microsoft power point - bmcf 2223 - ch 9 dimensional analysis e2
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DIMENSIONAL ANALYSISDIMENSIONAL ANALYSIS
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DimensionDimension
5 basic dimensions?5 basic dimensions?
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Most physicalMost physical
quantities can bequantities can beexpressed in terms ofexpressed in terms ofthe combinations ofthe combinations of
MassMass MM
LengthLength LL
AbbreviationAbbreviationDimensionsDimensionsDimensionDimension
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i.e. speed is always ai.e. speed is always alength divided a timelength divided a time
So dimensions ofSo dimensions of
speed are lengthspeed are lengthdivided by time or L/Tdivided by time or L/T
meme
ElectricElectric
currentcurrent
II
TemperatureTemperature
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DimensionDimension
What is theWhat is the
dimensions of thedimensions of thefollowing quantities?following quantities?
VolumeVolume
AreaArea
DensityDensity
LL33
LL22
M/LM/L33
22
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ForceForce ML/TML/T22
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Dimensional HomogeneityDimensional Homogeneity
Any equation describing a physical situationAny equation describing a physical situationwill only be true if both sides have the samewill only be true if both sides have the same
dimensions, i.e.dimensions, i.e.1 meter + 3 kilograms = 4 days (not true)1 meter + 3 kilograms = 4 days (not true)
1 meters + 3 meters = 4 meters (true)1 meters + 3 meters = 4 meters (true)
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In other words, the dimensions must beIn other words, the dimensions must beconsistentconsistent
The property of dimensional homogeneityThe property of dimensional homogeneitycan be useful for:can be useful for: --
Checking units of equationsChecking units of equations
Converting between two sets of unitsConverting between two sets of units
Defining dimensionless relationshipsDefining dimensionless relationships
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Dimension and UnitsDimension and Units
Dimensions must have aDimensions must have astandardised unit i.e. meter, foot,standardised unit i.e. meter, foot,
yardyardThere are 2 systems of unit beingThere are 2 systems of unit beingwidely used:widely used: --
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(International system) units(International system) units
US (United States) unitsUS (United States) unitsHere we are using SI unitsHere we are using SI units
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Dimension and UnitsDimension and Units
Some basic SI unitsSome basic SI units
LengthLength metermeter
metremetre
mm
SymbolSymbolNameNameQuantityQuantity
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MassMass kilogramkilogram kgkg
TimeTime secondsecond ss
TemperatureTemperature kelvinkelvin KK
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Dimension and UnitsDimension and Units
Between dimensions and units:Between dimensions and units: Dimensions are properties which can beDimensions are properties which can be
measuredmeasured Unit are the standard elements we use toUnit are the standard elements we use to
quantify these dimensionsquantify these dimensions
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Dimensional AnalysisDimensional Analysis
Useful technique in allUseful technique in allexperimentally based areas ofexperimentally based areas ofengineeringengineering
If you know the factors involved inIf you know the factors involved in
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,,analysis can form a relationshipanalysis can form a relationshipbetween thembetween them
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Dimension and UnitsDimension and Units
In dimensional analysis we areIn dimensional analysis we areonly concerned with the natureonly concerned with the natureof the dimension, i.e. theof the dimension, i.e. the qualityqualitynotnot thethe quantityquantity
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The man weights 50 kg,standing at 60 m height
and 9.81 m/s2 gravity
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Dimension and UnitsDimension and Units
In fluid mechanics, all the physical propertiesIn fluid mechanics, all the physical propertiescan be presented with L, T, M and Fcan be presented with L, T, M and F
Force can also be presented in LTMForce can also be presented in LTM
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QuantityQuantity SI unitSI unit DimensionDimension
VelocityVelocity m/sm/s msms--11 LTLT--11
AccelerationAcceleration m/sm/s22 msms--22 LTLT--22
ForceForce N or kgm/sN or kgm/s22 kg mskg ms--22 MLTMLT--22
EnergyEnergy J or kgmJ or kgm22/s/s22 kg mkg m22 ss--22 MLML22TT--22
-- --
Dimensions of Some Common Physical Quantities:Dimensions of Some Common Physical Quantities:
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PressurePressure Pa or kg/m/sPa or kg/m/s22 kg mkg m--11 ss--22 MLML--11TT--22
DensityDensity kg/mkg/m33 kg mkg m--33 MLML--33
Specific weightSpecific weight N/mN/m33 or kg/mor kg/m22/s/s22 Kg mKg m--22ss--22 MLML--22TT--22
viscosityviscosity N s/mN s/m22 or kg/msor kg/ms Kg mKg m--11 ss--11 MLML--11TT--11
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Result of Dimensional AnalysisResult of Dimensional Analysis
