Drop on demand ink jet technology for producing printed media has been employed in commercial products such as printers, plotters, and facsimile machines. Generally, an ink jet image is formed by selective placement on a receiver surface of ink drops emitted by a plurality of drop generators implemented in a printhead or a printhead assembly. For example, the printhead assembly and the receiver surface are caused to move relative to each other, and drop generators are controlled to emit drops at appropriate times, for example by an appropriate controller. The receiver surface can be a transfer surface or a print medium such as paper. In the case of a transfer surface, the image printed thereon is subsequently transferred to an output print medium such as paper.
A known ink jet drop generator structure employs an electromechanical transducer to displace ink from an ink chamber into a drop forming outlet passage, and it can be difficult to control drop velocity and/or drop mass.
The ink 33 can be melted or phase changed solid ink, and the electromechanical transducer 39 can be a piezoelectric transducer that is operated in a bending mode, for example.
The time varying non-firing waveform can be configured to set the condition of the drop generator 30 for the next fire interval.
For example, the time varying non-firing waveform 52 can be shaped or configured to place the drop generator 30 in a fluid dynamics condition similar to the fluid dynamics condition the drop generator 30 would be in after firing a drop. In this manner, the drop generator 30 is placed in substantially the same fluid dynamics condition each time the drop generator fires, which can provide for more consistent drop velocity and/or drop mass over a broad range of operating conditions.
As another example, the time varying non-firing waveform 52 can be shaped or configured such that the spectral energy of the drive signal is approximately the same for different firing patterns. In other words, the spectral energy of the drive signal is approximately the same regardless of whether a sequence of fire intervals includes only drop firing waveforms or includes drop firing waveforms and non-firing waveforms.
Alternatively, the time varying non-firing waveform can be shaped or configured so that it does affect the spectral energy of the drive signal, which can affect the condition of the drop generator. That is, the spectral energy of the drive can vary with firing pattern.
In a further example, the time varying non-firing waveform 52 can be shaped or configured to reduce variation in drop velocity such that drop velocity is approximately constant regardless of whether a given drop firing waveform follows a drop firing waveform or a non-firing waveform. In other words, the drop velocity is not substantially affected by the firing pattern.
Also, the time varying non-firing waveform 52 can be shaped or configured to reduce variation in drop mass such that drop mass is approximately constant regardless of whether a given drop firing waveform follows a drop firing waveform or a non-firing waveform. In other words, drop mass is not substantially affected by the firing pattern.
The time varying non-firing waveform 52 can further be shaped or configured to change a drop parameter when a given drop firing waveform follows a non-firing waveform.
By way of illustrative example, as depicted in
The time varying non-firing waveform can be a unipolar voltage signal such as a pulse that can be positive or negative, for example relative to a reference. A non-firing pulse can have a pulse duration that is less than a fire interval, for example, wherein pulse duration can be measured for convenience between pulse transition times (i.e., the transition from the reference and the transition to the reference. A non-firing pulse can be located anywhere in a fire interval. For example, a non-firing pulse can be approximately centered in a fire interval or it can be located only in either the first half or the second half of a fire interval. By way of specific example, the time varying non-firing waveform can be a negative going pulse having a width that is in the range of about 10% to about 90% of the firing interval T (i.e., about 0.1 T to about 0.9 T).
As another example, illustrated in
As a further example illustrated in
The invention has been described with reference to disclosed embodiments, and it will be appreciated that variations and modifications can be affected within the spirit and scope of the invention.
This is a divisional of U.S. Continuation application Ser. No. 10/897,527, filed Jul. 22, 2004 now abandoned, which is a continuation of U.S. application Ser. No. 10/283,888, filed Oct. 30, 2002, now abandoned.
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WO 9735167 | Jun 1997 | WO |
Number | Date | Country | |
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20060082608 A1 | Apr 2006 | US |
Number | Date | Country | |
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Parent | 10897527 | Jul 2004 | US |
Child | 11296142 | US |
Number | Date | Country | |
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Parent | 10283888 | Oct 2002 | US |
Child | 10897527 | US |