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4.1 The Velocity Field 149<br />

E XAMPLE 4.1<br />

Velocity Field Representation<br />

GIVEN A velocity field is given by V 1V 0/2 1 xî yĵ2<br />

where and / are constants.<br />

V 0<br />

FIND At what location in the flow field is the speed equal to<br />

V 0 ? Make a sketch of the velocity field for x 0 by drawing arrows<br />

representing the <strong>fluid</strong> velocity at representative locations.<br />

SOLUTION<br />

The x, y, and z components of the velocity are given by<br />

u V 0 x/, v V 0 y/, and w 0 so that the <strong>fluid</strong> speed, V, is<br />

V 1u 2 v 2 w 2 2 1 2 V 0<br />

/ 1x 2 y 2 2 1 2<br />

The speed is V V 0 at any location on the circle of radius / centered<br />

at the origin 31x 2 y 2 2 12 /4 as shown in Fig. E4.1a. (Ans)<br />

The direction of the <strong>fluid</strong> velocity relative to the x axis is given<br />

in terms of u arctan 1vu2 as shown in Fig. E4.1b. For this flow<br />

tan u v u <br />

V 0 y/<br />

V 0 x/ <br />

Thus, along the x axis 1y 02 we see that tan u 0, so that<br />

u 0° or u 180°. Similarly, along the y axis 1x 02 we obtain<br />

tan u q so that u 90° or u 270°. Also, for y 0 we<br />

find V 1V 0 x/2î, while for x 0 we have V 1V 0 y/2ĵ,<br />

y<br />

x<br />

(1)<br />

indicating 1if V 0 7 02 that the flow is directed away from the origin<br />

along the y axis and toward the origin along the x axis as<br />

shown in Fig. E4.1a.<br />

By determining V and u for other locations in the x–y plane, the<br />

velocity field can be sketched as shown in the figure. For example,<br />

on the line y x the velocity is at a 45° angle relative to the x axis<br />

1tan u vu yx 12. At the origin x y 0 so that<br />

V 0. This point is a stagnation point. The farther from the origin<br />

the <strong>fluid</strong> is, the faster it is flowing 1as seen from Eq. 12. By careful<br />

consideration of the velocity field it is possible to determine considerable<br />

information about the flow.<br />

COMMENT The velocity field given in this example approximates<br />

the flow in the vicinity of the center of the sign shown in<br />

Fig. E4.1c. When wind blows against the sign, some air flows<br />

over the sign, some under it, producing a stagnation point as indicated.<br />

y<br />

2V 0<br />

2<br />

<br />

V 0<br />

V 0 /2<br />

V<br />

u<br />

θ<br />

v<br />

(b)<br />

V 2V 0<br />

0<br />

0 x<br />

y<br />

−<br />

V 0<br />

V = 0<br />

x<br />

−2<br />

2V 0<br />

(c)<br />

(a)<br />

F I G U R E E4.1

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