Patent Grant
6851780
1. Field of the Invention
The present invention relates to a driving method and apparatus for a liquid discharge head for use in printing as well as in manufacturing color filters, thin film transistors, light-emitting devices, DNA devices, and the like.
2. Related Background Art
A liquid discharge apparatus has begun to be used for producing printed materials as well as for a patterning process in manufacturing color filters, thin film transistors, light-emitting devices, DNA devices, and the like.
Photolithography is widely adopted for such an industrial patterning method. However, the photolithography requires many steps and the cost for devices is huge, while providing extremely low material-use efficiency. Meanwhile, offset printing has a limitation on use as an industrial patterning technique due to the precision thereof.
Under the circumstances, a patterning method using a liquid discharge head, which is also called ink jet method, has become popular. The ink jet method allows for direct plotting on a patterning portion, thereby providing extremely high material-use efficiency while requiring a small number of steps, which is a useful patterning technique with low running cost.
Well-known ink jet methods are of the Kyser type described in Japanese Patent Publication No. 53-12138 and of the thermal jet type disclosed in Japanese Patent Publication No. 61-59914 (U.S. Pat. No. 5,754,194).
A shear-mode ink jet method using a piezoelectric ceramic is disclosed in Japanese Patent Application Laid-Open No. 63-247051 (U.S. Pat. No. 4,879,568).
As shown in
An orifice plate 512 having a nozzle 510 is bonded to one end of each ink flow path 506, and electrodes 513 and 514 are provided as metallized layers on both sides of each actuator wall 503. More specifically, each actuator wall 503 is provided with the electrode 514 on the side of the ink flow path 506, and is provided with the electrode 513 on the side of the air chamber 508. The electrodes 513 facing the air chamber 508 are connected to a control circuit 520 for supplying an actuator driving signal, while the electrodes 514 defining the ink flow path 506 are connected to a ground.
A voltage is applied by the control circuit 520 to the electrodes 513 beside the air chambers 508, thus causing the actuator walls 503 to produce shear strain deformation in the direction where the volume of the ink flow paths 506 increases.
For example, as shown in
If the hydrodynamic resonant frequency of the inside of the ink flow path 506 is indicated by Fr, an inverse thereof is indicated by Tr (=1/Fr), and the time during which the voltage is applied is set to Tr/2, resonance across the system can be used, thereby making the amount of deformation greater than the original amount obtained as shear strain (non-resonance).
The hydrodynamic resonant frequency Fr can be determined by electric measurement using a well-known impedance measurement device.
After the lapse of the voltage-applying time Tr/2, the voltage applied to the electrodes 513 beside the air chambers 508 is reset to zero. Then, the actuator walls 505 and 507 are deformed so that the ink flow path 506 may contract more than the normal state where the actuator walls 505 and 507 are not deformed and form a straight flow path, thus causing ink to be pressurized. This allows the ink to flow into the nozzles 510, and ink droplets are expelled from the nozzles 510.
In conventional ink ejecting apparatuses of this type, the volume of an ink droplet to be ejected depends upon the shape of an ink flow path, a driving voltage, and the like. Therefore, the shape of an ink flow path and the driving voltage are determined so that desired volume of an ink droplet can be obtained. If an ink jet apparatus is used as an industrial plotter, however, there are demands for high-definition ink jet performance, and for shorter plotting time. In order to shorten the plotting time, it is necessary to reduce the number of pulses required for plotting as much as possible. For higher definition, the pitch of an ink flow path is made narrower, thereby increasing the definition. In order to narrow the pitch of an ink flow path, in view of the limitation of machining, the thickness of a PZT (lead zirconate titanate) wall, which is a piezoelectric ceramic wall and which can change the volume of the ink flow path, must be reduced, and the depth of the ink flow path must also be reduced. This further leads to a limitation of driving voltage. Eventually, a high-definition head reduces the amount of deformation cause by the PZT wall, resulting in a reduced amount of discharge per dot.
