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(11) | EP 1 275 760 A2 |
(12) | EUROPEAN PATENT APPLICATION |
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(54) | Weft conveying nozzle in an air jet loom |
(57) A deflective inflow portion 18 is formed at the forward end of a flow passage forming
portion 141 of a thread guide 14. The deflective inflow portion 18 is formed by cutting
the forward end portion of the flow passage forming portion 141 along a plane S obliquely
intersecting the center axis line L of a weft passage 143. When forming the deflective
inflow portion S by cutting along the plane S, the cutting is effected from the outlet
144 of the weft passage 143 toward the inlet 145 of the weft passage 143. The deflective
inflow portion 18 is entirely surrounded by an air flow passage 16. |
BACKGROUND OF THE INVENTION
1. Field of the Invention
2. Description of the Related Art
SUMMARY OF THE INVENTION
BRIEF DESCRIPTION OF THE DRAWINGS
Figs. 1A through 1C show a first embodiment of the present invention, in which Fig. 1A is a side sectional view, Fig. 1B is an enlarged main portion sectional view, and Fig. 1C is an enlarged main portion perspective view;
Fig. 2 is an enlarged main portion side sectional view for illustrating flow velocity distribution of the present invention;
Fig. 3 is an enlarged main portion side sectional view showing a second embodiment of the present invention;
Fig. 4 is an enlarged main portion side sectional view showing a third embodiment of the present invention;
Fig. 5 is an enlarged main portion side sectional view showing a fourth embodiment of the present invention; and
Fig. 6 is an enlarged main portion side sectional view for illustrating flow velocity distribution in the prior art.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
(1-1) In Fig. 2, the arrows in the air flow passage 16, in the vicinity of the outlet
of the weft passage 143, and in the traction passage 133 directly in front of the
outlet of the weft passage 143 indicate air flow velocity. Fig. 2 shows the flow velocity
distribution in the air flow passage 16, in the vicinity of the outlet of the weft
passage 143, and in the traction passage 133 directly in front of the outlet of the
weft passage 143 in the first embodiment when the pressure of the compressed air supplied
to the weft conveying nozzle 11 is 1 kg/cm2. In Fig. 6, the arrows in the air flow passage 16A, in the vicinity of the outlet
of the weft passage 143A, and in the traction passage 133A directly in front of the
outlet of the weft passage 143A indicate air flow velocity. Fig. 6 shows the flow
velocity distribution in the air flow passage 16A, in the vicinity of the outlet of
the weft passage 143A, and in the traction passage 133A in the base tube 131A directly
in front of the outlet of the weft passage 143A when the pressure of the compressed
air supplied to the weft conveying nozzle 11 is 1 kg/cm2 in the prior art with no deflective inflow portion 18. In both Figs. 2 and 6, the
flow velocity distribution is obtained through theoretical calculation on the assumption
that the diameter of the weft passage 143, 143A is approximately several mm. In Figs.
2 and 6, the longer the arrow, the higher the flow velocity. The maximum flow velocity
is approximately equal to sound velocity.
In the conventional weft conveying nozzle 11A of Fig. 6, the air flow velocity directly
in front of the outlet of the thread guide 14A is minimum in the vicinity of the extension
of the center axis line L of the weft passage 143A in the thread guide 14A. The air
flow around the outlet of the thread guide 14A is symmetrical with respect to the
periphery of the outlet of the thread guide 14A. Most of the air flow from the air
flow passage 16A to the traction passage 133A is substantially parallel to the inner
peripheral surface of the base tube 131A. This directivity in outflow is due to the
symmetry of the cylindrical configuration of the thread guide 14A at the outlet of
the thread guide 14A, that is, the symmetry of the air flow passage 16A in the periphery
of the outlet of the thread guide 14A.
In the weft conveying nozzle 11 of Fig. 2, the air flow velocity directly in front
of the outlet of the thread guide 14 is minimum in the close vicinity of the inner
peripheral surface of the base tube 131. And, the air flow velocity in the vicinity
of the extension of the center axis line L of the weft passage 143 is high. The air
flow around the outlet of the thread guide 14 is asymmetrical with respect to the
periphery of the outlet of the thread guide 14. The outflow of air from the air flow
passage 16 to the traction passage 133 shows a wide directivity ranging from the direction
substantially parallel to the plane S for forming the deflective inflow portion 18
to the direction substantially parallel to the inner peripheral surface of the base
tube 131. This directivity in outflow is due to the existence of the deflective inflow
portion 18.
The existence of the deflective inflow portion 18 shifts, directly in front of the
outlet of the thread guide 14, the minimum velocity portion of the air flow from the
vicinity of the extension of the center axis line L of the weft passage 143 toward
the inner peripheral surface of the base tube 131, causing a high velocity air flow
to enter the vicinity of the extension of the center axis line L. Thus, the high velocity
portion of the air flow directly in front of the outlet of the thread guide 14 is
effectively utilized in the flying of the weft Y, and an improvement is achieved in
terms of weft driving force. Thus, it is possible to provide a weft conveying nozzle
advantageous in achieving an increase in weft inserting speed.
(1-2) As shown in Fig. 6, a swirl Q1 is symmetrically generated in the forward end
portion of the thread guide 14A. When injection-inserting two wefts of the same kind
alternately from a pair of weft conveying nozzles 11, air under a pressure of approximately
1 kg/cm2 is supplied to the weft conveying nozzle 11 for the weft at standby for weft insertion
so that the weft at standby for weft insertion may not be detached from the weft conveying
nozzle 11. In this case, it is likely that the symmetrical swirl Q1 adversely affect
the weft Y at standby for weft insertion. In particular, in the case of a filament
thread, unweaving is likely to occur, which leads to a weaving flaw.
As shown in Fig. 2, a swirl Q2 is also generated in the forward end portion of the
thread guide 14. However, the generation of the swirl Q2 is asymmetrical. This difference
between the swirls Q1 and Q2 is due to the existence of the deflective inflow portion
18, and the influence of the swirl Q2 on the weft at standby for weft insertion is
smaller than that of the swirl Q1 on the weft at standby for weft insertion, no unweaving
occurring even in the case of a filament thread.
(1-3) Generally speaking, the diameter of the weft passage 143 of the thread guide 14 for passing the weft Y is as small as severalmm. Thus, when forming a number of deflective in flow portions at the forward end of the thread guide by cutting as in the case of the thread passing nozzle disclosed in Japanese Patent Application Laid-Open No. Hei 9-21035, a very sophisticated machining technique is required. In contrast, the formation of the unitary deflective inflow portion 18 by cutting can be effected relatively easily.
(1-4) The construction in which the deflective inflow portion 18 is formed by cutting the forward end portion of the thread guide 14 along the plane S so as to slice the weft passage 143 is the most simple from the viewpoint of the formation of the deflective inflow portion 18.