dU
c1-- - c2 VR = 0, (14)
dt
dV
c2-- + (c1 U + [xi])R = 0, (15)
dt
dR
c3-- - (c1U + [xi] - c2 U)V = 0; (16)
dt
showing the modification of the equations of plane motion, due to the
component [xi] of the circulation.
dU
c1-- - c2 VR = 0, (14)
dt
dV
c2-- + (c1 U + [xi])R = 0, (15)
dt
dR
c3-- - (c1U + [xi] - c2 U)V = 0; (16)
dt
showing the modification of the equations of plane motion, due to the
component [xi] of the circulation.