Technical Field
[0001] This invention relates generally to ink jet printing systems and more particularly
to such systems employing auxiliary ink pumping means for improving operational performance.
These systems are operative to maintain a positive pressure within an ink cavity and
ink channel of an ink jet pen for extending its maximum operating frequency.
Background Art and Related Application
[0002] In certain types of ink jet printing systems, such as thermal ink jet (TIJ) printers,
the maximum achievable operating frequency, F
max, is inherently limited by: 1) the inability of the natural capillary action in the
ink feed apparatus to adequately supply ink to the ink reservoir chamber (the ink
cavity) of the printhead and 2) by oscillations of the ink meniscus at the orifice
plate of the printhead which persist for some time, To, after drop ejection has occurred.
One approach to extending F
max as well as providing other operational improvements in thermal ink jet printheads
is disclosed and claimed in copending application Serial No. 120,300 of Marzio A.
Leban et al entitled "Integral Thin Film Injection System For Thermal Ink Jet Heads
and Method of Operation", filed November 13, 1987, assigned to the present assignee
and incorporated herein by reference (European Application No. 88310572.8).
[0003] Thermal ink jet printers having these operational characteristics are now generally
well known in the art and are described, for example in the
Hewlett-Packard Journal, Volume 38, No. 5, May 1985, incorporated herein by reference. These printers employ
printhead devices having resistive heater elements (resistors) which are normally
aligned with corresponding ink ejection orifices in an adjacent orifice plate and
are operative to receive electrical drive pulses from an external source. These pulses
rapidly heat the heater resistors and thereby cause ink in an adjacent ink reservoir
to vaporize and be forced out of the orifice plate during an ink jet printing operation.
Thus, as the operating frequency of the printhead is extended out beyond a certain
limit, there is a tendency for the natural capillary action of the ink feed system
of the TIJ printer to inadequately supply the required volume of ink to the ink reservoirs
associated with the heater resistors, the adjacent ink cavity and ink channel feeding
the cavity.
[0004] This "ink starvation effect" becomes even more pronounced as the viscosity of the
ink is increased. In many applications it is desirable to increase the ink viscosity
in order to achieve an improved print quality on a variety of paper types and particularly
plain paper. In addition to the above limitations imposed by this ink starvation effect,
natural meniscus oscillations of the ink at the orifice further place a limitation
on F
max and persist for some time, To, immediately after a drop is ejected. During this time,
To, further drop ejection is greatly restricted.
Disclosure of Invention
[0005] Accordingly, it is an object of this invention to overcome the above inability of
the natural ink feed capillary action to adequately supply ink to the ink jet printhead
during high frequency operation and thereby extend F
max beyond its present limits.
[0006] Another object is to provide a new and improved printhead of the type described which
is operative to generate meniscus oscillations of the ink at the orifice of a controlled
frequency, Fm, and a controlled amplitude, Im. This action allows firing of ink drops
of varying volume from the same orifice by timing the drop firing with meniscus height.
Small drops are ejected when firing occurs at low meniscus levels, and large drops
are ejected when firing occurs at high meniscus levels.
[0007] Another object is to extend the upper limit of the usable ink viscosity. This is
accomplished by employing the pumping action of a piezoelectric system to produce
a positive pressure over and above the natural capillary force within the ink capillary
cavity and ink capillary channel of the ink jet printhead.
[0008] To achieve the above objects and attendant advantages of this invention, we have
discovered and developed a new and improved ink feed system and method of operation
for an ink jet printhead wherein the amplitude and frequency of oscillations of the
meniscus at a fluid ejection orifice are controlled by ejecting fluid through an orifice
and at a natural resonant frequency and amplitude with respect to an equilibrium position.
The frequency or amplitude or both of the fluid meniscus at the orifice are modulated
in a controlled phase relation with respect to the phase position of the oscillations
of the meniscus above or below the equilibrium position.
