fluid_mechanics
340 Chapter 7 ■ Dimensional Analysis, Similitude, and Modeling E XAMPLE 7.1 Method of Repeating Variables GIVEN A thin rectangular plate having a width w and a height h is located so that it is normal to a moving stream of fluid as shown in Fig. E7.1. Assume the drag, d, that the fluid exerts on the plate is a function of w and h, the fluid viscosity and density, and , respectively, and the velocity V of the fluid approaching the plate. SOLUTION FIND Determine a suitable set of pi terms to study this problem experimentally. V ρ, μ w h V7.2 Flow past a flat plate From the statement of the problem we can write where this equation expresses the general functional relationship between the drag and the several variables that will affect it. The dimensions of the variables 1using the MLT system2 are We see that all three basic dimensions are required to define the six variables so that the Buckingham pi theorem tells us that three pi terms will be needed 1six variables minus three reference dimensions, k r 6 32. We will next select three repeating variables such as w, V, and r. A quick inspection of these three reveals that they are dimensionally independent, since each one contains a basic dimension not included in the others. Note that it would be incorrect to use both w and h as repeating variables since they have the same dimensions. Starting with the dependent variable, d, the first pi term can be formed by combining d with the repeating variables such that and in terms of dimensions d f 1w, h, m, r, V 2 d MLT 2 w L h L m ML 1 T 1 r ML 3 V LT 1 ß 1 dw a V b r c 1MLT 2 21L2 a 1LT 1 2 b 1ML 3 2 c M 0 L 0 T 0 Thus, for ß 1 to be dimensionless it follows that 1 c 0 1for M2 1 a b 3c 0 1for L2 2 b 0 1for T 2 and, therefore, a 2, b 2, and c 1. The pi term then becomes ß 1 d w 2 V 2 r Next the procedure is repeated with the second nonrepeating variable, h, so that ß 2 hw a V b r c F I G U R E E7.1 It follows that and so that a 1, b 0, c 0, and therefore with The remaining nonrepeating variable is m so that and, therefore, Solving for the exponents, we obtain a 1, b 1, c 1 so that ß 3 m wVr Now that we have the three required pi terms we should check to make sure they are dimensionless. To make this check we use F, L, and T, which will also verify the correctness of the original dimensions used for the variables. Thus, ß 1 ß 2 h w 1L2 1L2 F 0 L 0 T 0 ß 3 1L21L2 a 1LT 1 2 b 1ML 3 2 c M 0 L 0 T 0 c 0 1for M2 1 a b 3c 0 1for L2 b 0 1for T 2 ß 2 h w ß 3 mw a V b r c 1ML 1 T 1 21L2 a 1LT 1 2 b 1ML 3 2 c M 0 L 0 T 0 1 c 0 1for M2 1 a b 3c 0 1for L2 1 b 0 1for T2 d w 2 V 2 r 1F2 1L2 2 1LT 1 2 2 1FL 4 T 2 2 F 0 L 0 T 0 m wVr 1FL 2 T 2 1L21LT 1 21FL 4 T 2 2 F 0 L 0 T 0
7.4 Some Additional Comments about Dimensional Analysis 341 If these do not check, go back to the original list of variables and make sure you have the correct dimensions for each of the variables and then check the algebra you used to obtain the exponents a, b, and c. Finally, we can express the results of the dimensional analysis in the form d w 2 V 2 r f˜ a h w , m wVr b (Ans) Since at this stage in the analysis the nature of the function f˜ is unknown, we could rearrange the pi terms if we so desire. For example, we could express the final result in the form d w 2 rV f aw 2 h , rVw m b (Ans) which would be more conventional, since the ratio of the plate width to height, wh, is called the aspect ratio, and rVwm is the Reynolds number. COMMENT To proceed, it would be necessary to perform a set of experiments to determine the nature of the function f, as discussed in Section 7.7. 7.4 Some Additional Comments about Dimensional Analysis The preceding section provides a systematic approach for performing a dimensional analysis. Other methods could be used, although we think the method of repeating variables is the easiest for the beginning student to use. Pi terms can also be formed by inspection, as is discussed in Section 7.5. Regardless of the specific method used for the dimensional analysis, there are certain aspects of this important engineering tool that must seem a little baffling and mysterious to the student 1and sometimes to the experienced investigator as well2. In this section we will attempt to elaborate on some of the more subtle points that, based on our experience, can prove to be puzzling to students. It is often helpful to classify variables into three groups— geometry, material properties, and external effects. 7.4.1 Selection of Variables One of the most important, and difficult, steps in applying dimensional analysis to any given problem is the selection of the variables that are involved. As noted previously, for convenience we will use the term variable to indicate any quantity involved, including dimensional and nondimensional constants. There is no simple procedure whereby the variables can be easily identified. Generally, one must rely on a good understanding of the phenomenon involved and the governing physical laws. If extraneous variables are included, then too many pi terms appear in the final solution, and it may be difficult, time consuming, and expensive to eliminate these experimentally. If important variables are omitted, then an incorrect result will be obtained; and again, this may prove to be costly and difficult to ascertain. It is, therefore, imperative that sufficient time and attention be given to this first step in which the variables are determined. Most engineering problems involve certain simplifying assumptions that have an influence on the variables to be considered. Usually we wish to keep the problem as simple as possible, perhaps even if some accuracy is sacrificed. A suitable balance between simplicity and accuracy is a desirable goal. How “accurate” the solution must be depends on the objective of the study; that is, we may be only concerned with general trends and, therefore, some variables that are thought to have only a minor influence in the problem may be neglected for simplicity. For most engineering problems 1including areas outside of fluid mechanics2, pertinent variables can be classified into three general groups—geometry, material properties, and external effects. Geometry. The geometric characteristics can usually be described by a series of lengths and angles. In most problems the geometry of the system plays an important role, and a sufficient number of geometric variables must be included to describe the system. These variables can usually be readily identified. Material Properties. Since the response of a system to applied external effects such as forces, pressures, and changes in temperature is dependent on the nature of the materials involved in the system, the material properties that relate the external effects and the responses must be included as variables. For example, for Newtonian fluids the viscosity of the fluid is the property that relates the applied forces to the rates of deformation of the fluid. As the material behavior becomes more complex, such as would be true for non-Newtonian fluids, the determination of material properties becomes difficult, and this class of variables can be troublesome to identify.
