U.S. patent number 3,683,212 [Application Number 05/070,838] was granted by the patent office on 1972-08-08 for pulsed droplet ejecting system.
This patent grant is currently assigned to Clevite Corporation. Invention is credited to Steven I. Zoltan.
United States Patent |
3,683,212 |
|
August 8, 1972 |
PULSED DROPLET EJECTING SYSTEM
Abstract
An electro-acoustic transducer is coupled to liquid in a conduit
which terminates in a small orifice. Preferably, the acoustic
impedance of the supply portion of the conduit is large compared
with the acoustic impedance of the orifice. The liquid is under
small or zero static pressure. Surface tension at the orifice
prevents liquid flow when the transducer is not actuated. An
electrical pulse with short rise time causes sudden volume change
at the transducer, thereby creating an acoustic pressure pulse
having sufficient amplitude to overcome the surface tension at the
orifice and eject a small quantity of liquid therefrom. The
expelled liquid is replaced by forward flow of liquid in the
conduit under the influence of capillary forces in the orifice.
Inventors: |
Steven I. Zoltan (Shaker
Heights, OH) |
Assignee: |
Clevite Corporation
(N/A)
|
Family
ID: |
22097693 |
Appl.
No.: |
05/070,838 |
Filed: |
September 9, 1970 |
Current U.S.
Class: |
310/328;
261/DIG.48; 366/127; 417/322; 347/68; 310/317; 347/47 |
Current CPC
Class: |
B41J
2/04541 (20130101); B41J 2/04581 (20130101); H04R
17/08 (20130101); Y10S 261/48 (20130101) |
Current International
Class: |
B41J
2/045 (20060101); H04R 17/04 (20060101); H04R
17/08 (20060101); H01v 007/00 (); H04r
017/00 () |
Field of
Search: |
;310/8-8.3,8.5,8.6,8.7,9.1,9.4,9.6 ;259/1R,DIG.41,DIG.44 ;417/322
;346/75,140 |
References Cited
[Referenced By]
U.S. Patent Documents
Other References
Ultrasonics-October 1967, pp. 214-218, Article by E. G. Lierke
entitled .
"Ultrasonic Alomizer Incorporating a Self-Acting Liquid
Supply.".
|
Primary Examiner: J. D. Miller
Assistant Examiner: Mark O. Budd
Attorney, Agent or Firm: Eber J. Hyde
Claims
1. A system adapted upon pulsing to expel a small quantity or a
succession of small quantities of liquid in controlled manner,
comprising: a reservoir containing said liquid; a conduit connected
to said reservoir and communicating with the liquid therein and
filled with said liquid under low or zero static pressure, said
conduit having an exit orifice which is sufficiently small that
surface tension in the absence of pulsing prevents said liquid from
flowing therefrom; a tubular transducer of given diameter
surrounding said conduit in stress transmitting engagement
therewith and thereby coupled to the liquid therein adjacent said
orifice, said transducer being adapted to contract radially to
displace a small quantity of said liquid overcoming said surface
tension to expel a small quantity of said liquid through said
orifice and to expand to said given diameter prior to a subsequent
contraction; electrical circuit means connected to said transducer
for applying thereto an electrical pulse of a given polarity and
with short rise time to cause said transducer to contract rapidly,
and upon decay of said pulse to allow said transducer to expand;
said conduit during operation of said system at all times being
open from said reservoir to said orifice whereby the liquid within
said transducer is replaced by liquid from said reservoir to make
up for said expelled
2. A system as described in claim 1 in which the transducer is
a
3. A system as described in claim 1 in which the transducer
comprises a tubular piezoelectric member which changes internal
volume in response to an electrical signal, said tubular member
surrounding said second portion
4. A system as described in claim 1 in which the transducer is
an
5. A system as described in claim 1 in which the transducer is
a
6. A system as described in claim 1 wherein said means for applying
an electrical pulse includes means for adjusting the energy of said
pulse according to the quantity of liquid that is desired to be
expelled during said pulse.
Description
This invention pertains to a system for ejecting small quantities
of liquid suitable for use in apparatus such as ink jet printers
and recorders.
