thestressiskeptalmost constant, the riseinstresswithslightthinning ofthedough cylinder not being generally great enough to introduce any serious error, especially when relative, rather than absolute, viscosities of doughs are required. Bymeasuring the extensionatminute intervals it wouldappearthatthe
mean viscosity for each minute could be determined, and from this an
indication of the amount of work-hardening (i.e., change in viscosity withstrain) assessed. Thisisnot,however,practicable,sinceelastic after-effect is takingplace during thewhole process (seeintroduction).
The stress is released at the end of the five minutes and the dough allowed to relaxuntil no furtherchange in lengthtakes place (this takes about three to five minutes). The difference inthe length of the dough cylinder before any stress is applied to it and at the end of relaxation givesa measure of the non-recoverablestrain causedbythe stressacting for five minutes.6 From this a mean viscosity can be determined by dividing the non-recoverable strain per unit time into the stress. This is free from errors due to elasticafter-effect.
The amountof recoverableor elasticdeformationis obtained by noting the changein length of the dough cylinderbetweenthe time of releasing the stress and the end of relaxation. The value of the shear modulus whichisgivenbythe ratio
change in shearingstress changeinrecoverablestrain
8Strictlyspeaking, the strains shouldbecalculated from log,i/i0,asin the rheo-gram calculation, but for the small strains used the method described here is
is a mean value fora changeinstress from 500 to 0 dynes,7the modulus fallingprogressivelyduring the lowering ofthestressduetoelastic hystere-sis (see introduction).
Effectof temperature
Experiments have shown that the viscosity of a typical dough falls by about 10per cent perdegree Centigrade rise in temperature and the modulus by about5per cent. Thismakesit desirableto exercisecareful control over the temperature. The extensimeter is not easily thermo-stated, and, moreover, the processes of dough preparation should also becarried out ataconstant temperature. It would thusbebestto carry outallmeasurementsina constant temperatureroom.8
Although a suitable constant temperature room has now been built, thefactthat itwas not availablefor the earlierwork meantthatwe could
onlymakedirectcomparison between resultsobtainedover periodsduring
which laboratory temperature didnot fluctuate very widely,andin
conse-quencewe havehadtoforegomakingas fulluse ofour dataas we should otherwise havebeenable to do. Further, since the viscosity falls about twice as fast (with rise in temperature) as does themodulus, it is clear thatthe all-important9 viscosity modulus ratio (relaxation time)ishigher, the lower the temperature. Thissupportsthe viewheld bysome bakers thatdough shouldbefermented andput intotheoven ataslowa
tempera-ture as isconsistent withthe satisfactory working of theyeast.
The temperaturecoefficients alsovary withthe age ofthe dough, and it isthusclearthatthetemperature at whichit is agedplaysan important
part in defining its physical properties at any given time, and hence in determining thequality of theresulting bread. Further experiments are
needed to explorethis field.
WATER ABSORPTION
When determining the valueof a flour inthe bakehouse the first step isto turn it intodoughby mixingwithwaterandother ingredients. The bakerdoesnotuse aconstantratioofflourto waterfor allsamples, other-wisesome of his doughswouldbetoo softandsticky, whileotherswould betoo tough, extremesofcondition whichnot onlycause serious difficul-tiesin the handlingofthedoughs,butwhichdonot result inbread repre-sentativeof the valueofthe flour. In view of this, the bakervaries the
7The stress isnever allowed to fall quite to
zero, owing to the necessity for keeping the cotton taut, but thefinalstressis very small, and isthesame in all
experiments.
8Caremust beexercisedto ensure
properventilationand soprevent the danger of mercury poisoning(see Stock (9)).
amount of waterheadds toeachfloursothathis doughsare easytohandle and in general bake into as good quality bread as his various flours are
capable of making.