[0009] In a preferred embodiment of the invention, a resistive heater element is aligned
with respect to an orifice plate, and an ink flow path supplies ink into a chamber
or reservoir between the resistive heater element and the orifice plate. This improved
system includes, among other things: 1) a piezoelectric system which is mounted internal
to the ink cavity of an ink jet printhead; 2) an external piezoelectric system which
is mounted directly on the orifice plate of an ink jet printhead; 3) dual independent
piezoelectric systems which are both mounted internal to the ink cavity of the printhead;
and 4) dual piezoelectric systems with one being internal to the ink cavity of the
printhead and the other being external and mounted directly on the orifice plate of
the printhead. The above described ink feed systems may be used to: 1) produce oscillations
of controlled frequency, Fm, and controlled amplitude, Im, of the ink meniscus at
the ink ejection orifice and produce the ejection of ink drops from a single orifice
with varying and controlled volumes; 2) extend the maximum frequency of operation,
F
max, of the ink jet printhead; and 3) extend the viscosity range of inks which may be
used.
[0010] The above brief summary of invention will become better understood and appreciated
from the following description of the accompanying drawing.
Brief Description of the Drawings
[0011]
Figure 1 is an abbreviated perspective view showing a typical mounting arrangement
of a heater resistor within an ink feed channel.
Figure 2 is an abbreviated cross section view showing the position of the heater resistor
with respect to the main ink feed channel, the ink cavity and the orifice plate of
the thermal ink jet printhead.
Figures 3A-3C show, in abbreviated cross-section, three different meniscus positions
during its oscillation at an orifice opening.
Figures 4A-4B compare the natural meniscus oscillation with the induced meniscus oscillation
provided in accordance with the present invention.
Figure 5 is an abbreviated cross section view of an ink jet printhead which shows
the piezoelectric pump material mounted within the ink cavity of the printhead.
Figure 6 is an abbreviated cross section view of an ink jet printhead which shows
the piezoelectric pump material mounted on the orifice plate of the printhead.
Figure 7 is an abbreviated cross section view of an ink jet printhead which shows
two (2) separate piezoelectric pump transducers mounted within the ink cavity of the
printhead.
Figure 8 is an abbreviated cross section view of an ink jet printhead which shows
the piezoelectric pumps mounted on both the orifice plate outside the ink cavity and
within the ink cavity of the printhead.
Figures 9A-9B show the shifting of the induced meniscus oscillation about the meniscus
equilibrium position by an amount controlled by the timing of pressure pulses generated
by the piezoelectric pump or pumps of the ink jet printhead.
Detailed Description
[0012] Referring now to Figure 1, there is shown a perspective view of a single heater element
(resistor) 11 surrounded by a barrier material 12 forming an ink channel 13 immediately
adjacent to the resistor 11. The barrier material 12 also forms an ink cavity region
14 exterior to the ink channel 13. This type of three sided barrier layer construction
is generally well known in the art and is disclosed for example in copending applications
serial nos. 109,685 and 057,573 of Howard H. Taub et al assigned to the present assignee
and incorporated herein by reference (European Application Nos. 88309820.4 and 88304048.7).
[0013] Figure 2 is a cross section view which would be taken through the center of the resistor
in Figure 1 when the printhead structure therein, including the orifice plate, is
completed. Figure 2 further illustrates that the ink cavity 14 is formed between an
underlying substrate 15 and an outer orifice plate 16. An orifice 17 is positioned
immediately above the resistor 11, and ink from an ink feed system 18 is drawn into
the ink cavity 14 and into the ink channel 13 regions by a capillary force.
[0014] As the resistor 11 is fired by a suitable pulse applied thereto, a drop of ink is
ejected from the orifice 17. An ink jet printhead operating in this manner is considered
to be operating in the "equilibrium mode". Immediately after drop ejection in the
equilibrium mode, the meniscus of the ink at the 25 orifice 17 will oscillate from
the equilibrium position 19 as indicated in Figure 3A and achieves a maximum extension
20 and a minimum extension 21 as indicated in Figures 3B to 3C. These "natural oscillations"
continue for a length of time, labeled the "dead time", To, with a decaying amplitude
as shown in Figure 4A. During this time, ejection of an additional drop of ink is
not permitted.
