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Highly Flexible Dye-sensitized Solar Cells
Produced by Sewing Textile Electrodes
on Cloth
Min Ju Yun, Seung I. Cha, Seon Hee Seo & Dong Y. Lee
Nano Hybrid Technology Research Center, Creative and Fundamental Research Division, Korea Electrotechnology Research
Institute.
Textile forms of solar cells possess special advantages over other types of solar cells, including their light
weight, high flexibility, and mechanical robustness. Recent demand for wearable devices has promoted
interest in the development of high-efficiency textile-based solar cells for energy suppliers. However, the
weaving process occurs under high-friction, high-tension conditions that are not conducive to coated
solar-cell active layers or electrodes deposited on the wire or strings. Therefore, a new approach is needed for
the development of textile-based solar cells suitable for woven fabrics for wide-range application. In this
report, we present a highly flexible, efficient DSSC, fabricated by sewing textile-structured electrodes onto
casual fabrics such as cotton, silk, and felt, or paper, thereby forming core integrated DSSC structures with
high energy-conversion efficiency (,5.8%). The fabricated textile-based DSSC devices showed high
flexibility and high performance under 4-mm radius of curvature over thousands of deformation cycles.
Considering the vast number of textile types, our textile-based DSSC devices offer a huge range of
applications, including transparent, stretchable, wearable devices.
T
he demand for lightweight, highly flexible or bendable solar cells has grown rapidly as the application of
photovoltaic electric power generation has widened to encompass urban life in the form of building-
integrated photovoltaics (BIPV) or electronics-integrated photovoltaics (EIPV)1–5
. Until several years ago,
most of the research effort had focused on techniques involving flexible plastic substrates onto which transparent
conductive oxide (TCO) films were deposited6–8
. However, TCO films can be easily fractured, resulting in a loss of
conductivity due to their brittle nature. More recently, there has been a renewed interest in traditional material-
based flexible solar cells, such as those associated with paper, string/fiber, and textiles9–26
.
Textile forms of solar cells possess special advantages over other types of solar cells, including their light weight,
high flexibility, and mechanical robustness. Recent demand for wearable devices has promoted interest in the
development of high-efficiency textile-based solar cells for energy suppliers. Based on these demands, several
studies have investigated the fabrication of textile-based solar cells, using organic solar cells or dye-sensitized solar
cells18–24
. However, these research efforts were basically aimed at producing wires or strings of solar cells, ignoring
their condition during the weaving process. Generally, the weaving process occurs under high-friction, high-
tension conditions that are not conducive to coated solar-cell active layers or electrodes deposited on the wire or
strings. Additionally, current research results can only produce very short (tens of centimeters) strings, far less
than the length required for actual weaving or textile-based applications. Therefore, a new approach is needed for
the development of textile-based solar cells suitable for woven fabrics for wide-range application.
Dye-sensitized solar cells (DSSCs) have attracted much interest, due to their low fabrication costs, relatively
high, efficiency especially under weak illumination, and ability to incorporate the dye color employed1–5
. In terms
of textile solar cells, DSSCs offer several advantages, including spatial separation of the photoanode and counter
electrode via electrolyte insertion, which minimizes the possibility of a short circuit. By combining this approach
with the concept of core-integrated DSSCs for paper-based TCO-free DSSC9
, we propose a new prototype for
textile-based solar cells using DSSCs.
In this report, we present a highly flexible, efficient DSSC, fabricated by sewing textile-structured electrodes
onto casual fabrics such as cotton, silk, and felt, or paper, thereby forming core integrated DSSC structures. By
carefully fabricating the woven electrodes, the sewing process, one of characteristics of textiles, can be applied to
the fabrication of solar cells as well as to the process of weaving using a loom.
OPEN
SUBJECT AREAS:
SOLAR CELLS
DESIGN, SYNTHESIS AND
PROCESSING
Received
14 March 2014
Accepted
27 May 2014
Published
24 June 2014
Correspondence and
requests for materials
should be addressed to
S.I.C. (sicha@keri.re.
kr)
SCIENTIFIC REPORTS | 4 : 5322 | DOI: 10.1038/srep05322 1
Results
The process used to create the textile-based flexible solar cells to be
sewn onto cloth consisted of the following steps: weaving each elec-
trode by loom, depositing the photoanode material (i.e., TiO2) and
the counter-electrode material (Pt), administering heat treatment,
sewing to form the core-integrated DSSC device, and dye loading;
these steps are shown in Fig. 1(a). The photoanode and counter-
electrode textiles consisted of two parts: (1) a woven structure of
stainless steel ribbon with periodic holes of 70 mm as the wefts and
Ti wire of 100 mm as the wraps, and (2) the woven structure of glass
fiber yarn as the wefts and Ti wire as the wraps (Fig. 1 (b) and (c)).
