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Basics of Fluid Mechanics, 2014a

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10.4. CONFORMING MAPPING 371<br />

The uniform flow is revisited here with a connection to the complex numbers<br />

presentation. In the previous section, the uniform flow was present as the flow from<br />

the left to right. Here, this presentation will be expanded. The connection between<br />

the mathematical presentation to the physical flow is weak at best and experience is<br />

required. One can consider the flow that described by the function<br />

The the complex flow is<br />

F (z) =cz = c (x + i ) (10.213)<br />

W = dF<br />

dz = c (10.214)<br />

The complex velocity was found to be represented as<br />

W = c = U x − iU y (10.215)<br />

There are three extreme cases that need to be examined. The first case is when c is a<br />

real number. In that case, it requires that U x = c which is exactly the case that was<br />

presented earlier. The case the constant is imaginary resulting in<br />

U x − iU y = −ic (10.216)<br />

When it was chosen that the constant value is negative it yields<br />

U y = c (10.217)<br />

This kind <strong>of</strong> flow is when the direction is upward and was not discussed in the standard<br />

presentation earlier. The third case, the constant is a complex number. In that case,<br />

the complex number is present in either polar coordinate for convenience or in Cartesian<br />

coordinate to be as<br />

The complex velocity will be then<br />

Hence the component <strong>of</strong> the velocity are<br />

F (z) =ce −iθ z (10.218)<br />

W (z) =c cos θ − ic sin θ (10.219)<br />

U x = c cos θ<br />

U y = c sin θ (10.220)<br />

This flow is the generalized uniform flow where the flow is in arbitrary angle with the<br />

coordinates. In general the uniform flow is described in two–dimensional field as<br />

F (z) =U 0 e −iθ z (10.221)

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