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1
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0037061510
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Modeling of a continuous food pressing process by dimensional analysis
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in press
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E. Thurairajasingam, E. Shayan, and S. Masood,'"Modeling of a continuous food pressing process by dimensional analysis," Comput. Ind. Eng. (in press); J. R. Hutchinson and M. Garcia, "Tyrannosaurus was not a fast runner," Nature (London) 415, 1018-1022 (2002).
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Comput. Ind. Eng.
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Thurairajasingam, E.1
Shayan, E.2
Masood, S.3
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2
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0037186557
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Tyrannosaurus was not a fast runner
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E. Thurairajasingam, E. Shayan, and S. Masood,'"Modeling of a continuous food pressing process by dimensional analysis," Comput. Ind. Eng. (in press); J. R. Hutchinson and M. Garcia, "Tyrannosaurus was not a fast runner," Nature (London) 415, 1018-1022 (2002).
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(2002)
Nature (London)
, vol.415
, pp. 1018-1022
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Hutchinson, J.R.1
Garcia, M.2
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3
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0033611463
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Getting its from bits
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F. Wilczek, "Getting its from bits," Nature (London) 397, 303-306 (1999).
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(1999)
Nature (London)
, vol.397
, pp. 303-306
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Wilczek, F.1
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4
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0004143210
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Academic, New York
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This essay builds upon the introduction to dimensional analysis that can be found in most comprehensive fluid mechanics textbooks. Recent examples include P. K. Kundu and I. C. Cohen, Fluid Mechanics (Academic, New York, 2001); B. R. Munson, D. F. Young, and T. H. Okiishi, Fundamentals of Fluid Mechanics (Wiley, New York, 1998), 3rd ed.; D. C. Wilcox, Basic Fluid Mechanics (DCW Industries, La Canada, CA, 2000); F. M. White, Fluid Mechanics (McGraw-Hill, New York, 1994), 3rd ed. An older but very useful reference is by H. Rouse, Elementary Mechanics of Fluids (Dover, New York, 1946). A particularly good discussion of the relationship between dimensional analysis and other analysis methods is by C. C. Lin and L. A. Segel, Mathematics Applied to Deterministic Problems in the Natural Sciences (MacMillan, New York, 1974).
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(2001)
Fluid Mechanics
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Kundu, P.K.1
Cohen, I.C.2
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5
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85041148503
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Wiley, New York, 3rd ed.
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This essay builds upon the introduction to dimensional analysis that can be found in most comprehensive fluid mechanics textbooks. Recent examples include P. K. Kundu and I. C. Cohen, Fluid Mechanics (Academic, New York, 2001); B. R. Munson, D. F. Young, and T. H. Okiishi, Fundamentals of Fluid Mechanics (Wiley, New York, 1998), 3rd ed.; D. C. Wilcox, Basic Fluid Mechanics (DCW Industries, La Canada, CA, 2000); F. M. White, Fluid Mechanics (McGraw-Hill, New York, 1994), 3rd ed. An older but very useful reference is by H. Rouse, Elementary Mechanics of Fluids (Dover, New York, 1946). A particularly good discussion of the relationship between dimensional analysis and other analysis methods is by C. C. Lin and L. A. Segel, Mathematics Applied to Deterministic Problems in the Natural Sciences (MacMillan, New York, 1974).
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(1998)
Fundamentals of Fluid Mechanics
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Munson, B.R.1
Young, D.F.2
Okiishi, T.H.3
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6
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0004122635
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DCW Industries, La Canada, CA
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This essay builds upon the introduction to dimensional analysis that can be found in most comprehensive fluid mechanics textbooks. Recent examples include P. K. Kundu and I. C. Cohen, Fluid Mechanics (Academic, New York, 2001); B. R. Munson, D. F. Young, and T. H. Okiishi, Fundamentals of Fluid Mechanics (Wiley, New York, 1998), 3rd ed.; D. C. Wilcox, Basic Fluid Mechanics (DCW Industries, La Canada, CA, 2000); F. M. White, Fluid Mechanics (McGraw-Hill, New York, 1994), 3rd ed. An older but very useful reference is by H. Rouse, Elementary Mechanics of Fluids (Dover, New York, 1946). A particularly good discussion of the relationship between dimensional analysis and other analysis methods is by C. C. Lin and L. A. Segel, Mathematics Applied to Deterministic Problems in the Natural Sciences (MacMillan, New York, 1974).
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(2000)
Basic Fluid Mechanics
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Wilcox, D.C.1
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7
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0038038662
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McGraw-Hill, New York, 3rd ed
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This essay builds upon the introduction to dimensional analysis that can be found in most comprehensive fluid mechanics textbooks. Recent examples include P. K. Kundu and I. C. Cohen, Fluid Mechanics (Academic, New York, 2001); B. R. Munson, D. F. Young, and T. H. Okiishi, Fundamentals of Fluid Mechanics (Wiley, New York, 1998), 3rd ed.; D. C. Wilcox, Basic Fluid Mechanics (DCW Industries, La Canada, CA, 2000); F. M. White, Fluid Mechanics (McGraw-Hill, New York, 1994), 3rd ed. An older but very useful reference is by H. Rouse, Elementary Mechanics of Fluids (Dover, New York, 1946). A particularly good discussion of the relationship between dimensional analysis and other analysis methods is by C. C. Lin and L. A. Segel, Mathematics Applied to Deterministic Problems in the Natural Sciences (MacMillan, New York, 1974).
