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7.3 Determination of Pi Terms 339<br />

Step 1<br />

Δp = f(D, r, m , V)<br />

Step 2<br />

Δp = FL 3 , ...<br />

Step 3<br />

k–r = 3<br />

Step 4<br />

D, V, r<br />

Step 5<br />

1 = Δp D a V b r c<br />

Step 6<br />

2 = mD a V b r c<br />

Step 7<br />

_____ Δp D<br />

ρV 2 = F 0 L 0 T 0<br />

Step 8<br />

_____ Δp D<br />

ρV 2<br />

______ DΔp <br />

ρV 2<br />

m<br />

DVρ<br />

= ____<br />

<br />

_____ ρVD<br />

μ<br />

The method of repeating<br />

variables<br />

can be most easily<br />

carried out by following<br />

a step-bystep<br />

procedure.<br />

Note that we end up with the correct number of pi terms as determined from Step 3.<br />

At this point stop and check to make sure the pi terms are actually dimensionless 1Step 72.<br />

We will check using both FLT and MLT dimensions. Thus,<br />

or alternatively,<br />

Finally 1Step 82, we can express the result of the dimensional analysis as<br />

¢p / D<br />

f˜ rV a m<br />

2 DVr b<br />

This result indicates that this problem can be studied in terms of these two pi terms, rather than<br />

the original five variables we started with. The eight steps carried out to obtain this result are summarized<br />

by the figure in the margin.<br />

Dimensional analysis will not provide the form of the function f˜ . This can only be obtained<br />

from a suitable set of experiments. If desired, the pi terms can be rearranged; that is, the reciprocal<br />

of mDVr could be used, and of course the order in which we write the variables can be changed.<br />

Thus, for example, could be expressed as<br />

ß 2<br />

ß 1 ¢p /D<br />

rV 2<br />

ß 2 <br />

ß 1 ¢p /D<br />

rV 2<br />

ß 2 <br />

ß 1<br />

ß 2<br />

and the relationship between and as<br />

<br />

1FL 3 21L2<br />

1FL 4 T 2 21LT 1 2 2 F 0 L 0 T 0<br />

m<br />

DVr 1FL 2 T 2<br />

1L21LT 1 21FL 4 T 2 2 F 0 L 0 T 0<br />

1ML2 T 2 21L2<br />

1ML 3 21LT 1 2 2 M 0 L 0 T 0<br />

m<br />

DVr 1ML1 T 1 2<br />

1L21LT 1 21ML 3 2 M 0 L 0 T 0<br />

D ¢p /<br />

rV 2<br />

ß 2 rVD<br />

m<br />

f a rVD<br />

m b<br />

as shown by the figure in the margin.<br />

This is the form we previously used in our initial discussion of this problem 1Eq. 7.22. The<br />

dimensionless product rVDm is a very famous one in <strong>fluid</strong> <strong>mechanics</strong>—the Reynolds number.<br />

This number has been briefly alluded to in Chapters 1 and 6 and will be further discussed in Section<br />

7.6.<br />

To summarize, the steps to be followed in performing a dimensional analysis using the method<br />

of repeating variables are as follows:<br />

Step 1 List all the variables that are involved in the problem.<br />

Step 2 Express each of the variables in terms of basic dimensions.<br />

Step 3 Determine the required number of pi terms.<br />

Step 4 Select a number of repeating variables, where the number required is equal to the number<br />

of reference dimensions 1usually the same as the number of basic dimensions2.<br />

Step 5 Form a pi term by multiplying one of the nonrepeating variables by the product of<br />

repeating variables each raised to an exponent that will make the combination<br />

dimensionless.<br />

Step 6 Repeat Step 5 for each of the remaining nonrepeating variables.<br />

Step 7 Check all the resulting pi terms to make sure they are dimensionless and independent.<br />

Step 8 Express the final form as a relationship among the pi terms and think about what it<br />

means.

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