On the other hand, Japanese Patent Publication No. 3-30506 (U.S. Pat. No. 4,563,689) describes that an additional pulse is applied before an application of the main pulse in order to determine the top position of ink meniscus in a nozzle, thereby controlling the volume of an ink droplet. By applying an additional pulse, the volume of an ink droplet can be slightly, but not significantly, increased.
Japanese Patent Application Laid-Open No. 2000-280463 describes a proposed method in which the volume of an ink droplet is increased by providing a pulse having a width of 0.30 T to 1.10 T as an additional emission (first emission) pulse before an application of a main emission (second emission) pulse, where T denotes the pulse width of the main emission pulse. In this method, two ink droplets are discharged to form one dot, thus making it possible to increase the volume of an ink droplet by a factor of up to about 1.5. However, it is difficult to further increase the amount of discharge.
As proposed in Japanese Patent Publication No. 6-55513 (U.S. Pat. No. 5,202,659), in order to increase the amount of discharge, a plurality of ink droplets which are sequentially ejected using a resonant frequency are combined in the air to control the volume of the ink droplets. With this approach, it can be expected that the volume of ink droplets sufficiently increases.
In an industrial ink jet apparatus, however, if the distance between a nozzle and a plotted base is extremely shortened in order to increase the deposition precision, a plurality of liquid drops are not combined in the air, but reach the base individually. In other words, there occurs a time lag in ink droplets to be applied for one-dot plotting, causing the reached drops do not form perfect circles, resulting in a failure of deposition precision.
Accordingly, it is an object of the present invention to provide a driving method and apparatus for a liquid discharge head in which the volume of a liquid drop can increase and the drop can reach with high precision even if the distance between a head nozzle and a plotted base is short.
It is another object of the present invention to provide a driving method and apparatus for a liquid discharge head which are also suitably used for an industrial patterning apparatus.
In order to achieve the above-mentioned object, according to a gist of the present invention, there is provided a driving method for a liquid discharge head including: a discharge port for discharging liquid; a pressure-applying portion communicating with the discharge port, for applying a pressure for discharge to the liquid; and a pressure generating device for generating the pressure, the method including a step of applying a first discharge pulse for discharging liquid and a second discharge pulse for discharging liquid to the pressure generating device in a sequential manner in response to an instruction of one-dot discharge, in which the pulse width of the first discharge pulse, the pulse width of the second discharge pulse, and a rest time between the first discharge pulse and the second discharge pulse are determined so that a first liquid discharged in response to the first discharge pulse has a volume equal to or greater than a second liquid discharged in response to the second discharge pulse and the discharge speed of the first liquid is lower than the discharge speed of the second liquid.
According to another gist of the present invention, there is provided a driving apparatus for a liquid discharge head including: a discharge port for discharging liquid; a pressure-applying portion communicating with the discharge port, for applying a pressure for discharge to the liquid; and a pressure generating device for generating the pressure, the apparatus including a driving circuit for applying a first discharge pulse for discharging liquid and a second discharge pulse for discharging liquid to the pressure generating device in a sequential manner in response to an instruction of one-dot discharge, in which the pulse width of the first discharge pulse, the pulse width of the second discharge pulse, and a rest time between the first discharge pulse and the second discharge pulse are determined so that a first liquid discharged in response to the first discharge pulse has a volume greater than a second liquid discharged in response to the second discharge pulse and the discharge speed of the first liquid is lower than the discharge speed of the second liquid.
According to still another gist of the present invention, there is provided a liquid discharge apparatus including: a liquid discharge head having: a discharge port for discharging liquid; a pressure-applying portion communicating with the discharge port, for applying a pressure for discharge to the liquid; and a pressure generating device for generating the pressure; a driving circuit for applying a first discharge pulse for discharging liquid and a second discharge pulse for discharging liquid to the pressure generating device in a sequential manner in response to an instruction of one-dot discharge; and a support for supporting a liquid-receiving member for receiving the liquid, in which the pulse width of the first discharge pulse, the pulse width of the second discharge pulse, and a rest time between the first discharge pulse and the second discharge pulse are determined so that a first liquid discharged in response to the first discharge pulse has a volume greater than a second liquid discharged in response to the second discharge pulse and the discharge speed of the first liquid is lower than the discharge speed of the second liquid, and in which a position of the liquid discharging head and a position of the support are determined so that the first liquid and the second liquid are combined to be applied to the liquid-receiving member.