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7.4 Some Additional Comments about Dimensional Analysis 341<br />
If these do not check, go back to the original list of variables and<br />
make sure you have the correct dimensions for each of the variables<br />
and then check the algebra you used to obtain the exponents<br />
a, b, and c.<br />
Finally, we can express the results of the dimensional analysis<br />
in the form<br />
d<br />
w 2 V 2 r f˜ a h w , m<br />
wVr b<br />
(Ans)<br />
Since at this stage in the analysis the nature of the function f˜ is<br />
unknown, we could rearrange the pi terms if we so desire. For<br />
example, we could express the final result in the form<br />
d<br />
w 2 rV f aw 2 h , rVw<br />
m b<br />
(Ans)<br />
which would be more conventional, since the ratio of the plate<br />
width to height, wh, is called the aspect ratio, and rVwm is the<br />
Reynolds number.<br />
COMMENT To proceed, it would be necessary to perform a<br />
set of experiments to determine the nature of the function f, as<br />
discussed in Section 7.7.<br />
7.4 Some Additional Comments about Dimensional Analysis<br />
The preceding section provides a systematic approach for performing a dimensional analysis. Other<br />
methods could be used, although we think the method of repeating variables is the easiest for the<br />
beginning student to use. Pi terms can also be formed by inspection, as is discussed in Section 7.5.<br />
Regardless of the specific method used for the dimensional analysis, there are certain aspects of<br />
this important engineering tool that must seem a little baffling and mysterious to the student 1and<br />
sometimes to the experienced investigator as well2. In this section we will attempt to elaborate on<br />
some of the more subtle points that, based on our experience, can prove to be puzzling to students.<br />
It is often helpful to<br />
classify variables<br />
into three groups—<br />
geometry, material<br />
properties, and external<br />
effects.<br />
7.4.1 Selection of Variables<br />
One of the most important, and difficult, steps in applying dimensional analysis to any given problem<br />
is the selection of the variables that are involved. As noted previously, for convenience we will<br />
use the term variable to indicate any quantity involved, including dimensional and nondimensional<br />
constants. There is no simple procedure whereby the variables can be easily identified. Generally,<br />
one must rely on a good understanding of the phenomenon involved and the governing physical<br />
laws. If extraneous variables are included, then too many pi terms appear in the final solution, and<br />
it may be difficult, time consuming, and expensive to eliminate these experimentally. If important<br />
variables are omitted, then an incorrect result will be obtained; and again, this may prove to be<br />
costly and difficult to ascertain. It is, therefore, imperative that sufficient time and attention be<br />
given to this first step in which the variables are determined.<br />
Most engineering problems involve certain simplifying assumptions that have an influence on<br />
the variables to be considered. Usually we wish to keep the problem as simple as possible, perhaps<br />
even if some accuracy is sacrificed. A suitable balance between simplicity and accuracy is a desirable<br />
goal. How “accurate” the solution must be depends on the objective of the study; that is, we may be<br />
only concerned with general trends and, therefore, some variables that are thought to have only a minor<br />
influence in the problem may be neglected for simplicity.<br />
For most engineering problems 1including areas outside of <strong>fluid</strong> <strong>mechanics</strong>2, pertinent variables<br />
can be classified into three general groups—geometry, material properties, and external effects.<br />
Geometry. The geometric characteristics can usually be described by a series of lengths<br />
and angles. In most problems the geometry of the system plays an important role, and a sufficient<br />
number of geometric variables must be included to describe the system. These variables can usually<br />
be readily identified.<br />
Material Properties. Since the response of a system to applied external effects such as<br />
forces, pressures, and changes in temperature is dependent on the nature of the materials involved<br />
in the system, the material properties that relate the external effects and the responses must be included<br />
as variables. For example, for Newtonian <strong>fluid</strong>s the viscosity of the <strong>fluid</strong> is the property<br />
that relates the applied forces to the rates of deformation of the <strong>fluid</strong>. As the material behavior becomes<br />
more complex, such as would be true for non-Newtonian <strong>fluid</strong>s, the determination of material<br />
properties becomes difficult, and this class of variables can be troublesome to identify.