Abstract:
A droplet emitter with an array of droplet emitting devices constructed such that one flowing liquid is used to create the droplets while a second low acoustic impedance liquid can be used to both make the transfer of acoustic energy to the first liquid more efficient and help maintain a uniform temperature of the droplet emitter array. Both liquids can be circulated through the droplet emitter to allow for excess heat generated by control electronics to be transferred to the flowing liquids. This prevents, for instance excess heat build-up within the droplet emitter and allows for higher more accurate droplet emission rates.

Description:
INCORPORATION BY REFERENCE 
     The following U.S. Patents are fully incorporated by reference: 
     U.S. Pat. No. 5,786,722 by Buhler et al. titled &#34;Integrated RF Switching Cell Built In CMOS Technology And Utilizing A High Voltage Integrated Circuit Diode With A Charge Injecting Node&#34; issued Jul. 28, 1998. 
     U.S. Pat. No. 5,565,113 by Hadimioglu et al. titled &#34;Lithographically Defined Ejection Units&#34; issued Oct. 15, 1996. 
     U.S. Pat. No. 5,389,956 by Hadimioglu et al. titled &#34;Techniques For Improving Droplet Uniformity In Acoustic Ink Printing&#34; issued Feb. 14, 1995. 
    
    
     BACKGROUND 
     This invention relates generally to droplet emitters and more particularly concerns an acoustically actuated droplet emitter which is provided with a continuous, high velocity, laminar flow of cooling liquid in addition to a continuous flow of liquid to be emitted as droplets. 
     Acoustic droplet emitters are known in the art and use focussed acoustic energy to emit droplets of fluid. Acoustic droplet emitters are useful in a variety of applications due to the wide range of fluids that can be emitted as droplets. For instance, if marking fluids are used the acoustic droplet emitter can be employed as a printhead in a printer. Acoustic droplet emitters do not use nozzles, which are prone to clogging, to control droplet size and volume, and many other fluids may also be used in an acoustic droplet emitter making it useful for a variety of applications. For instance, it is stated in U.S. Pat. No. 5,565,113 issued Oct. 15, 1996 by Hadimioglu et al. titled &#34;Lithographically Defined Ejection Units&#34; and incorporated by reference hereinabove, that mylar catalysts, molten solder, hot melt waxes, color filter materials, resists and chemical and biological compounds are all feasible materials to be used in an acoustic droplet emitter. 
     One issue when using high viscosity fluids in an acoustic droplet emitter is the high attenuation of acoustic energy in high viscosity fluids. High attenuation rates require larger amounts of acoustic power to achieve droplet emission from such liquids. One solution to this problem has been shown in U.S. Pat. No. 5,565,113 issued Oct. 15, 1996 by Hadimioglu et al. titled &#34;Lithographically Defined Ejection Units&#34; and incorporated by reference hereinabove and is shown in FIG. 1. 
     FIG. 1 shows a cross-sectional view of a droplet emitter 10 for an acoustically actuated printer such as is shown in U.S. Pat. No. 5,565,113 by Hadimioglu et al. titled &#34;Lithographically Defined Ejection Units&#34; and incorporated by reference hereinabove. The droplet emitter 10 has a base substrate 12 with a transducer 16 interposed between two electrodes 17 on one surface and an acoustic lens 14 on an opposite surface. Attached to the same side of the base substrate 12 as the acoustic lens is a top support 18 with a liquid cell 22, defined by sidewalls 20, which holds a low attenuation liquid 23. Supported by the top support 18 is an acoustically thin capping structure 26 which forms the top surface of the liquid cell 22 and seals in the low attenuation liquid 23. 
     The droplet emitter 10 further includes a reservoir 24, located over the acoustically thin capping structure 26, which holds emission fluid 32. As shown in FIG. 1, the reservoir 24 includes an aperture 30 defined by sidewalls 34. The sidewalls 34 include a plurality of portholes 36 through which the emission fluid 32 passes. A pressure means forces the emission fluid 32 through the portholes 36 so as to create a pool of emission fluid 32 having a free surface 28 over the acoustically thin capping structure 26. 
     The transducer 16, acoustic lens 14, and aperture 30 are all axially aligned such that an acoustic wave produced by the transducer 16 will be focussed by its aligned acoustic lens 14 at approximately the free surface 28 of the emission fluid 32 in its aligned aperture 30. When sufficient power is obtained, a mound 38 is formed and a droplet 39 is emitted from the mound 38. The acoustic energy readily passes through the acoustically thin capping structure 26 and the low attenuation liquid 23. By maintaining only a very thin pool of emission fluid 32 acoustic energy loss due to the high attenuation rate of the emission fluid 32 is minimized. 