According to the present invention, the first and second liquid drops are combined in a short discharge range, thus allowing the combined larger droplet to reach a liquid-receiving member with high precision.
In the present invention, the pulse width T1 and the pulse width T2, and the rest time K12 may be determined based on the hydrodynamic resonant frequency of the liquid discharge head. This enables liquid drops to be most effectively applied to the liquid-receiving member.
Also, according to another gist of the present invention, there is provided a driving method for a liquid discharge head including: a discharge port for discharging liquid; a pressure-applying portion communicating with the discharge port, for applying a pressure for discharge to the liquid; and a pressure generating device for generating the pressure, the method including a step of applying a first discharge pulse for discharging liquid and a second discharge pulse for discharging liquid to the pressure generating device in a sequential manner in response to an instruction of one-dot discharge, in which the following three equations are satisfied:
T1=k1×N×Tr/2
T2=k2×Tr/2
K12=k3×(3Tr/4−T2/2),
for k1, k2, and k3 each ranging from 0.9 to 1.1,
where N denotes an odd number more than one, Tr denotes an inverse of the hydrodynamic resonant frequency of the liquid discharge head, T1 denotes the pulse width of the first discharge pulse, T2 denotes the pulse width of the second discharge pulse, and K12 denotes the rest time between the first discharge pulse and the second discharge pulse.
According to still another gist of the present invention, there is provided a driving apparatus for a liquid discharge head including: a discharge port for discharging liquid; a pressure-applying portion communicating with the discharge port, for applying a pressure for discharge to the liquid; and a pressure generating device for generating the pressure, the apparatus including a driving circuit for applying a first discharge pulse for discharging liquid and a second discharge pulse for discharging liquid to the pressure generating device in a sequential manner in response to an instruction of one-dot discharge,
wherein the following three equations are satisfied:
T1=k1×N×Tr/2
T2=k2×Tr/2
K12=k3×(3Tr/4−T2/2),
for k1, k2, and k3 each ranging from 0.9 to 1.1,
where N denotes an odd number more than one, Tr denotes an inverse of the hydrodynamic resonant frequency of the liquid discharge head, T1 denotes the pulse width of the first discharge pulse, T2 denotes the pulse width of the second discharge pulse, and K12 denotes the rest time between the first discharge pulse and the second discharge pulse.
According to the present invention, the second liquid drop has a slightly smaller volume than that of the first liquid drop, while increasing the discharge speed of the liquid drops. Thus, two liquid drops can be combined in a short discharge range.
Also, according to the present invention, it is preferable that the driving circuit applies a non-discharge pulse, in response to which liquid is not discharged, subsequently to the second discharge pulse, and the following equations are satisfied:
T3=k4×Tr/2
K23=k5×(3Tr/2−T2/2−T3/2),
for k4 ranging from 0.2 to 0.5 and k5 ranging from 0.9 to 1.1,
where T3 denotes the pulse width of the non-discharge pulse, and K23 denotes the rest time between the second discharge pulse and the non-discharge pulse.
In this case, vibration, which is often large up to now, after discharging a liquid drop, can immediately be suppressed.
Also, according to the present invention, it is preferable that there is provided a driving signal including the first discharge pulse and the second discharge pulse to liquid discharge heads, the liquid discharge heads forming a liquid discharge head group having a plurality of the discharge ports, a plurality of the pressure-applying portions, and a plurality of the pressure generating devices, in which the pulse width of the first discharge pulse, the pulse width of the second discharge pulse, and the rest time have the same value.
In this case, there is no need for optimizing a pulse train for each liquid discharge head. Therefore, liquid discharge heads having some non-uniform discharge characteristics due to fluctuation in production would successfully be driven.
