| w = (U2 + V2) | a2 | z | + | a2b2 | U + Vi | ||
| b2 − a2 | U + Vi | b2 − a2 | z |
| −(U12 + V12) | b2 | z | − | a2b2 | U1 + V1i | . | ||
| b2 − a2 | U1 + V1i | b2 − a2 | z |
(19)
The resultant impulse of the liquid on the cylinder is given by the component, over r = a (§ 36),
| X = ∫ ρφ cos θ·a dθ = πρa2 ( U | b2 + a2 | − U1 | 2b2 | ); |
| b2 − a2 | b2 − a2 |
(20)
and over r = b
| X1 = ∫ ρφ cos θ·b dθ = πρb2 ( U | 2a2 | − U1 | b2 + a2 | ), |
| b2 − a2 | b2 − a2 |
(21)
and the difference X − X1 is the component momentum of the liquid in the interspace; with similar expressions for Y and Y1.