This paper describes flow characteristics in a weft-acceleration pipe of an air-jet loom, when a pressurized flow is given to a weft-guide pipe of the model-main nozzle. The central flow (flow in the wefl-guide pipe) includes not only flow naturally induced by pressurized annular flow, but also pressurized flow. Flow in the weftacceleration pipe was measured with a hot-wire anemometer when the flow-rate ratio, M, was changed stepwise. Where, M means the ratio of flow rate of the central flow to that of annular flow of the nozzle. Reynolds number in the acceleration pipc, Re, is constant (Re=1.7×10
4).
The following results are obtained by this experiment :
(1) When the central flow is only naturally-induced flow, the mean-velocity-vector distribution toward downstream from the nozzle exit is biased slightly to the pipe wall. Velocity defect along an axis of the acceleration pipe increases remarkably owing to entrainment by annular flow. A point, which shows the minimum ratio ofU
c to U
m, moves toward upstream according to reduction of M, and the minimum value of U √U
m decreases, where U
c is mean velocity along the axis of the pipe and U
m is mean velocity through a section of the pipe. Especially, when only naturally-induced flow is considered, U
cian, has two extreme values at two points, x/D is 1 and 2, where x is an axial distance from the inlet of the acceleration pipe and D is diameter of the pipe. However, when x/D≥4, the values of U
c/U
m are nearly equal at any Ms and recovered slowly. And, when x/D≥6, no significant difference among velocity-vector distribution according to change of M can be found.
(2) Under any Ms, the wall pressure near the exit of the nozzle goes terribly upand down along the axis of the pipe. As a result, flow is separated from nozzle-side edge of the acceleation-pipewall. It is assumed that recirculation zone occurs along the pipe wall when M≤0.76. When M is smaller, recirculation zone becomes wider accordingly.
(3) With M being smaller, stronger turbulent flow occurs across each section of the pipe, and turbulence is dampened more slowly toward downstream.
As described above, when an appropriate nozzle-flow-rate ratio, the ratio of central-flow rate to annular-flow rate, is applied to flow of the weft-acceleration pipe, it can be found that flow, effective to acceleration of weft, is generated under the conditions such as reduced velocity defect along the axis of the pipe and dampened turbulent flow in the pipe.
The results obtained by this experiment prove indirectly that the main nozzles inserial structure, being employed recently, is useful for establishing steady-flying behaviour of weft.
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