Forces and Moment

The flow is assumed to be inviscid, Cd = 0. At the blade element j the flow config­uration is as depicted in Fig. 10.11.

The local incidence is

Подпись: aПодпись: - tjForces and Moment(10.29)

where фj is called the flow angle and tj is the angle of twist at the element. The local lift coefficient is obtained from the result of thin airfoil theory or from an experimental or numerical profile lift curve C;(a). In thin airfoil theory, the lift is given by


Ci (a) = 2n(a + 2-) (10.30)


Подпись: d c Подпись: 1 2n Forces and Moment Подпись: (10.31)

d is the profile mean camber defined as

where d (x) is the equation of the camber line. According to the Kutta-Joukowski lift theorem, the lift force per unit span is perpendicular to the incoming flow, its

Fig. 10.11 Blade element

Подпись: z flow configuration

magnitude is L’ = pq Г and its orientation is 90° from the incoming flow direc­tion, rotating opposite to the circulation. q = q = ^(1 + u)2 + (ad – + wj2 is the normalized magnitude of the incoming flow velocity vector. This can be expressed mathematically as

~L ‘ = pU~cf Л URr~-f (10.32)

where dimensionless quantities have been introduced. ~j is the unit vector along the y-axis and Г < 0in Fig. 10.11. Upon a dimensionalization of the lift, the circulation is obtained as


Г] = — qjcJci (a j) (10.33)

The contribution of the blade element to thrust and torque can now be derived. Projection in the x-direction gives

dTj = L j cos фJRdyJ = – pUqj cos фJURГJRdyJ = —pU2 R2 гД^- + w Д dyj

Forces and Moment

or, upon integration

Projection of the lift force in the z-direction and accounting for the distance from the axis, the torque contribution reads

dTj = L’j sinфjRyjRdyj = pUqj sin ф^ URFjRyjRdyj = pU2R3rj (1 + Uj)yjdyj


Подпись: T = pU2 R3 Forces and Moment Подпись: (10.38)

which integrates to give

Подпись: CT Подпись: T 2 pU 2n R3 Forces and Moment Подпись: (10.39)

or, in dimensionless form

These results are for one blade. Total thrust and torque must account for all the blades.