The present invention relates to droplet deposition apparatus and to methods for manufacturing such droplet deposition apparatus. It may find particularly beneficial application in a method for manufacturing an inkjet printhead involving the use of laser ablation on an apparatus having a plurality of chambers.
A typical droplet deposition apparatus construction involves an array of fluid chambers, each chamber being provided with a respective aperture through which fluid is forced in the form of droplets during use of the apparatus.
A variety of alternative fluids may be deposited by such an apparatus: droplets of ink may travel to, for example, a paper or other substrate to form an image in inkjet printing applications; alternatively, droplets of fluid may be used to build structures, for example electrically active fluids may be deposited onto a substrate such as a circuit board so as to enable prototyping of electrical devices.
In order to effect such droplet deposition, the apparatus may be provided with electrically actuable means, such as one or more resistive elements, which may cause rapid heating of the fluid in a chamber in response to an applied voltage, or electrostrictive elements, such as piezoelectric members, which may deform in response to an applied voltage so as to apply a force to the liquid in a chamber. As a result, the electrically actuable means may increase the pressure inside a given fluid chamber and thus cause the release a droplet of fluid through the respective aperture. The electrically actuable means may typically be electrically connected, for example by a system of electrodes, to control circuitry, so that droplet deposition from the array may be controlled.
Oftentimes, a portion of the electrically actuable means, together with the electrical connection for such means, may be closely coupled with the chamber array and, indeed, may provide a portion of the walls of the chamber, in particular where the electrically actuable means comprise electrostrictive elements, such as piezoelectric members. The electrical connectors may similarly form a portion of the chamber walls, for example by being arranged on an interior surface as a result of electroplating and patterning an electrode layer.
In order to provide a droplet deposition apparatus operable to deposit drops at high resolution it may be desirable to provide an array of chambers with very fine spacing, which accordingly requires that the apertures for the chambers are disposed with a similarly fine spacing. In addition, in order that droplets produced by all chambers are of a consistent desired size, it may be desirable that the apertures for the chambers are formed with high accuracy.
To provide for these requirements, the manufacture of droplet deposition apparatus may involve the use of one or more beams of radiation, such as those produced by a high-power laser, to form the apertures for the chambers by ablation. The chambers may be formed by a various methods of manufacture, such as photolithography, wet or drying etching, or mechanical working, for example sawing using a diamond-impregnated blade.
In some constructions, chambers will mainly be formed in the face of one component, a nozzle plate component being attached to this component to enclose the chambers. This component may be, for example, an actuator component and may be provided with one or more connections to a fluid supply. The nozzle plate component may then be formed from, or include materials that expedite the formation of nozzles; for example, polymeric material, which may be easily ablated, can be used for the regions where the nozzles are to be formed.
With such constructions, it is possible to form nozzles in the nozzle plate component either before or after attachment of the nozzle plate component to the chamber-carrying component. However, it has been found that the alignment of preformed nozzles with the chambers is complex and, more importantly, generally less accurate than the processes used to form the nozzles. This is found to be particularly the case where nozzles are formed with high accuracy by laser ablation. For this reason, it is generally preferred that the nozzle formation is carried out following the attachment of the nozzle plate component. Nozzle formation following attachment of the nozzle plate component may also be preferred through the increased mechanical and thermal stability of the nozzle plate component when attached to other components.
Further, in other constructions that do not comprise a nozzle plate component, because of the high accuracy of nozzle formation processes it is nonetheless often found to be advantageous to carry out nozzle formation at an advanced stage of assembly of the apparatus.
More generally, forming the nozzle in an apparatus at an advanced stage of assembly reduces the risk of contamination or clogging of the nozzles by, for example, bonding materials.
A common problem that arises from the manufacture of droplet deposition apparatus is for certain chambers within an array to be defective or inoperable during use, in that they are unable to produce droplets of a desired size or at all. If too many such defective chambers are present in the apparatus it may be necessary to discard the apparatus, thus reducing the efficiency of the overall manufacturing process. Indeed, the number of such defective chambers that may be tolerated is typically very small, and thus the efficiency of the overall process may be very sensitive to such defects. Further, in view of the considerable expense of raw materials and the complexity of the process, any decreases in manufacturing efficiency will be costly.