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(1994)
Fluid Mechanics
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White, F.M.1
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8
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0004247668
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Dover, New York
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This essay builds upon the introduction to dimensional analysis that can be found in most comprehensive fluid mechanics textbooks. Recent examples include P. K. Kundu and I. C. Cohen, Fluid Mechanics (Academic, New York, 2001); B. R. Munson, D. F. Young, and T. H. Okiishi, Fundamentals of Fluid Mechanics (Wiley, New York, 1998), 3rd ed.; D. C. Wilcox, Basic Fluid Mechanics (DCW Industries, La Canada, CA, 2000); F. M. White, Fluid Mechanics (McGraw-Hill, New York, 1994), 3rd ed. An older but very useful reference is by H. Rouse, Elementary Mechanics of Fluids (Dover, New York, 1946). A particularly good discussion of the relationship between dimensional analysis and other analysis methods is by C. C. Lin and L. A. Segel, Mathematics Applied to Deterministic Problems in the Natural Sciences (MacMillan, New York, 1974).
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(1946)
Elementary Mechanics of Fluids
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Rouse, H.1
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9
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0003454592
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MacMillan, New York
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This essay builds upon the introduction to dimensional analysis that can be found in most comprehensive fluid mechanics textbooks. Recent examples include P. K. Kundu and I. C. Cohen, Fluid Mechanics (Academic, New York, 2001); B. R. Munson, D. F. Young, and T. H. Okiishi, Fundamentals of Fluid Mechanics (Wiley, New York, 1998), 3rd ed.; D. C. Wilcox, Basic Fluid Mechanics (DCW Industries, La Canada, CA, 2000); F. M. White, Fluid Mechanics (McGraw-Hill, New York, 1994), 3rd ed. An older but very useful reference is by H. Rouse, Elementary Mechanics of Fluids (Dover, New York, 1946). A particularly good discussion of the relationship between dimensional analysis and other analysis methods is by C. C. Lin and L. A. Segel, Mathematics Applied to Deterministic Problems in the Natural Sciences (MacMillan, New York, 1974).
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(1974)
Mathematics Applied to Deterministic Problems in the Natural Sciences
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Lin, C.C.1
Segel, L.A.2
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10
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33646604947
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note
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An algorithm for computing nondimensional variables has been implemented in MATLAB and can be downloaded from the author's web page, 〈http://www.whoi.edu/science/PO/people/jprice/misc/Danalysis.m〉 or from the MATLAB archive (the file name is Danalysis.m). Also available is a manuscript that treats aspects of dimensional analysis that are not touched on here, 〈http://www.whoi.edu/science/PO/people/jprice/class/ ND.pdf〉.
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11
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0003837398
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Yale U.P., New Haven, CT, 2nd ed.
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The simple pendulum is the starting point for most discussion of dimensional analysis including the classic text by P. W. Bridgman, Dimensional Analysis (Yale U.P., New Haven, CT, 1937), 2nd ed., which is an excellent introduction to the topic, and the more advanced treatment by L. I. Sedov, Similarity and Dimensional Methods in Mechanics (Academic, New York, 1959). Still more advanced is G. I. Barenblatt, Scaling, Self-Similarity and Intermediate Asymptotics (Cambridge U.P., Cambridge, 1996).
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(1937)
Dimensional Analysis
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Bridgman, P.W.1
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12
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0004245736
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Academic, New York
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The simple pendulum is the starting point for most discussion of dimensional analysis including the classic text by P. W. Bridgman, Dimensional Analysis (Yale U.P., New Haven, CT, 1937), 2nd ed., which is an excellent introduction to the topic, and the more advanced treatment by L. I. Sedov, Similarity and Dimensional Methods in Mechanics (Academic, New York, 1959). Still more advanced is G. I. Barenblatt, Scaling, Self-Similarity and Intermediate Asymptotics (Cambridge U.P., Cambridge, 1996).
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(1959)
Similarity and Dimensional Methods in Mechanics
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Sedov, L.I.1
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13
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84953280783
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Cambridge U.P., Cambridge
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The simple pendulum is the starting point for most discussion of dimensional analysis including the classic text by P. W. Bridgman, Dimensional Analysis (Yale U.P., New Haven, CT, 1937), 2nd ed., which is an excellent introduction to the topic, and the more advanced treatment by L. I. Sedov, Similarity and Dimensional Methods in Mechanics (Academic, New York, 1959). Still more advanced is G. I. Barenblatt, Scaling, Self-Similarity and Intermediate Asymptotics (Cambridge U.P., Cambridge, 1996).
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(1996)
Scaling, Self-Similarity and Intermediate Asymptotics
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Barenblatt, G.I.1
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14
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0038400504
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This unpublished manuscript is available
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An excellent discussion of physical measurement and much else that is relevant to dimensional analysis is given by A. A. Sonin, "The physical basis of dimensional analysis," 2001. This unpublished manuscript is available from 〈http://me.mit.edu/people/sonin/html〉.