Printers and recorders of various kinds have been developed which
employ a stream of ink droplets. The ink under static pressure is
expelled through a small orifice. The emerging stream of ink breaks
up into droplets which tend to be of non-uniform size and spacing.
It has been found that ultrasonic vibrations of suitable frequency
applied to the nozzle or to the ink supply tend to regularize the
spacing and size of the droplets. In some applications, such as
character printers and facsimile recorders, it is necessary to
prevent, controllably, some of the droplets from reaching the
record medium. In U.S. Pat. No. 3,298,030 to Lewis and Brown, the
unwanted droplets are deflected electrostatically away from the
record medium into an ink dump. In U.S. Pat. No. 3,416,153 to Hertz
et al, the ink jet is propelled through an opening in a shield to
the record medium. When droplets are not wanted, the stream is
dispersed by an electric field so that it is intercepted by the
shield. These methods of droplet generation and control are
relatively complicated and expensive. Streams of ink droplets may
be developed without employing static pressure. In U.S. Pat. No.
2,512,743 to Hansell, a piezoelectric ultrasonic transducer
vibrates at a mechanical resonance frequency of the transducer. The
pressure to eject the droplets is said to result from cavitation in
the ink, with the quantity of ink expelled being controlled by
modulating the ultrasonic power source.
In U.S. Pat. No. 3,452,360 to Williamson, a magnetostrictive
transducer rod vibrates at a frequency well above the fundamental
length mode resonance of the rod, presumably at a length mode
overtone. One end of the vibrating rod is coupled to the ink
adjacent to a flexible nozzle. The flexibility of the nozzle and a
non-circular orifice provide a check valve action so that ink is
expelled during each expansion stroke of the rod. The ink stream
may be modulated by modulating the high frequency power source
which drives the transducer.
The principal object of this invention is to provide a system which
ejects a small quantity of liquid only upon electrical command.
Another object is to provide such a system which does not require a
pressurized liquid supply.
Another object is to provide a system which ejects liquid upon
electrical command, the quantity at each command being
controllable.
According to the invention a reservoir supplies liquid through a
conduit to an orifice which has acoustic impedance. A supply
portion of the conduit, which communicates with the reservoir, is
adapted for flow of liquid in both directions and has acoustic
impedance at least as high as the acoustic impedance of the
orifice. The conduit has a second portion located between the
supply portion and the orifice. Means are provided for causing a
droplet to be expelled from the orifice upon command comprising an
electroacoustic transducer coupled to the liquid in the second
portion of the conduit, and means for applying an electrical pulse
to the transducer each time it is desired to have a droplet
expelled from the orifice.
FIG. 1 shows a system according to the invention partly in section
and partly schematic.
FIG. 1a shows a modification of the system of FIG. 1.
FIG. 1b shows another modification of the system of FIG. 1.
FIG. 2 shows one of many alternate circuit arrangements suitable
for use in this invention.
FIG. 1a shows a modification of the circuit of FIG. 2.
FIG. 2b shows another modification of the circuit of FIG. 2.
FIG. 3 shows another suitable circuit arrangement.
FIG. 4 is a partial, sectional view illustrating a modified
transducer-orifice arrangement.
FIG. 5 shows another transducer-orifice arrangement.
FIG. 6 is a sectional view of still another transducer-orifice
arrangement.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
Referring to FIG. 1, a reservoir shown schematically at 1 contains
ink or other liquid 2. A conduit indicated generally be reference
characters 4 communicates with liquid 2 in the reservoir and is
filled with the liquid. A small orifice 5 in conduit 4 is provided
for exit of liquid, shown as droplets 7.
Conduit 4 comprises a length of small bore tubing 8,
electroacoustic transducer 10, and orifice plate 11. Tube 8 may
extend to the reservoir, or, as shown, conduit 4 may include a
larger diameter portion 6, such as plastic tubing, connecting tube
8 with the reservoir.