     FIG. 2 shows a perspective view of two arrays of the droplet emitter 10 shown in FIG. 1. The arrays 31 of apertures 30 can be clearly above the two reservoirs 24. Each array 31 has a width W and a length L where the length L of the array 24 is the larger of the two dimensions. Having arrays of droplet emitters 10 is useful, for instance, to enable a color printing application where each array might be associated with a different colored ink. This configuration of the arrays allows for accurate location of each individual droplet emitter 10 and precise alignment of the arrays 31 relative to each other which increases, among other things doplet placement accuracy. 
     However, the low attenuation liquid 23, the emission fluid 32 and the substrate 12 will heat up from the portion of the acoustic energy that is absorbed in the low attenuation liquid 23, the emission fluid 32 and the substrate 12 which is not transferred to the kinetic and surface energy of the emitted drops 39. This will in turn cause excess heating of the emission fluid 32. The emission fluid 32 can sustain temperature increases by only a few degrees centigrade before emitted droplets show drop misplacement on the receiving media. In a worst case scenario, the low attenuation liquid 23 can absorb enough energy to cause it to boil and to destroy the droplet emitter 10. The practical consequences of this are that the emission speed must be kept very slow to prevent the low attenuation liquid 23 from absorbing too much excess energy in a short time period and heating up to unacceptable levels. 
     Therefore, it would be highly desirable if a droplet emitter 10 could be designed to operate while maintaining a uniform thermal operating temperature at high emission speeds. 
     Further advantages of the invention will become apparent as the following description proceeds. 
     SUMMARY OF THE INVENTION 
     Briefly stated and in accordance with the present invention, there is provided a droplet emitter which has a first substrate which has been constructed to provide an array of focussed acoustic waves. The array of focussed acoustic waves has a length and a width wherein the length is greater than the width. The droplet emitter also has a second substrate which is spaced from the first substrate. The second substrate has an acoustically thin portion and an array of apertures which are so arranged such that each aperture may pass substantially unimpeded focussed acoustic waves. The droplet emitter also has a third substrate which is spaced from the second substrate. The third substrate has an array of apertures which are so arranged such that each aperture may receive focussed acoustic waves after they have passed through the array of apertures in the second substrate. Further, there are two liquid chambers, the first at least partially interposed between the first and second substrates and the second at least partially interposed between the second and third substrates. The second liquid flow chamber has an inlet and an outlet and is constructed and arranged to receive a laminar flow of a liquid where a free surface of the liquid is formed by each of the apertures in the third substrate. The focussed acoustic waves received by each aperture are focussed substantially at the free surface of the liquid formed in the aperture. The laminar flow of liquid flows in through the inlet, out through the outlet and at least a portion of the laminar flow of liquid flows in substantially in the same direction as the length of the array of focussed acoustic waves. A fluid can then be flowed through the second fluid chamber to remove excess heat from the droplet emitter. 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS 
     FIG. 1 shows a cross-sectional view of a prior art droplet emitter for an acoustically actuated printer. 
     FIG. 2 shows a perspective view of arrays of prior art droplet emitters shown in FIG. 1. 
     FIG. 3 show a cross-sectional view of a droplet emitter according to the present invention. 
     FIG. 4 shows a perspective view of the droplet emitter shown in FIG. 3. 
     FIG. 5 shows a cross-sectional view of the droplet emitter shown in FIG. 3 with an emission fluid manifold attached. 
     FIG. 6 shows a ross-sectional view of the droplet emitter shown in FIG. 3 with a low attenuation fluid manifold attached. 
     FIG. 7 shows a perspective view of the droplet emitter shown in FIG. 4 with the addition of liquid level control plate supports. 
     FIG. 8 shows a perspective view of cross-sectional view of the droplet emitter shown in FIG. 5 with additional thermally conductive components. 
     FIG. 9 shows an exploded view of the parts used to assemble an upper manifold. 
     FIG. 10 shows an exploded view of the parts used to assemble a droplet emitter with a lower manifold and flex circuitry. 
    
    
     While the present invention will be described in connection with a preferred embodiment and method of use, it will be understood that it is not intended to limit the invention to that embodiment or procedure. On the contrary, it is intended to cover all alternatives, modifications and equivalents as may be included within the spirit and scope of the invention as defined by the appended claims. 
