The present invention relates to an impact head and a printing apparatus such as an impact printer.
A conventional impact printer includes an impact head having a magnetic circuit formed of a york and an armature. In the impact head, the armature rotates to drive a print wire, so that the print wire hits a printing surface through an ink ribbon, thereby performing a printing operation (refer to Patent Reference).
Patent Reference: Japan Patent Publication No. 2806871
As shown in
A coil 4′ is disposed around the protruding portion F′ of the core 3′, and a control unit (not shown) applies a current to the coil 4′. A wire 2′ is fixed to a distal end portion of the armature 1′ through welding and the likes. A circular portion A′ is formed at a rear end portion of the armature 1′ as a rotational pivot.
A spring plate 8′ formed of an elastic member such as a plate spring urges the armature 1′ at a rear end portion thereof. Accordingly, the circular portion A′ formed at the rear end portion of the armature 1′ is pressed against the armature york 6′ and the core york 7′ in an arrow direction b, thereby functioning as the rotational pivot of the armature 1′.
The spring plate 8′ is fixed to a side of a head cover (not shown). A groove portion D′ is formed in a guide holder 9′ for guiding the distal end portion of the armature 1′ in the left to right direction to be movable in the vertical direction. A reset spring 5′ is disposed in a hole formed in a bottom surface of the groove portion D′ of the guide holder 9′.
The reset spring 5′ is formed of an urging member such as a coil spring. When the armature 1′ is set in the groove portion D′ of the guide holder 9′, the reset spring 5′ lifts the armature 1′ toward an upper surface of the core 3′ (in a reset direction). It is configured that the armature 1 moves to impact toward a bottom surface of the core 3′ (in an impact direction) against the urging force of the reset spring 5′.
As shown in
As shown in
In the reset state shown in
When an initial operation time T0 passes after the current Ia is applied at the timing (t=0), the armature force f1 balances with the urging force Qf2, and then the armature force f1 exceeds the urging force Qf2, thereby rotating the armature 1′ in the impact direction. When an impact time QTimp passes after the current Ia is applied at the timing (t=0), the armature 1′ reaches the impact position, thereby becoming the impact state shown in
When the current Ia is turned off, the armature force f1 disappears, so that the armature 1′ returns in the reset direction with the urging force of the reset spring 5′. When a reset time QTres passes after the current Ia is turned off, the armature 1′ returns to the reset state shown in
In order to shorten the cycle time QTc and perform the printing operation at a high speed, it is necessary to shorten both the impact time QTimp and the reset time QTres constituting the cycle time QTc.
In the conventional impact head 24′ of the clapper type described above, when the urging force Qf2 of the set spring 5′ decreases and the drive force Qf3 increases, the armature 1′ performs the impact operation in a shorter period of time. Accordingly, it is possible to decrease the initial operation time T0 and the impact time QTimp. In this case, however, the armature 1′ returns with the urging force Qf2 of the set spring 5′, thereby increasing the reset time QTres. Accordingly, it is difficult to shorten the cycle time Qtc after all.
When the urging force Qf2 of the set spring 5′ increases, on the other hand, it is possible to shorten the reset time QTres. However, the drive force Qf3 decreases, thereby increasing the initial operation time T0. As a result, the impact time QTimp increases, thereby increasing or making no change in the cycle time Qtc.
In view of the problems described above, an object of the present invention is to provide an impact head capable of solving the problems of the conventional impact head
Further objects and advantages of the invention will be apparent from the following description of the invention.
According to an aspect of the present invention, an impact head includes an arm member moving to a protruding position when a magnetic flux is generated and to a return position when the magnetic flux disappears; an impact member connected to the arm member for protruding when the arm member moves to the protruding position and returning to an original position when the arm member moves to the return position; and an urging member for urging the arm member with a restricted urging force when the magnetic flux is generated and urging the arm member to the return position when the magnetic flux disappears.
In the aspect of the present invention, the impact head includes the arm member moving to the protruding position when the magnetic flux is generated and to the return position when the magnetic flux disappears; the impact member connected to the arm member for protruding when the arm member moves to the protruding position and returning to the original position when the arm member moves to the return position; and the urging member for urging the arm member with the restricted urging force when the magnetic flux is generated and urging the arm member to the return position when the magnetic flux disappears. Accordingly, it is possible to shorten both an impact time and a reset time, thereby shortening a cycle time and performing a printing operation at a high speed.
