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Mechanics of Fluids

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9.6.2 Flow from a line source<br />

A source is a point from which fluid issues uniformly in all directions. If, for<br />

two-dimensional flow, the flow pattern consists <strong>of</strong> streamlines uniformly<br />

spaced and directed radially outwards from one point in the reference plane<br />

(as in Fig. 9.16), the flow is said to emerge from a line source. (We remember<br />

that for two-dimensional flow what appears on the diagram as a point is to<br />

be regarded as a line seen end on.) The strength m <strong>of</strong> a source is the total<br />

volume rate <strong>of</strong> flow from it, the line source <strong>of</strong> two-dimensional flow being<br />

considered <strong>of</strong> unit length. The velocity q at radius r is given by<br />

Volume rate <strong>of</strong> flow ÷ Area perpendicular to velocity = m/2πr<br />

for unit depth, since the velocity is entirely in the radial direction. As r → 0,<br />

q →∞and so no exact counterpart <strong>of</strong> a source is found in practice. However,<br />

except at the singular point r = 0, a similar flow pattern would be<br />

achieved by the uniform expansion <strong>of</strong> a circular cylinder forcing fluid away<br />

from it, or, more approximately, by the uniform emission <strong>of</strong> fluid through<br />

the walls <strong>of</strong> a porous cylinder. Nevertheless, the concept <strong>of</strong> a source has its<br />

chief value in providing a basic mathematical pattern <strong>of</strong> flow which, as we<br />

shall see, can be combined with other simple patterns so as to describe flows<br />

closely resembling those found in practice.<br />

In cases such as this, where circular symmetry is involved, polar coordinates<br />

are more suitable. The velocity qr radially outwards = ∂ψ/∂n =<br />

−∂ψ/r∂θ. The minus sign arises from the ‘right-to-left’ convention and the<br />

fact that the angle θ is considered positive anti-clockwise; the length ∫ r dθ <strong>of</strong><br />

a circumferential line therefore increases in the anti-clockwise direction, and<br />

to an observer on this line and facing that direction, the radially outward<br />

flow would appear to move from left to right, that is, in the negative direction.<br />

A tangential velocity qt is given by ∂ψ/∂r; if one looked outwards along<br />

the radius one would see a positive (i.e. anticlockwise) tangential velocity<br />

coming from one’s right and so the sign here is positive.<br />

Basic patterns <strong>of</strong> flow 375<br />

Fig. 9.16

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