     Alpha-Numeric List of Elements 
     d 1  capping structure support aperture diameter 
     d 2  liquid level control aperture diameter 
     h height of emission fluid 
     Hf flow direction of heat 
     Lf flow direction of liquid 
     L length of an array 
     W width of an array 
     F 1  flow direction of emission fluid 
     F 2  flow direction of low attenuation fluid 
     10 droplet emitter 
     12 base substrate 
     14 acoustic lens 
     16 transducer 
     17 electrode 
     18 top support 
     20 sidewall 
     22 liquid cell 
     23 low attenuation liquid 
     24 reservoir 
     26 acoustically thin capping structure 
     28 free surface 
     30 aperture 
     31 array 
     32 emission fluid 
     34 sidewall 
     36 portholes 
     38 mound 
     39 droplet 
     40 droplet emitter 
     42 base substrate 
     44 acoustic lens 
     46 transducer 
     48 emission fluid 
     49 aperture 
     50 acoustically thin capping structure 
     51 capping structure support 
     52 flowing low attenuation liquid 
     54 array 
     56 liquid level control plate 
     58 free surface 
     60 aperture 
     62 fluid manifold 
     64 sheet flow partition 
     66 manifold inlet liquid tube 
     68 manifold outlet liquid tube 
     70 heat sink 
     72 heat conductive back plane 
     74 thermally conductive connection 
     76 circuit component 
     78 spring clip 
     80 circuit chip 
     82 bridge plate 
     84 flexible seal 
     86 manifold inlet 
     88 manifold outlet 
     90 liquid sheet flow chamber 
     92 lower manifold 
     94 LLC gap protrusion 
     96 bond wire 
     98 upper manifold 
     100 flex 
     102 baffle 
     120 manifold inlet 
     122 manifold outlet 
     128 liquid flow chamber 
     DETAILED DESCRIPTION OF THE INVENTION 
     Turning now to FIG. 3, there is shown a cross-sectional view of a droplet emitter 40 configured according to the present invention. The droplet emitter 40 has a base substrate 42 with transducers 46 on one surface and acoustic lenses 44 on an opposite surface. Spaced from the base substrate 42 is an acoustically thin capping structure 50. The acoustically thin capping structure 50 may be either a rigid structure made from, for example, silicon, or a membrane structure made from, for example, parylene, mylar, or kapton. In order to preserve the acoustic transmission properties the acoustically thin capping structure 50 should preferably have either a very thin thickness such as approximately one-tenth of the wavelength of the transmitted acoustic energy in the membrane material or a thickness substantially equal to a multiple of one-half the wavelength of the transmitted acoustic energy in the membrane material. Whether the acoustically thin capping structure 50 is made from a rigid material or a membrane it will structurally be relatively thin and have a tendency to be fragile and susceptible to breakage. To provide additional stability for the acoustically thin capping structure 50 it is supported by a capping structure support 51. The capping structure support 51 is interposed between the base substrate 42 and the acoustically thin capping structure 50, adjacent to the acoustically thin capping structure 50 and spaced from the base substrate 42. The capping structure support 51 has a series of spaced apart apertures 49 positioned in a like manner to lens array 44 so that focussed acoustic energy may pass by the capping structure support 51 substantially unimpeded. The apertures 49 have a capping structure support aperture diameter d 1 . The addition of the capping structure support 51 allows for a wider variety of materials to be used as the acoustically thin capping structure 50 and adds strength and stability to the acoustically thin capping structure 50. 
     The chamber created by the space between the base substrate 42 and the acoustically thin capping structure 50 is filled with a low attenuation fluid 52. The chamber could be filled with the low attenuation fluid 52 and sealed as described hereinabove with respect to FIG. 1, however, benefits can be achieved if the chamber is not sealed and the low attenuation fluid 52 is allowed to flow through the chamber. FIG. 3 shows a flow direction of the low attenuation fluid F 2  which is orthogonal to the plane of the drawing and out of the plane of the drawing. However, while a droplet emitter 40 which has a flow direction of the low attenuation fluid F 2  in this direction may possibly be the easiest to construct, other flow directions are possible and may even in some circumstances be preferable. For instance, the droplet emitter 40 could also be constructed such that the flow direction of the low attenuation fluid F 2  was flowing in the plane of the drawing in either a &#34;right&#34; or &#34;left&#34; direction. 