Weare therefore facedwith theproblemof determiningthe significance ofthis optimum amount ofwater, or “water absorption” as it iscalledin the bakehouse, and alsowith the necessity of determining some method
wherebyit couldbefixed. In assessingwater absorptionthebakerrelies
on hissense of touch,and one of the impressionswhichhelpsinhis judg-ment of correct absorption is the extent to which the dough sticks to hishands.10
It appeared to us that thebakermade up his doughsso thatthe sticki-ness was justshortof beinga trouble,andon thisassumptionwe basedour
TABLE 2
Effectofwater contenton viscosityandmodulusofflourdoughs
WATER CONTENT
— 1gal.
-1gal. Normal +igal. + 1gal.
No.1Manitoba:
10.0 7.5 5.8 4.8 4.1
Modulus (X 104)... 4.1 3.6 3.1 2.6 2.1 BarussoPlate:
15.0 8.3 5.7 4.4 3.5
Modulus (X104) ...",... 4.6 4.0 3.4 2.8 2.2
Australian:
7.5 4.8 3.5 2.8 2.3
5.5 4.6 3.6 2.6 1.6
Normal absorptions: No. 1 Manitoba, 15.6gals, persack; Barusso Plate, 15.3
gals, persack; Australian, 14.0gals, per sack.
first attempt to connect water absorption with a physical property, so
that by themeasurementof thelatter we couldfix the former.
Measurements of stickinesswere madebymeasuringtheforcerequired
to overcome the adhesion of a metal weight to the surface of a dough.
Themethodusedwas a modification of those proposedby Kachinski (3) and others (1, 2, 5, 7) formeasuringthe stickinessofsoils. It has, how-ever,notbeenpossible to make the measurementsreproducibleenough to
use as a means ofassessingwater absorption.
The connection between water content andtwo other physical proper-ties, namely, viscosity and rigidity modulus,was next investigated.
For this a series of flours was obtained, and from each flour several doughs were made containing different amounts of water. The data
10For experiments on the psychological
obtained by measuring the viscosities and moduli of the doughs made from three of these flours, a No. 1 Manitoba, a Barusso Plate, and an
Australianare givenin table 2.
Each flour was examined at the absorption chosen in the bakehouse whichwe havecalled “normal,”andatfour other watercontents
±§
gal-lonand ±1 gallon per 280-lb. sackofflour.11 Each doughwas fermented forfourhours, atthe end ofwhichtimesampleswere taken for viscosityand modulus measurements. In figure 2 curves nre drawn showing the relationship betweenthese two properties at each of the five water
con-tentsforeachof thethree flours.
An examination ofthesecurves showsthat witheachflourboth viscosity and modulus fell with increasing water content and vice versa. The
relative effects on these two properties were not the same, and differed from flour to flour. Theeffectsofa change of2 gallonsin water content
on viscosityandmodulusare givenin table3,thefiguresrepresentingthe difference in values for the driest and wettest doughs expressed as a
percentage of theaverage.
These figures show that the effect bothon viscosityand modulus was
least in thecase ofthe Manitoba, whichisinkeepingwiththeexperience
of the bakerthatthis typeofflourhasamuch greater tolerance to changing
water contentthan anyother. ThePlateflourdifferedfromtheManitoba chiefly on account of the much greater effect of changing water content
on viscosity, while in thecase of theAustralianboth viscosityand modulus, and particularlythe latter, were more markedlyaffectedthan in thecase
of the Manitoba. It is probable that a big upward change in viscosity with decreasing water content is ofmuch less account in the bakehouse thanabigincreaseinmodulus,asthelatter wouldmakethedoughs“dead” and lifeless (seelater).
Thethree doughs ofparticular interestare the “normal”doughs, and it
will benoticedthat these doughs differed veryconsiderably in viscosity, butonly to a small extent in modulus. It is probablethat the baker is unconsciously more influenced in choosing his water absorption by the moduli of his doughs than by their viscosities, and in consequence we
may be able to use measurements of the former property as a means of determining correct water absorption. This point,however, needsmuch furtherinvestigationbefore it can besettled.
