Information
-
Patent Grant
-
6685295
-
Patent Number
6,685,295
-
Date Filed
Tuesday, January 30, 200124 years ago
-
Date Issued
Tuesday, February 3, 200421 years ago
-
Inventors
-
Original Assignees
-
Examiners
- Gordon; Raquel Yvette
- Stewart, Jr.; Charles W.
Agents
-
CPC
-
US Classifications
Field of Search
US
- 347 85
- 347 23
- 347 14
- 347 19
- 347 12
- 347 10
- 347 11
- 347 84
- 347 6
- 347 5
- 347 86
- 347 20
- 347 7
- 347 9
- 347 16
- 347 59
- 073 290 R
-
International Classifications
- B41J29393
- B41J2175
- B41J2938
-
Abstract
In an inkjet printer using ink reservoirs located physically remote from the print head, tubes are used to deliver ink from the ink reservoirs to the print heads. Air initially present within the tubes can interfere with the proper operation of the print heads and cause print head reliability problems Additionally, air present within the tubes can interfere with the proper flow of ink from the ink reservoirs to the print heads through the tubes. An embodiment of a fluid continuity measurement apparatus includes current sources for each of the tubes. Each of the current sources delivers a substantially constant current to the corresponding tube. Voltage measurement circuits are coupled across each of the tubes. Each of the voltage measurement circuits generates an output corresponding to the voltage across the corresponding tube. The voltages appearing between the ends of the tubes changes as the volume of the air within the tubes changes. Increasing the volume of air within the tubes increases the resistance of the tubes there by increasing the voltages resulting from the application of a substantially constant current. A controller coupled to the output of the voltage measurement circuits compares each of the voltages output from the voltage measurement circuits to an empirically determined threshold value to determine if the volume of air within the tubes has reached an unacceptable level.
Description
FIELD OF THE INVENTION
This invention relates to the measurement of fluid continuity in the fluid inside of a fluid carrying member.
BACKGROUND OF THE INVENTION
In a certain class of imaging devices, known as off axis inkjet printers, liquid colorant is delivered from a reservoir to an imaging head through a fluid carrying member, such as a tube. The reservoir and the imaging head are separated to reduce the mass of the imaging head and allow lower cost replenishment of the ink in the inkjet printer. Through a variety of ways, voids can form in the liquid colorant. These voids can interfere with the proper working of the imaging head. Another possible problem is that replacement of an ink reservoir is done improperly so that liquid colorant cannot flow from the reservoir to the imaging head. A need exists for a method and apparatus to detect voids within a fluid carrying member.
SUMMARY OF THE INVENTION
Accordingly, in an imaging device an apparatus for measuring a parameter relate to a flow of power through a fluid within a member includes a power source arranged to supply the power to the fluid within the member. In addition, the apparatus includes a measurement device configured to measure the parameter and generate a corresponding signal.
In an imaging device, a method for measuring continuity of a fluid, includes applying power to the fluid within a member and measuring a parameter related to a flow of power through the fluid. In addition, the method includes generating a signal corresponding to the parameter.
An inkjet imaging device includes an imaging mechanism configured to place ink onto media using a print head. In addition, the inkjet imaging device includes a container for holding the ink and a fluid carrying member coupled between the container and the print head. The inkjet imaging device also includes a controller coupled to the imaging mechanism and configured to generate signals used by the imaging mechanism to place the colorant onto the media. Furthermore, the inkjet imaging device includes a power source configured to supply power to the ink thin the fluid carrying member and a measurement device configured to measure a parameter related to a flow of the power through the ink.
DESCRIPTION OF THE DRAWINGS
A more thorough understanding of embodiments of the fluid continuity measurement apparatus may be had from the consideration of the following detailed description taken in conjunction with the accompanying drawings in which:
Shown in
FIG. 1
is a simplified diagram of an embodiment of the fluid continuity measurement apparatus.
Shown in
FIGS. 2A-2I
are alternative embodiments of the fluid continuity measurement apparatus.
Shown in
FIG. 3A
is a high level block diagram of an inkjet imaging device.