Further, according to another gist of the present invention, there is provided a driving method for a liquid discharge head including: a discharge port for discharging liquid; a pressure-applying portion communicating with the discharge port, for applying a pressure for discharge to the liquid; and a pressure generating device for generating the pressure, the method including a driving circuit for applying a first discharge pulse for discharging liquid and a second discharge pulse for discharging liquid to the pressure generating device in a sequential manner in response to an instruction of one-dot discharge, in which the following three equations are satisfied:
T1>Tr
T2=T1/N
K12=3T1/2N−T2/2,
where N denotes an odd number more than one, Tr denotes an inverse of the hydrodynamic resonant frequency of the liquid discharge head, T1 denotes the pulse width of the first discharge pulse, T2 denotes the pulse width of the second discharge pulse, and K12 denotes the rest time between the first discharge pulse and the second discharge pulse.
Also, according to still another gist of the present invention, there is provided a driving apparatus for a liquid discharge head including: a discharge port for discharging liquid; a pressure-applying portion communicating with the discharge port, for applying a pressure for discharge to the liquid; and a pressure generating device for generating the pressure, the apparatus including a driving circuit for applying a first discharge pulse for discharging liquid and a second discharge pulse for discharging liquid to the pressure generating device in a sequential manner in response to an instruction of one-dot discharge, in which the following three equations are satisfied:
T1>Tr
T2=T1/2
K12=3T1/2N−T2/2,
where N denotes an odd number more than one, Tr denotes an inverse of the hydrodynamic resonant frequency of the liquid discharge head, T1 denotes the pulse width of the first discharge pulse, T2 denotes the pulse width of the second discharge pulse, and K12 denotes the rest time between the first discharge pulse and the second discharge pulse.
According to the present invention, the second liquid drop has a slightly smaller volume than that of the first liquid drop, while increasing the discharge speed of the liquid drops. Thus, two liquid drops can be combined in a short discharge range.
Also according to the present invention, it is preferable that the driving circuit applies a non-discharge pulse, in response to which liquid is not discharged, subsequently to the second discharge pulse, and the following equations are satisfied:
T3<Tr/2,
K23=3T1×N−T2/2−T3/2,
where T3 denotes the pulse width of the non-discharge pulse, and K23 denotes the rest time between the second discharge pulse and the non-discharge pulse.
Also in this case, vibration, which is often large up to now, after discharging a liquid drop, can immediately be suppressed.
At time t0, when a driving pulse (first discharge pulse VA) rises and reaches voltage Vop, the pressure generating device causes shear strain deformation, thus increasing the volume of the pressure-applying portion, so that liquid is introduced to the pressure-applying portion from the upstream.
At time t1, when the driving pulse falls, the shear strain deformation of the pressure generating device is cancelled, and a force for restoring the deformed pressure generating device to the original state causes the volume of the pressure-applying portion to decrease, so that the liquid is pressurized within the pressure-applying portion. The vibration makes the volume of the pressure-applying portion lower than that at the time t0, and causes the liquid to be pressurized and discharged from the discharge port.
At time t2, when the driving pulse (second discharge pulse VB) rises again, the discharged liquid forms a large liquid drop 22.
In response to the second discharge pulse VB, the pressure-applying portion expands again.
At time t3, when the second discharge pulse VB falls, the vibration amplitude of the pressure generating device is maximum. Then, the pressure-applying portion contracts again, allowing liquid corresponding to a second liquid drop 23 to be discharged.
At time t4, the discharged liquid forms the second liquid drop 23, and outgoes from the discharge port. Since the second liquid drop 23 has large vibration amplitude at the time t3, the second liquid drop 23 is discharged at a higher speed than the first liquid drop 22.
In short, two liquid drops are emitted in response to two discharge pulses for an instruction of one-dot discharge. The first liquid drop 22 discharged in response to the first discharge pulse can be discharged with delay by 15 to 20% with respect to the second liquid drop 23 discharged in response to the second discharge pulse. Therefore, even if the distance between the discharge port and the plotted base (liquid-receiving member) is as small as 500 μm or lower, the first liquid drop 22 can be combined in the air with the second liquid drop 23 to become a large liquid drop 24 before the first liquid drop 22 reach the liquid-receiving member. In addition, the volume of the first liquid drop 22 is the same as or slightly smaller than that of the second liquid drop 23.