Hereunder, embodiments of the present invention will be described in detail with reference to the accompanying drawings. In the drawings and the following description, similar components are designated with the same reference numerals. An impact printer will be explained as a printing apparatus, and the present invention is not limited thereto.
A first embodiment of the present invention will be explained with reference to
As shown in
In the embodiment, the carriage 33 is attached to the guide shaft 30 to be slidable thereon. When the pinion 40 engaging the rack 36 rotates, the carriage 33 moves along the platen 26 in the axial direction thereof. The impact head 24 is driven in synchronizing with the movement of the carriage 33, so that the impact head 24 prints on the sprocket sheet 22 around the platen 26.
More specifically, the carriage 33 with the impact head 24 mounted thereon slides along the guide shaft 30 extending in parallel to the platen 26, so that the impact head 24 moves in an arrow direction B′-B. In synchronizing with the movement of the impact head 24, a plurality of wires is driven in an arrow direction A to impact the sprocket sheet 22 through an ink ribbon (not shown) retained in an ink ribbon cassette 31, thereby printing on the sprocket sheet 22.
A configuration of the impact head 24 will be explained next.
As shown in
In the embodiment, a wire 2 is fixed to a distal end portion of the armature 1 through welding and the likes. A circular portion A is formed at a rear end portion of the armature 1 as a rotational pivot thereof. A spring plate 8 formed of an elastic member such as a leaf spring urges the armature 1 at a rear end portion thereof. Accordingly, the circular portion A formed at the rear end portion of the armature 1 is pressed against the armature york 6 and the core york 7 in an arrow direction b, thereby functioning as the rotational pivot of the armature 1.
In the embodiment, the spring plate 8 is fixed to a side of a head cover (not shown). A groove portion D is formed in a guide holder 9 for guiding the distal end portion of the armature 1 in the left to right direction to be movable in the vertical direction. A reset spring 5 is disposed in a hole formed in a bottom surface of the groove portion D of the guide holder 9. The reset spring 5 is formed of an urging member such as a coil spring. When the armature 1 is set in the groove portion D of the guide holder 9, the reset spring 5 lifts the armature 1 toward an upper surface of the core 3 (in a reset direction).
In the embodiment, the impact head 24 further includes a sub-spring 10 formed of an urging member such as a leaf spring with a magnetic property. An outer circumference of the sub-spring 10 is fixed with the armature york 6 or the core york 7. It may be configured such that the outer circumference of the sub-spring 10 is fixed with both the armature york 6 and the core york 7.
In the embodiment, an inner circumference of the sub-spring 10 is formed in a tongue shape, and each of the tongue shape is arrange to face the armature 1. A small piece 11 is disposed at a distal end portion of the tongue shape portion of the sub-spring 10 for lifting a lower portion of the armature 1. The distal end portion of the tongue shape portion of the sub-spring 10 is situated at a position facing the protruding portion F of the core 3.
In the embodiment, the sub-spring 10 has an urging force Δfs smaller than an urging force Δfr of the reset spring 5 (Δfs>Δfr). When a current is applied to the coil 4 to generate a magnetic flux, the protruding portion F of the core 3, the core 3, the core york 7, the sub-spring 10, the circular portion A of the armature 1, and the protruding portion E of the armature 1 constitute a first magnetic circuit. Further, when a current is applied to the coil 4 to generate a magnetic flux, the protruding portion F of the core 3, the core 3, the core york 7, and the sub-spring 10 constitute a second magnetic circuit.
In the embodiment, the small piece 11 is arranged to abut against the lower portion of the armature 1 upon resetting. Accordingly, it is preferred that the small piece 11 is formed of a non-magnetic material with a vibration absorbing property such a resin material as polyacetal (POM) and 66-nylon (PA66) containing 10% of glass beads or glass fibers.
An operation of the impact head 24 will be explained next with reference to
More specifically,
As shown in
In the embodiment, the spring plate 8 has a portion C for restricting the armature 1 urged by the reset spring 5 and the sub-spring 10 from rising. Accordingly, the protruding portion E of the armature 1 is separated from the protruding portion F of the core 3 by a distance Δx.
At this moment, as described above, the sub-spring 10 lifts the armature 1 with the urging force Δfs in the reset direction. Accordingly, the lower portion of the sub-spring 10 is separated from the protruding portion F of the core 3 by the distance Δx as well.