Shown in
FIG. 3B
is an exemplary inkjet imaging device.
Shown in
FIG. 4
are assemblies from the inkjet imaging device of FIG.
3
B.
Shown in
FIG. 5A
is a circuit configuration used to measure the voltage across an ink filled tube as the volume of ink within in the tube changes.
Shown in
FIG. 5B
is a table including measurement data obtained using the circuit configuration shown in FIG.
5
A.
DETAILED DESCRIPTION OF THE DRAWINGS
Although an embodiment of the fluid continuity measurement apparatus will be discussed in the context of detecting an absence of continuity between an ink reservoir and a print head or a decrease in the ability of ink to easily move in a tube between an ink reservoir and a print head in an inkjet printer, it should be recognized that the disclosed principles are broadly applicable. For example, an embodiment of the fluid continuity measurement apparatus could be used in an application in which it is important to deliver a fluid at a substantially constant rate through a fluid carrying member. The embodiment of the fluid continuity measurement apparatus would detect the presence of voids in the fluid inside of the fluid carrying member and signal a controller. In response to receiving the signal the controller would either stop dispensing fluid through the fluid carrying member or generate a warning that the fluid dispensing is not being performed correctly.
Shown in
FIG. 1
is a simplified diagram of an embodiment of the fluid continuity measurement apparatus. A power source, such as electric power source
10
, provides electric energy to fluid carrying member
12
. In
FIG. 1
, electric power source
10
is shown as delivering electric power to fluid carrying member
12
in a general fashion. That is, the coupling of electric power source
10
to fluid carrying member
12
shown in
FIG. 1
could be implemented in a wide variety of specific ways depending upon the type of electric power source used and the circuit configuration in which it is used. The electric energy supplied could be substantially constant with respect to time or it could be time varying. Fluid carrying member
12
is adapted to carry a fluid. The fluid inside of fluid carrying member
12
is at least somewhat conductive. A measuring device, such as measuring device
14
, measures a parameter related to the flow of electrical energy through the fluid included within fluid carrying member
12
. The measuring device
14
generates a signal corresponding to the parameter measured by measuring device
14
. In
FIG. 1
, measuring device
14
is shown as measuring the parameter related to the flow of electrical energy in a general fashion That is, the coupling of measuring device
14
to fluid carrying member
12
shown in
FIG. 1
could be implemented in a wide variety of specific ways depending upon the type of measuring device used and the circuit configuration in which it is used. If the continuity of fluid present in fluid carrying member
12
is obstructed, the flow of electric energy through the fluid will change. The magnitude of the change in the flow of electric energy is dependent upon the degree of obstruction. Consider the case in which electric power source
10
include a voltage source, the current flowing through the fluid will be inversely proportional to the effective resistance of the fluid over the length of fluid carrying member
12
. When voids are present within the fluid in fluid carrying member
12
, the effective electrical resistance between the ends of fluid carrying member
12
is above the value present when fluid substantially fills the interior volume of fluid carrying member
12
. As the fluid flow is progressively obstructed in fluid carrying member
12
, the effective resistance increases, thereby reducing the flow of current. Corresponding to the decrease in the flow of current, the signal generated by measuring device
14
changes as the flow of electric energy through the fluid changes. Therefore, the signal generated by measuring device
14
provides an indication of the continuity of fluid within fluid carrying member
12
. The relationship between the effective resistance and the fraction of the volume inside fluid carrying member
12
filled by voids can be empirically derived or analytically estimated. Using this relationship, the degree to which fluid carrying member
12
is filled by voids can be estimated from the measured values of the parameter.
