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    DIMENSIONAL ANALYSIS

    Is that all there is?

    W. J. Wilson

    Department of Physics and Engineering

    University of Central OklahomaEdmond, Oklahoma 73034-5209

    [email protected]

    (The Secrets of Physics Revealed)

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    Outline

    A. Whats the secret of being a Scientist or an Engineer?

    B. What are Units and Dimensions anyway?

    C. What is Dimensional Analysis and why should I care?

    D. Why arent there any mice in the Polar Regions?

    E. Why was Gulliver driven out of Lillipute?F. What if Pythagorus had known Dimensional Analysis?

    G. But what do I really need to know about Dimensional

    Analysis so that I can pass the test?

    H. Can I get into trouble with Dimensional Analysis? Theballad of G.I. Taylor.

    I. But can it be used in the Lab ?

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    How to be a Scientist or Engineer

    The steps in understanding and/or control

    any physical phenomena is to

    1. Identify the relevant physical variables.2. Relate these variables using the known

    physical laws.

    3. Solve the resulting equations.

    Secret #1: Usually not all of these are

    possible. Sometimes none are.

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    ALL IS NOT LOST BECAUSE OF

    Physical laws must be independent of

    arbitrarily chosen units of measure. Nature

    does not care if we measure lengths in

    centimeters or inches or light-years or

    Check your units! All natural/physical

    relations must be dimensionally correct.

    Secret #2: Dimensional Analysis

    Rationale

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    Dimensional AnalysisDimensional Analysis refers to

    the physical nature of the

    quantity and the type of unit

    (Dimension) used to specify it.

    Distance has dimension L.

    Area has dimension L2.

    Volume has dimension L3.

    Time has dimension T.

    Speed has dimension L/T

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    Why are there no smallanimals in the polar regions?

    Heat Loss Surface Area (L2)

    Mass Volume (L3)

    Heat Loss/Mass Area/Volume

    = L2/ L3= L-1

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    Heat Loss/Mass Area/Volume

    = L2/ L3

    = L-1

    Mouse (L = 5 cm)

    1/L = 1/(0.05 m)

    = 20 m-1

    Polar Bear (L = 2 m)

    1/L = 1/(2 m)= 0.5 m-1

    20 : 0.5 or 40 : 1

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    Gullivers Travels: Dimensional Analysis

    Gulliver was 12x the Lilliputians

    How much should they feed him?

    12x their food ration?

    A persons food needs are

    related to their mass

    (volume)This dependson the cube of the linear

    dimension.

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    Gulliver is 12x taller than theLilliputians, LG=12 LL

    Now VG (LG)3 and VL (LL)3, so

    VG / VL = (LG)3 / (LL)

    3= (12 LL)

    3 / (LL)3

    = 123= 1728

    Gulliver needs to be fed 1728times the amount of food eachday as the Lilliputians.

    Let LG and VG denote Gullivers linear and volume dimensions.

    Let LL and VL denote the Lilliputians linear and volume dimensions.

    This problem has direct relevance to drug dosages in humans

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    Pythagorean Theorem

    Area =F(q) c2

    A1 =F(q) b2

    A2=F(q) a2

    Area = A1 +A2

    F(q) c2

    =F(q) a2

    +F(q) b2

    c2= a2+b2

    ca

    b

    qq A1

    A2

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    Dimensions of Some CommonPhysical Quantities

    [x], LengthL

    [m], MassM

    [t], TimeT

    [v], VelocityLT-1

    [a], AccelerationLT-2

    [F], ForceMLT-2

    [r], Mass DensityML-3[P], PressureML-1T-2

    [E], EnergyML2

    T-2

    [I], Electric CurrentQT-1

    [q], Electric ChangeQ

    [E], Electric Field - MLQT

    -2

    All are powers of the fundamental dimensions:

    [Any Physical Quantity] = MaLbTcQd

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    Dimensional Analysis Theorems

