Published In: Proc. SPIE 9116, Next-Generation Robots and Systems
Date: 4 June, 2014
Human-robot interaction can be made more sophisticated and intuitive if the entire body of a robot is covered with multimodal sensors embedded in artificial skin. In order to efficiently interact with humans in unstructured environments, robotic skin may require sensors such as touch, impact, and proximity. Integration of various types of sensors into robotic skin is challenging due to the topographical nature of skin. Printing is a promising technology that can be explored for sensor integration as it may allow both sensors and interconnects to be directly printed into the skin. We are developing Electrohydrodynamic (EHD) inkjet printing technology in order to co-fabricate various devices onto a single substrate. Using strong applied electrostatic forces, EHD allows the printing of microscale features from a wide array of materials with viscosities ranging from 100 to 1000cP, highly beneficial for multilateral integration
2. Pressure
High voltage
Ink chamber
and nozzle
Sample
X,Y Programmable Stage
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Liquid meniscus
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Jet diameter
Nozzle diameter
complex topographies. Among many printing techniques, inkjet printing can be used at various stages of micro/nano
systems manufacturing; for instance, direct device printing (gas sensors, organic LEDs, and thin film transistors), mask-
less lithography (front-end fabrication as well as PCB production for back-end applications), and packaging (dispensing
epoxies and printing interconnects). The ability to integrate several disparate materials into one fabrication platform is a
key for multi-modal sensor fabrication on robotic skin. It is also drawing attention due to its cost effectiveness as
printing sensors does not require a large amount of ink materials and does not generate waste.
In this paper, we explore Electrohydrodynamic (EHD) printing as a versatile printing method that can be used for sensor
integration onto robotic skin. The main benefit in using our EHD printing for sensor fabrication is its flexibility in
printing various liquids and metals onto conductive and even potentially nonconductive substrates of differing
topographies. As robotic skin would require a fusion of materials, a system with the capability to dispense nearly any
material with minimal reworking is very advantageous. We will discuss here the printability of disparate materials
(conductive, non-conductive, and colloidal) with experimental results. We will also highlight the applicability of these
materials for sensor integration onto robotic skins.
1.2 Electrohydrodynamic Printing (EHD)
EHD printing uses an electric field to eject fluids. The applied electric field enables fine jetting which creates smaller
features by an order of magnitude below the nozzle size3
. In EHD, a pressure is applied to the ink chamber until a fluid
meniscus is formed at the end the nozzle tip before applying an electric field across the nozzle and substrate for jetting.
Figure 1(a) shows a generic configuration of a typical EHD setup. The fine jetting feature is possible due to the pulling
and focusing effect from the electric field, in comparison to pushing through applied pressure as in the case in piezo-
driven jetting. Electric field-driven ejection enables creating smaller features by an order of magnitude below the nozzle
size thereby vastly improving the resolution as shown in Figure 1(b) and (c). Applying a DC electric field produces
stable and continuous jetting which is suitable for printing uniform lines4,5
. Drop-on-demand printing can be achieved by
using external pulsating voltage. This mode is very useful in printing complicated patterns such as those required for
sensor fabrication. Micro-dripping is another jetting mode that uses pulsating voltage to deliver droplets to a substrate
without a spreading effect. It has been demonstrated by making uniform patterns out of micro/nano sized droplets and
would be highly beneficial for fabrication of a sensor array with minimal sensor to sensor variation 6
.
Figure 1. (a) Generic printer configuration of EHD printing. (b) Nozzle tip with fluid meniscus before applying electric
field, and (c) jetting characteristics after applying electric field.
One advantage of using strong electric fields for fluid ejection is the ability to print materials with viscosities as high as
1000cP. This expands the choice of available materials and is highly beneficial for the fabrication of various types of
sensors. In comparison piezo-jet based printing can only handle inks with viscosities of up to 50cP. The printability of
high viscosity materials enables the printing of thicker microstructures; a key feature that sets EHD apart from other
inkjet printing methods which typically use multiple superimposed print runs to achieve this. Despite these apparent key
advantages, one of the drawbacks of EHD is the requirement of a conductive substrate surface for generating an
electrical potential. The requirement of a conductive substrate can be eliminated by using a ring electrode for electric
field generation, which is an active research area for EHD printing.
