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Basics of Fluid Mechanics, 2014a

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372 CHAPTER 10. POTENTIAL FLOW<br />

This flow contains two extremes cases discussed earlier horizontal and vertical flow.<br />

Flow in a Sector<br />

The uniform flow presentation seem to be just repeat <strong>of</strong> what was done in the<br />

presentation without the complex numbers. In sector flow is an example where the<br />

complex number presentation starts to shine. The sector flow is referred to as a flow in<br />

sector. Sector is a flow in opening with specific angle.The potential is defined as<br />

F (z) =U 0 z n (10.222)<br />

where n ≥ 1 the relationship between the n and opening angle will be established in<br />

this development. The polar represented is used in this derivations as z = re iθ and<br />

substituting into equation (10.222) provides<br />

The potential function is<br />

and the stream function is<br />

F (z) =U 0 r n cos(nθ)+iU 0 r n sin(nθ) (10.223)<br />

φ = U 0 r n cos(nθ) (10.224)<br />

ψ = U 0 r n sin(nθ) (10.225)<br />

The stream function is zero in two extreme cases: one when the θ =0and two when<br />

θ = π/n. The stream line where ψ =0are radial lines at the angles and θ =0and<br />

θ = π/n. The zone between these two line the streamline are defined by the equation<br />

<strong>of</strong> ψ = U 0 r n sin(nθ). The complex velocity can be defined as the velocity along these<br />

lines and is<br />

W (z) =nU 0 z n−1 = nU 0 r n−1 e i (n−1)θ =<br />

= nU 0 r n−1 cos(nθ)+inU 0 r n−1 sin(nθ) e iθ (10.226)<br />

Thus the velocity components are<br />

and<br />

U r = nU 0 r n−1 cos(nθ) (10.227)<br />

U θ = −nU 0 r n−1 sin(nθ) (10.228)<br />

It can be observed that the radial velocity is positive in the range <strong>of</strong> 0

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