By driving in response to the first and second discharge pulses for an instruction of one-dot discharge, a liquid drop having a volume 1.8 to 2.0 times that when driving in response to either the first or second discharge pulse for an instruction of one-dot discharge can be reached as the same dot. Volumes of the drops 22 and 23 can be calculated approximately based on a circle on an oval formed by projecting the same drops onto a plan view as shown in FIG. 2.
In this embodiment of the present invention, preferably, a third non-discharge pulse subsequent to the second discharge pulse may be applied at about time t5. This makes it possible to effectively reduce vibration of the liquid in the pressure-applying portion after the discharge, resulting in ejection of relatively low viscosity ink at a high frequency.
In order to successfully form the above-described liquid drops, the driving pulse train should be set as follows:
The following three equations are satisfied:
T1>Tr
T2=T1/2
K12=3T1/2N−T2/2,
where N denotes an odd number more than one, Tr denotes an inverse of the hydrodynamic resonant frequency of the liquid discharge head, T1 denotes the pulse width of the first discharge pulse, T2 denotes the pulse width of the second discharge pulse, and K12 denotes the rest time between the first discharge pulse and the second discharge pulse.
More preferably, the following equations are satisfied:
T3<Tr/2
K23=3T1/N−T2/2−T3/2,
where T3 denotes the pulse width of the non-discharge pulse, and K23 denotes the rest time between the second discharge pulse and the non-discharge pulse.
Preferably, T1 is N times Tr/2 based on the hydrodynamic resonant frequency.
While the example where N=3 is shown in
A preferred form of the driving method for a liquid discharge head according to the present invention is now described in more detail with reference to
When a discharge pulse VA having a pulse width of T1=N×Tr/2, for N=3, is applied to a liquid discharge head having such a characteristic, the vibration shown in
If a second discharge pulse is applied after an application of the first discharge pulse VA shown in
Then, the maximum amplitude at the time t3 allows the second liquid drop to be discharged at a higher speed than the first liquid drop, while the first and second liquid drops have substantially the same volume.
In the liquid discharge head group to be driven, the hydrodynamic resonant frequency FR may often vary from one head to another due to lack of uniformity in production, etc. In order to overcome this problem, if the pulse widths and the rest time are to be optimized for each head, a complicated driving circuit is required. Taking variation in characteristics of the liquid discharge head group into consideration, the pulse widths and the rest time should be set within a range having an allowance of 0.9 to 1.1 times the optimal values as a requirement for the aforementioned advantages. Selectable ranges of the pulse widths and the rest time are set as follows:
T1=k1×N×Tr/2
T2=k2×Tr/2
K12=k3×(3Tr/4−T2/2)
where k1, k2, and k3 denote values each ranging from 0.9 to 1.1.
At time t5, which is a time when M23 has elapsed from the intermediate time of the pulse VB or the intermediate time point between the rising time t2 and the falling time t3 of the pulse VB, a non-discharge pulse VC is applied.
Preferably, M23=3×Tr/2.
As shown in
In particular, in
If the pulse width of the non-discharge pulse VC applied subsequently to the second discharge pulse VB is indicated by T3, then, T3<Tr/2, and, preferably, T3 (0.5×Tr/2. For a liquid discharge head group having a plurality of discharge ports, in particular, preferably, T3=k4×Tr/2, where k4 ranges from 0.2 to 0.5.
If the period from the falling time t3 of the second discharge pulse VB to the rising time of the non-discharge pulse VC, that is, the rest time between the second discharge pulse VB and the non-discharge pulse VC, is indicated by K23, preferably, K23=3T1/N−T2/2−T3/2.
More preferably, from a value obtained by subtracting, from M23, the half the pulse width of the second discharge pulse and the half the pulse width of the non-discharge pulse, i.e., K23=3Tr/2−T2/2−T3/2, K23=k5×(3Tr/2−T2/2−T3/2) is derived, where k5 ranges from 0.9 to 1.1.