The former (stainless steel/Ti wire) was used as the collector and as a
substrate for the device; additionally, the later part provided mech-
anical support and robustness for sewing to the other textiles, as
shown in Fig. 1(c). It should be noted that the textile electrodes
consisted of heat-resistant materials, such as metal and glass fibers.
Therefore, each electrode can be heat treated after the deposition of
the TiO2 porous film and Pt, which is an important factor for high-
efficiency DSSCs.
The photoanode and counter-electrode textiles were woven using
a 351 twill structure, providing relatively high flexibility and a flat
woven surface. (See Supporting Information Fig. S1 for schematics of
twill structured textile) Combined with stainless steel ribbon as the
wefts, the textile structure photoanodes had quite flat structures
compared with those expected in woven structures, as shown in
Fig. 1(c). Therefore, the conventional doctor-blade process or
screen-printing process was applied to deposit the electrode materi-
als. The counter electrodes were prepared using two-step deposition
of Pt. First, the Pt was deposited onto the counter-electrode textile
using an electroplating method, and this was followed by the depos-
ition of Pt-containing paste. The structure was then heat treated.
Using this two-step deposition process, Pt thin flakes resembling
flowers can be prepared (see Supporting Information Fig. S2 and
S3 for images of the counter electrode and photoanode deposited).
The prepared textile electrodes were assembled by sewing, placing
each electrode on either side of the cloth, followed by electrolyte
infiltration, as shown Fig. 1(d). The textile-structured electrodes were
attached to the cloth (in this case, paper) using a sewing machine. As
a result, core-integrated forms of DSSCs were fabricated; Figs. 1(e)
and 1(f) show a cross-sectional schematics and a plane view, respect-
ively. In the cross-sectional schematics, the DSSC prepared by the
sewing process consisted of three layers, similar to conventional
DSSCs; however, no TCO films or glass plates were employed, which
is a particular feature of core-integrated DSSCs.
The photovoltaic performance of the textile-based DSSC sewn on
Hanji, a Korean traditional paper, is shown in Fig. 2(a). The rela-
tionship between the current density and applied voltage shows a
high short-circuit current (.17 mA cm22
). However, the fill factor
was low at only 0.37, which is the main limitation for energy con-
version efficiency. The low fill factor can come from the low porosity
of Hanji infiltrated with electrolyte and the evaporation of electrolyte
on the surface of electrode due to lack of sealing during measure-
Figure 1 | (a) Schematic illustration of the fabrication concept for textile-based dye-sensitized solar cells (DSSCs) made by sewing textile electrodes onto
cloth or paper. (b) Photograph of the loom (inset) used to weave the textile electrodes, and (c) a woven electrode. The inset shows an image of the stainless
steel ribbon with periodic holes. (d) Photograph of the sewing process to attach the woven electrodes to Hanji, a Korean traditional paper. (e) Schematic
illustration showing the cross-sectional structure of the textile-based DSSC prepared by sewing and (f) photograph of a core-integrated textile-based
DSSC fabricated by sewing textile electrodes onto Hanji.
www.nature.com/scientificreports
SCIENTIFIC REPORTS | 4 : 5322 | DOI: 10.1038/srep05322 2
ment. The overall efficiency under 1-Sun illumination was ,4.3%
despite the high current density, with 5.3% corresponding to the
maximum conversion efficiency observed.
The textile-based DSSC fabricated by sewing exhibited consid-
erable bending ability, as shown in Fig. 2(b), where the prepared cell
was wound around a rod of 0.4-cm radius of curvature. The cell
underwent thousands of bending cycles of 90u. The photovoltaic
performance under bending conditions was maintained at 80% of
the flat cell value with bending to a 10-cm radius of curvature and
30% with a 4-mm radius of curvature, as shown in Fig. 2(c).