The Applicant has found that certain classes of defects may be caused at least in part during the ablation of apertures for the chambers.
a), (b), (c) and (d) display a cross-sectional view through an exemplary apparatus undergoing such an ablation process.
As shown in
In the example shown, the beam (30) is focussed at a focal point (32) above the surface of the aperture member (13) so that the aperture (16) tapers outwardly. By appropriate changes to the focal point (32), and more generally the shape of the beam (30), a wide variety of shapes for the aperture (16) may be achieved.
Ablation debris (31) generally moves out of the bore in a plume back towards the source of the beam (upwards in
Further, it is also believed that, once the radiation beam (30) breaks through one wall of the chamber (10) and into its interior, ablation debris (31) may cause damage to the walls of the chamber by entering and adhering or otherwise contaminating the surfaces of the interior of the chamber (10). As a result, during use of the apparatus, fluid deposition may be hindered by the reaction of the ablation debris (31) with the fluid. This may be caused, for example, by flocculation (for example in the case of gel fluids) or sedimentation of components within the fluid, or other change in properties of the fluid. Further, the debris (31) may form a corrosive mixture with the fluid. Furthermore, even before use of the apparatus, it is possible that the ablation debris (31) may react directly with the materials of the interior of the chamber (10).
Typically the depth of cut into the aperture member (13) is controlled by means of limiting the amount of radiation energy applied, for example by limiting the period of time for which the beam (30) is incident on the surface. In some cases energy may be delivered by way of a number of pulses, with the number and/or energy of these pulses being limited to control the total amount of energy applied. Such an aperture formation process may be optimised by adjusting the beam energy across the series of pulses which are used to form each aperture.
However, despite the availability of such means to limit the total amount of radiation energy delivered to the surface, efforts to prevent excess radiation energy being applied have been frustrated by unavoidable variations in the characteristics of the surface resulting from the manufacturing process. For example, if the aperture member (13) is thinner than expected, excess radiation energy may still be transmitted to the interior surfaces of the channel (10), which, as described above, may cause a variety of problems. Equally, the material at a particular location may be less easily ablated.
Further, erring on the side of caution in the amount of radiation to deliver may equally lead to defects in the apparatus since the radiation beam (30) may fail to completely form the desired aperture (16).
In addition, some materials are found to be best ablated with a moderate energy beam (or a number of moderate-energy pulses) to remove the bulk of the material, with a high-energy finishing beam (which again may be delivered by a number of pulses) used to ensure a high-quality finish to the internal surfaces of the aperture (16). Such a method is discussed in EP1 393 911B. However, given the above considerations, such a process further increases the risk of damage due to excess radiation energy since the radiative flux may remain high after the point in time when the beam has broken through into the chamber.
As noted above and exemplified in
Furthermore, it has been previously proposed to pass a coating material through or over droplet deposition apparatus during manufacture so as to provide a coating or passivating layer (15) that forms part of—or in some cases substantially all of—the interior surfaces of the walls of a fluid chamber (10) (as is discussed, for example, in WO 2006/129072, where Parylene is utilised). This coating layer (15) may thus reduce chemical, electro-chemical and/or physical interaction between the fluid in the chamber and components that might otherwise form part of the chamber walls' interior surfaces such as the electrically actuable means (11) and electrodes (12) mentioned above.
Those skilled in the art will recognised that many alternative coating processes are known, such as line-of-sight deposition processes and alternative coating materials such as Silicon Nitride may suitably be used.
It should be noted that, while materials such as Parylene that are typically used in such coating processes are generally effective at reducing chemical and physical interaction between the materials of the chamber walls and the fluid within the chamber, they may have a tendency to be less resistant to the radiation used to ablate the apertures. Thus, the coating (15) will typically provide little protection to the apparatus during ablation of the apertures (16).