A preferable liquid discharge head used in the present invention includes a pressure generating device which is displaced at least in a part in response to an application of an electric signal so that a pressure can be applied to liquid introduced into a pressure-applying portion, and a discharge port communicating with the pressure-applying portion. In particular, a piezoelectric actuator which is displaced in response to an application of a unipolar voltage to decrease the pressure applied to the liquid and which is displaced back in response to a cancellation of that voltage to expel the liquid is suitably used.
An exemplary liquid discharge head is now described with reference to the drawings. As in that shown in
An air chamber 508 formed of a gap containing no ink is provided between adjacent ink flow paths 506.
An orifice plate 512 having a nozzle (discharge port) 510 is bonded to one end of each ink flow path 506, and electrodes 513 and 514 are provided as metallized layers on both sides of each actuator wall 503. More specifically, each actuator wall 503 is provided with the electrode 514 on the side of the ink flow path 506, and is provided with the electrode 513 on the side of the air chamber 508. The electrodes 513 facing the air chamber 508 are connected to a control circuit (driving circuit) 520 for supplying an actuator driving signal, while the electrodes 514 defining the ink flow path 506 are connected to a ground.
A driving circuit used in the present invention may be implemented as a circuit for supplying the driving signal shown in
When an ON signal (+5 V) is input to the input terminal 204, the transistor TR101 is conducting via the resistor R101, thus causing a current from a positive power source 101 to flow from the collector toward the emitter of the transistor TR101 via the resistor R103. Therefore, the divided voltages applied to the resistors R104 and R105 connected to the positive power source 101 increase, allowing a current flowing to the base of the transistor TR102 to increase, so that the emitter and collector of the transistor TR102 are electrically connected with each other. This allows a voltage of +20 V to be applied from the positive power source 101 to the electrode 513 beside the air chamber 508 via the collector and emitter of the transistor TR102 and via the resistor R120. This operation is performed at times Tm1, Tm3, and Tm5 shown in the timing charts in
The pulse control circuit 203 which generates a pulse signal which is input to the input terminal 204 of the charging circuit 201 and to the input terminal 205 of the discharging circuit 202 at the times Tm1, Tm2, Tm3, Tm4, Tm5 and Tm6 is now described.
In
For example, the pulse generator 215 has a register 31 and a counter 32, and the pulse generator 216 has a register 33 and a counter 34. Counter values corresponding to the rising and falling time of the pulses VA, VB, and VC are stored in the registers 31 and 33 from the ROM 212. When the counters 32 and 34 count up to these counter values based on the reference clock, the signal is supplied to the input terminals 204 and 205 at the aforementioned times.
The same number of pulse generators 215 and 216, charging circuits 201, and discharging circuits 202 as the number of nozzles of the ink jet head is provided. Although only one nozzle is described in this embodiment, similar control is performed on other nozzles.
The voltage values of the pulses VA, VB and VC may be separately determined, or may be the same, as described above. If the voltage value of the pulse VB is greater than that of the pulse VA, a higher discharge speed can be obtained. The voltage value of the pulse VC may be smaller than those of the pulses VA and VB.
A liquid discharge apparatus incorporating a driving apparatus for a liquid discharge head according to the present invention is now described.
Reference numeral 1 denotes a liquid discharge head group including the aforementioned charging circuit and discharging circuit. Reference numeral 2 denotes a container for receiving liquid supplied to the liquid discharge heads. Reference numeral 3 denotes a guide member for guiding the head group 1 in the X direction. Reference numeral 4 denotes a guide member for guiding the container 2 in the X direction.
Reference numeral 5 denotes a linear guide for guiding the guide members 3 and 4 in the Y direction orthogonal to the X direction.
Reference numeral 6 denotes a driving apparatus for the head group 1. The driving apparatus 6 includes the aforementioned pulse control circuit, and is connected to the heads by a flexible cable.
Reference numeral 7 denotes a substrate stage that is a support for supporting a liquid-receiving member 10. Reference numeral 8 denotes a stepping motor serving as a driving unit for driving the head group 1 to reciprocate in the X direction. Reference numeral 9 denotes a stepping motor serving as a driving unit for driving the container 2 to reciprocate in the X direction.
