THE VELOCITY INDUCED BY A STRAIGHT VORTEX SEGMENT

In this section, the velocity induced by a straight vortex line segment is derived, based on the Biot-Savart law. It is clear that a vortex line cannot start or end in a fluid, and the following discussion is aimed at developing the contribution of a segment that is a section of a continuous vortex line. The vortex segment is placed at an arbitrary orientation in the (x, y, z) frame with constant circulation Г, as shown in Fig. 2.14. The velocity induced by this

Подпись: /  /  d?e P У
Подпись: z

FIGURE 2.14

Velocity induced by a straight vortex segment.

Подпись: vortex segment will have tangential components only, as indicated in the figure. Also, the difference r0 -14 between the vortex segment and the point P is r. According to the Biot-Savart law (Eq. 2.68a) the velocity induced by a segment dl on this line, at a point P, is 4 Г dl X r A, = 4* r' (2.68 b) This may be rewritten in scalar form л r sin P J, A<7e = 2 dl Ал r (2.68c)

From the figure it is clear that

d = r cos /3

d

l = d tan в and dl = —5— dp

cos p

Substituting these into Дqe

Подпись:—%To dP = T~Jsin P dP

cos P And

This equation can be integrated over a section (1—»2) of the straight vortex segment of Fig. 2.15

(<?e)1’2 = 4ndjp sin PdP = ^ (cos /^i – cos P2) (2.69)

The results of this equation are shown schematically in Fig. 2.15. Thus, the velocity induced by a straight vortex segment is a function of its strength Г, the distance d, and the two view angles /3,, p2.

For the two-dimensional case (infinite vortex length) рг=0, p2~ л and

image63(2.70)

For the semi-infinite vortex line that starts at point О in Fig. 2.14, /31 = л/2 and p2 = л and the induced velocity is

image64(2.71)

which is exactly half of the previous value.

Equation (2.68b) can be modified to a form that is more convenient for numerical computations by using the definitions of Fig. 2.16. For the general three-dimensional case the two edges of the vortex segment will be located by Г! and r2 and the vector connecting the edges is

ro = r2 – rl

FIGURE 2.16

image65,image66

as shown in Fig. 2.16. The distance d, and the cosines of the angles /3 are then

The direction of the velocity qt 2 is normal to the plane created by the point P and the vortex edges 1, 2 and is given by

fi Xr2

ІГі X r2|

and by substituting these quantities, and by multiplying with this directional vector the induced velocity is

image67(2.72)

A more detailed procedure for using this formula when the (x, y, z) values of the points 1, 2, and P are known is provided in Section 10.4.5.