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Basics of Fluid Mechanics, 2014a

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CHAPTER 9<br />

Dimensional Analysis<br />

This chapter is dedicated to my adviser, Dr. E.R.G.<br />

Eckert.<br />

9.1 Introductory Remarks<br />

Genick Bar-Meir<br />

Dimensional analysis refers to techniques dealing with units or conversion to a unitless<br />

system. The definition <strong>of</strong> dimensional analysis is not consistent in the literature which<br />

span over various fields and times. Possible topics that dimensional analysis deals with<br />

are consistency <strong>of</strong> the units, change order <strong>of</strong> magnitude, applying from the old and<br />

known to unknown (see the Book <strong>of</strong> Ecclesiastes), and creation <strong>of</strong> group parameters<br />

without any dimensions. In this chapter, the focus is on the applying the old to unknown<br />

as different scales and the creation <strong>of</strong> dimensionless groups. These techniques gave birth<br />

to dimensional parameters which have a great scientific importance. Since the 1940s 1 ,<br />

the dimensional analysis is taught and written in all fluid mechanics textbooks. The<br />

approach or the technique used in these books is referred to as Buckingham–π–theory.<br />

The π–theory was coined by Buckingham. However, there is another technique which<br />

is referred to in the literature as the Nusselt’s method. Both these methods attempt<br />

to reduce the number <strong>of</strong> parameters which affect the problem and reduce the labor in<br />

solving the problem. The key in these techniques lays in the fact <strong>of</strong> consistency <strong>of</strong> the<br />

dimensions <strong>of</strong> any possible governing equation(s) and the fact that some dimensions<br />

are reoccurring. The Buckingham–π goes further and no equations are solved and even<br />

no knowledge about these equations is required. In Buckingham’s technique only the<br />

1 The history <strong>of</strong> dimensional analysis is complex. Several scientists used this concept before Buckingham<br />

and Nusselt (see below history section). Their work culminated at the point <strong>of</strong> publishing the<br />

paper Buckingham’s paper and independently constructed by Nusselt. It is interesting to point out<br />

that there are several dimensionless numbers that bear Nusselt and his students name, Nusselt number,<br />

Schmidt number, Eckert number. There is no known dimensionless number which bears Buckingham<br />

name. Buckingham’s technique is discussed and studied in <strong>Fluid</strong> <strong>Mechanics</strong> while almost completely<br />

ignored by Heat and Mass Transfer researchers and their classes. Furthermore, in many advance fluid<br />

mechanics classes Nusselt’s technique is used and Buckingham’s technique is abandoned. Perhaps this<br />

fact can be attributed to tremendous influence Nusselt and his students had on the heat transfer field.<br />

Even, this author can be accused for being bias as the Eckert’s last student. However, this author<br />

observed that Nusselt’s technique is much more effective as it will demonstrated later.<br />

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