GENERAL CONSIDERATIONS
Although it isquitepossible to makea doughfrom any flourwhatsoever
so thatit shall haveanydesiredviscosityor modulus (withinwidelimits), byusing the appropriate amount of water, it iswell known that a poor flour cannotby anysuchmeans bemade to give a dough ofsatisfactory
plastic and elastic properties. The reason for this is clearly seen from
table 3. It ishere apparentthat if a “strong” flour dough (Manitoba) iscomparedwitha“weak” (Australian) at thesame viscosity,the modulus of the strongflourismuchlowerthanthatof the weak. If the comparison ismadeatthesame modulus value,thestrong flourhasby farthe greater viscosity. The intermediate Plate flour fallsbetweenthe two extremes. This suggests that the relaxation time
( / ,
see paperI)
is of primary importance. This suggestion has been amply verified. It is, of course, clearthatwe cannot regardrelaxationtimeas a constant ofa dough,since it varieswithboth stressanddeformation,but ithas becomeincreasingly evident during the course ofthisw'orkthatif doughs are comparedundersimilar conditionsofstressandstrain, andiftheseconditions approximate as closelyas possibleto those obtained in the commercial dough, a
com-parison ofrelaxation times (“viscosity^-modulusratios”) gives a primary measure of the differences in flour quality (although as is shown later, many other factors have to be taken into consideration as well). In
of aplastic filmby which theelastic elements are connected. It isquite possible that the elements are capable of complete elastic recovery, but there is at present no criterion for testing this. The time of relaxation isa characteristicoftheconnectedstructure as awhole andits valueisas
much determined by the elasticity of the elements as by the viscosity
associated with their plastic
junctions....
In relating these deductions to theknown structure ofthe dough, one may safelyidentifythe elastic elementswiththe protein partoftheflour.”When a doughrises under the action of yeast, it is advantageous for
ashighapercentageaspossibleof the deformation to beelastic (recover-able). Non-recoverabledeformationsimplyflow ofthecell-walls, leading to theirrupture, and collapse ofthe dough dueto inabilityforit to hold itsshape,resulting inaloaf havinglarge andbadly shaped holes,a poor
volume, and badover-allshape. Bigelastic extensionresulting from low modulus tendsto producea bigrisewhenthe dough isfirstplacedin the oven, and hencebig loafvolume.
TABLE 3
Effectofchangein watercontent
MANITOBA PLATE AUSTRALIAN
83 124 106
64 70 105
The property by which an extended dough on release recovers a high
percentage ofitsextension, is calledby bakers“spring.” It isclearthat the extent to which thedough fails to return to its original length after suchan extensionwilldependon howfartheelastic elements have slipped pastone another. Thisdependson theamount offrictionbetween them, which, as we have seen, corresponds to the viscosity of the dough (as normallymeasured). The higher the viscosity, thelessthe slippage. But
the amountof slippage dependsnot onlyon the viscosity,butalsoon the internal stress set up in the elastic elements. If we think of these as
coiled springs, it is easy to see that the
“lighter”
the springs (i.e., thelowertheirmoduli), thelessstresswillbebuiltupforany givenextension, andhencethelesswillbethe slippageforagivenviscosity. Thusadough
showing good“spring” willhavearelatively high viscosityandlow modu-lus, whereasa doughhavingbadspringwillhavearelatively low viscosity
and high modulus.
It isnow clearwhy the bakerattachesso much importance to “spring”
in his doughs. Good spring means a high viscosity modulus ratio (big
It ispertinent toenquireas tothe significance of the extent of the varia-tion of viscosity and modulus with stress, strain, and stress history for differentflours. Experiment has shownthat even widely different flours
show a very similar degree of elastic hysteresis, and no marked differ-ences in their elastic after-effect behavior. As explained in paper III elasticafter-effect is important in that unlessattention is paid to elimi-nate its effect, it is liable to interfere seriously with the correct deter-mination ofviscosity.