A variety of different measuring devices could be used for measuring device
14
. For example, measuring device
14
could be a voltage measuring device, a current measuring device, or an electric power measuring device. In addition, the different types of measuring devices may be used in a variety of circuit configurations to measure continuity of fluid. Shown in
FIG. 2A
is a first configuration of an embodiment of the fluid continuity measurement apparatus using a voltage measuring device, such as voltage measurement circuit
100
. Voltage measurement circuit
100
generates a signal related to the voltage between the ends of fluid carrying member
12
(with voltage measurement circuit
100
coupled between the ends of fluid carrying member
12
). A resistance, such as resistive element
102
, is coupled in series with electric power source
104
and fluid carrying member
12
. In this embodiment of the fluid continuity measurement apparatus, electric power source
104
could be either a voltage source or a current source. The signal from the output of voltage measurement circuit
100
changes substantially proportionally to the voltage appearing across fluid carrying member
12
.
Where electric power source
10
includes a voltage source and voltage measurement circuit
100
is coupled across fluid carrying member
1
2
, an increase in the effective resistance across fluid carrying member
12
increases the voltage across fluid carrying member
12
. Where electric power source
10
includes a substantially constant current source and voltage measurement circuit
100
is coupled across fluid carrying member
12
, an increase in the effective resistance across fluid carrying member
12
substantially proportionally increases the voltage across fluid carrying member
12
. The signal from the output of voltage measurement circuit
100
will change correspondingly.
It should be recognized that alternative circuit configurations could be used to measure a change in the effective resistance across fluid carrying member
12
. For Example, in an alternative embodiment of the fluid continuity measurement apparatus shown in
FIG. 2B
, voltage measurement circuit
100
could be coupled across resistive element
102
. In this alternative embodiment, electric power source
104
includes a voltage source and voltage measurement circuit
100
is coupled across resistive element
102
. An increase in the effective resistance across fluid carrying member
12
will decrease the voltage across fluid carrying member
12
. The signal from the output of voltage measurement circuit
100
will change correspondingly. In another embodiment of the fluid continuity measurement apparatus shown in
FIG. 2C
, electric power source
104
includes a current source coupled in series with fluid carrying member
12
. In this embodiment, there is no series connected resistance and voltage measurement circuit
100
is coupled across fluid carrying member
12
. An increase in the effective resistance across fluid carrying member
12
substantially proportionally increases the voltage across fluid carrying member
12
. The signal from the output of voltage measurement circuit
100
will change correspondingly. Shown in
FIG. 2D
is another embodiment of the fluid continuity measurement apparatus in which electric power source
10
includes a voltage source. Current measurement circuit
106
is coupled in series with fluid carrying member
12
. An increase in the effective resistance decreases the current flowing through the fluid inside of fluid carrying member
12
. The signal from the output of current measurement circuit
100
will change correspondingly. Shown in
FIG. 2E
is another embodiment of the fluid continuity measurement apparatus in which electric power source
10
includes either a voltage source or a current source. Electric power measurement circuit
108
measures the electric power delivered by electric power source
10
to the fluid within fluid carrying member
12
. An increase in the effective resistance changes the electric power dissipated within the fluid. The signal from the output of power measurement circuit
100
changes as a result of the change in the power dissipated within the fluid.
Shown in
FIGS. 2F through 2I
are additional embodiments of the fluid continuity measurement apparatus in which time varying electric power source
110
, either a voltage source or a current source, is used to generate a waveform having characteristics related to the resistance across the fluid in fluid carrying member
12
. For each of the circuit configurations shown in
FIGS. 2F through 2I
, time varying electric power source
110
creates a time varying waveform of voltage across the components or current through the components within the circuits having a shape dependent upon the values of the reactive components and he magnitude of the resistance across the fluid in fluid carrying member
12
.
Although
FIGS. 2F through 2I
show the voltage measurement circuit
112
electrically coupled in a variety of configurations, it should be recognized that Voltage measurement circuit
112
could be coupled across any of the components or across the fluid in fluid carrying member
12
. Similarly, current measurement circuit
114
could be coupled in series with any of the components or with the fluid in fluid carrying member
12
. With respect to the configuration of voltage measurement circuit
112
and current measurement circuit
114
, the most useful configurations are those for which a waveform can be measured having a shape related to the resistance across the fluid in fluid carrying member
12
.