It has been found by the Applicant that, when apertures (16) are ablated in apparatus having chambers (10) coated in such a manner, the ablation debris (31) and the radiation beam (30) may also affect such a coating layer (15), thus exposing components forming part of the chamber walls but otherwise covered by the coating layer (15) to the fluid within the chamber. This is shown in
It should further be noted that constructions where a coating layer (15) is formed conformally over all the internal surfaces of the chamber (10) such as that shown in
Such damage (42) to a coating layer (15) may also lead to failure of fluid deposition from the chamber by flocculation (for example in the case of gel fluids), sedimentation of components within the fluid, or other change in properties of the fluid, as a result of exposure to the underlying materials of the chamber interior. In particular, where conductive fluids are used, these may contact the electrodes within the chambers (10) causing blockages or flow restrictions in the apparatus owing to agglomeration of conductive particles within the fluid.
It should be noted that such problems may occur even where the coating layer (15) is not completely removed, since over time the coating layer (15) may unavoidably be worn away and thus even minor damage causes a reduction in the expected operating lifetime of the apparatus.
It is therefore an object of aspects of the present invention to overcome or ameliorate some or all of such defects and/or malfunctions caused by ablation during manufacture of droplet deposition apparatus.
Thus, there is provided in accordance with a first aspect of the present invention a method of forming a component for a droplet deposition apparatus, the component comprising an array of fluid chambers, the method comprising the steps of: providing protection material so as to fill, at least in part, said chambers; directing at least one beam of radiation at said component so as to form an array of apertures by ablation of said component, each aperture extending through a portion of said component so as to communicate with a respective chamber, in use fluid being released from said chambers through said apertures in the form of droplets to be deposited; wherein said protection material acts to inhibit damage to the walls of said chamber during said ablation; and removing said protection material.
Suitably, said protection material may inhibit damage at least in part by absorbing energy from said radiation. Specifically, such energy absorption may involve a phase change of the protection material. The phase change may include melting, which term is intended to include the transition from an amorphous solid, wax, glass or such like to a liquid. Additionally, the protection material may inhibit damage by capturing and carrying away the debris created by the ablation step when the protection material is removed.
Suitably, a chamber is filled, at least in part, with protection material prior to the formation by ablation of the aperture for that chamber. Preferably, said protection material is removed from a chamber following the formation by ablation of the aperture for that chamber. Said removal of protection material may comprise flowing a flushing fluid through the apparatus. Said flushing fluid may preferably be heated and/or may be a solvent for the protection material.
In some embodiments, protection material may be caused to flow through said chambers simultaneously with said step of forming apertures.
The one or more beams of radiation may be provided by a high-power laser.
Preferably, said protection material is in an incompressible state immediately prior to said step of directing at least one beam of radiation at the component. Protection material that does not absorb substantial amounts of radiation may remain in an incompressible state during said step of directing at least one beam of radiation at the component. As a result or otherwise, it may provide mechanical support to the wall of the chamber through which an aperture is formed. Advantageously, the protection material thus reduces the movement of the wall of the chamber through which an aperture is formed during said ablation step. Such movement may result from shock waves, which, by causing the apparatus to move, can result in poor aperture quality.
Preferably, the protection material is solid immediately prior to said step of directing at least one beam of radiation at the component. More preferably still, the protection material is preferably provided as a liquid and subsequently solidifies. Protection material that does not absorb substantial amounts of radiation may remain in a solid state during said step of directing at least one beam of radiation at the component.
Alternatively, the protection material may be provided as a liquid. Preferably, this liquid may be caused to flow continuously through the chamber during the ablation step. Suitably, the chamber may be substantially enclosed at the point when said protection material is enclosed. Such a continuous flow may improve the removal of ablation debris from the chamber. In addition, it is preferred that, immediately upon a beam of radiation breaking through the wall of a chamber in which an aperture is being formed, the beam will contact the protection material thus preventing ablation debris from spreading through the chamber. This may also enhance the ability of the protection material to mechanically support the wall of the chamber through which an aperture is formed.