Transducer 10 comprises a length of small diameter piezoelectric
ceramic tubing 13. The diameter may, for example, be about 0.05
inch. Tube 13 is provided with electrode 14 on the inner surface
and electrode 16 on the outer surface. The electrodes, as shown, do
not extend to the ends of tube 13, but full length electrodes may
be employed if desired. Tube 13 is polarized radially.
A thin wire 17 is wrapped around tube 13 in contact with outer
electrode 16 and soldered thereto, as shown at 19. Wire 17 thus
serves as one electrical terminal of the transducer.
Tube 8, made of any suitable metal, such as copper or stainless
steel, is cemented into the end of ceramic tube 13 by means of
conductive epoxy 9 which contacts inner electrode 14. Thus, tube 8
serves as the second electrical terminal for the transducer.
For orifice plate 11, it is convenient to use a jewel watch
bearing. Such jewels are readily available at low cost and have
accurately controlled dimensions in the range suitable for the
present use. Orifice 5 may, for example, have diameter and length
on the order of 0.06 millimeter. Jewel 11 may be attached to the
end of transducer 10 by means of an epoxy adhesive 12.
Transducer 10 operates by virtue of the wellknown piezoelectric
effect. When a d-c voltage is applied between the electrodes the
length and the inside diameter of the tube both increase or
decrease slightly, depending on the polarity in relation to the
polarity of the polarizing d-c voltage used during manufacture. The
response is nearly instantaneous, being retarded very slightly by
inertia reaction.
When it is desired to have a small quantity of liquid expelled from
orifice 5, a short rise time voltage pulse is applied to the
transducer at terminals 8 and 17, the polarity being selected to
cause contraction of the transducer. The resulting sudden decrease
in the enclosed volume causes a small amount of liquid to be
expelled from orifice 5. Some liquid also is forced by the pressure
pulse back into tube 8, but the amount is relatively small, due to
the high acoustic impedance created by the length and small bore of
the tube.
From the foregoing, it may be seen that the system of this
invention ejects a small quantity of liquid on command. The command
signal is the short rise time pulse. By means of simple circuitry,
command pulses may be supplied to cause ejection of a succession of
small quantities of liquid according to any desired time pattern,
limited only by the maximum response speed of the system. In FIG. 1
a train of command pulses corresponding to exiting droplets 7 is
illustrated at 22.
Static pressure on the liquid is not required. However, small
positive or negative pressure does not interfere with operation,
the chief requirement being that such static pressure alone must
not be great enough to overcome the surface tension of the liquid
at orifice 5; otherwise liquid may run out, or air may enter the
system under quiescent conditions.
When the actuating electrical pulses have energy below the level
required to overcome the surface tension at the orifice, droplets
are not expelled, but under stroboscopic illumination the liquid
can be observed bulging out of the orifice momentarily during each
pulse. At somewhat higher drive energy levels, well developed
single droplets are expelled, one for each pulse. At still higher
energy levels, additional liquid is expelled in the form of
additional, separate droplets, or the total amount of liquid
expelled at each drive pulse may take the form of long cylinders of
liquid with rounded ends. Thus, the quantity of liquid expelled at
each pulse can be controlled by controlling the energy in the
driving pulse. This enables use of the invention in recorders
required to print with controlled shading, i.e., with gray scale,
without the necessity of producing multiple ink spots per picture
element.
Considerable latitude is available in the design of systems
according to this invention. The interacting design variables are
numerous and, as yet, a mathematical design technique has not been
developed. However, the following guide lines and example should
enable those skilled in electroacoustics to arrive at a
satisfactory design.
To avoid wasting an excessive part of each transducer pulse in
driving liquid from the transducer toward the reservoir, it is
desirable to have relatively high acoustic impedance looking from
the transducer into the supply portion of the conduit, as provided
by small bore tube 8 in FIG. 1. However, this is not a requirement.
Satisfactory performance may be obtained without providing any
constriction in the conduit. A suitable arrangement is shown in
FIG. 1a.
In FIG. 1a, liquid from a reservoir, not shown, is supplied to
transducer 10' by plastic hose 6' which is forced over the end of
the transducer. Electrical connection to the inner electrode 14 is
provided by extending the electrode over the end of ceramic tube 13
to the outer surface, as shown at 14'. Thin wire conductor 17' is
secured to electrode extension 14' by solder 19' and acts as a
terminal for the transducer. With this arrangement, somewhat higher
amplitude electrical pulses are required to expel liquid.