Time varying electric power source
110
could include a voltage source or current source configured to deliver pulses of various possible shapes, such as a square wave pulse or a sawtooth pulse. Alternatively, time varying electric power source
110
could provide periodic signals, such as a square wave or a sine wave. Voltage measurement circuit
112
and current measurement circuit
114
could be configured to successively sample, respectively, the voltage or current waveform which they are configured to measure. Alternatively, voltage measurement circuit
112
and current measurement circuit
114
could generate an output related to the measured RMS voltage or current. This alternative would be particularly well adapted where time varying electric power source
110
generates a sinusoid.
For the cases in which voltage measurement circuit
112
and current measurement circuit
114
provide a succession of sampled values from, respectively, a voltage waveform or a current waveform, these samples could be use to compute the time constant of the circuit that gave rise to the waveforms. The resistive element of the circuit is contributed, primarily, by the resistance across the fluid in fluid carrying member
12
. The value of the reactance in the circuit is contributed, primarily, by the reactive component
116
(such as capacitor or inductor) in the circuit. The values of these components are known. From the successive samples of the voltage or current waveform values, a time constant of the circuit can be computed. Because the time constant of a resistive-capacitive circuit is computed as R×C and the time constant of a resistive-inductive circuit is computed as L÷R, with the values of C and L known and having the computed value of the time constant, R (the resistance of the fluid across fluid carrying member
12
) can be computed. For the cases in which voltage measurement circuit
112
and current measurement circuit
114
provide RMS values of, respectively, voltage and current in the circuit and where time varying electric power supply supplies a periodic sinusoid, the value of the resistance of the fluid across fluid carrying member
12
can be computed knowing the frequency of the sinusoid, the value of the inductance or capacitance in the circuit, and the measured RMS value of voltage or current.
Shown in
FIG. 3A
is a high level block diagram of an inkjet imaging device, inkjet printer
110
. Inkjet printer
110
includes an embodiment of an imaging mechanism, imaging mechanism
112
. Imaging mechanism
112
includes the hardware needed for forming an image on media using ink. Imaging mechanism
112
includes print heads
114
used to eject ink onto media according to signals received from print head driver electronics
116
. Controller
118
receives image data defining an image through interface
120
from computer
122
. From this image data, controller
118
generates print data supplied to print head driver electronics
116
corresponding to the image data. The signals supplied by print heal driver electronics
116
to print heads
114
power the resistors used to eject ink from the nozzles of print heads
114
.
Shown in
FIG. 3B
is an exemplary inkjet imaging device, inkjet printer
200
, including an embodiment of the fluid continuity measurement apparatus. Fluid continuity measurement apparatus
201
is shown schematically for simplicity of illustration. In inkjet printer
200
, an imaging head, such as print heads
202
-
208
, eject ink onto media, such as paper. Print heads
202
-
208
are mounted onto carriage
210
. During an imaging operation, carriage
210
is precisely moved along a guide, such as rail
212
, across the width of paper. Print head driver electronics, electrically coupled to print heads
202
-
208
, provide signals used to eject colorant, such as ink, from nozzles included within print heads
202
-
208
. Typically, the colorants include cyan, magenta, yellow, and black. Reservoirs, such as ink cartridges
214
-
220
are mounted within inkjet printer
200
at a physically separate location from carriage
210
. Each of ink cartridges
214
-
220
stores ink for one of the cyan, magenta, yellow, and black colors. Tubes
222
-
228
are coupled between each of the respective colors of ink cartridges
214
-
220
and the corresponding ones of print heads
202
-
208
.
Included with each of print heads
202
-
208
is a small volume for storing the ink that will be ejected from the respective ink cartridges
214
-
220
during an imaging operation. Typically, a predetermined amount of ink is deposited into print heads
202
-
208
during manufacture. As imaging operations are performed, the ink initially deposited into print heads
202
-
208
is depleted. As ink within print heads
202
-
208
is depleted, ink is forced, under pressure, through tubes
222
-
228
from ink cartridges
214
-
220
into the corresponding print heads
202
-
208
.