TENSILE STRENGTH
Inthe bakehouse occasional doughsare encounteredwhich“tear” badly during thebaker’smanipulationandduringtherisingofthedoughs under the pressure of the gas generated inside them. Such doughs are said to be “short” and bakeinto unsatisfactorybread. Owingto thetearing, excessive gas leakage occurs which results in poor loafvolume, and the actual tearinggives the outside of theloafa ragged appearance. In addi-tion,the insides ofsuchloaves easily crumble whenpressedwiththe fingers. It thus appears that for such flours tensile strength is also a factor of
major importance. This propertyis now beinginvestigated.
AGING AND FERMENTATION OF DOUGHS
In the process of bread making the doughs are kept for some hours before bakinginto bread. Not only do their handlingproperties depend on thelengthofthisperiod,butthetypeofbreadalsoshowsconsiderable variation.
In order to determine the changeswith age in the physical properties of such doughs, and to findwhatconnections exist betweenthese changes and bakehouse behavior, a series of flourswas obtained whichhadbeen previously examined by thebaker. The doughswere made upwith the same ingredients as had been used in the bakehouse and were kept at 27°C., samplesbeingtaken at hourly intervals for viscosity andmodulus measurements,whichwere madeat room temperature.
The data obtained on four ofthese flours, a No. 1 Manitoba, a No. 3
Manitoba, a Barusso Plate, anda SouthAustralian, are givenin table 4,
andcurves drawnfromthesedataare giveninfigures3, 4, and5.
It will be noticed that no data are given for freshly made doughs. This is because of the difficulty of obtaining reproduciblemeasurements
on them. Rapid changes take place during this initial period and are
probably connected with the rate of absorption of water by the flour. Afterone-half toone hourtheseeffects disappear, and thephysical proper-tiesthenchangeina normalandregularfashion.
In the case ofthe above four flours,the changesin physical properties
TABLE4
Effect of fermentationon viscosity,modulus, andtheij/raratio
FLOUR TIMEIN HOURS viscosity X10e MODULUSX10* / RATIO
No. I Manitoba 1.23 3.97 3.16 126
2.12 3.82 3.02 126
3.05 3.79 3.21 118
4.93 3.32 2.99 111
6.00 3.27 3.21 102
6.93 3.25 3.09 105
No.3Manitoba 1.10 3.25 2.61 124
2.03 2.84 2.37 120
3.08 2.68 2.53 105
5.02 1.88 2.18 86
6.07 2.04 2.18 93
7.03 1.83 2.03 90
BarussoPlate 1.18 3.33 3.53 94
2.03 3.46 3.47 100
3.13 2.83 3.23 87
5.02 2.56 3.08 83
6.00 2.45 2.76 89
7.07 2.07 2.39 89
Australian 1.07 2.52 3.21 78
2.05 2.18 2.92 74
3.00 1.97 2.82 70
5.00 1.39 2.32 60
6.13 1.00 2.06 48
7.00 0.76 1.58 48
A
3
2
/
Fig.3. The effectofageofthe doughon theviscosity
-BLAIR
The data given in table 5 have been obtained from the curves (see
of each flour the viscosity fellmore rapidly than the modulus, resulting
in theratioofthesetwo propertiesalsofallingwithincreasingtime. In attempting to correlate thesechanges with the changes which took placeinthéhandling properties of the doughsin thebakehouse, we were
at once confrontedwith thefact that the baker reportedthat the No. 1
Manitobadoughimproved in bodyand springas fermentationprogressed, that the Plate remained unchanged, and that the No. 3 Manitoba and Australian doughs became softerwithincreasingtime.