The results of performingThe results of performingdimensional analysis (on adimensional analysis (on a
physical problem) isphysical problem) is a singlea singleequationequation
This equationThis equation relatesrelates all of theall of the
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p ys ca ac orsp ys ca ac ors var a es, .e.var a es, .e.velocity, force, time) involved tovelocity, force, time) involved toone anotherone another
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Result of Dimensional AnalysisResult of Dimensional Analysis
For example:For example: --
If we want to find theIf we want to find the forceforce on aon a
propeller blade we must first decidepropeller blade we must first decidewhat might influence this forcewhat might influence this force
It would be reasonable to assume thatIt would be reasonable to assume thatthe force F de ends on the followinthe force F de ends on the followin
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physical propertiesphysical properties diameter, ddiameter, d
forward velocity of the propeller, uforward velocity of the propeller, u
fluid density,fluid density,
revolutions per second, Nrevolutions per second, N
fluid viscosity,fluid viscosity,
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Before we do any analysis we write thisBefore we do any analysis we write thisequation:equation:
F =F = (d, u,(d, u, , N,, N, ))
oror0 =0 = 11(F, d, u,(F, d, u, , N,, N, ))
WhereWhere andand 11 are unknown functionsare unknown functions
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These can be expanded into an infiniteThese can be expanded into an infiniteseries which can itself be reduced toseries which can itself be reduced to
F = K dF = K dmm uupp qq NNrr ss
Where K is a numerical constantWhere K is a numerical constantAnd m, p, q, r, s are unknown constant powerAnd m, p, q, r, s are unknown constant power
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From dimensional analysis weFrom dimensional analysis we
obtain these powerobtain these power
form the variable into severalform the variable into severaldimensionless groupsdimensionless groups
The value of K and the functionThe value of K and the function andand 11 must be determinedmust be determinedfrom experimentfrom experiment
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The knowledge of theThe knowledge of thedimensionless group oftendimensionless group oftenhelps in deciding whathelps in deciding what
experimental measurementsexperimental measurementsshould be takenshould be taken
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BuckinghamsBuckinghams TheoremsTheorems
One of the methods used to performOne of the methods used to performdimensional analysisdimensional analysis
Provides better generalised strategy inProvides better generalised strategy inobtaining a solution (compared to indicialobtaining a solution (compared to indicialmethod)method)
11stst theorem:theorem: --
A relationship between n variables (physicalA relationship between n variables (physical
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properties such as velocity, density etc.) canproperties such as velocity, density etc.) canbe expressed as a relationship betweenbe expressed as a relationship betweennn m nonm non--dimensional groups of variablesdimensional groups of variables(called(called group), where m is the number ofgroup), where m is the number ofthe fundamental dimensions (such as mass,the fundamental dimensions (such as mass,length and time) required to express thelength and time) required to express thevariablesvariables
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BuckinghamsBuckinghams TheoremsTheorems
So if a physical problem can beSo if a physical problem can beexpressed as:expressed as: --
(Q(Q11, Q, Q22, Q, Q33, , Q, , Qnn) = 0) = 0
Then, according to the above 1Then, according to the above 1
stst
theorem, this can be expressed as:theorem, this can be expressed as: --
11((11,, 22,, 33, ,, , nn mm) = 0) = 0
In fluid we can normall taken m = 3In fluid we can normall taken m = 3
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(corresponding to M, L and T)(corresponding to M, L and T)
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22ndnd theorem:theorem: --
EachEach group is a function ofgroup is a function ofm repeating variables plusm repeating variables plusone of the remainingone of the remainingvariablesvariables
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== (Q(Q11, Q, Q22, , Q, , Qmm, Q, Qm+1m+1) = 0) = 0
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Choice of Repeating VariableChoice of Repeating Variable
From the 2From the 2ndnd theorem there cantheorem there canbe m (= 3) repeating variablebe m (= 3) repeating variable
When combined, these repeatingWhen combined, these repeatingvariables must contain all of thevariables must contain all of thedimensions (M, L, T)dimensions (M, L, T)A combination of the repeatingA combination of the repeatingvariables will not form avariables will not form a
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mens on ess groupmens on ess group
The repeating variables do notThe repeating variables do nothave to appear in allhave to appear in all groupsgroups
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Choice of Repeating VariableChoice of Repeating Variable
The repeating variables shouldThe repeating variables shouldbe chosen to be measurable inbe chosen to be measurable inan experimental investigation.an experimental investigation.