208
. It should be recognized that embodiments of the fluid continuity measurement apparatus would also work in systems that do not use pressure greater than atmospheric pressure in tubes
222
-
228
. For example, embodiments of the fluid continuity measurement apparatus could be used in systems the pressure within tubes
222
-
228
falls below atmospheric pressure as ink is ejected from print heads
202
-
208
.
An excessive volume of air entering print heads
202
-
208
will interfere with their proper operation. One failure mode of print heads
202
-
208
that can result from excessive air involves the unintended leakage of ink out of the nozzles of print heads
202
-
208
. Another failure mode of print heads
202
-
208
that can result from excessive air includes damage to resistive elements associated with each of the nozzles in print heads
202
-
208
. Excessive air can displace ink in regions near the resistive elements associated with each of the nozzles. The heat result from the application of electric power to the resistive elements without ink present can damage the respective resistive elements.
Prior to the first imaging operations performed, tubes
222
-
228
are filled with air. There are several techniques for handling the presence of air in tubes
222
-
228
. In inkjet printer
200
, a fluid interconnect system allows print heads
202
-
208
to be disconnected and reconnected to and from tubes
222
-
228
. A first technique for purging the air from tubes
222
-
228
includes the use of inoperable print heads in place of print heads
202
-
208
during a purging operation that pushes ink into tubes
222
-
228
to push air out of tubes
222
-
228
and into the inoperable print heads. A second technique is to include additional volume within print heads
202
-
208
for containing air purged from tubes
222
-
228
. After print head
202
-
208
are installed into inkjet printer
200
, ink is moved into tubes
222
-
228
228
which displaces air into print heads
202
-
208
. For this alternative, print head
202
-
208
are designed with additional volume to store air purged from tubes
222
-
228
so that air is stored ink print heads
202
-
208
.
Consider the alternative in which inoperable print heads are used to store the air purged from tubes
222
-
228
. In the fluid interconnect system used with this alternative, a hollow needle is pushed through a hole in a rubber membrane so that fluid in tubes
222
-
228
can be delivered to print heads
202
-
208
. Occasionally, when an attempt is made to make a fluid connection between tubes
222
-
228
and the inoperable print heads, the rubber membrane blocks a hole in the sidewall of the hollow needle. If this occurs, air remains trapped in tubes
222
-
228
after the purging operation because ink is not able to move from ink cartridges
214
-
220
through tubes
222
-
228
to push air into the inoperable print heads. When a fluid connection is made between print heads
202
-
208
and tubes
222
-
228
, ink will not initially flow in an unobstructed manner through tube
222
-
228
because of the air remaining in tubes
222
-
228
. Displacement of the air remaining in tubes
222
-
228
into print heads
202
-
208
will likely cause premature failure of print heads
202
-
208
.
The other technique for addressing the air in tubes
222
-
228
may also not be completely effective in removing air from tubes
222
-
228
. Air trapped in tubes
222
-
228
forms voids within the ink in tubes
222
-
228
. These voids may be of sufficient size to significantly obstruct the flow of ink through tubes
222
-
228
. Void formed from air trapped against the sidewalls of tubes
222
-
228
are able to grow in size over time. Once air is trapped against a sidewall of tubes
222
-
228
, air can diffuse through the sidewall and increase the size of the void so that ink flow through the respective tubes
222
-
228
is significantly reduced or stopped.
For wide variety of techniques used to address the air in tubes
222
-
228
(including other techniques not disclosed in this specification or those later developed), an embodiment of the fluid continuity measurement apparatus can be used to detect the presence of voids within the ink in tubes
222
-
228
. The embodiment of the fluid continuity measurement apparatus included within inkjet printer
200
detects the presence of voids within the ink present in tubes
222
-
228
by measuring a parameter related to the flow of electric power through the ink for each of tubes
222
-
228
. Included within the embodiment of the fluid continuity measurement apparatus are measurement devices
230
configured for measuring the parameter related to the flow of electric power through the ink for each of tubes
222
-
228
. Electric power is supplied to the ink within each of tubes
222
-
228
228
by electric power sources
232
. Measurement devices
230
generate signals related to the parameter for each of tubes
222
-
228
. Controller
234
receives these signals and compares each of them to a threshold value to determine if the detected void is sufficiently large to interfere with the proper delivery of ink to the respective print heads
202
-
208
.