The liquid-receiving member 10 is situated on the substrate stage 7. The head group 1 discharges liquid in the above-described way, while moving in the X direction, to form a dot pattern. When the dot pattern has been formed for one row, the head group 1 one row proceeds in the Y direction to form the dot pattern for the next row. This operation is repeated to plot the dot pattern on the liquid-receiving member 10. While the example where only the head group 1 moves with respect to the fixed substrate stage 7 has been described, the head group 1 and the substrate stage 7 may relatively move, such that the head group 1 may move in the X direction while the substrate stage 7 may move in the Y direction.
The liquid-receiving member 10 may be implemented as a semiconductor wafer, a glass substrate, a plastic substrate, woven fabric, or the like, and may be formed by coating a liquid-receiving layer on any of these materials.
The present invention may be used for manufacturing the source and drain of an organic transistor; a gate electrode; a source electrode; a drain electrode; an electroluminescent layer, anode electrode, or cathode electrode of an organic EL device; a colored layer or light-shielding layer of a color filter; an electrode or electron-emission layer of a light-emitting device; and the like. The present invention may also be applied to production of a DNA chip. Of course, the present invention may be applied to printing onto a sheet of normal paper.
A head group having the shear-mode actuator shown in
The length L1 of the ink flow path 506 is 8.0 mm. The nozzle 510 on the ink emission side has a diameter φ1 of 25 μm, and the nozzle 510 on the ink flow path side has a diameter φ2 of 40 μm. The nozzle 510 has a length (the thickness of the orifice plate 512) L2 of 50 μm.
The ink used in the experiment has a viscosity of 6 mPa·s at 25° C., and a surface tension of 50 mN/m. The hydrodynamic resonant frequency of an association system of ink and a pressure-applying portion in the ink flow path was measured using an impedance measurement device, and an inverse thereof Tr=20 μsec was determined.
A liquid-receiving member is placed on a substrate stage, and the distance between the surface of the liquid-receiving member and the surface of the orifice plate of the head was set to 300 μm.
The driving waveform shown in
The width T2 of the second emission pulse signal B was set to T2=Tr/2=10 μsec.
The time interval K12 from the falling time of the emission pulse A to the rising timing of the emission pulse B was set to K12=Tr/2=10 μsec.
The width T3 of the non-emission pulse signal C was set to T3=0.4×Tr/2=4 μsec.
The time interval K23 from the falling time of the emission pulse signal B to the rising time of the non-emission pulse signal C was set to K23=3×Tr/2−T2/2−T3/2=23 μsec.
In this way, the emission pulse signals A and B, and the non-emission pulse signal C were sequentially applied to the actuators in response to one-dot emission signal to perform plotting while moving the head group so that a plurality of dots are not applied to the same position on the liquid-receiving member.
A larger liquid drop was ejected in response to the emission pulse A while a slightly smaller but faster liquid drop was ejected in response to the emission pulse B, thus allowing a large-volume liquid drop to be applied as one dot. In addition, the non-emission pulse signal C was applied at a normal-position timing in which the piezoelectric device changes from the expanding state to the contracting state due to vibration of the residue in the ink flow path in response to the emission pulse signal, thereby applying a force in the expanding direction to the piezoelectric device. This allows cancellation between the deformation of the piezoelectric device to the expanding state and to the contracting state, thereby reducing the vibration of the residue that may affect the piezoelectric device.
The head group was driven in a similar manner as that in Example 1 to perform an emission test. The result is now described in conjunction with Table 1. Table 1 indicates the result when the first emission pulse A and the second emission pulse B in the driving waveform shown in
Table 1 indicates the total amount of discharge of two ink droplets ejected in response to the emission pulses A and B with a driving voltage of 24 V. Table 1 further indicates the discharge speed and deposition precision of the main drop in the two ink droplets which are combined in the air. The variation (fluctuation) in the position accuracy of the arriving liquid drop and the circularity of the arriving liquid drop are used as indexes of the deposition evaluation.
