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┃          ┃            ┃  ┃            ┃          ┃
┃          ┃            ┃  ┃            ┃          ┃
┃          ┣━━━━━━╋━╋━━━━━━┻━━━━━┫
┃          ┃            ┃  ┃                        ┃
┃          ┣━━━━━━┫  ┃                        ┃
┃          ┃      -.    ┃  ┃                        ┃
┃  b/2     ┃bl2 T       ┃  ┃                        ┃
┣━━━━━╋━━━━━━┻━┫                        ┃
┃          ┃                ┃                        ┃
┗━━━━━┻━━━━━━━━┻━━━━━━━━━━━━┛
Fig.4 27    Wingin rolling and yawing motion.
The resultant velocitjr at the strip RT is given by
VR
= ~Z+ (Py)2
N Uo
(4.559)
(4.560)
Let c(y) be the local chord and ao(Y) be the local sectionallift-curve slope of the
wing. The lift on the elemental strip RT is given by
                                     dL - ;:p Uo2ao(y)rytc(y)dy
                                     1
                               = ~pUo2ao(Y) [  + 7jY],(y)dy
The drag ori the elemental strip RT is given by
                                dD = ;:'pU2CD,lc(y)dy
(4.561)
(4.562)
(4.563)
EQUATIONS OF MOTION AND ESTIMATION OF STABILITY DERIVATIVES 409
where
                                             CD,I = CDO,L + CDor,ICt                               (4.564)
Here,  CD OJ iS the sectional zero-lift drag coefficient (profile drag coefficient when
CL  - O), and CDa,l is the incremental sectional profile drag coefficient per urut
angle of attack  Note that the strip theory ignores the induced drag.
     The normal force on the elemental strip RT is given by
                        dZ ~ -dL cos aP - dD sin a'P                                                        (4.565)
                 - -dL -
　
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