When the control unit (not shown) supplies a current to the coil 4 to generate a magnetic flux, the impact head 24 becomes the transition state shown in
Then, the armature 1 is attracted in the impact direction against the urging force Δfr of the reset spring 5, thereby becoming the impact state shown in
After applying the impact, when the control unit stops supplying the current to the coil 4, the magnetic flux disappears. Accordingly, the sub-spring 10 moves away from the core 3 and lifts the armature 1 with the urging force Δfs thereof. Further, the reset spring 5 lifts the armature 1 with the urging force Δfr thereof, so that the armature 1 returns to the reset state with a combinational force of the urging force Δfs and the urging force Δfr.
Note that, in
In the reset state shown in
As described above, it is configured that the sub-spring 10 has the urging force Δfs smaller than the urging force Δfr of the reset spring 5 (Δfs<Δfr). Accordingly, from the timing (t=0) to a timing (t=Δt), before the armature 1 is attracted to move, the sub-spring 10 with the smaller urging force is attracted to the protruding portion F of the core 3 as shown in
In the conventional impact head 24′ without the sub-spring 10, after the period of time T0, the combinational force f3 is generated to move the armature 1′. In the embodiment, with the sub-spring 10, after the period of time Δt, the combinational force f3 is generated to move the armature 1. When an impact time Timp passes after the current Ia is applied at the timing (t=0), the impact head 24 becomes the impact state as shown in
When the wire 2 reaches the impact position and the current Ia is turned off, the armature force f1 disappears. At the same time, the sub-spring 10 stops urging and the urging force Δfs is generated. Accordingly, the armature 1 returns in the reset direction with the combinational force f2 of the urging force Δfr of the reset spring 5 and the urging force Δfs of the sub-spring 10. When a reset time QTres passes after the current Ia is turned off, the armature 1 returns to the reset state shown in
As described above, in the embodiment, the small piece 11 is formed of the non-magnetic material with a vibration absorbing property. Accordingly, when the sub-spring 10 returns to the original shape to abut against the armature 1, it is possible to reduce a noise.
As described above, in the embodiment, the sub-spring 10 is provided in the impact head 24. Accordingly, when the current is turned on, the armature 1 quickly performs the impact operation and the impact time Timp decreases. When the current is turned off, the armature 1 quickly returns to the reset state, and the reset time Tres decreases. As a result, when the impact time QTimp and the reset time QTres represent a cycle time QTc, it is possible to shorten the cycle time QTc.
In the embodiment, it is configured that the sub-spring 10 functions as an auxiliary member for retuning the armature 1 to the reset state, thereby preserving energy corresponding to a current ΔP1 shown as a hatched portion in
As described above, in the printing apparatus in the first embodiment, the impact head 24 is configured such that the armature 1 or an arm member is driven toward the protruding portion of the core 3, and the reset spring 5 returns the arm member to the reset state. The small piece 11 formed of the non-magnetic material is disposed at the position away from the protruding portion of the core 3. Further, the sub-spring 10 is provided for urging the arm member away from the protruding portion of the core 3. Accordingly, it is possible to shorten the impact time and the reset time, thereby shortening the cycle time and increasing the print speed. Further, the sub-spring 10 functions as the auxiliary member for retuning the armature 1 to the reset state, thereby reducing energy consumption.
A second embodiment of the present invention will be explained next.
As shown in
An operation of the impact head 24 will be explained next. As described above, in the second embodiment, the protruding portion F of the core 3 is provided with the step portion 3a at the position near the small piece 11 of the sub-spring 10. Accordingly, when a same current is applied, it is possible to quickly increase a magnetic flux of the step portion 3a.
In general, an attraction force F of a coil is expressed as follows:
F=B
2
×S/2μ0
where B is a magnetic flux density, S is a sectional area of the core, and μ0 is a magnetic permeability. Further, the magnetic flux density B is expressed as follows:
B=Φ/S
where Φ is a magnetic flux.
From the above equations, the attraction force F is expressed as follows:
F=Φ
2(2μ0×S)
The magnetic flux Φ and the magnetic permeability μ0 are constant values, so that the attraction force F is disproportional to the sectional area S of the core.
As compared with the protruding portion F of the core 3 in the first embodiment, in the impact head 24 in the second embodiment, the protruding portion F of the core 3 has a smaller sectional area. Accordingly, the attraction force F increases disproportionally, thereby attracting the sub-spring 10 quicker.