A value ranging from 27 μs to 33 μs was satisfactory for the emission pulse width dependency for any evaluation. In this embodiment, if Tr=1/Fr, where Fr denotes the hydrodynamic resonant frequency of an association system of ink and a pressurizing unit in the ink flow path, then, Tr=20 μs is found, proving that a satisfactory pulse width is within 0.9×3×Tr/2≦T1≦1.1×3×Tr/2.
In a similar manner as that in Example 2, the pulse width of the emission pulse B was used as a variable parameter to perform a similar evaluation.
T1=30 μs was used as another parameter, and others are the same as those in Example 2.
In Example 3, it was found that the pulse width T2 when a satisfactory result was obtained is within 9 μs≦T2≦11 μs.
As comparison, although not shown in
It is therefore found that the amount of discharge can doubly increase when the emission pulses A and B are applied compared with when the single emission pulse (10 μs) is used.
A similar experiment to that of Example 2 was performed using low-viscosity ink, and a similar result to that of Example 2 was obtained.
Only the emission pulses A and B were used for driving. Then, it was found that the discharge state is unstable when the driving frequency increases (for example, 10 kHz or higher) compared with Example 2 (in which high-viscosity ink is used).
The non-emission pulse C was applied in the manner shown in
The satisfactory pulse width T3 ranged from 2 μs to 5 μs, and the rest time K23 ranged from 20.7 μs to 25.3 μs.
As described in the embodiment of the present invention, therefore, if Tr=1/Fr, where Fr denotes the hydrodynamic resonant frequency of an association system of ink and a pressurizing unit in the ink flow path, the first pulse width T1 of the driving pulse which is first applied for one-dot plotting is not Tr/2 (that is, the piezoelectric device does not contract at the timing when the amplitude of the piezoelectric device to which a pulse is applied becomes first maximum) but 3×Tr/2 (that is, the piezoelectric device contacts at the timing when the amplitude of the piezoelectric device is secondly maximum). This makes it possible to reduce the discharge speed without reducing the amount of discharge when a liquid drop is discharged in response to a first emission pulse. Thus, the first ejected liquid drop and the second ejected liquid drop can be combined before the first and second ejected liquid drops reach the liquid-receiving member. When the liquid drops are combined in the air, the combined liquid drop, which is transformed into an elliptic drop, vibrates for a while until the combined liquid drop becomes sphere and is stabilized. In the embodiment of the present invention, the combined liquid drop stops vibrating, and the resulting sphere drop reaches the base. In order to immediately stop vibration of the combined liquid drop in the air, it is necessary to reduce the difference in momentum between the first liquid drop and the second liquid drop as much as possible. The embodiment of the present invention makes it possible to reduce the difference in momentum between the first liquid drop and the second liquid drop, thereby immediately stopping vibration of the combined liquid drop.
Although one embodiment of the present invention has been described in detail, the present invention is not limited to this embodiment. While a positive power source is used in the embodiment, a negative power source may be used by reversing the polarization direction of the piezoelectric device. The polarization direction of the piezoelectric device may be reversed, and ink chambers may be connected to the positive power source while air chambers are connected to a ground. A pressurizing unit for pressurizing ink may be placed as a portion of an ink flow path. In other words, the present invention is not limited to any mechanism such as ink pressurizing mechanisms or power source mechanisms.
According to the present invention, therefore, two discharge pulses are applied at a predetermined timing in response to an instruction of one-dot discharge, thereby obtaining required amount of discharge. Furthermore, an extremely satisfactory deposition condition can be achieved, and, in particular, liquid can be ejected in a manner suitable for industrial plotting.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2001-300896 | Sep 2001 | JP | national |
This is a divisional application of application Ser. No. 10/241,537, filed on Sep. 12, 2001 now U.S. Pat. No. 6,676,238.
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| Number | Date | Country | |
|---|---|---|---|
| 20040061731 A1 | Apr 2004 | US |
| Number | Date | Country | |
|---|---|---|---|
| Parent | 10241537 | Sep 2002 | US |
| Child | 10673582 | US |