Shown in
FIG. 4
is a simplified representation of the connections between print heads
202
-
208
, ink cartridges
214
-
220
, and tubes
222
-
228
with the embodiment of the fluid continuity measurement apparatus. In this embodiment of the fluid continuity measurement apparatus, electric power sources
232
included current sources
300
-
306
electrically connected in series, respectively, with print heads
202
-
208
, tubes
222
-
228
, and ink cartridges
214
-
220
. Measurement devices
230
include voltage measurement circuits
308
-
312
coupled, respectively, across tubes
222
-
228
. Each of current sources
300
-
306
delivers a substantially constant current that flows from the respective ones of ink cartridges
214
-
220
through the ink in tubes
222
-
228
and returns to current sources
300
-
306
through print heads
202
-
208
. The output of voltage measurement circuits
308
-
312
are coupled to analog multiplexer
314
. Analog multiplexer
314
uses two bits from controller
316
to select one of the four voltage signals provide by voltage measurement circuits
308
-
314
. The selected one of the four voltage signals is coupled to analog to digital converter
318
. Analog to digital converter
31
8
converts the selected voltage to an eight bit digital value received by controller
316
.
The voltage values generated by each of voltage measurement circuits
308
-
312
312
re directly related to the resistance of the ink volume in each of the respective ones of tubes
222
-
228
. As the resistance of the ink in ones of tubes
222
-
228
increases, the voltage measure across the respective ones of tubes
222
-
228
will also increase. Controller
316
compares the digital value of the voltages measured for each of tubes
222
-
228
to a threshold value. If the digital value of the voltage exceeds the threshold, controller
316
generates a signal indicating to the user that air must be purged from the ones of tubes
222
-
228
having digital value exceeding the threshold. The threshold value could be empirically determined by measuring the voltage across tubes
222
-
228
for a range of voids with tubes
222
-
228
. The threshold value would be set at a level corresponding to some maximum tolerable level of voids within tubes
222
-
228
. Alternatively, if the relationship between the resulting voltage across tubes
222
-
228
and the void within tubes
222
-
228
was well known, the threshold could be determined analytically.
Shown in
FIG. 5A
is a circuit that was used to measure the relationship between the volume of ink in a tube and the resulting voltage that is measured across the ink in the tube. A variable amount of ink is stored in tube
400
. Electric power supply
402
is connected in series with tube
400
and meter
404
. Electric power supply
402
is set to supply 15 volts. The volume of ink in tube
400
was measured by measuring the length of tube
400
filled with ink. For a tube length of 34.5 inches, the amount of ink in tube
400
ranged from 0 inches to 31 inches.
Shown in
FIG. 5B
is a table showing the relationship between the voltage measured by meter
404
as the amount of ink within tube
400
varies from 0 inches to 31 inches. Electric power supply
402
is configured to provide a substantially constant 15 volts. A plot of this data reveals a strong correlation to a linear relationship. As the length of tube
400
containing ink decreases, the voltage dropped across the ink in tube
400
increases. Although the distribution of ink within the tube in the test configuration is likely different than the distribution of ink that will occur when voids form within tubes
222
-
228
, the experimentally measured data from the test configuration does demonstrate that reducing the volume of ink within the tube will increase the resistance through the ink between the ends of tubes
222
-
228
. It should be recognized that the test configuration used to generate the data shown in
FIG. 5B
will yield different results depending upon factors such as the ink chemistry (which affects ink conductivity), the cross sectional area of the fluid carrying member, and the length of the fluid carrying member.