FIG. 1b shows a modification of the construction of FIG. 1a in
which the supply line acoustic impedance is made at least as high
as the impedance of the exit orifice, not including the effect of
surface tension at the orifice. The modification consists in
cementing to the inlet end of the transducer 10' a jewel 11' having
opening 5' with the same dimensions as exit orifice 5.
Although the arrangements of FIGS. 1a and 1b are satisfactory,
generally it is desirable to provide higher acoustic impedance at
the transducer inlet. In the construction of FIG. 1, this is
accomplished by use of small bore tube 8. Other alternatives
include a thin slit, or a porous member, or other acoustic
resistance, at the transducer inlet through which the liquid must
pass. Furthermore, some advantage would accrue when using a tube
such as 8 in FIG. 1, by adding an acoustic resistance at the inlet
end dimensioned to act as a matched acoustic termination for the
tube as a transmission line. This would reduce, or eliminate,
acoustic resonance effects in tube 8. However, excellent results
have been obtained without such termination.
The change in volume within transducer 10, when the latter is
pulsed, must exceed the volume of liquid to be ejected at orifice
5. The ceramic composition and the dimensions of tube 13 and the
energy of the actuating pulses are factors that may be traded in
arriving at a suitable design. Good results have been attained with
transducer volume change calculated to be about four times the
volume of the liquid to be expelled. For a fully electroded thin
wall tube, unrestrained by end clamping or acoustic load, the
fractional volume change due to the piezoelectric effect is
approximately:
(.DELTA.V/V) = -3d.sub.31 E/t where (.DELTA.V/V) = volume change
per unit volume d.sub.31 = piezoelectric strain constant E =
applied voltage t = thickness of tube wall Care must be taken to
measure wall thickness t in units consistent with the units used in
expressing d.sub.31, usually MKS units. THe negative sign indicates
contraction when the applied voltage has the same polarity as the
original polarizing voltage.
Another requirement is that the rate of change of volume must be
sufficient in relation to the acoustic impedance loading the
transducer to develop enough pressure to overcome the surface
tension at orifice 5.
A variety of simple circuits may be used to apply suitable command
pulses to the transducer. FIG. 2 shows one example in which the
capacitance of the transducer is used as part of the pulse shaping
circuit. In FIG. 2, transducer 10 is shown schematically in cross
section. The encircled polarity signs indicate that the ceramic
tube employed in this example was polarized during manufacture with
the inner electrode positive, and the outer electrode negative. A
d-c supply 20, shown for simplicity as a battery, has the negative
terminal connected to the inner electrode 14. The positive terminal
of supply 20 is connected through series resistors 23, 25 to the
outer electrode 16. Resistor 23 has a relatively high resistance
and resistor 25 has a relatively low resistance.
Transistor 26 is used as a switch. Collector 32 is connected to the
junction between resistors 23 and 25, and the emitter 34 is
connected to the negative side of supply 20. Control pulses 31 may
be applied between base 28 and emitter 34 via terminals 29.
Under quiescent conditions, the switch is open and the transducer
capacitance is charged to the voltage of supply 20. Since the
polarity of the applied voltage is the opposite of the original
polarizing polarity, the transducer is in an expanded state.
When a pulse 31 is applied to terminals 29, transistor 26 switches
to a low value of collector-emitter resistance for the duration of
the pulse. This permits the capacitance of the transducer to
discharge rapidly through low resistance 25 and the transistor "ON"
resistance. The transducer responds by contracting suddenly,
expelling a small quantity of liquid at orifice 5, as previously
described.
When pulse 31 falls approximately to zero, transistor 26 turns off,
allowing the transducer capacitance to recharge through resistors
23, 25 to the voltage of supply 20. Due to the higher value of
resistor 23, the charging takes place relatively slowly. The
transducer responds by expanding slowly, while liquid from tube 8
replaces the liquid expelled, as previously described. Thus, in
response to control pulses 31, the circuit provides short rise time
command pulses having relatively long decay times, as shown at 33.
