adfm_201002508_sm_suppl
Transcript of adfm_201002508_sm_suppl
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CopyrightWILEYVCHVerlagGmbH&Co.KGaA,69469Weinheim,Germany,2010.
SupportingInformation
forAdv.Funct.Mater.,DOI:10.1002/adfm.201002508AMicrofluidic,ReversiblyStretchable,LargeAreaWirelessStrainSensor
Shi Cheng* and Zhigang Wu*
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Electronic Supplementary Information
Microfluidic Reversibly Stretchable Large-Area Wireless Strain
Sensor
Shi Cheng1,
and Zhigang Wu2,
1Advanced Technology, Laird Technologies, Box 1146, SE 164 22, Kista, Sweden
2Microsystems Technology, Department of Engineering Sciences, Uppsala University, Box
534, The Angstrom Laboratory, SE 751 21, Uppsala, Sweden
To whom correspondence should be addressed ([email protected] and [email protected])
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1. Principles and Implementation1.1. RF Transmitter and Receiver Sub-Modules
RF
GND GND
EN
VCC
VOUT
DCpowersupply
PRL1
C1
C2
C1
Power
de
tector
(L55
34)
DCpowersupply
C =1nF,1 C =100pF,C =0.1 F,C =1.5pF,L =19nH2 3 4 1
NC
VCC
GO1555
GND
GND GND
O/PGND
VCTR
Tomicrovoltdigitalmultimeter(DMM)
C3
PR
Controlvoltage
C =1nF,1 NC=Noconnection
C4
b)
a)PT
Figure S1. Circuit schematics of a) the RF transmitter sub-module in the integrated strain
sensor (coupling capacitor: C1), and b) the RF power detection unit in the PC-assisted receiver
(decoupling capacitors: C2 and C3, coupling capacitor: C1, matching capacitor: C4, matching
inductor: L1).
The simplified RF transmitter in the integrated wireless sensor device is composed of a
voltage controlled oscillator (VCO) (Gennum, GO1555), and a coupling capacitor (C1), on a
flexible laminate of 13 mm 10 mm in size, cf. Figure S1(a). The choice of the VCO is based
on its proper oscillation frequency range, miniaturized package size, relatively low power
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consumption, as well as sufficient RF output power. The chosen VCO generates stable
continuous wave (CW) RF signals around 1.5 GHz when a supply voltage in the range of
2.25-2.75V and a control voltage ranging from 1.0V to 1.5V are applied. Moreover, it only
draws a maximum supply current of 8 mA. This factor implies that this RF transmitter
circuitry can be effectively powered by two serially connected commercially available AA or
other types of standard portable batteries.
Figure S1(b) shows the circuit schematic of the RF power detection sub-module in the PC-
assisted receiver. In addition to an RF power detector (Linear Technology, LT 5534), this unit
also contains two decoupling capacitors (C2 and C3), one coupling capacitor (C1), one
matching capacitor (C4), and one matching inductor (L1), all soldered on a small piece of
FPCB with a size of 10 mm 20 mm. The integrated RF power detection circuitry is capable
of precisely converting the injected RF signals, in a decibel scale ranging from -60 dBm to 0
dBm, into DC voltage in a linear scale around 1.5 GHz.
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1.2. Strain Sensor Contained Liquid Metal Antenna
c)
d)
e)
f)
g)
Blanksheet
Sealinlet3withadhesivetape
Injectupperfluidmetallayer,encapsureoutletsintopreplicawithuncuredPDMSdroplets&sealinlets1&3
Flipsample&injectlowerfluidmetallayer,encapsulateinlet2andoutletsinbottomreplicawithuncuredPDMSdroplets
Removeadhesivetapeoninlets1&3
PDMS Upperfluidmetallayer Adhesivetapefortemporarilysealinginlets
Bottomfluidmetallayer
Topreplica&blanksheetPunchoutaholeforinlet3&sealtobottomreplica
Bottomreplica
Topreplica&blanksheet&bottomreplica
Topreplica&blanksheet&bottomreplica
Bottomreplica&blanksheet&topreplica
Topreplica&blanksheet&bottomreplica
Inlet3
b)
a)
TopreplicabondedtoablankPDMSsheet
Topreplica
To p a nd b ot t om P DM S e la st o me r patterned by replica molding, withpunchedholesforinlets1&2,andoutletsBottomreplica Outlets
Inlet1
Inlet2
Topreplica
Figure S2. Fabrication process steps of the multi-layer microfluidic stretchable patch antenna
integrated in the presented wireless strain sensor.
Minor modifications have been made to adapt the previously reported fabrication processes to
the multi-layer FSRFEs based wireless strain sensor presented in this paper.[1-2]
The
implementation of the integrated sensor device can be briefly summarized as the following
steps: fluidic patch antenna fabrication, active circuit assembly, and hybrid device integration.
The latter two resemble the manufacturing and integration processes presented in the previous
work. Concerning the antenna fabrication, one more PDMS as well as liquid metal alloy
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layers have been added to implement multi-layer FSRFEs. More detailed process steps are
illustrated in Figure S2 and described as below:
First of all, the upper (antenna patch) and lower (ground plane) microfluidic channels were
respectively constructed in the top and the bottom PDMS slabs, with a standard soft
lithography. And then a few inlets and outlets were punched as depicted in Figure S2. In
addition, the blank middle PDMS sheet with a thickness of 1.5 mm was also fabricated. Later,
the micro-structured top PDMS layer was bonded to the blank PDMS slab using corona
discharging activation, and the inlet 3, cf. Figure S2, was punched on the bonded PDMS sheet.