Embodiments of the fluid continuity measurement apparatus have been described in the context of a fluid carrying member adapted for carrying ink, such as cyan ink, magenta ink, yellow ink, or black ink. It should be recognized that the conductivity of the ink is related to the chemistry of the specific ink. For example, dye based inks may have different conductivity than pigment based inks. Consequently, the threshold values for detection of a void of sufficient size to interfere with the proper delivery of ink will vary depending upon the specific type of ink in use. Furthermore, although this specification makes reference to “cyan ink”, “magenta ink”, and “yellow ink”, it should be recognized that these terms are used generically. That is, these terms refer to a variety of inks having a particular color of pigment or dye in a range of concentrations yielding a range of color intensities. In addition, although embodiments of the fluid continuity measurement apparatus are disclosed in the context of an inkjet imaging device using a CMYK color space, embodiments of the fluid continuity measurement apparatus could be usefully applied in inkjet imaging devices using other types of color spaces. Also, embodiments of the fluid continuity measurement apparatus could be used in systems that distribute other types of fluid.
As previously mentioned, embodiments of the fluid continuity measurement apparatus can be used to determine if a fluid connection has been established between ink cartridges
214
-
220
and print heads
202
-
208
. Consider the embodiment of the fluid continuity measurement apparatus shown in FIG.
4
. If a fluid connection has not been established between any one of ink cartridges
214
-
220
and the corresponding ones of print heads
202
-
208
, the voltage appearing across the corresponding ones of tubes
222
-
228
will be the maximum voltage that can be generated by the corresponding ones of current sources
300
-
306
. The voltage values measured by the corresponding ones of voltage measurement circuits
308
-
312
will be substantially above the threshold value. The user will then be notified that a fluid connection has not been established.
Consider the embodiment of the fluid continuity measurement apparatus show in
FIG. 4
when inoperable print heads are installed in place of print head
202
-
208
for an air purging operation. Initially, the voltage measured across tubes
222
-
228
will be the maximum voltage that can be generated by the corresponding ones of voltage measurement circuits
308
-
312
because each of tubes
222
-
228
will be initially filled with air. As air is purged from tubes
222
-
228
and a continuous path of ink between ink cartridges
214
-
220
and the inoperable print heads is formed, the voltage measured across tubes
222
-
228
by voltage measurement circuits
308
-
312
will decrease. When the air has been substantially purged from tubes
222
-
228
, the measured voltage for each of tubes
222
-
228
will reach a minimum value. When controller
316
determines (by making successive voltage measurements for each of tubes
222
-
228
) that the voltage across tubes
222
-
228
has reached a minimum, then controller
316
will generate a signal to indicate to the user that the air purging operation is complete.
Another way in which an embodiment of the fluid continuity measurement apparatus could be implemented involves the use of time domain reflectometry. This type of alternative embodiment of the fluid continuity measurement apparatus would use a simplified implementation of time domain reflectometer (TDR) to propagate an electrical pulse through the fluid within fluid carrying member
12
.
To create a transmission line like structure using fluid carrying member
12
and the fluid within it, a conductive sheath would be placed over the non-conductive wall of fluid carrying member
12
. The somewhat conductive fluid within fluid carrying member
12
would form the center conductor of a coaxial cable. The conductive sheath would form the outer conductor and the wall of fluid carrying member
12
would serve as the insulative material between the center conductor and the outer conductor. Waves would propagate through the insulative material. The greater the conductivity of the fluid, the more ideal the resulting transmission line will be because of the reduced resistive loss within the center conductor. To create a waveguide like structure using fluid carrying member
12
, the wall of fluid carrying member
12
would be formed from a conductive material. Waves would propagate through the fluid within fluid carrying member
12
. The lower the conductivity of the fluid, the more ideal the resulting waveguide will be because of the reduced resistive loss within the medium through which the waves propagate.
If the termination impedance at the end of fluid carrying member
12
substantially matches the characteristic impedance of fluid carrying member
12
filled with fluid, then the magnitude of the pulse reflected back toward the TDR will be substantially zero. A void within the fluid will create an impedance discontinuity in the transmission line or waveguide. The impedance discontinuity associated with the void will cause part of the electrical energy of the incident pulse to reflect from the discontinuity and propagate back toward the TDR.