In order to achieve this, or otherwise, the method may further comprise, prior to said step of directing at least one beam of radiation at the component, evacuating substantially all gaseous material from and applying a fluid-tight seal to said fluid chambers.
Suitably, for each chamber for which a communicating aperture is formed, the aperture may extend through one wall of the chamber, and further said protection material may fill the chamber so as to abut said wall leaving substantially no space adjacent said wall. Again, this may stop debris from spreading within the chamber once a beam of radiation has broken through the wall in which an aperture is being formed, and may also enhance the mechanical support of that wall.
Optionally, the method may further comprise providing a plate bounding said fluid chambers so as to form at least a portion of said walls of the fluid chambers. Preferably, said apertures extend through said plate. The plate may comprise polymeric material, and indeed may consist entirely of polymeric material. Polymeric material may allow for accurate formation of said apertures. Suitably, a continuous flow of protection material may be provided subsequently to said plate.
Further the method may optionally further comprise the step, prior to providing said protection material, of passing a coating material into said chambers, at least some of said material being deposited as a coating layer, so as to form at least a portion of said walls of the fluid chambers. The coating layer may thus form a continuous layer providing the interior surfaces of the walls of the at least some of the chambers. Preferably, at least some of said coating layer remains during use of said component so as to protect said chambers from fluid contained therein. For this reason, or otherwise, the coating material may be a chemically inert substance, such as for example poly p-xylylene or poly chloro-p-xylylene.
Optionally, the method may further comprise, prior to said step of passing a protection material into said chambers, providing one or more piezoelectric members operable to cause release of fluid from said fluid chambers through said apertures during use. The piezoelectric members may be arranged as elongate walls dividing adjacent chambers within said array, the chambers also being elongate with their lengths extending in parallel.
According to a further aspect of the present invention there is provided a component for a droplet deposition apparatus comprising a plurality of chambers, each chamber being provided with actuation means, operable during use to cause a change in pressure in fluid within said chambers, said chambers being filled at least in part with a protection material comprising a waxy material, wherein said protection material acts to inhibit damage to the walls of said chamber during ablation of apertures communicating with said chambers.
According to a still further aspect of the present invention there is provided a component for a droplet deposition apparatus comprising a plurality of chambers, each chamber being provided with actuation means, operable during use to cause a change in pressure in fluid within said chambers, said chambers being filled at least in part with a protection material that undergoes a phase change between 50 and 150° C., and preferably between 60 and 130° C., wherein said protection material acts to inhibit damage to the walls of said chamber during ablation of apertures communicating with said chambers.
Preferably, such components further comprise a plate bounding said fluid chambers so as to form at least a portion of said walls of the fluid chambers. The plate may comprise polymeric material, and indeed may consist entirely of polymeric material. Polymeric material may allow for accurate formation of said apertures.
Embodiments of the invention will now be described with reference to the accompanying drawings, in which:
Referring now to
Prior to the laser ablation, a block of piezoelectric material is fixed to an alumina substrate (14). The actuator member (9) is then formed from the block of piezoelectric material by sawing a plurality of closely-spaced elongate channels in its top surface. The lengths of these channels extend in parallel from one edge of the block of piezoelectric material to the opposite edge, so that each channel has two opposing open ends. As will be described below, the open roofs of these channels are later closed so as to provide an array of fluid chambers (10) disposed side-by-side in an array.
Support members (17) are then fixed either side of the piezoelectric actuator member (9), thus completing the construction shown in
The construction of
The construction of
A protection material (8) is then introduced into the fluid chambers (10). The protection material (8) may be a waxy material and, in a particular embodiment is 2,6-Diisopropyl naphthalene. Such waxy protection materials may be softened by heating and applied from the top surface of the construction into the fluid chambers (10), as shown in
The protection material (8) is allowed to harden and the entire construction—including the protection material—is planarised, for example by milling from the top surface, so that the top surface is made substantially flat and some or all of the coating layer (15) is removed from the top surface. Preferably, only a small amount of material is removed from the piezoelectric actuator member (9), because of its high cost. A nozzle plate (13), which may comprise polymeric material for improved nozzle formation, is then fixed to the thus-flattened top surface, as shown in
As the top surface of the construction is substantially flat before the nozzle plate (13) is attached, the protection material (8) contacts the bottom surface of the nozzle plate leaving very little space between.