     Flowing the low attenuation liquid 52 enables the low attenuation liquid 52 to help maintain thermal uniformity of the droplet emitter 40. In particular, not only does the low attenuation liquid 52 itself have less opportunity to heat up due to excess heat generated during the acoustic emission process but because the low attenuation liquid 52 is in thermal contact with the substrate 42 the low attenuation liquid 52 may also absorb excess heat generated in the substrate 42 during operation and prevent excess heating of the substrate 42 as well. Further, it can be appreciated that this structure of a thin capping structure over a relatively rigid capping support creates a fluidically sealed flow chamber enabling relatively high flow rates of the low attenuation fluid without changing the position of the capping structure with respect to the focussed acoustic beam. Consequently, rapid removal of excess generated heat and temperature uniformity is achieved. 
     Spaced from the acoustically thin capping structure 50 is a liquid level control plate 56. The acoustically thin capping structure 50 and the liquid level control plate 56 define a channel which holds an emission fluid 48. The liquid level control plate 56 contains an array 54 of apertures 60. The transducers 46, acoustic lenses 44, apertures 49 and apertures 60 are all axially aligned such that an acoustic wave produced by a single transducer 46 will be focussed by its aligned acoustic lens 44 at approximately a free surface 58 of the emission fluid 48 in its aligned aperture 60. When sufficient power is obtained, a droplet is emitted. It should be noted that the apertures 60 in the liquid level control plate 56 have a liquid level control plate aperture diameter d 2 . In order to insure that the acoustic wave produced by a transducer will propagate substantially unimpeded through the aperture 49 in the capping structure support the capping structure support aperture diameter d 1  should be larger than the diameter of the acoustic beam as it passes through the aperture 49. 
     FIG. 4 shows a perspective view of the droplet emitter 40 shown in FIG. 3. The array 54 of apertures 60 can be clearly seen on the liquid level control plate 56. The flow direction of the low attenuation fluid F 2  between the base substrate 42 and the acoustically thin capping structure 50 can be clearly seen as well as the flow direction of the emission fluid F 1  between the acoustically thin capping structure 50 and the liquid level control plate 56. In FIG. 4 a length L and a width W of the array 54 can also be seen and the width W is the smaller dimension. The flow direction of the emission fluid F 1  is arranged such that the emission fluid 48 flows along the shorter width W of the array 54 instead of along the longer length L of the array 54 as in. When the flow direction of the emission fluid F 1  is arranged to be orthogonal to the flow direction of the low attenuation fluid F 2 , then it is preferable to arrange the flow direction of the emission fluid F 1  such that the emission fluid 48 flows along the shorter width W of the array 54 instead of along the longer length L because the emission fluid is more sensitive to constraining factors. For instance, small pressure deviations in the emission fluid 48 along the array 54 can lead to misdirectionality of the emitted droplets. However, in this configuration, the flow velocity of the emission fluid 48 is substantially independent of many of the constraining factors. 
     If however, the droplet emitter 40 is constructed such that the flow direction of the emission fluid F 1  and the flow direction of the low attenuation fluid F 2  are substantially parallel instead of orthogonal to each other, then it is preferable that both the flow direction of the emission fluid F 1  and the flow direction of the low attenuation fluid F 2  be along the width of the array for the reasons stated above. 
     FIG. 5 shows a cross-sectional view of how the droplet emitter of FIGS. 3 and 4 can be assembled with a fluid manifold 62 to provide the emission fluid 48 to the droplet emitter. While unitary construction of the fluid manifold 62 may in some circumstances be desirable, in this implementation the fluid manifold 62 is divided into two portions, an upper manifold 98 and a lower manifold 92 with a flexible seal 84 therebetween. 
     The lower manifold 92, which is in direct contact with the base substrate 42 and the liquid level control plate 56 must be made from materials which have a thermal expansion coefficient relatively similar to the material the base substrate 42 is made from and preferably within a range of +/-0.5×10 -6  per degree centigrade. This is primarily because the base substrate 42 during the course of alignment to the lower manifold and the liquid level control plate 56 and subsequent bonding and curing steps may go through large temperature variations of up to 250 degrees centigrade and a differential thermal expansion of the parts of more than 5 microns can damage the assembly. The most common material for constructing the base substrate 42 is glass which has a thermal expansion coefficient of approximately 3.9×10 -6  per degree centigrade. 
     Possible materials for constructing the lower manifold 92, when the substrate 42 is made from glass, include alloy 42, Kovar, various ceramics and glass, which all have acceptable thermal expansion. However, as the length of the droplet emitter 40 increases, and hence the length of the base substrate 42 and the liquid level control plate 56, either the allowable variation in thermal expansion coefficients, or the maximum temperature variation, or both must be correspondingly decreased. 