Additionally, the photovoltaic performance remained over 70% of
the initial value even after 1000 bending cycles over a 1-cm radius of
curvature, as shown in Fig. 2(d). (See Supplementary Information
Figure S5 and S6 for status of cell after repeated bending by pressing
plunge).
The energy conversion efficiency of the textile-based DSSC sewn
on cloth was affected by several factors; some of these factors, to the
best of our knowledge, have yet to be considered for textile-based
DSSCs. One such factor is the contact between the metal wires in the
woven electrodes. If the contact between the metal wrap and weft is
lost, then an electrical open circuit forms within the cell that acts as a
recombination site during operation. Under these conditions, the
energy conversion efficiency can be degraded considerably by loss
of contact between the woven electrodes. It is not totally clear when
the contact becomes lost; however, tension maintained during the
weaving process, as well as the pattern of the weave, could have an
effect on the electrical contact of the woven electrode.
Another factor that may affect photovoltaic performance of the
textile-based DSSC is the cloth itself, which contains the electro-
lyte and plays the role of a spacer to prevent electrical short
circuits from forming between the electrodes. Hanji has very
few pores for diffusion within the electrolyte, as shown in
Fig. 3(a), which induces a low fill factor during photovoltaic
operations. To investigate the effect of cloth on photovoltaic per-
formance, other types of cloth including cotton and silk (both in
the form of gauze) were used for the textile-based DSSC as a
spacer. The woven electrodes were attached to either side of the
cotton and silk gauze using a sewing machine, as shown in
Fig. 3(b); note that a mechanically robust core-integrated DSSC
can be fabricated using these cloth types. This is particularly useful
and meaningful with respect to the application of wearable devices
for energy supply. The microscopic structures of the cotton and
silk gauze are shown in Figs. 3(c) and 3(d). Compared with Hanji,
the gauze offers more space for electrolyte filling and diffusion.
Figure 2 | (a) Relationship between current density and applied voltage (red circle) and specific power and applied voltage (blue line) of a textile-based
DSSC prepared by sewing the woven electrode onto Hanji; measurements were obtained under 1-Sun, 1.5-AM conditions. (b) Photographs showing a
textile-based DSSC wrapped around a rod with a 4-mm radius of curvature under cyclic bending deformation (inset). (c) Relative energy conversion
efficiency of the flat-state textile-based DSSC and (d) relative efficiency after cyclical bending of 1000 and 2000 times.
www.nature.com/scientificreports
SCIENTIFIC REPORTS | 4 : 5322 | DOI: 10.1038/srep05322 3
The open area of cotton gauze is measured as about 48%, while
that of silk gauze is about 47%.
The effect of cloth type on photovoltaic performance indicates that
the inserted cloth considerably affects energy conversion efficiency
and the relationship between current density and applied voltage, as
shown in Fig. 4(a). High current densities for the textile electrodes
can be expected as a result of light reflection from the metal and
enhanced photon harvesting25,26
. The woven metal ribbon can reflect
over 10% of incident light when it is oxidized. (See Figure S4 for light
reflection from metal ribbon) It is also shown in wire-shaped solar
cell that the light concentration by focusing light or luminescent
concentrator could enhance energy conversion efficiency. In the case
of cotton gauze, the current density decreased slightly, whereas the
fill factor increased; hence, the energy conversion efficiency
improved to 5%. When silk gauze is inserted between textile electro-
des, the energy conversion efficiency was enhanced to 5.8%. For the
champion cell, the efficiency is measured as nearly 7%; in this case,
the current density increased to nearly 20 mA cm22
, which is a high
value, even for conventional sandwich-structured DSSCs, as sum-
marized in Table 1. The enhancement observed with cotton gauze
compared with Hanji can be explained in terms of the ease of dif-
fusion in the electrolyte due to the large free space; the chemical
status of the cotton and paper did not change significantly within
the electrolyte under Fourier-transform infrared (FTIR) spectro-
scopy analysis, as shown in Fig. 3(b). However, in the case of the silk
gauze, the electrolyte changed the chemical status of the yarn, as
shown in Fig. 3(b), where absorption near 3200–3500 and
1600 cm21
was observed after soaking the silk in the electrolyte for
one day. The absorption that occurred was attributed to the forma-
tion of hydroxyl groups, amide groups, and aromatic groups, which
exist in protein molecules. The electrolyte and spacer, chemically
modified in the silk gauze, enhanced the energy conversion effi-
ciency. Thus, the potential exists for further improvement beyond
the results presented here.