TABLE 5
Changein physical properties with time
FLOUR
VISCOSITYAT
ACTUAL
PERCENT-1sthr. 7thhr. DECREASE
4.05 X 10*
3.01 X 10*
3.17 X 10*
1.83 X 10*
0.88 X 10*
1.18 X 10* 22 39 3.37 X 10® 2.12 X 106 1.25 X 106 37
2.84 X 10* 0.77 X 10® 2.07 X 10* 70
FLOUR
MODULUS AT
ACTUAL
PERCENT-let hr. 7thhr. DECREASE
3.19 X 10*
2.66 X 101
3.05 X 104
2.04 X 104
0.14 X 104
0.62 X 104
4 23 3.62 X 10*
3.23X 104
2.55 X 104
1.87X 104
1.07 X 104
1.36 X 104
30
Australian... 42
FLOUR
VISCOSITY-MODULUS RATIOAT
ACTUAL DECREASE
PERCENT-DECREASE
1sthr. 7thhr.
No.1Manitoba... 127 104 23 18
No.3Manitoba... 123 89 31 28
Plate... 94 87 7 7
Australian... 79 48 31 39
This improvement or toughening is associated by bakers with good quality. Severalflours which have shown this response to fermentation in the bakehouse have been examined in the laboratory, and in every
case both viscosityandmodulushave beenfound to decreasewith aging; in fact, no flour has yet been examined which showed a rise in either property during fermentation. It hasbeennoticed, however, that those flours which have been reported as toughening in the bakehouse, were
those which showed the smallest fall-off in physical properties when examinedinthelaboratory.
G. SCOTT BLAIR
baker, dough does toughen,12 but this happens with all flours, and in addition the effect disappears on resting. The toughening the baker speaksofinconnectionwithgoodqualityfloursonly,isconsideredby him to be dueto theaction of fermentation.
Careful tests have now been carried out in the bakehouse in which freshly made doughswere comparedwith fermented doughs made from
the same Manitoba flour, which the baker considered had toughened. When the doughswere mouldedsideby side, one ineach hand, andthen allowed a few minutes to rest, it was reported by the baker that when tested by “feel” the older dough was very slightly the softer. It thus appearsthat bakers havebeenmistakenin theirimpressions thatcertain doughstoughenduring fermentation.
When a series of replicate doughs is made from the same flour and allowed to fermentfor varyingtimes,it isfoundthat withincreasingtime the volume and crumb quality of the bread atfirstimproves, and then fallsoff. This improvementis consideredbythebakerto bedueto what is calledthe“ripening” ofthedough, theactualtimeto obtain maximum improvementvaryingwiththe amount of yeast, andwiththetypeofflour used. “Strong” flours like Manitoba require much longer fermentation for optimum results than “weak” flours like English or Australian. In-creasing the amountof yeastin thedoughdecreasesthetimeofripening. Since viscosity, modulus, and relaxation time all fall consistently as
the dough ages,it isdifficult to explain the initial improvement inbread quality withtime offermentation in terms ofthe changestakingplace in thesephysical properties.
Thedecreaseinrigiditymoduluswithtimeisin itselfdesirable,butsince it is the ratio of viscosity to modulus which is of primary importance in determining flour quality, the general result ivould be expected to be a fall-off, and not an improvement in bread quality. Also, if a fall in
both of these physical properties were desirable, then a similar
improve-ment inbread qualityto thatwhichtakes place withfermentationcould be brought about by using more water in the dough. This is not so, andeven whenthebaker adds too much water to theflour,hestillgetsan
improvement in breadquality with increasing fermentation time. Although this improvement or “dough ripening” may be partly due to changestakingplacein some physicalproperty other than viscosityor
modulus,itispossible to accountforit on purelymechanical lines. Before agoodloaf can bemade, the necessary cell structure hasto bebuilt upin the dough, andthiscellstructure mustbedeterminedbythe number and distribution of the yeast cells. Now normal bakehouse mixing is
com-parativelycrude, andinconsequencethisdistributionisprobably anything
12See
but uniform. Owing to the activity of the yeast, however, the dough swells,andthis probably helpsto spread theyeast cells. Inaddition, at variousstagesoffermentation, the bakerknocksthegasout of thedough andmoulds it up, thusagain helping towardsmore uniformdistribution.