Subsequently, a beam (30) produced by a high-powered laser is directed towards the top surface of the nozzle plate (13) so as to form an aperture (16) communicating with a corresponding chamber (10). The beam (30) ablates material from the nozzle plate (13), forming a bore; in the process, debris (31) is discharged upwards in a plume, as shown in
The laser beam (30) heats protection material (8) in the vicinity of the point of contact; the protection material (8) thus absorbs the energy from the high-powered laser beam (30) and further assists in preventing damage occurring to the interior surfaces of the fluid chambers (10).
More specifically, in embodiments where the protection material (8) is a waxy material, a portion of this waxy material in the vicinity of the point of contact is caused to melt or sublime. The energy from the radiation is thus absorbed and used to provide the latent heat required for causing a phase change in the protection material (8). Thus, the waxy material is able reduce the amount of absorbed energy that is converted to thermal energy and as a result the temperature within the chamber (10) is moderated.
Having broken through the nozzle plate (13), the laser (30) is deactivated and re-directed at a point on the nozzle plate (13) above a different chamber (10). The ablation process is then repeated until the desired number of apertures (16) are formed communicating with respective chambers (10). Following completion of the ablation process, the protection material (8) is removed from the apparatus, for example, by passing a flushing fluid through the apparatus the from inlet port (18) to the outlet port (19), and/or by use of the apparatus to deposit the protection material (8) in the form of droplets. Further, in embodiments where the protection material (8) is a waxy material, the protection material (8) may be removed by removing the plugs occluding the inlet (18) and outlet (19) ports, gently heating the apparatus so as to melt the waxy material , and then allowing it to drain from the ports (18, 19), as shown in
Similarly to the introduction of the protection material, the flushing liquid (hot or otherwise) may be introduced into the head from either inlet or outlet, and may leave the head through either outlet or inlet and/or the nozzles. The basic requirements of the flushing liquid may include: compatibility with the apparatus or printhead (does not attack/damage the head); and solubility of the protection material in the flushing fluid, or miscibility with the protection material substance above the melting point of the protection material (miscible enough so that agglomerates of protection material are not formed to block the channels or chambers).
The function of the flushing fluid may be to physically displace the protection material (by application of pressure) or as a medium to transport volumes of the protection material from the chamber or to act as a solvent to dissolve and subsequently remove the protection material. The solubility may be sufficient that any material left in the head after flushing will remain in solution at subsequent processing temperatures, and may be removed later in a further flushing procedure, which may utilise the droplet fluid intended for use with the apparatus.
a) shows a further embodiment of the present invention, where a construction is provided initially that is similar to that described with reference to
In more detail, as shown in
As also shown in
Subsequently, as shown in
Following the filling of the apparatus with the protection material (8), apertures (16) may be ablated in the nozzle plate (13) by applying the beam of a high-powered laser (30) at the top surface of the nozzle plate (13), as shown in
Once the ablation of apertures (16) is completed, the inlet (18) and outlet (19) ports may be unblocked and the protection material (8) removed in a similar manner to that described with reference to
In an optional modification of the embodiment of
Constructions, such as those depicted in
In the construction of
A cover member (20) is then attached to the top surface of the block of piezoelectric material (9) (attachment shown by large arrow in
Further, a blank nozzle plate (13) (one in which no apertures have yet been formed) is attached to close the open ends of the channels (10a).