Discussion
However, questions remain regarding the determination of energy
conversion efficiency in these devices. High current densities for the
textile electrodes can be expected as a result of light reflection from
the metal and enhanced photon harvesting. For electrochemical
impedance spectroscopy (EIS) results under open-circuit conditions,
as shown in Figs. 3(c) and 3(d), the cloth type appeared to affect the
resistance during electrode reactions. Nyquist plots indicated that
this effect was smallest in cotton gauze and highest in silk gauze in
short circuit condition. The Bode plots showed that the resistance
was related to the reaction near the 10–100 Hz range, which may
correspond to recombination in the photoanode. In this case, the
recombination rate was related to the ionic concentration near the
photoanode, which can be affected by diffusion and the initial ionic
concentration. To find the optimum operating conditions for textile-
based solar cells, further research on the cloth material is needed. It
should be noted that in this study, we used conventional commer-
cially available materials, including TiO2 nanoparticle paste, com-
mon electrolytes, and a Pt counter electrode. This suggests the
possibility for considerable improvement in photovoltaic perform-
ance of these structured DSSCs with suitable material optimization.
The woven pattern is another critical factor that may allow further
improvement in performance. As mentioned earlier, the woven
structure and the applied tension in the wraps and wefts determine
the electrical contact within the woven electrodes. By considering
various forms of textiles developed, semi-transparent electrodes or
stretchable electrodes could be fabricated by proper selection of the
weave pattern. In this sense, the preparation of DSSCs by sewing
textile electrodes on various types of cloth provides vast potential
for possible application.
In summary, highly bendable, mechanically robust DSSCs with
high energy-conversion efficiency (,5.8%) can be fabricated by sew-
ing textile electrodes prepared by loom weaving onto various types of
cloth. The fabricated textile-based DSSC devices showed high flex-
ibility and high performance under 4-mm radius of curvature over
thousands of deformation cycles. Considering the vast number of
textile types, our textile-based DSSC devices offer a huge range of
applications, including transparent, stretchable, wearable devices.
Mothods
The etched mesh of 304 stainless steel (Tech-Etch MicroEtchH) and 50-mm-diameter
Ti wire (iNexus) were used as the weft, and 100-mm-diameter Ti wire (iNexus) was
Figure 3 | (a) Scanning electron microscopy (SEM) image of the Hanji surface. (b) Photograph of the process of sewing woven electrodes onto silk gauze
using a sewing machine. SEM images of the surface of (c) cotton gauze and (d) silk gauze. Inset shows prepared textile-based DSSCs using (c) cotton gauze
and (d) silk gauze.
www.nature.com/scientificreports
SCIENTIFIC REPORTS | 4 : 5322 | DOI: 10.1038/srep05322 4
used as the warp of the woven electrode. The sewn part of the electrode, a glass fiber
(D450 1/2, Hyunmin Fiber), was used as weft. A Daesung Hi-tech loom (Daesung Hi-
Tech Co., Ltd., Korea) was used for weaving.
The woven electrode was rinsed with acetone, ethanol, and deionized water by
sonication and dried with nitrogen gas. After cleaning, the woven textile for the
working electrode was heat treated at 480uC for 1 h in air for oxidation of the metal
surface. After oxidation, a coating of TiO2 paste containing 20-nm TiO2 nanoparticles
(EnB Korea) was applied using a 3M tape mask and the doctor blade method; the
sample was then heat treated at 480uC for 1 h in air. For measurements, the active area
size was 8 3 3 mm. The other woven electrode for the counter electrode was elec-
troplated for deposition of Pt. Electrodeposition was carried out using an aqueous
solution of 50 mM H2PtCl6 6H2O (Sigma Aldrich) at room temperature under 2 V
direct current (DC) power for 5 min and then calcined at 180uC for 1 h. After
calcination, Pt paste (Solaronix) was applied using the doctor blade method, followed
by heat treatment at 400uC for 30 min.