[0015] In accordance with the present invention, a piezoelectric material 22 such as quartz
or barium titanate crystals or a kynar piezoelectric film is introduced into the ink
cavity 14 as shown in Figure 5, or is mounted externally on the outer surface of the
orifice plate 16 as shown in Figure 6. The material 22 is connected in such a manner
that it can be energized with a controlled electrical signal, and this signal induces
oscillations, of controlled frequency and magnitude, within the material 22. This
action in turn produces a positive ink pressure within the ink cavity 14 and the ink
channel 13 and thereby behaves as an ink pump. Both internally and externally mounted
piezoelectric systems function in an equivalent manner.
[0016] There are various available piezoelectric driving circuits suitable for providing
the piezoelectric drive signals described herein, and the choice of circuit design
of these drivers is considered well within the skill of the art. Therefore, a detailed
description of specific driver circuit design has been omitted for sake of brevity.
However, piezoelectric driver circuits have been described in many U.S. Patents, such
as U.S. Patents 4,714,935, 4,717,927, 4,630,072, 4,498,089 and 4,521,786. Piezoelectric
driver circuits have also been enclosed in the following four textbook references,
and these four textbook references as well as the above patents are incorporated herein
by reference:
1. Precision Frequency Control; E. A. Gerber, Ed. Academic Press, 1985.
2. Acoustic Waves: Devices, Imaging and Analogue Signal Devices; Gordon Kino, Prentice-Hall, 1987.
3. Standard Methods for the Measurement of Equivalent Circuits; American National Standards, Electronic Industries Association, 1985.
4. PVF2 - Models. Measurements, Device Ideas, John Linvill, Stanford Technical Report number 4834-3, Stanford University, 1978.
[0017] The oscillations of the piezoelectric material 22 produce a constant, symmetric and
continuous oscillation of the ink meniscus as shown in Figure 4B. These continuous,
induced, symmetric and controlled meniscus oscillations of frequency, Fm, and amplitude,
Im, in Figure 4B are superimposed on the "natural oscillations" in Figure 4A. The
net result of this superposition of these two kinds of meniscus oscillations is a
virtual "swamping out" of the natural meniscus oscillations in Figure 4A, and the
virtual elimination of the "dead time", To, which is responsible for limiting the
maximum operating frequency, F
max, of the ink jet printhead.
[0018] The timing of the firing of resistor 11 with respect to the meniscus amplitude, Im,
of the induced meniscus oscillations is crucial. If the resistor 11 is fired at the
equilibrium position, or points (T) in Figure 4B, the ink jet printhead is operating
in the "equilibrium mode" and medium volume ink drops, Veq, are ejected. These ejected
ink drops are of a volume equal to the case where the piezoelectric material is not
pulsed. The maximum achievable operating frequency, F
max, of the ink jet printhead operating in the "equilibrium mode" is limited only by
the frequency of induced meniscus oscillations, Fm. If the resistor 11 is fired at
the maximum meniscus extension position, namely at points (U) in Figure 4B, then the
ink jet printhead is operating in the "rich mode" and maximum volume ink drops, V
max, are ejected. If the resistor 11 is fired at the minimum meniscus extension position,
which is point (V) in Figure 4B, then the ink jet printhead is operating in the "lean
mode" and minimum volume ink drops, Vmin, are ejected. Firing the resistor 11 at different
points between the rich and lean modes will cause ink drops to be ejected in varying
and controlled volumes.
[0019] The range of ejected ink drop volume may be extended by employing dual independently
controlled piezoelectric systems within an ink jet printhead. Figure 7 illustrates
such a system where both independently controlled piezoelectric drivers 22 are incorporated
within the ink cavity 14.
[0020] Figure 8 illustrates another system where the piezoelectric drivers 22 are incorporated
both inside and outside the ink cavity 14, with the outside driver mounted on the
orifice plate 16. The method of operation of both these systems in Figures 7 and 8
is the same.