    Dimensional Homogeneity Theorem: Anyphysical quantity is dimensionally a power lawmonomial - [Any Physical Quantity] = MaLbTcQd

    Buckingham Pi Theorem: If a system has kphysical quantities of relevance that depend on

    depend on rindependent dimensions, then thereare a total ofk-rindependent dimensionlessproducts p1, p2, , pk-r. The behavior of thesystem is describable by a dimensionless equation

    F(p1, p

    2, , p

    k-r

    )=0

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    Exponent Method1. List all kvariables involved in the problem

    2. Express each variables in terms of [M] [L] [T ]dimensions (r)

    3. Determine the required number of dimensionlessparameters (kr)

    4. Select a number of repeating variables = r(All dimensions must be included in this set and eachrepeating variable must be independent of the others.)

    5. Form a dimensionless parameterpby multiplying one ofthe non-repeating variables by the product of the

    repeating variables, each raised to an unknown exponent.6. Solved for the unknown exponents.

    7. Repeat this process for each non-repeating variable

    8. Express result as a relationship among the dimensionless

    parametersF(p

    1,p

    2,p

    3, ) = 0.

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    G. I. Taylors 1947 Analysis

    Published

    U.S.

    Atomic

    Bomb was

    18 kiloton

    device

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    Nuclear Explosion Shock Wave

    r f(E,r,t)

    5/15/25/1

    5/15/25/1

    1

    322000

    1

    5

    220:

    5

    13210:

    0:

    )()())((

    )(

    rrp

    rp

    tE

    RtRE

    bbaT

    acaL

    accaM

    MLTTMLLTLM

    tEr

    cba

    cba

    The propagation of a nuclear

    explosion shock wave depends on:E,

    r,r, and t.

    n = 4 No. of variables

    r= 3 No. of dimensions

    n r = 1 No. of dimensionless parameters

    Select repeating variables:

    E, t, andrCombine these with the rest of the

    variables: r

    E r r t

    ML2T-2 ML-3 L T

    5/15/25/15/15/25/1

    11 0)(

    rr

    pp

    tECRCtE

    R

    CF

    5/12

    r

    EtCR

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    r 1 kg/m3

    R = (E/r)1/5t2/5

    logR = 0.4 log t+0.2 log(E/r)

    0.2 log(E/r) 1.56

    E= 7.9x1013 J= 19.8 kilotons TNT

    Blast Radius vs Time

    log R = 0.4058 log t + 1.5593

    1

    2

    3

    -2 -1 0 1 2

    log (t)

    log(R)

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    Dimensional Analysis in the Lab Want to study pressure drop as

    function of velocity (V1) and

    diameter (do)

    Carry out numerous experiments

    with different values ofV1 and do

    and plot the data

    5 parameters:Dp,r, V1, d1, do

    2 dimensionless parameter groups:

    DP/(rV2/2), (d1/do)

    p1

    p0

    V1

    A1

    V0A0

    Much easier to establish functional relations with 2 parameters, than 5

    DP r V1 d1 d2

    ML-1T-2 ML-3 LT-1 L L

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    References1. G. I. Barenblatt, Scaling, Self-Similarity, and Intemediate Asymptotics

    (Cambridge Press, 1996).

    2. H. L. Langhaar, Dimensional Analysis and the Theory of Models (Wiley,

    1951).

    3. G. I. Taylor, The Formation of a Blast Wave by a Very Intense Explosion.The Atomic Explosion of 1945,Proc. Roy Soc. LondonA201, 159 (1950).

    4. L. D. Landau and E.M. Lifshitz, Fluid Mechanics (Pergamon Press, 1959).

    Section 62.

    5. G. W. Blumen and J. D. Cole, Similarity Methods for Differential Equations

    (Springer-Verlag, 1974).

    6. E. Buckingham, On Physically Similar Systems: Illustrations of the Use of

    Dimensional Equations,Phys. Rev. 4, 345 (1921).