They should be the majorThey should be the majorinterest to the designerinterest to the designer
In fluid mechanics, it is usuallyIn fluid mechanics, it is usuallyossible to takeossible to take uu andand dd asas
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the three repeating variablesthe three repeating variablesThis freedom of choice resultsThis freedom of choice resultsin there being many differentin there being many different group which can be formed,group which can be formed,
and all are valid (there is noand all are valid (there is noreally a wrong choice)really a wrong choice)
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Example:Example:
Taking the example discussedTaking the example discussedpreviously, force F induced on apreviously, force F induced on apropeller blade, we have thepropeller blade, we have theequationequation
F =F = (d, u,(d, u, , N,, N, ))n = 6 and m = 3n = 6 and m = 3
There are nThere are n m = 3m = 3 groups, sogroups, so
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((11,, 22,, 33) = 0) = 0The choice ofThe choice of , u, d as the, u, d as therepeating variables satisfies therepeating variables satisfies thecriteria above:criteria above: --
They are measurableThey are measurable good design parameters andgood design parameters and
in combination contain all thein combination contain all thedimensions M, L, Tdimensions M, L, T
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Example:Example:
We can now form the three groupsWe can now form the three groupsaccording to the 2according to the 2ndnd theorem,theorem,
11 == aa11uubb11ddcc11FF
22 == aa22uubb22ddcc22NN
33 == aa33uubb33ddcc33
As theAs the groups are allgroups are alldimensionless i.e. they havedimensionless i.e. they have
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dimensions Mdimensions M
00
LL
00
TT
00
we use thewe use theprinciple of dimensionalprinciple of dimensionalhomogeneity to equate thehomogeneity to equate thedimensions for eachdimensions for each groupgroup
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For the firstFor the first group,group,
11 == aa11
uu
bb11
dd
cc11
FFIn terms of dimensionsIn terms of dimensions
MM00LL00TT00 = (ML= (ML--33))aa11(LT(LT--11))bb11(L)(L)cc11(MLT(MLT--22))
For each dimension the powers must be equalFor each dimension the powers must be equal
on both sides of the equation, soon both sides of the equation, soFor M:For M: 0 = a0 = a11 + 1+ 1
aa11 == 11
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For L:For L: 0 =0 = 3a3a11 + b+ b11 + c+ c11 + 1+ 10 = 4 + b0 = 4 + b11 + c+ c11For T:For T: 0 =0 = bb11 22
bb11 == 22
cc11 == 44 bb11 == 22
GivingGiving 11 asas
11 == --11uu--22dd--22FF
11 = F/= F/uu22
dd22
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or:or:
11 = F/= F/uu22dd22
FF == 11 uu22dd22
Where,Where, 11 is a force coefficientis a force coefficient
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Example:Example:Similar procedure is followed for the otherSimilar procedure is followed for the other