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3. Camera
Tube to supply
pneumatic
pressure
Ink chamber
Mirror
Substrate
Nozzle
2. EXPERIMENTAL
2.1 EHD Setup
The EHD system used in this experiment consists of an ink chamber, interchangeable nozzle tips, a high-voltage power
supply, a function generator, a precision pressure regulator, and an automated positioning stage. Figure 2 shows the
current configuration of the EHD set up used in this work. A high DC voltage is maintained between the nozzle tip and
the substrate to create continuous jetting while a pulsating voltage generated through a function generator is used for
drop-on-demand printing. Voltage settings applied in the experiments vary for different inks. The distance between the
nozzle tip and substrate varies based on the size of the nozzle tip and the voltage applied. The use of precision staging
includes four degrees of freedom (X, Y, Z, and Theta) allowing the system to scan non-planer surfaces with micron
precision and maintain a constant distance between nozzle and substrate for EHD printing.
Figure 2. The current configuration of the EHD setup (a) CAD model showing gantry system with x-y-z-theta stages (b) A
photograph of the current EHD setup (high voltage amplifier, function generator and precision pressure regulator are not
shown in this photograph)
2.2 Printing Experiments
Three different types of custom inks with different characteristics were used. The first type of ink was used to
demonstrate the mask-less lithography capability of EHD. Commercial KMPR 1010 photoresist7
, a non-conductive
polymeric solution, was modified using N-Methylpyrrolidone (NMP) and OMNOVA PolyFox Fluorosurfactants to
achieve the desired properties for printing. The measured viscosity of the modified KMPR 1010 was 520cP. Gold coated
silicon, silicon oxide, and Kapton were used as substrates. Drop-on demand experiments were performed with a square
wave of 600Hz with a 20% duty cycle. The peak of the square wave was 600V with a bias of 400V. A gold coated 10µm
glass nozzle was used with a gap of 160µm between the nozzle and the substrate. After printing gold was selectively
etched and KMPR was removed from the substrate to form patterned gold traces.
The second type of ink made of PEDOT:PSS, Poly(2,3-dihydrothieno-1,4-dioxin)-poly(styrenesulfonate), a widely used
pressure sensor fabrication material was tested for the development of an EHD printed sensor fabrication process. This
test used 5.0 wt. % conductive screen printable paste from Orgacon™ EL-P-5015, PEDOT:PSS, with a resistance and
viscosity of 50-150Ω/sq and 50,000-90,000cP, respectively. The material was diluted with NMP to reduce the viscosity
and the initial experiments were performed using the ink with viscosity at 230cP. A 100µm stainless steel nozzle was
used and a DC voltage of 1.6kV with an 800 µm gap between the nozzle and the substrate were used during printing.
The last set of experiments were performed using highly conductive zinc ion (Zn2+) ink to demonstrate the EHD
capability of direct device printing. The viscosity of the ink was 455cP, made using zinc acetate (precursor), ethylene
glycol (solvent), and polyvinylpyrrolidone (binding matrix). A continuous jetting mode with a DC voltage of 850V was
used. A gold coated 10 µm glass nozzle was used with printing speeds (substrate travel) of 600, 1000, 1400, and 1800
mm/min. Printing was followed by a soft bake step (100ºC for one minute) to evaporate the solvents. Finally, a sintering
process was performed above 400ºC for transforming printed structures into polycrystalline Zinc Oxide (ZnO). .
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5. (a) (b) 150µm
A
2220µm
< >
` 2160 µm
of a size, shape, and topography that are not suited for conventional lithography. This data encourages replacing
photolithography processes with direct EHD printing of photoresist for mask-less lithography-based patterning of metal
interconnects and other materials for sensor integration onto robotic skin
Figure 5. EHD-based mask-less lithography patterned gold lines on (a) silicon (linewidth 23.5μm), (b) silicon oxide (linewidth
31.3μm) and (c) Kapton (linewidth 16.8μm).
3.2 Printing PEDOT:PSS Sensing Layers
In recent years, PEDOT:PSS has been the sensing material used in touch screen technology. PEDOT:PSS is a
transparent, conjugated conducting polymer that is highly ductile and stretchable along with having good environmental
stability. Several researchers have fabricated and characterized tactile sensors using PEDOT:PSS8,9,10,11
. The resistance
of ink-jet printed PEDOT:PSS is about a few kilo ohms. It has elongation of 10% or more. The gauge factor of
PEDOT:PSS is 5 to 20, whereas the gauge factor of a conventional metal film is 2. Calvert et al. fabricated piezoresistive
sensors using PEDOT:PSS inkjet printing for smart textiles8
. That tactile sensor showed a resistance of 5 kilo Ohms and
a gauge factor of 5 after 500 cycles of testing. Here we report the results of a first attempt at printing PEDOT:PSS in
order to fabricate pressure and strain sensors as well as interconnects on robotic skin. Figure 6 shows the printing results
for an array of interconnected square pads printed on a gold coated glass substrate. By examining the results as printed, it
is apparent that solvent pooling and surface tension-driven restructuring are occurring. Currently, optimization of the
PEDOT:PSS ink and printing process is progressing to mitigate this issue. Future plans include characterization of the
printed material and implementation of the printing process to tactile sensor fabrication on skin like substrates.