     The lower manifold 92 has a liquid level control gap protrusion 94. The liquid level control plate 56 is attached to a liquid level control gap protrusion 94. The liquid level control gap protrusion 94 is used to achieve a precise spacing between the base substrate 42 and the liquid level control plate 56 when the parts are assembled into the droplet emitter 40 and attached to the lower manifold 92. 
     The assembly of the droplet emitter 40 and attachment to the fluid manifold 62 creates a liquid sheet flow chamber 90 starting at the manifold inlet 86, proceeding through the gap between the acoustically thin capping structure 50 and the liquid level control plate 56 and ending at the manifold outlet 88. Both the manifold inlet 86 and the manifold outlet 88 have a sheet flow partition 64 which creates and maintains a sheet flow of the liquid flowing through the liquid sheet flow chamber 90. 
     An additional part assembled with the lower manifold 92 and the droplet emitter stack 40 is a bridge plate 82 as shown in FIG. 5. The bridge plate 82 is used to mount a flex cable 100. The flex cable 100 is used to provide connections for discrete circuit components 76 which are mounted on the flex cable 100 and are used to generate and control the focussed acoustic wave. Bond wires 96 provide electrical connections between the flex cable 100 and circuit chips 80 mounted on the base substrate 42. Control circuitry for the droplet emitter has described for instance in U.S. Pat. No. 5,786,722 by Buhler et al. titled &#34;Integrated RF Switching Cell Built In CMOS Technology And Utilizing A High Voltage Integrated Circuit Diode With A Charge Injecting Node&#34; issued Jul. 28, 1998 or U.S. Pat. No. 5,389,956 by Hadimioglu et al. titled &#34;Techniques For Improving Droplet Uniformity In Acoustic Ink Printing&#34; issued Feb. 14, 1995 both incorporated by reference hereinabove. 
     FIG. 6 shows a cross-sectional view of how the droplet emitter of FIGS. 3 and 4 can be assembled with a fluid manifold 62 to provide the low attenuation fluid 52 to the droplet emitter. While unitary construction of the fluid manifold 62 may in some circumstances be desirable, in this implementation the fluid manifold 62 is divided again into two portions as described hereinabove, an upper manifold 98 and a lower manifold 92 with a flexible seal 84 therebetween. 
     The lower manifold 92, which is in direct contact with the base substrate 42 and the capping support plate 51 must be made from materials which have a thermal expansion coefficient relatively similar to the material the base substrate 42 is made from and preferably within a range of +/-0.5×10 -6  per degree centigrade. This is primarily because the base substrate 42 during the course of alignment to the lower manifold and the capping support plate 51 and subsequent bonding and curing steps may go through large temperature variations of up to 250 degrees centigrade and a differential thermal expansion of the parts of more than 5 microns can damage the assembly. The most common material for constructing the base substrate 42 is glass which has a thermal expansion coefficient of approximately 3.9×10 -6  per degree centigrade. 
     Possible materials for constructing the lower manifold 92, when the substrate 42 is made from glass, include alloy 42, Kovar, various ceramics and glass, which all have acceptable thermal expansion. However, as the length of the droplet emitter 40 increases, and hence the length of the base substrate 42 and the capping support plate 51, either the allowable variation in thermal expansion coefficients, or the maximum temperature variation, or both must be correspondingly decreased. 
     The capping support plate 51 is positioned below the substrate 42 and sealed around the substrate in a manner such as to achieve a precise spacing between the base substrate 42 and the acoustically thin capping structure 50 when the parts are assembled into the droplet emitter 40 and attached to the lower manifold 92. 
     The assembly of the droplet emitter 40 and attachment to the fluid manifold 62 creates a liquid flow chamber 128 starting at the manifold inlet 120, proceeding through the gap between the base substrate 42 and the acoustically thin capping structure 50 and ending at the manifold outlet 122. 