For best results, the decay time should be at least four times the
rise time.
Some improvement in performance is obtained by adding an inductance
36 in series with the collector of the transistor, as shown in FIG.
2a, or in series with the transducer, as shown in FIG. 2b.
For a transducer having capacitance of about 5,000 picofarads an
inductance in the range of 1 to 10 millihenries has given good
results. A typical wave form for the pulse voltage applied to the
transducer is shown at 33'.
An example of a satisfactory system design is summarized in the
following table, referring to the construction of FIG. 1: ceramic
tube 13 Length 12.7 millimeters Inside diameter .76 millimeters
Wall thickness .25 millimeters Composition -- lead zirconate-lead
titanate type having the following published nominal
characteristics: K.sub.3 3400 k.sub.31 -.388 d.sub.31 - 274 .times.
10.sup.-.sup.12 meter/volt s.sub.11.sup.E 16.5 .times.
10.sup.-.sup.12 meter.sup.2 /newton 7.5 .times. 10.sup.3
Kilograms/meter.sup.3 Orifice 5 Diameter .06 millimeter Length .06
millimeter Supply tube 8 Inside diameter .41 millimeter Length 12.7
millimeters Liquid Water base ink having viscosity and surface
tension similar to water Drive circuit - FIG. 2b Supply 20 50 volts
Transistor 26 MJ 421 resistor 25 200 ohms Resistor 23 1000 ohms
Inductor 36 2 millihenries Control pulse 31 Amplitude 3
milliamperes Duration 20 microseconds Droplets Diameter of ink spot
.13 millimeter Exit velocity 1 to 2 meter/second Repetition rate up
to 50,000/second
For definitions of the characteristics listed for the ceramic
material, reference may be made to: IRE Standards of Piezoelectric
Crystals - Measurements of Piezoelectric Ceramics. Proceedings of
the IRE Vol. 49, No. 7, July 1961 (IEEE 179-1961).
With the circuit of FIG. 2 there is a limit to the supply voltage
20 beyond which depolarization of the ceramic may result. The limit
depends on the composition of the ceramic material and on the wall
thickness of tube 13. FIG. 3 illustrates a circuit arrangement that
does not have these limitations but requires additional
components.
In FIG. 3 the positive terminal of supply 20 is connected to the
inner electrode 14 of transducer 10 and the negative terminal is
connected through transistor switch 26 and resistor 25 to outer
electrode 16. When the transistor is off, no voltage appears at the
transducer. When the transistor is on, the voltage of supply 20 is
applied to the transducer with the same polarity used during
polarization of the ceramic tube, thus, depolarization due to the
excessive voltage cannot take place. Blocking capacitor 35 couples
the control pulses applied at terminals 29 to the transistor base
28. Diode 37 permits the normal quiescent charge to be
reestablished at capacitor 35 as the control pulse falls to
zero.
Under quiescent conditions transistor 26 is turned off and,
therefore, transducer 10 has no charge. When a control pulse 31'
occurs, transistor 26 turns on and the capacitance of transducer 10
charges rapidly through low resistance 25 and the "ON" resistance
of the transistor. This requires a low impedance supply at 20. The
transducer responds by contracting rapidly, expelling liquid
through the orifice. As pulse 31' falls to zero, transistor 26 is
turned off and the capacitance of the transducer discharges
relatively slowly through large resistance 23. The transducer
responds by expanding slowly while the expelled liquid is replaced.
An inductance may be connected in series with the transistor or
transducer as in FIGS. 2a or 2b.
If the liquid is corrosive to the electrode material of the ceramic
tube, the construction of FIG. 4 may be employed. In this case, the
small bore liquid supply tube 38 extends through transducer tube
13. It is shown necked down at the end to form nozzle shaped
orifice 39. However, a watch jewel, such as 11 in FIG. 1, or other
orifice arrangement may be used. Transducer tube 13 surrounding the
conduit is in stress transmitting engagement with the wall of the
conduit by virtue of epoxy cement 40 and, therefore, the transducer
is coupled to the liquid within the conduit. This arrangement
results in reduced sensitivity because of the stiffness of conduit
tube 38, and, therefore, higher pulse energy is required to expel
liquid and it is advantageous to use a circuit such as shown in
FIG. 3.