In the embodiment, as shown in
Accordingly, in the impact state, it is possible to apply the impact in a period of time smaller than the impact time QTimp of the conventional impact head. Further, after an impact time Timp, the armature 1 returns to the reset state with a combinational force f2* of the urging force Δfs* of the sub-spring 10 and the urging force Δfr of the reset spring 5. Accordingly, it is possible to return the armature 1 to the reset state in a reset time Tres* shorter than the reset time Tres in the first embodiment, that is improved from the reset time QTres of the conventional impact head. As a result, when the impact time Timp and the reset time Tres* represent a cycle time Tc*, it is possible to further shorten the cycle time Tc*.
In the embodiment, it is configured that the sub-spring 10 functions as an auxiliary member for retuning the armature 1 to the reset state, thereby preserving energy corresponding to a current ΔP2 shown as a hatched portion in
As described above, in the embodiment, the protruding portion F of the core 3 is provided with the step portion 3a. Further, the sub-spring 10 has the urging force larger than that in the first embodiment. Alternatively, the sub-spring 10 may have the urging force the same as that in the first embodiment. In this case, the reset time Tres* becomes the same as the reset time Tres in the first embodiment. However, the protruding portion F of the core 3 is provided with the step portion 3a, so that the magnetic flux increases more quickly. Accordingly, it is possible to shorten the period of time Δt from when the armature 1 starts moving in the impact direction at the timing (t=0).
As described above, in the embodiment, the protruding portion F of the core 3 is provided with the step portion 3a at the position facing the small-piece 11 of the sub-spring 10, so that the magnetic flux increases more quickly. Further, the sub-spring 10 has the urging force larger than that in the first embodiment. Accordingly, it is possible to further shorten the reset time Tres*, thereby decreasing the cycle time Tc* and the print speed.
Further, it is configured that the sub-spring 10 functions as the auxiliary member for retuning the armature 1 to the reset state with the larger urging force, thereby further reducing energy consumption.
A third embodiment of the present invention will be explained next.
As shown in
As shown in
An operation of the impact head 24 will be explained next. As described above, the protruding portion F of the core 3 has the first opposite surface facing the protruding portion E of the armature 1, and the first opposite surface is situated at the level lower than the upper surface of the coil 4. Accordingly, the protruding portion F of the core 3 faces the protruding portion E of the armature 1 inside the coil 4. At this moment, the protruding portion F of the core 3 is provided with the protruding portion G at the position near the small piece 11 of the sub-spring 10, thereby having a positional relationship similar to those in the first and second embodiments.
Accordingly, it is possible to stably generate a strong magnetic flux. When the current Ia is supplied, it is possible to generate the attraction force f1 with a high level for attracting the armature 1 in the impact direction, and further to quickly rise the magnetic flux in the protruding portion G. More specifically, it is possible to shorten the impact time Timp with the attraction force f1 with the high level, and further to shorten the reset time with the urging force of the sub-spring 10 in the reset state, similar to the first and second embodiments.
As described above, in the embodiment, it is possible to increase the attraction force f1. Accordingly, when the urging force Δfr of the reset spring 5, i.e., the reaction force thereof, increases, and the combinational force f3 of the attraction forces f1 and f2 (=Δfs+Δfr) is set to be the same as the combinational force in the second embodiment, it is possible to further shorten the reset time Tres, as compared with those in the first and second embodiments.
In the third embodiment, similar to the second embodiment, the protruding portion F of the core 3 is provided with the step portion 3a. Alternatively, the protruding portion F of the core 3 may not be provided with the step portion 3a.
As described above, the protruding portion F of the core 3 is provided with the protruding portion G (the second opposite surface) at the position near the small piece 11 of the sub-spring 10. Further, the protruding portion F of the core 3 has the first opposite surface facing the protruding portion E of the armature 1, and the first opposite surface is situated at the level lower than an upper surface of the coil 4. Accordingly, it is possible to further shorten the reset time Tres, thereby decreasing the cycle time and the print speed.
In the embodiment described above, the armature york 6 and the core york 7 are laminated and fixed on the outer circumference of the sub-spring 10, and may be modified.
As shown in
As described above, the present invention is applicable to the printing apparatus such as the impact printer provided with the impact head of the clapper type, in which the wire is driven through the magnetic flux.
The disclosure of Japanese Patent Application No. 2008-086481, filed on Mar. 28, 2008, is incorporated in the application by reference.
While the invention has been explained with reference to the specific embodiments of the invention, the explanation is illustrative and the invention is limited only by the appended claims.
Number | Date | Country | Kind |
---|---|---|---|
2008-086481 | Mar 2008 | JP | national |