Subsequently, the bottom PDMS slab was bonded to the upper PDMS layers with plasma
bonding. After sealing the inlet 3 with a small piece of Scotch
tape, the upper microfluidic
channels were filled with galinstan fluid, and the ventilation outlets in the top PDMS slab
were encapsulated using PDMS prepolymer afterwards. Whereafter, both the inlets 1 and 3
were sealed with Scotch
tape, and galinstan alloy was injected into the lower microfluidic
channels from the bottom side. All remaining ventilation outlets together with the inlet 2 were
encapsulated, and the inlets 1 and 3 were reserved for connecting the RF transmitter circuitry
in the hybrid sensor device.
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PDMSUpperfluidmetallayer
CrossView hupper
d
h
f
z
y
x
xy
z
q
TopView
-+
Lowerfluidmetallayer
-+
h lowerhmiddle
Wms
L inset
Wpatch
Lpatch
Lground
Wground
Two openings for connecting RFfeedcableinthestandaloneantennacharacterizations or RF transmittersub-moduleintheintegrateddevice
Figure S3. Geometric configuration of the elastic fluid metal patch antenna. Dimensions are:
Lpatch = 56.0 mm, Wpatch = 50.0 mm,Lground = 110.0 mm, Wground= 80.0 mm,Linset= 16.0 mm,
Wms = 3.7 mm, h = 2.5 mm, hupper= 75.0 m, hmiddle = 1.5 mm, and hlower= 75.0 m.
Assuming that the PDMS elastomer had the relative permittivity of 3.0 and the dissipation
factor of 0.01 around 1.5 GHz, the conductivity of the liquid alloy, galinstan, was about 3.46
106
S/m, and the spacing (hmiddle) and the width (Wpatch) of the patch antenna were 1.5 mm
and 50.0 mm, an initial value of 57.3 mm for Lpatch was found, according to the transmission
line model of the rectangular microstrip patch antennas.[3]
Of course, electrical performance
of the patch antenna based on the proposed geometrical configuration must be verified in
more accurate numerical simulations, and some minor adjustments are probably needed for
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tuning its resonant frequency. Since the thickness of the PDMS membrane on top of the
antenna patch is only approximately 425 m, 1/500 of the operational wavelengths at 1.5 GHz,
its influence on the antenna electrical performance are negligible.
1.3. Integrated Wireless Strain Sensor
C
GO1555
b)
a)
c)
d)
e)
f)
C
GO1555GO1555
C
GO1555
PDMSUpperfluidmetallayer
Lowerfluidmetallayer
Kaptonfoil VCOchip
MetallicpinCopper Capacitor Anode Cathode
C
Solder
Figure S4. Schematic drawings of the integration procedure for the demonstrated
microfluidic stretchable wireless strain sensor.
In brief, two tin-plated contact pins resembling cantilevers were first soldered to the RF
output and the ground pads on the FPCB of the RF transmitter, respectively. And then a semi-
spherical solder ball was mounted to the bottom surface of each pin at the other end.
Whereafter, three thin wires were respectively soldered to the supply voltage, the control
voltage, and the ground pads of the RF transmitter circuitry for external power supply
connection, as observed in Figure 1. Subsequently, this RF transmitter sub-module was
attached to the top surface of the previously fabricated liquid metal patch antenna, and each
solder ball at the end of the contact pin was directly immersed in the fluid metal enclosed in
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the micro-structured elastomeric channels, via the two opening in the upper PDMS membrane,
cf. Figures 1, S3 and S4. In the end, the complete RF transmitter including the two contact
pins were locally encapsulated in a PDMS LSC for protecting from stretching.
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1.4. System Demonstration
RemoteMonitor
PR
IntegratedWirelessStrainSensor
Hornantenna
Voltage-controlledosillator(VCO)
DCpowersupply
Microfluidicelasticantenna
Flexiblecircuitry
PT
5m
RFpowerdetector
MicrovoltDMM
DCpowersupply
PC
Tunableattenuator
DCpowersupply
RFamplifier
Figure S5. Schematic illustration of the system demonstration setup for remotely sensing
mechanical strains in real-time, using the integrated sensor device.
Besides the self-contained sensor device, a custom-designed PC-assisted RF receiver has also
been implemented for remote monitoring in the system demonstration, as illustrated in Figure
S5. Of course, similar receiving function can also be realized using commercially available
RF measurement instruments, for instance, spectrum analyzers or RF power meters, but the
intention here was to remove all costly and bulky RF test equipment, and replace them with
cost-effective modules. Figure S5 displays the schematic illustration of the system
demonstration setup for remotely sensing high tensile mechanical strains in real-time, of
which the receiver part consists of a standard gain horn (Flann Microwave, 08240-10), a
coaxial amplifier (Mini-circuits, ZKL-2R5), a tunable HP attenuator (HP, 8495A), a Keithley
197A autoranging microvolt digital multimeter, a laptop, a DC power supply, and an RF
power detection unit powered by four serially connected AA rechargeable batteries with a DC
supply voltage of 5.23V.
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2. Results and Discussion2.1. RF Power Detection Unit
-70 -60 -50 -40 -30 -20 -10 00
0.5
1
1.5
2
2.5
InputRFPower(dBm)
OutputDC
Voltag
e(V)
Figure S6. Measured output DC voltages of the RF power detection sub-module in the
custom-designed RF receiver versus varying input RF power around 1.5 GHz.
[1]
S. Cheng, Z.G. Wu,Lab Chip.
2010
,10
, 3227.
[2] S. Cheng, Z.G. Wu, P. Hallbjorner, K. Hjort, A. Rydberg,IEEE T. Antenn. Propag.2009,57, 3756.
[3] C. A. Balanis,Antenna Theory, 2nd ed, John Wiley & Sons, New York, 1997.