group, i.e.group, i.e.22 ==
aa22uubb22ddcc22NN
MM
00
LL
00
TT
00
= (ML= (ML
--33
))
aa22
(LT(LT
--11
))
bb22
(L)(L)
cc22
(T(T
--11
))For M:For M: 0 = a0 = a22For L:For L: 0 =0 = 3a3a22 + b+ b22 + c+ c22
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22 22
For T:For T: 0 =0 = bb22 11bb11 == 11
cc11 == 11
GivingGiving 22 asas22 ==
00uu--11dd11NN
22 = Nd/u= Nd/u
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Example:Example:For the third,For the third,
33 == aa33uubb33ddcc33
MM00LL00TT00 = (ML= (ML--33))aa33(LT(LT--11))bb33(L)(L)cc33(ML(ML--11TT--11))
For M:For M: 0 = a0 = a33 + 1+ 1aa33 == 11
For L:For L: 0 =0 = 3a3a33 + b+ b33 + c+ c33 11
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33 ++ 33==
For T:For T: 0 =0 = bb33 11
bb33 == 11
cc33 == 11
GivingGiving 33 asas33 ==
--11uu--11dd--11
33 == //udud
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Example:Example:Thus, the problem may be described by theThus, the problem may be described by the
following function of the three nonfollowing function of the three non--dimensionaldimensional groupgroup
((11,, 22,, 33) = 0) = 0
(F/(F/uu22dd22, Nd/u,, Nd/u, //ud) = 0ud) = 0
May also be written:May also be written:
F/F/ uu22dd22 == Nd/uNd/u // udud
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or:or:FF == uu22dd22 11(Nd/u,(Nd/u, //ud)ud)
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ADVANTAGE OF PERFORMING DIMENSIONAL ANALYSISADVANTAGE OF PERFORMING DIMENSIONAL ANALYSIS
To determine experimentally howTo determine experimentally how
F =F = (d, u,(d, u, , N,, N, ))
If number of level to be testedIf number of level to be testedfor each parameter is 5for each parameter is 5
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For uFor u22,,
22, N, N
22,,
22
dd11 F = ?F = ?
dd22 F = ?F = ?
dd33 F = ?F = ?
dd44 F = ?F = ?
dd55 F = ?F = ?
For uFor u33,, 33, N, N33,, 33
dd11 F = ?F = ?
dd22 F = ?F = ?
dd33
F = ?F = ?
dd44 F = ?F = ?
dd55 F = ?F = ?
For uFor u11,, 11, N, N11,, 11
dd11 F = ?F = ?
dd22 F = ?F = ?
dd33 F = ?F = ?
dd44 F = ?F = ?
dd55 F = ?F = ?
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ADVANTAGE OF PERFORMING DIMENSIONAL ANALYSISADVANTAGE OF PERFORMING DIMENSIONAL ANALYSIS
F =F = (d, u,(d, u, , N,, N, ))
Number of independent parameters, n = 5Number of independent parameters, n = 5
For number of level = 5,For number of level = 5,
Total runTotal run = 5n = 55 = 3125 experiments
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Through dimensional analysis:Through dimensional analysis:
number ofnumber of group = ngroup = n m = 3m = 3
11 == ((22,, 33))
Total run =Total run = 52 = 25 experiments!
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If 1 day you can perform 25 experimentsIf 1 day you can perform 25 experimentsFor 3125 experiments = 125 daysFor 3125 experiments = 125 days
if you work 5 days per week = 25 weeksif you work 5 days per week = 25 weeks
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= .= .
= YEAR +!= YEAR +!