During fermentation theyeast cells multiply, and thus as time goes on
the gas-producing centers increase innumber.
If the abovepictureiscorrect, andit isthe building upofthenecessary cellstructure whichdetermines how muchfermentationisrequired for any flour to give itsbest bread, then it shouldbe possible to cut down this time by theuse ofmore yeast and/or thorough mixing. That thisisso
is well known, and it has moreover been verified experimentally by us.
During fermentationwe therefore havetwo processes goingon sideby side, an improvement due to the multiplication and better distribution oftheyeast, andafalling-off in bread-makingqualitydueto thedecrease in value ofviscosityand relaxation time. The improvement dueto the yeast appearsto becomparativelyindependent ofthe physicalproperties of the dough. With a good quality flour suchas Manitoba, thefall-off in physicalpropertiesissoslightthatgood bread isproducedover alarge
range oftime, whileon theotherhandthefall-offin physical propertiesis so greatwitha poorqualityflour like English, thatthe best breadis pro-duced early, and isfollowed byarapidfall-offin quality.
Returning to the data in table5,the No. 1 Manitobahadthehighest
initial viscosity and showed the smallest decrease in this property with time. Thisflouralsohadthehighestviscosity-modulus ratio either after
one or after seven hours. Thisisall inkeeping withthe generalquality of theflourasshowninthe bakehouse, whereit behavedasby far thebest ofthe four.
TheNo.3Manitoba,however, hadamuchlower
initial
viscosityandamuch greater fall in this property with time. This low viscosity was
accompaniedbyalowmodulus,sothattheinitialvalueof theratioofthese two was high,althoughit fellconsiderablywithtime. This flourwas not
up to standard foritsgrade, andalthoughit produced bread of excellent volume (low modulus) the best loafwas “thrown” relatively early, and
thelaterloaveshadmuch poorer“crumbs,”owingto thefallin viscosity. The Plate flourhad a much higher viscosity than the No.3 Manitoba throughout theseven hours, butthiswas accompaniedby a rather high
modulus. The ratio was lowerthanthat for the No. 3 Manitoba at the beginning offermentation, but decreasedvery little, so that at the later times the two flours approached one anotherin this respect. ThePlate
the best bread would probably have had greater volume, it would have beenmade earlier, and mighthavehada poorer crumb structure.
TheAustralian flourwithitslowinitial viscosity, lowviscosity-modulus ratio, and considerable fall in both with time, would be expected to be much the poorest flour of the four, and this was found to be so in the
bakehouse.
So far we have only dealt withdoughs containing yeast. This ingre-dient is necessary to produce the gas which builds up dough structure, buthasit any other function inbread-making?
Testshavebeen carried out in which the physicalproperties of doughs withandwithoutyeast havebeencompared. The general results ofthese tests showthat in small amounts such as are usedincommercial bread-making, the effect of the yeaston theviscosityandmodulus of the dough isprobably notgreat enough to beofimportance inthe bakehouse. Very large amounts of yeast do affect viscosity, forexample, in one case 8per
cent yeast loweredthe viscosity from3.6 X 106to 2.9 X 106. The effect
on themodulus and on the rate of change of either propertywith age of the doughwas, however, insignificant.
CONCLUSIONS
1. Viscosity and rigidity modulus appear to be of major importance. The viscosity must be high enough to prevent undesirable flowing-out ofthe dough, but on the otherhand themodulus must below, to allow bigelastic expansion underthe relatively low pressure ofgasinside a fer-menting dough. The relaxation time (which is the ratio of these two properties) isperhaps themostimportantsingle criterion ofquality.
2. The water content ofa dough determinesthe magnitude ofits
vis-cosity and modulus, and it is desirable thatvariations in water content should haveassmallan effecton thesepropertiesaspossible,thus helping
towards making the flour more fool-proof in the bakehouse. Whether water absorption is important in other ways, apart from financial
con-siderationsto thebaker, isnot known.