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(2001)
The Physical Basis of Dimensional Analysis
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Sonin, A.A.1
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15
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33646632773
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note
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-1 is the rotation rate of the earth and R is the distance normal to the rotation axis).
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17
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33646612237
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University of Stuttgart Pi-Group
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S. Brückner and the University of Stuttgart Pi-Group 〈http:// www.pigroup.de/〉, is an excellent resource for advanced applications of dimensional analysis.
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Brückner, S.1
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18
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33646616693
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Dover, New York
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The calculation of a null space basis is, in effect, what all computational methods accomplish, and was noted by E. A. Bender, An Introduction to Mathematical Modelling (Dover, New York, 1977). We delegate the calculation to the computer, and emphasize those properties of the null space basis that are essential for the present purpose.
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(1977)
An Introduction to Mathematical Modelling
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Bender, E.A.1
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19
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33646631003
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note
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5.
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21
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33646629871
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note
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0=π. Is dimensional analysis of any further use for explaining this? Consider energy conservation.
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22
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0037724543
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Pendulum damping
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Detailed treatment of damping processes are by P. T. Squire, "Pendulum damping," Am. J. Phys. 54, 984-991 (1986) and R. A. Nelson and M. G. Olsson, "The pendulum: Rich physics from a simple system," ibid. 54, 112-121 (1985).
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(1986)
Am. J. Phys.
, vol.54
, pp. 984-991
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Squire, P.T.1
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23
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84955019718
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The pendulum: Rich physics from a simple system
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Detailed treatment of damping processes are by P. T. Squire, "Pendulum damping," Am. J. Phys. 54, 984-991 (1986) and R. A. Nelson and M. G. Olsson, "The pendulum: Rich physics from a simple system," ibid. 54, 112-121 (1985).
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(1985)
Am. J. Phys.
, vol.54
, pp. 112-121
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Nelson, R.A.1
Olsson, M.G.2
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24
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33646626671
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note
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1.
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25
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33646625900
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note
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More recent textbooks (Ref. 3), like this article, show only the curve that runs through the middle of a tight cloud of data points that have accumulated from many laboratory experiments, see for example, Rouse (Ref. 3). What is most important, but not evident from this kind of presentation, is that drag coefficients inferred from experiments made using a very wide range of spheres and cylinders moving at widely differing speeds and through many different viscous fluids (Newtonian fluids) do indeed collapse to a well-defined function of Reynolds number alone, just as dimensional analysis had indicated. This is a result, characteristic of dimensional analysis generally, that is at once profound and trivial. One might say trivial because, after all, dimensional analysis told us that the drag coefficient must depend upon Re alone. From this perspective, an effective collapse of the data verifies that carefully controlled laboratory conditions can indeed approximate the idealized physical model. It is profound in that dimensional analysis has shown the way to a useful result (Fig. 5), where there would otherwise have been be an unwieldy mass of highly specific data (as in going from Fig. 1 to Fig. 2). An open question of considerable practical importance is whether the steady drag laws are robust in the sense of giving useful estimates in practical problems, say our pendulum, in which the idealized conditions are inevitably violated. Other data sets have been developed to define the effects of idealized surface roughness, for example, but our pendulum has a long list of violations - time-dependence, a nearby solid boundary (the floor), slight surface roughness, etc., all present at once, so that we are on our own. About all that can be said is that it is important to understand the full set of assumptions under which a similarity law has been defined, and to be skeptical of applications outside of those bounds.
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26
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0033407885
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Princeton U.P., New York
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5 due to changes in the viscous boundary layer and the width of the wake behind a moving sphere. This is the Re range of a well-hit golf ball or tennis ball, and is part of the reason that aerodynamic drag on these objects has a surprising sensitivity to surface roughness or spin. For much more detail on these phenomenon see S. Vogel, Life in Moving Fluids (Princeton U.P., New York, 1994), and P. Timmerman and J. P. van der Weele, "On the rise and fall of a ball with linear and quadratic drag," Am. J. Phys. 67, 538-546 (1999).
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(1994)
Life in Moving Fluids
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Vogel, S.1
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27
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0033407885
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On the rise and fall of a ball with linear and quadratic drag
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5 due to changes in the viscous boundary layer and the width of the wake behind a moving sphere. This is the Re range of a well-hit golf ball or tennis ball, and is part of the reason that aerodynamic drag on these objects has a surprising sensitivity to surface roughness or spin. For much more detail on these phenomenon see S. Vogel, Life in Moving Fluids (Princeton U.P., New York, 1994), and P. Timmerman and J. P. van der Weele, "On the rise and fall of a ball with linear and quadratic drag," Am. J. Phys. 67, 538-546 (1999).
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(1999)
Am. J. Phys.
, vol.67
, pp. 538-546
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Timmerman, P.1
Van der Weele, J.P.2
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28
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33646611182
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note
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2/s at a temperature = 40°C). Given these results, can you think of a name more apt than "viscous" pendulum?
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