Subsequently, as shown in
Next, as shown in
Following the ablation of apertures (16), the construction is inverted and to cause the protection material (8) to drain out via the port in the cover member (21), as illustrated in
Subsequently, as shown in
The entire top surface of the construction, including the protection material (8), is then milled, so as to provide a flat top surface, to which a cover plate (20) such as that shown in
It should be noted that a block of piezoelectric material having channels that extend from one edge to a point only part way across the block—such as that shown in FIG. 6—may be formed in a variety of ways.
a) shows a view from above a generally planar block of piezoelectric material (9), and illustrates a dicing pattern (51, 52) that may be carried out by a diamond impregnated saw. A plurality of parallel cuts (52) is made in the top surface of the block of piezoelectric material (9). As is visible in
As also shown in
The thus-formed blocks of piezoelectric material may then be filled with protection material as shown in
Alternatively, however, the protection material (8) may be introduced into the channels prior to the carrying out of the separating cut (51). In more detail,
The construction may then be planarised as shown in
As shown in
The protection material (8) is preferably caused to solidify or substantially increase in viscosity before the separating cut (51) is made, so that the protection material (8) may be retained within the channels (10) in the divided blocks of piezoelectric material (9a, 9b). Where a waxy material is used as a protection material (8) it may suitably be allowed to harden.
While not shown, a coating material may optionally be utilised in conjunction with the embodiments of
It should be noted that “end-shooter” constructions have been proposed where a flow may be set up from one manifold to another along the lengths of the chambers in the array. This may be accomplished by an array of small supply channels (23) extending perpendicularly to the lengths of the fluid chambers (10).
In the example shown in FIG. 10—which is substantially similar to the construction shown in
In such a construction, it will be appreciated that protection material (8) may be flowed along a similar path to fill the chambers (10) before ablation. Thus, a similar method to that described with reference to
More generally, where the constructions above are provided with both an inlet (18) and an outlet port (19), or as in the embodiment of
In this way, the protection material may be introduced and/or removed via the same path which is used for ink or deposition fluid during use of the apparatus. However, the use of ink or deposition fluid paths may be indicated whether a continuous flow of protection fluid is provided or not. Nonetheless, it will be appreciated that where ink or deposition fluid supply systems allow for a continuous flow of ink or deposition fluid such a continuous flow of protection material may be particularly straightforward to achieve.
Further, with such a continuous flow of protection material (or indeed otherwise), it may be preferable to maintain a negative static pressure in the protection material within the fluid chambers of the apparatus during the ablation process. Negative pressure (lower than the pressure of the atmosphere exterior the apparatus) may ensure that the protection material remains contained within the chamber when the ablation beam breaks through into the chamber. It is noted that control of ink or droplet fluid at negative static pressures may be afforded with existing fluid supply systems, so that such systems may be adapted to provide a similar effect for the protection material.
Whilst certain of the above examples have made use of a waxy material as a protection material, this is of course not essential to the operation of the invention. The protection material may indeed be a liquid, gel, amorphous solid, glass, crystalline solid, or indeed in any other appropriate state.
For arrangements where it is desired to have a continuous flow of protection material through the apparatus during the ablation process it may be preferable to utilise a protection material that is a liquid or a gel. It may also be preferred that such protection material remains in this state during ablation and does not undergo a phase change.
Such a process may be beneficial as it can be carried out at low-temperatures and/or without a flushing step to remove the protection material. As noted above, a liquid or gel protection material might make use of existing droplet fluid supply systems, although it is noted that hot-melt fluid supply systems might equally be used for introducing waxy protection materials.
As noted above, it may, in some applications, be preferable for the protection material to exhibit a phase change in response to the application of radiation. This phase change may draw energy away from the more sensitive components within the chamber.
In addition, or alternatively, the protection material may undergo a phase change from a solid or highly viscous state to a liquid or low-viscosity state at a temperature moderately in excess of room temperature. This allows the protection material to be introduced and removed easily in its low-viscosity or liquid state by gentle heating of the apparatus, or by flushing with suitably heated fluid. In this way, the temperature increase required to cause the phase change is unlikely to damage any of the sensitive components of the apparatus.