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Wrong Choice of Physical PropertiesWrong Choice of Physical Properties
If important / influentialIf important / influential
variable was missed, thenvariable was missed, thenthe importantthe important group will begroup will bemissingmissing
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on these results may misson these results may missthe significant behaviouralthe significant behaviouralchangeschanges
Therefore, the choice ofTherefore, the choice ofvariables is very importantvariables is very important
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Wrong Choice of Physical PropertiesWrong Choice of Physical Properties
If extra/unimportant variableIf extra/unimportant variable
are introduced, then theare introduced, then theextra/unimportantextra/unimportant groupsgroupswill be formwill be form
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They will play very little roleThey will play very little roleinfluencing the physicalinfluencing the physicalbehaviour of the problembehaviour of the problem
And should be identify duringAnd should be identify duringthe experimental workthe experimental work
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Manipulation of TheManipulation of The GroupGroupManipulation of theManipulation of the group isgroup ispermittedpermitted
These manipulation did notThese manipulation did notchange the number of groupschange the number of groupsinvolved, butinvolved, but
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May change their appearanceMay change their appearance
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Manipulation of TheManipulation of The GroupGroup
Any number of groups can beAny number of groups can becombined by multiplication orcombined by multiplication or
((11,, 22,, 33, ,, , nn mm) = 0) = 0
Taking the definingTaking the definingequation as:equation as:
Then,Then,
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which replace one of thewhich replace one of theexisting, i.e.existing, i.e.
11 andand 22 is combined to formis combined to form
1a1a == 11//22 so thatso that
((1a1a,, 22,, 33, ,, , nn mm) = 0) = 0
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Manipulation of TheManipulation of The GroupGroup
The reciprocal of any group isThe reciprocal of any group isvalid, i.e.valid, i.e.
((11,, 22,, 33, ,, , nn mm) = 0) = 0
Taking the definingTaking the definingequation as:equation as:
Then,Then,
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((11, 1/, 1/22,, 33, , 1/, , 1/nn mm) = 0) = 0
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Manipulation of TheManipulation of The GroupGroup
Any group may be raised toAny group may be raised toany power, i.e.any power, i.e.
((11,, 22,, 33, ,, , nn mm) = 0) = 0
Taking the definingTaking the definingequation as:equation as:
Then,Then,
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((1122
,, 221 21 2
,, 3344
, ,, , nn mm) = 0) = 0
M i l i f ThM i l i f Th GG
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Manipulation of TheManipulation of The GroupGroup
Any group may be multipliedAny group may be multipliedby a constant, i.e.by a constant, i.e.
((11,, 22,, 33, ,, , nn mm) = 0) = 0
Taking the definingTaking the definingequation as:equation as:
Then,Then,
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(k(k1111,, 22, k, k2233, ,, , nn mm) = 0) = 0
M i l ti f ThM i l ti f Th GG
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Manipulation of TheManipulation of The GroupGroup
Any group may be expressedAny group may be expressedas a function of the otheras a function of the other
((11,, 22,, 33, ,, , nn mm) = 0) = 0
Taking the definingTaking the definingequation as:equation as:
Then,Then,
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, . ., . .
22 == 11((11,, 33, ,, , nn mm))
M i l ti f ThM i l ti f Th GG
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Manipulation of TheManipulation of The GroupGroup
((11, 1/, 1/22,, 33ii, , k, , knn mm) = 0) = 0
In general, the definingIn general, the definingequation may look like:equation may look like:
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CommonCommon GroupsGroups
During dimensional analysis,During dimensional analysis,several groups will appearseveral groups will appear
again and again for differentagain and again for differentproblemproblem
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their namestheir names
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CommonCommon GroupsGroups
Reynolds numberReynolds number Inertial, viscous forceInertial, viscous forceratioratio
Euler numberEuler number Pressure, inertial forcePressure, inertial force
ud=Re
2En
p=
Some commonSome commondimensionless groups are:dimensionless groups are:
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Froude numberFroude number Inertial, gravitationalInertial, gravitationalforce ratioforce ratio
Weber numberWeber number Inertial, surface tensionInertial, surface tension
force ratioforce ratioMach numberMach number Local velocity, localLocal velocity, local
velocity of sound ratiovelocity of sound ratio
gd
u2Fn =
ud=We
c
u=Mn
Example:Example:
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Example:Example:
Determine the drag forceDetermine the drag forceexerted on a submergedexerted on a submergedsphere as it moves through asphere as it moves through aviscous fluidviscous fluid
Step 1: Consider which physicalStep 1: Consider which physicalfactors influence the drag forcefactors influence the drag force
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Diameter of the sphere, dDiameter of the sphere, d
Velocity of the sphere, uVelocity of the sphere, u
Density of the fluid,Density of the fluid,
Viscosity of the fluid,Viscosity of the fluid,
Thus we can write:Thus we can write:Drag force, F =Drag force, F = (d, u,(d, u, ,, ))
n = 5n = 5
Example:Example:
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Example:Example:
Step 2: List the dimensions of eachStep 2: List the dimensions of eachvariablevariable
dd LL
uu LTLT--11
MLML--33
--11 --11
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FF MLTMLT--22So,So,
m = 3m = 3 (L, M, T)(L, M, T)
Example:Example:
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Example:Example:
Step 3: Determine the number ofStep 3: Determine the number ofdimensionless group (dimensionless group ( group)group)
nn m = 5m = 5 3 = 23 = 2
So we write:So we write:
1st p theorem:1st p theorem: --A relationship between nA relationship between nvariables can be expressed asvariables can be expressed as
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((11,, 22) = 0) = 0 a re at ons p etween na re at ons p etween n mmdimensionless groups, where mdimensionless groups, where mis the number of theis the number of thefundamental dimensionsfundamental dimensionsrequired to express therequired to express the
variablesvariables
Example:Example:
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Example:Example:
Step 4: Select m (= 3) repeating variablesStep 4: Select m (= 3) repeating variables
Generally it helps to choose variables thatGenerally it helps to choose variables thatrelates to:relates to: --
GeometryGeometry dd
Fluid PropertyFluid Property
?
?
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Example:Example:
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Example:Example:
Step 5: Write theStep 5: Write the groups according to 2groups according to 2ststtheorem:theorem: --
EachEach group is a function of m (= 3)group is a function of m (= 3)repeating variables plus one of therepeating variables plus one of the
remaining variablesremaining variablesremaining variablesremaining variables
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From the problemFrom the problemSo we write,So we write,
11 == aa11uubb11ddcc11
22 == aa22uubb22ddcc22FF
F =F = (d, u,(d, u, ,, ))repeating variablesrepeating variables
?
?
Example:Example:
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Example:Example:
Step 6: Solve for the exponents and theStep 6: Solve for the exponents and theforms of the dimensionless groupsforms of the dimensionless groups
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Example:Example:
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For the firstFor the first group,group,
11 == aa11uubb11ddcc11
MM00LL00TT00 = (ML= (ML--33))aa11(LT(LT--11))bb11(L)(L)cc11(ML(ML--11TT--11))
For M:For M: 0 = a0 = a11+ 1+ 1
aa11 == 11
For L:For L: 0 =0 = 3a3a11 + b+ b11 + c+ c11 11
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11 ++ 11==
For T:For T: 0 =0 = bb11 11bb11 == 11
cc11 == 11
GivingGiving 11 asas11 ==
--11uu--11dd--11
11 == //ud orud or ud/ud/ = Re= Re
For the secondFor the second group,group,
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For the secondFor the second group,group,
22 == aa22uubb22ddcc22FF
In terms of dimensionsIn terms of dimensions
MM00LL00TT00 = (ML= (ML--33))aa22(LT(LT--11))bb22(L)(L)cc22(MLT(MLT--22))
For each dimension the powers must be equalFor each dimension the powers must be equal
on both sides of the equation, soon both sides of the equation, soFor M:For M: 0 = a0 = a22 + 1+ 1
aa22 == 11
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For L:For L: 0 =0 = 3a3a22 + b+ b22 + c+ c22 + 1+ 1
0 = 4 + b0 = 4 + b22 + c+ c22For T:For T: 0 =0 = bb22 22
bb22 == 22
cc22 == 44 bb22 == 22GivingGiving 22 asas
22 == --11uu--22dd--22FF
22 = F/= F/uu22
dd22
Example:Example:
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pp
Step 7: Rearrange theStep 7: Rearrange the group as desiredgroup as desired
Thus, the problem may beThus, the problem may bedescribed by the following functiondescribed by the following functionof the 2 dimensionlessof the 2 dimensionless groupgroup
((11,, 22) = 0) = 0
(Re, F/(Re, F/uu22dd22) = 0) = 0
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That is:That is:
F/F/uu22dd22 == 11(Re)(Re)
or:or:
FF == uu22dd22 11(Re)(Re)
Example:Example:
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pp
FF == uu22dd22 11(Re)(Re)
Thus dimensional analysisThus dimensional analysis
indicates that the drag force isindicates that the drag force isproportional toproportional to ,, uu22 and dand d22, and, andalso depends on the Realso depends on the Re
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WHAT IFWHAT IF
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WHAT IFWHAT IF
nn m = 0 ?m = 0 ?