     It should be noted that in the embodiments shown in FIGS. 3, 4, and 5, the liquid sheet flow chamber 90 has no physical or structural obstructions in the path of the flow, particularly in the portion of the sheet flow chamber 90 between the base substrate 42 and the acoustically thin capping structure 50. This is the preferred embodiment as it ensures a uniform flow velocity for all the emitters across the entire length of the array. Furthermore, this decreases the possibility of trapped air-bubbles created during filling of the printhead or by perturbations in the emission fluid 48 flow and allows for the rapid removal of air bubbles that may get introduced into the system. However, it should be noted that as the length L of the droplet emitter gets larger, it may be desirable to provide additional support to the liquid level control plate 56. Such liquid level control plate supports 130 may be placed within the liquid flow chamber 90 provided they have a minimal footprint and are placed a minimal distance of at least five times the channel height h from both the ends of the liquid flow channel 90 and each other as shown in FIG. 7. Note that the liquid level control plate supports are placed in the flow direction, effectively creating several large flow chambers 132 within a portion of the liquid sheet flow chamber 90. 
     FIG. 8 shows a perspective view of the cross section of the droplet emitter shown in FIG. 5 with additional thermally conductive components. Specifically, a heat conductive backplane is inserted in the gap between the flex cable 100 and the low fluid manifold 62. Additionally, a thermally conductive connection 74 is made between the heat conductive back plane 72 and the upper manifold 98. The thermal conduction between the heat conductive backplane 72 and the fluid manifold 62 allows heat generated by the circuit chips 80 to be transferred to the low attenuation fluid 52 and the emission fluid 32 via the fluid manifold 62. This allows excess heat to be carried away from the droplet emitter 40 and helps to maintain thermal uniformity within the droplet emitter 40. 
     Additionally, manifold inlet fluid tube 134 and manifold outlet fluid tube 136 are also shown attached to the fluid manifold 62. 
     Another feature shown in FIG. 8 is spring clip 78. The spring clip 78 is used to secure the entire assembly but allows for some movement of upper manifold 98 relative to the lower manifold 92 due to the different thermal expansion coefficients of the upper manifold 98 and the lower manifold 92. However, other fastening methods that would accomplish the same function are also known. For instance, the upper manifold 98 could be attached to the lower manifold 92 with an elastomer glue joint. An elastomer glue joint would fixedly attach the upper manifold 98 to the lower manifold 92 while also allowing for some movement of the upper manifold 98 relative to the lower manifold 92 due to the different thermal expansion coefficients. However, when spring clips 78 are used, their number and position should such that the flexible seal is leak free and the seal compression is uniformly distributed along the length L of the array 54 of the droplet emitter 40 in order to minimize resultant gap nonuniformities between the base substrate 42 and the liquid level control plate 56. In order to accomplish this, it should be noted that the two flexible seals 84, in the embodiment shown in FIG. 5 are two elongated o-rings. The compliance or stiffness of this type of o-ring seal is fairly uniform along the length of the o-ring except for the ends of the o-ring. This type of o-ring is much stiffer at the ends than along the rest of the length of the o-ring. Therefore, in order to insure that the seal is under substantially uniform compression, more force is needed at the ends of the o-ring than along the rest of the length of the o-ring. One method of accomplishing this is to do as shown in FIG. 9, and place the spring clips 78 over the stiffer ends of the o-rings. However, this is not the only method available, for instance, a full lengthwise spring clip with applies more clamping force above the ends of the o-ring than along the rest of the length of the o-ring could be used. Also, a series of small spring clips applying a small force could be placed along the length of the o-ring while using larger spring clips which apply a greater force at the ends of the o-ring. 
     FIG. 9 shows an exploded view of the upper manifold 98 while FIG. 10 shows an exploded view of the lower manifold 92. Again, while many manufacturing techniques are known, one method to make the upper manifold 98 is to divide the upper manifold 98 into easily manufacturable components which can then be assembled into the upper manifold 98. The upper manifold 98 is divided into an upper portion 98a and a lower portion 98b which are then assembled with a pair of baffles 102 which is inserted therebetween. The baffles 102 are used aide in the conversion of the liquid flow of the emission fluid 48 into the upper manifold 98 in a sheet flow. The manifold inlet tubes66, 68, and outlet tubes 134, 136 can then be inserted into the upper portion 98a to complete assembly of the upper manifold 98. 
     The lower manifold 92 can be assembled from a stack of parts in a similar manner along with the flex cable 72, base substrate 42, and the liquid level control plate 56. The lower manifold 92 is manufactured in four sheet-like portions 92a, 92b, 92c, and 92d. This allows for easy manufacture of the lower manifold 92 because each portion can be easily and accurately stamped, chemically etched or laser cut out of a sheet material such as readily available sheet metal stock. The liquid sheet flow chambers 90, 128 are defined by the patterns removed out of each portion 92a, 92b, 92c, 92d when the portions are stacked and assembled together with the base substrate 42, the capping structure support 51 and the liquid level control plate 56.