By measuring the time delay between the initiation of the forward propagating pulse and the detection of the reflected pulse, the presence of a discontinuity and its location can be determined. The location of the discontinuity would be determined from the time interval between the launch of the forward propagating pulse and detection of the reflected pulse, knowing the propagation velocity of the pulse with fluid carrying member
12
. Furthermore, because a discontinuity results from both sides of the void along the length of fluid carrying member
12
, reflections would occur from both the front and back sides of the void. The time difference between the detection of these reflections could be used to determine the length of the void.
It should be recognized that the TDR technique would work regardless of whether the termination impedance at the end of fluid carrying member
12
matches the characteristic impedance of fluid carrying member
12
. If there was a mismatch reflection would be detected at the TDR at a later time then a reflected pulse resulting from a void. The time difference allows the TDR to distinguish between a void within fluid carrying member
12
and an impedance mismatch at the end of fluid carrying member
12
. However, there could be simplification of the TDR if, instead of requiring the capability to differentiate between different reflected pulses, it only had to detect a reflected pulse.
The detection of a reflected pulse or the detection of reflected pulse within a window of time (depending on the termination impedance) indicates the presence of an impedance discontinuity (such as a void) with fluid carrying member
12
. The magnitude of the reflected pulse is related to the magnitude of the impedance discontinuity. Using the magnitude of the reflected pulse measured by the TDR, the controller could determine whether the void is of sufficient size to indicate that an air purging operation needs to be performed.
Yet another way in which an embodiment of the fluid continuity measurement apparatus could be implemented involves the use of a power source, such as a sonic power source, to propagate power, such as sonic power, down fluid carrying member
12
. A sonic wave launched down fluid carrying member
12
would be reflected from a void within fluid carrying member
12
. Measurement of the time between the launching of the sonic wave down fluid carrying member
12
and the detection of the reflected sonic wave allows determination of the location of the void within fluid carrying member
12
. A sonic wave would be reflected from both sides of the void along the length of fluid carrying member
12
. By measuring the time difference between the sonic waves reflected from the front and back sides of the void, the length of the void could be determined.
The sonic power source could be implemented using a transducer that generates the sonic wave from the application of an electric signal. For this implementation, the transducer generating the sonic wave could also be used to detect the reflected sonic waves and provide an electric signal at the time at which the reflection is detected. Associated electronic circuitry would be used to process the electric signals corresponding to reflections and determine the location and length of the void. In addition, the electronic circuitry would be used to generate the signal that launches the sonic wave.
Although embodiments of the fluid continuity measurement apparatus have been illustrated, and described, it is readily apparent to those of ordinary skill in the art that various modifications may be made to these embodiments without departing from the scope of the appended claims.
Claims
- 1. An inkjet imaging device, comprising:an imaging mechanism configured to place ink onto media using a print head; a container for holding the ink; a fluid carrying member coupled between the container and the print head; a controller coupled to the imaging mechanism and configured to generate signals used by the imaging mechanism to place the colorant onto the media; a power source configured to supply power to the ink within the fluid carrying member; and a measurement device configured to measure a parameter related to a flow of the power through the ink.
- 2. The inkjet imaging device as recited in claim 1, further comprising:a resistance coupled in series with the ink, with the power source coupled in series with the resistance and the ink, the measurement device including a voltage measurement device coupled across the resistance, the parameter including a voltage across the resistance, the power source including an electric power source, and the power including electric power.
- 3. The inkjet imaging device as recited in claim 1, wherein:the electric power source includes a current source coupled in series with the ink within the fluid carrying member; the measurement device includes a voltage measurement device coupled across the ink; and the parameter includes a voltage across the ink.
- 4. The inkjet imaging device as recited in claim 1, wherein:the electric power source includes a voltage source coupled in series with the ink within the fluid carrying member; the measurement device includes a current measurement device coupled in series with the ink within the fluid carrying member; and the parameter includes a current through the ink within the fluid carrying member.
- 5. The inkjet imaging device as recited in claim 4, wherein:the print head includes a configuration for placing cyan colorant, magenta colorant, yellow colorant, and black colorant onto the media.
- 6. The inkjet imaging device as recited in claim 5, wherein:the fluid carrying member includes a tube.
US Referenced Citations (4)