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Do the following:Do the following: Check your list of parametersCheck your list of parameters
Check your algebraCheck your algebra
Reduce m by oneReduce m by one
Cengel pg 290Cengel pg 290
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Cengel pg. 290Cengel pg. 290
You are curious as to theYou are curious as to the
relationship between soap bubblerelationship between soap bubble
radius and the pressure inside theradius and the pressure inside the
soap bubblesoap bubble
You reason that pressure inside theYou reason that pressure inside the
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bubble must be greater thanbubble must be greater than
atmospheric pressure, andatmospheric pressure, and
Shell of the bubble is underShell of the bubble is under
tension, alsotension, also
Surface tension must be importantSurface tension must be important
Not knowing other physic, you decide toNot knowing other physic, you decide to
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g p y yg p y y
approach the problem usingapproach the problem using
dimensional analysisdimensional analysis
Establish a relationship between:Establish a relationship between: --
Pressure different,Pressure different, p = pp = pinsideinside ppatmatm Soap bubble radius, RSoap bubble radius, R
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ss
Assumptions:Assumptions:
Bubble is neutrally buoyant, and soBubble is neutrally buoyant, and so
gravity is not importantgravity is not importantNo other variables are importantNo other variables are important
List variables and its dimensionsList variables and its dimensions
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pp (ML(ML--11
TT--22
)) RR (L)(L)
ss (MT(MT--22))
n = 3 m = 3n = 3 m = 3nn m = 0m = 0
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List variables and its dimensionsList variables and its dimensions
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pp (ML(ML--11
TT--22
)) RR (L)(L)
ss (MT(MT--22))
n = 3 m = 3n = 3 m = 3nn m = 0m = 0
Do the following:Do the following: Check your list of parametersCheck your list of parameters
Check our al ebraCheck our al ebra
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SoSo
mm 1 = 31 = 3 1 = 21 = 2
Reduce m by oneReduce m by one
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NowNow
n = 3 m = 2n = 3 m = 2
nn m = 1m = 1
--
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11 groupgroup
2 repeating variables2 repeating variables
Now write:Now write:
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11 = R= Raa
ss
bb
ppIn terms of dimensionsIn terms of dimensions
MM00LL00TT00 = (L)= (L)aa(MT(MT--22))bb(ML(ML--11TT--22))
Solve for the exponentsSolve for the exponentsFor M:For M: 0 = b + 10 = b + 1
b =b = 11
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For L:For L: 0 = a0 = a 11a = 1a = 1
For T:For T: 0 =0 = 2b2b 22
b =b = 11GivingGiving 11 asas
11 = R= Rss--11p =p = RR p/p/ss
Rearrange theRearrange the group as desiredgroup as desired
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((11) = 0) = 0((RR p/p/ss) = 0) = 0
That is:That is:
RRp/p/ss == 11(Nothing)(Nothing)
This is possible only whenThis is possible only when
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RRp/p/
ss == constantconstantThereforeTherefore
pp == constantconstant ss/R/R
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pp == constantconstant ss/R/R
Note:Note:
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mens ona ana ys s canno pre cmens ona ana ys s canno pre c
the value of the constantthe value of the constantFurther experimental works reveals thatFurther experimental works reveals that
the constant is equal to 4the constant is equal to 4