Appropriate protection materials may comprise waxy materials, such as 2,6-Diisopropyl naphthalene, for at least the reason that they exhibit such a transition from a very high viscosity state at room temperature, to a low viscosity state at temperatures moderately in excess of room temperature. As will be discussed below, protection materials may of course comprise other waxy materials, such as paraffin wax.
In particular, it may be desirable that the phase change occurs between 50 and 150° C., or more preferably between 60 and 130° C. The exemplary protection material mentioned above 2,6-Diisopropyl naphthalene—exhibits a sharp decrease in viscosity at around 70° C.
It will be appreciated by those skilled in the art that other means for achieving a phase change may also be utilised. For example, fluids with complex rheology may be utilised which under high shear conditions become significantly less viscous. Equally, particulate matter may be introduced and removed by application of high-frequency mechanical vibration.
Additionally, it may be preferable for a protection material to be chosen in accordance with the wavelength or wavelengths of radiation utilised in the ablation process. Accordingly, the protection material may exhibit a higher absorbance at such wavelengths than elsewhere in its absorption spectrum. More specifically, it is envisaged that the attenuation provided by the protection material is at least 10 times greater than air, more preferably 100 times greater than air, and still more preferably 1000 times greater than air. Alternatively, or in addition, the protection material may have a peak in its absorption spectrum within +50 nm of the wavelength of the radiation, and preferably within +25 nm. This peak in the absorption spectrum may be a major peak.
Further, while certain materials, such as 2,6-Diisopropyl naphthalene, may exhibit desirable radiation absorbing properties and also desirable phase-change properties, it is possible to combine materials with desirable radiation absorbing properties specific to the wavelength of wavelengths of radiation utilised, and to combine such a radiation absorber with a further component to provide a protection material which exhibits the desired solidity or viscosity.
An example of such a combination would be a mixture comprising carbon black and paraffin wax: the carbon black acts as an effective radiation absorber, while the paraffin wax acts as a carrier and ensures that the mixture is highly viscous at room temperature but of suitably low viscosity with a moderate temperature increase that it may be easily introduced or removed. Equally, where a liquid radiation absorber is suitable for the particular wavelength or wavelengths, such a radiation absorber may be mixed with a solid gellant to form a protection material in a gel phase. By appropriate variations in the ratios of components within the mixture, the phase change may be set to occur at a desired temperature.
Further suitable materials will be apparent to the skilled person. For example, where it is desired to provide a liquid protection material, rather than using a mixture of a carrier and a radiation absorber, a liquid radiation absorber may be used on its own, a specific example being di-isopropyl naphthalene (mixed isomers).
More generally, the Applicant envisages that the following chemicals may serve as appropriate radiation absorbers for a range of different wavelengths:
Further, the Applicant envisages that the following chemicals may serve as appropriate carriers for radiation absorbers:
Still further, the Applicant envisages that the following chemicals may serve as appropriate gellants for radiation absorbers:
It should be appreciated that the use of protection material is of course not limited to the particular constructions shown in, and described with reference to, the figures. The skilled person will appreciate that methods according the present invention may be utilised with constructions where the array of chambers is neither linear, nor evenly spaced. Further, such methods may be applied to two-dimensional arrays of chambers, just as with the linear arrays described above.
It should further be appreciated that the while the above embodiments concern devices having piezoelectric actuating elements, that these are simply examples of an electrically actuable means that is operable to cause controlled release of droplets from fluid chambers. As noted above, such electrically actuable means may equally comprise resistive elements operable to heat the fluid within chambers.
Still further, the skilled reader will appreciate that while the examples above may have referred to individual apertures being formed consecutively, the teaching may equally be applied to parallel processes where a plurality of apertures are formed simultaneously. In an example of such a procedure, a single beam source may suitably be split into a plurality of sub-beams, each being focussed with respect to a different aperture (though, equally, a plurality of separate sources might be used).
Number | Date | Country | Kind |
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1013123.3 | Aug 2010 | GB | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/GB2011/051481 | 8/4/2011 | WO | 00 | 2/15/2013 |