[0021] Each independently driven piezoelectric driver 22 may be energized with a controlled
signal and caused to oscillate which in turn induces a symmetric meniscus oscillation
as described above. If both piezoelectric drivers within an ink jet printhead are
caused to oscillate in phase with each other and with equivalent amplitudes, then
the induced meniscus oscillation remains symmetric as described above with reference
to Figure 4B.
[0022] Within the ink jet printhead, both piezoelectric drivers 22 may be caused to: 1)
oscillate out of phase with each other at the same frequency and amplitude; or 2)
oscillate out of phase with each other at the same amplitude and with a different
frequency. The combination of frequency, amplitude and phase shift may be selected
to induce a meniscus oscillation which is asymmetric as shown in Figures 9A and 9B.
[0023] If the induced asymmetric meniscus oscillation is skewed to the positive as shown
in Figure 9A, the maximum volume ink drop, Vmax, ejected may be further extended from
the symmetric case due to the greater meniscus extension in the asymmetric case. The
limiting situation is attained when the asymmetric positive meniscus extension is
so great that actual drop ejection begins to occur. Large positive asymmetric meniscus
extensions may be favored by suitable choice of ink viscosity and surface energy of
the ink.
[0024] Alternatively, if the asymmetric meniscus oscillation is skewed to the negative as
shown in Figure 9B, the minimum volume ink drop, Vmin, ejected may be further extended
from the symmetric case. The limiting situation is attained when the asymmetric negative
meniscus extension is so great that the printhead will begin to aspirate air through
an orifice opening in the orifice plate of the printhead. Air aspiration may be modified
by suitable choice of ink viscosity and ink surface energy.
[0025] The pumping action of the added piezoelectric system described above enables the
ink jet printhead to be used not only with current inks, with their low viscosities
(< about 3 cps) and higher surface tensions (> about 55 dyne/cm), but also with inks
having a lower surface tension and a higher viscosity. Generally, higher viscosity
inks penetrate slower into the surface of paper such that the print quality on a variety
of papers, and particularly on xerographic or bond papers, is improved. Printheads
using higher viscosity inks therefore print more consistently on a wider set of plain
papers. The ability to use both high viscosity and low surface tension inks yield
faster drytimes on plain papers as well.
[0026] The ability to use higher viscosity inks with a lower surface tension has significant
advantages over current technology. Standard ink technology, which employs soluble
dyes in a usually aqueous based vehicle, could be expanded to use a much larger group
of allowable solvents. For example, higher molecular weight glycols, ethers, ketones,
and the like could be used in conjunction with water to obtain the desired vehicle
properties. This expanded group of solvents allow dyes to be used in the new printhead
described herein which are not currently acceptable because of solubility or reactivity
with the ink vehicle. These additional dyes improve contrast, color, hue and print
quality on the printed medium. Besides the improved print quality inherent in higher
viscosity inks, other solvent and dye mixtures could yield improved waterfastness,
reliability, smearfastness, lightfastness and archivability. Also, additional color
dyes could be used, with a possible attendant improvement in color gamut and bleed
characteristics.
[0027] The ability to lower the requirements of surface tension and raise the allowable
limit on viscosity would enable the printhead to be used with "non standard" ink jet
inks (e.g. non-aqueous, dye based). For example, pigment based, microemulsion or encapsulation
inks could be used. These new colorant systems would offer higher waterfastness, improved
smearfastness, better color gamut, better reliability and better lightfastness and
bleed.
[0028] Various modifications may be made to the above described embodiments without departing
from the scope of this invention. For example, the present invention is not strictly
limited to the specific printhead cross-section geometries shown and may be practiced
using various printhead geometries including the well known "side shooter", "face
shooter" and "edge-shooter" constructions and the use of offsets between heater resistor
center lines and orifice centers. Additionally, the geometries of the ink feed channel
and the ink reservoir cavities may be modified in accordance with the design constraints
applicable to a variety of thermal ink jet printhead applications, and may include
various state of the art hydraulic tuning and crosstalk reduction features.