Figure 6. The results of an array of interconnected square pads printed on gold coated glass substrate (a) as printed and (b)
after room temperature drying for three hours.
3.3 Printing Metal Oxide Microstructures
As multifunctional materials, metal oxides are poised to play a critical role in many advanced technologies that include
flat panel displays, printed electronics, sensors, and actuators. Although printing and fabrication methods described here
may not lead to fabrication of these devices directly onto robotic skin due a high temperature processing step, EHD
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6. et A's
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printing can be used to integrate metal oxide-based miniature gas sensors, thin film transistors, and energy harvesters to
other parts of a robotic platform. This investigation was focused on printing ZnO from a highly conductive (135µS/cm)
zinc ion containing ink. The printing results discussed in this section not only demonstrate the formation of ZnO
microstructures but also show the capability of EHD as a versatile printing method by printing non-conductive KMPR
ink to highly conductive Zinc ion containing ink.
After printing on a silicon oxide substrate, printed microstructures were subjected to a sintering process for creating ZnO
microstructures. X-Ray Diffraction (XRD) analysis performed on the printed ZnO films sintered at various temperatures
confirmed that the ink produces polycrystalline ZnO upon heating above 400ºC. Figure 7(a) displays the representative
XRD data showing the polycrystalline nature of the sintered film. Figure 7(b) shows the SEM image of formed ZnO
lines with no detectable cracks or pinholes. Further investigation is needed to better understand the effect of matrix
loading and sintering on grain characteristics and film stress.
Figure 7. (a) the representative XRD data of the sintered ZnO film at 400ºC and (b) the SEM image of ZnO microstructure.
Figure 8 (a) shows the linewidth of the printed structures based on printing speed using at an jetting voltage of 850V.
After the sintering process, one of the key aspects to note is the shrinkage of the structure due to the removal of matrix
materials. It is therefore essential to build a correlation between printed and final microstructure geometry in order to
obtain desired device geometry. Figure 8 (b) shows the representative surface profile of ZnO ink printed at 850V with a
printing speed of 1000 mm/min before and after sintering. The lateral and thickness shrinkage percentage for this
particular ink were determined to be 3% and 92% respectively. With the negligible lateral shrinkage, this printing has
resulted in ZnO microstructures with linewidths ranging from 18 to 65µm and thicknesses ranging from 33 to 62nm. The
capability of printing a wide range of thickness by changing process parameters is encouraging as this can lead to
different types of device using EHD.
Figure 8. (a) Linewidth of printed structures as a function of printing speed using a jetting voltage of 850V and (b) surface
profile data on ZnO ink printed at 850V with a printing speed of 1000 mm/min before and after sintering.
4. CONCLUSIONS AND FUTURE DIRECTIONS
Based on the preliminary experimental work performed here, it is evident that EHD printing could be an attractive
method for integrating sensors into robotic skins for human-robot interactions. We have shown the printing of high
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7. viscosity materials with varying conductivity and the ability to achieve geometries ranging from a few tens of microns to
millimeters. This clearly shows that the EHD is an enabling technology that can be used to co-fabricate various devices
onto a single substrate. Although many technological advancements are necessary to fully tap the potential of EHD, the
experimental results discussed here evidently show the possibility of EHD as a manufacturing platform for integrating
sensors into robotic skin.
Our immediate future research is focused on two main areas: (1) further development of the EHD printer technology,
and (2) fabricating an array of pressure sensors onto flexible substrates by printing PEDOT:PSS. The primary goal of
EHD technology development is to integrate a ring electrode to the nozzle head so that printing can be performed
regardless of substrate conductivity. Though several attempts have been made by a few research groups to integrate ring
electrodes into EHD printers, this is a major technological barrier that hampers the application of EHD printing
technology to a wide array of substrates. In terms of sensors for robotic skins, we plan to fabricate an array of pressure
sensors onto a flexible substrate by using EHD printing. The work will starts with characterization of printed materials
and ends with the fabrication of an entire sensor array by printing PEDOT:PSS and interconnects using EHD.
5. ACKNOWLEDGMENTS
This work was supported in part by the Office of Naval Research Grants #N00014-08-C-0390, #N00014-11-C-0391, and
the National Science Foundation NRI Grant #IIS-1208623. We wish to thank Raminderdeep Sidhu, Lester Corwin, and
the UTA Research Institute staff for their help with the experimental work presented in this paper.
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