3. Thedegreeto which viscosityand moduluschange duringthe aging of the dough is of the utmost importance. The fall in viscosity with time is probably a major factor in determining the fermentation toler-ance of a flour, and not only is the absolute rate offall of this property important,butequallysoisits relativerate comparedwiththerateoffall of modulus,sincethisdeterminesthefallin relaxation time.
4. Tensilestrengthisamajor factor in determiningtheextensibilityand
5. Stickinessisimportant in affectingthe dough’s handling properties; the dough mustnot betoo sticky to workover thatrangeof moisturebest suited to its other properties, nor should excessive stickiness develop during fermentation.
6. It is realized that such properties as work-hardening, structural
viscosity, elastic hysteresis, and elastic after-effect must playtheirparts in determining the behavior of dough in the bakehouse, but although their significance is not yet fully understood, it iscertainthat they are
only of secondary importance in determining the relative values of dif-ferent flour samplesexcept perhaps in certain abnormal cases.
7. It is considered that measurements of the physical properties of doughs,as faraspossibleinabsoluteunitsandunder standardreproducible conditions, should lead to a far better appreciation of flour qualitythan
any number of empirical tests, and should afford a sound basis for the control ofqualityin flour.
SUMMARY
Methods described in earlier papers for measuring the viscosity and rigiditymodulus of flourdoughs have been extended anddeveloped.
The physical properties of dough are markedly affected by excessive handling, either during thepreparation of the dough itselfor during the
preparation of the test piece. The methods used have therefore to be carefully controlled.
Viscosity and modulus measured under standard conditions of stress andstrainbothdecreasewithincreasingwater content or withincreasing age ofthe dough.
Goodbread-makingqualityisassociatedwitha relatively high viscosity
andlow modulus; the relaxation time,i.e., viscosity-modulusratio, there-fore appearstobethechief singlecriterionofquality.
Yeast in small amounts has little effect on viscosity or modulus, and
its importance in bread-making appears to be entirely due to its gas-producing activities.
Tensile strength is a major factor in determiningthe extensibility and gas-holdingproperties ofadough,butworkon this propertyisstillattoo earlya stage to bediscussed.
Stickiness is an independent property whichcan be roughlymeasured. Its principal importance lies in its effect on the handling properties of the dough.
Our best thanksare due to Dr. E. A. Fisher, Directorof the Research Association of British Flour Millers, and to Dr. R. K. Schofield of the PhysicsDepartment, Rothamsted Experimental Station, for helpful sug-gestionsduringthe progress ofthis work.
REFERENCES
(1) Ballu,T.: Ann. agron.4, 373 (1934).
(2) Bouyoucos, G. J.: SoilSci.34, 393 (1932).
(3) Kachinski,N.A.: Studieson the Physical PropertiesofSoilandon the
Root-systems of Plants (in Russian), published by Selkolkhozghiz, Moscow (1931); also Proc. 2ndIntern. Congr. SoilSci. Comm.I,p.153,Leningrad
(1930).
(4) KosutAny, T.: Der ungarischeWeizenunddasungarische Mehl. Verlag Mol-narok Lapja, Budapesth (1907).
(5) Okhotin,V. V., and Smirnof, O. F.: Pedology U. S. S.R. 2,237 (1934).
(6) Ostwald, W.:Kolloid-Z. 36, 99 (1925), andmany other papers. (7) Pankof,A. M.: Pedology U. S. S.R. 1, 80 (1934).
(8) Schofield,R.K., and Scott Blair, G.W.: PaperI, Proc.Roy. Soc.London
138A,707 (1932);PaperII, ibid. 139A,557 (1933);Paper
III,
ibid. 141A,72(1933). SeealsoSchofield and Scott Blair: Mühlenlab.4,41(1934).
(9) Stock: Z. angew. Chem. 39, 461 (1926), and others.