It is not necessary that the liquid flow through the transducer.
For example, in FIG. 5, conduit 42 comprises small bore supply
section 8' enlarged at the end thereof for attachment of orifice
plate 11. A T extension 41 couples to one end of transducer 10. The
other end of transducer 10 is closed by cap 43. When a command
pulse is applied, the transducer contracts suddenly, expelling
liquid from the transducer into conduit 42. The resulting acoustic
pressure pulse overcomes surface tension at orifice 5, causing
ejection of liquid such as droplet 7. The high acoustic impedance
of supply portion 8' retards flow back toward the reservoir.
This invention is not limited to the use of tubular piezoelectric
transducers. Different geometries and constructions may be used, as
well as different transducer principles. One variation is to
replace piezoelectric ceramic tube 13 of FIGS. 1, 4, 5 with a tube
formed from an electrostrictive material having little or no
remanent polarization. In this case, a pulse of either polarity
will cause the same volume contraction, and a circuit such as shown
in FIG. 3 would be used.
Magnetostrictive transducers also may be employed. One way to do
this is to use magnetostrictive material in forming tube 38 of FIG.
4. Transducer tube 13 then is replaced by an energizing winding
magnetically coupled to the tube. To eject liquid, a short rise
time current pulse is applied to the winding.
As another example, FIG. 6 shows a sectional view of a
transducer-conduit assembly employing a thin piezoelectric ceramic
disc 44. It is clamped around the periphery between O-ring gaskets
46, 47 within a housing made up of members 49, 50. A small cross
section annular passageway 51 is formed around the disc by the
inner walls of body members 49, 50, O-rings 46, 47, and the exposed
edge of disc 44. A small bore liquid supply tube 8 is secured in
opening 52 in body member 50. The opening communicates with annular
passageway 51. Tube 8 may extend to a liquid reservoir or may be
coupled thereto by larger tube 6. A second opening 54 also
communicates with annular passageway 51 and terminates at orifice
plate 11. Thus, a liquid conduit is formed by supply tubes 6 and 8,
opening 52, two parallel portions of annular passageway 51, opening
54, and orifice plate 11.
Ceramic disc 44, exposed to the liquid only at the rim, acts as an
electroacoustic transducer coupled to the liquid. Flexible lead
wires 55, 56 are soldered to the electrodes 58, 59 of disc 44 and
act as terminals for the transducer.
When it is desired to expel liquid from orifice 5 a short rise time
voltage pulse is applied to terminal wires 55, 56. This results in
sudden expansion of the diameter of transducer 44, displacing
liquid from annular passageway 51. The resulting acoustic pressure
pulse expels liquid from orifice 5. As the pulse slowly goes to
zero, liquid is pulled into annular passageway 51 from tube 8 to
replace the liquid previously expelled.
Although many different circuit arrangements may be constructed to
drive transducer 44, it is convenient to use a circuit similar to
the circuit of FIG. 2. In this case, however, the negative side of
supply 20 is connected to the electrode of transducer 44 that was
negative during polarization. With this polarity, the quiescent
voltage applied to transducer 44 holds the disc in diameter
contracted condition. When transistor 26 is turned on by a pulse at
terminals 29 the capacitance of the transducer discharges rapidly
through the transistor and low resistance 25. The transducer
responds by expanding suddenly to the diameter it had prior to
connection of power supply 20 and expels liquid, as previously
described. When the control pulse falls to zero, the transducer
recharges to the voltage of supply 20, contracting in diameter as
it does so.
While there have been described what are at present considered to
be the preferred embodiments of this invention, it will be obvious
to those skilled in the art that various changes and modifications
may be made therein without departing from the invention, and it is
aimed, therefore, in the appended claims to cover all such changes
and modifications as fall within the true spirit and scope of the
invention.
* * * * *