The two electrodes and spacer were attached using a Toyota sewing machine. After
sewing, the thickness of the devices is ranged from 0.7 mm to 0.8 mm. The prepared
cell after sewing process was immersed in 0.3 mM ethanol solution of cis-di(thio-
cyanato)- N,N’-bis(2,2’-bipyridyl-4-carboxylic acid-4’-tetrabutylammoniumcarbox-
ylate ruthenium(II) dye (N719 dye, Solaronix) for 20 hours to load dye on the
nanoporous TiO2 electrode at room temperature. An acetonitrile-based electrolyte
containing 50 mM tri-iodide (Solaronix SA, Iodolyte-AN50) was used for the elec-
trolyte. (See Supplementary Information, Figure S7 for experimental procedures)
Field-emission scanning electron microscopy (FE-SEM, Hitachi S4800) was per-
formed to observe the sample surface. The energy conversion performance of the
DSSCs was evaluated using a solar simulator (Abet Technologies, model Sun 2000,
1000 W Xe source, Keithley 2400 source meter) under 1.5-AM 1-Sun conditions,
calibrated by a KG-3 filter and NREL-certified reference cell without a mask. The
electrochemical characterizations were performed using a BioLogic SP-300 poten-
tiostat. The impedance spectra were acquired under open-circuit voltage, 1 Sun
conditions.
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Figure 4 | (a) Relationship between current density, specific power, and applied voltage according to the cloth used: Hanji (blue circle), cotton gauze
(black triangle), and silk gauze (red triangle). (b) Fourier-transform infrared (FTIR) spectra of Hanji, cotton gauze, and silk gauze before (black line)
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gauze under open-circuit conditions and 1-Sun, 1.5-AM illumination.
Table 1 | Photovoltaic performance of textile-based dye-sensitized
solar cells (DSSCs) prepared by sewing textile electrodes onto
Hanji, cotton gauze, and silk gauze
Spacer Voc (V) Jsc (mA) FF g(%)
Paper 0.69 17.20 0.37 4.36
Cotton 0.67 15.59 0.47 5.00
Silk 0.69 19.70 0.43 5.83
www.nature.com/scientificreports
SCIENTIFIC REPORTS | 4 : 5322 | DOI: 10.1038/srep05322 5
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Acknowledgments
This work was supported by the ‘‘New & Renewable Energy Core Technology Program’’ of
the Korea Institute of Energy Technology Evaluation and Planning (KETEP) grant funded
by the Ministry of Trade, Industry & Energy, Republic of Korea (No. 2011T100100678).
Author contributions
M. J. Y. and S. I. C. performed the textile based DSSC fabrication and wrote the manuscript.
S. H. S. and D. Y. L. contributed in Fig. 2 and Fig. 4 by characterization and feedback to the
fabrication process during study. All authors have reviewed the manuscript and agreed to
submission.
Additional information
Supplementary information accompanies this paper at http://www.nature.com/
scientificreports
Competing financial interests: The authors declare no competing financial interests.
How to cite this article: Yun, M.J., Cha, S.I., Seo, S.H. & Lee, D.Y. Highly Flexible
Dye-sensitized Solar Cells Produced by Sewing Textile Electrodes on Cloth. Sci. Rep. 4,
5322; DOI:10.1038/srep05322 (2014).
This work is licensed under a Creative Commons Attribution-NonCommercial-
ShareAlike4.0InternationalLicense.Theimages or other third party material in this
article are included in the article’s Creative Commons license, unless indicated
otherwise in the credit line; if the material is not included under the Creative
Commons license, users will need to obtain permission from the license holder
in order to reproduce the material. To view a copy of this license, visit http://
creativecommons.org/licenses/by-nc-sa/4.0/
www.nature.com/scientificreports
SCIENTIFIC REPORTS | 4 : 5322 | DOI: 10.1038/srep05322 6

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Srep05322

  • 1. Highly Flexible Dye-sensitized Solar Cells Produced by Sewing Textile Electrodes on Cloth Min Ju Yun, Seung I. Cha, Seon Hee Seo & Dong Y. Lee Nano Hybrid Technology Research Center, Creative and Fundamental Research Division, Korea Electrotechnology Research Institute. Textile forms of solar cells possess special advantages over other types of solar cells, including their light weight, high flexibility, and mechanical robustness. Recent demand for wearable devices has promoted interest in the development of high-efficiency textile-based solar cells for energy suppliers. However, the weaving process occurs under high-friction, high-tension conditions that are not conducive to coated solar-cell active layers or electrodes deposited on the wire or strings. Therefore, a new approach is needed for the development of textile-based solar cells suitable for woven fabrics for wide-range application. In this report, we present a highly flexible, efficient DSSC, fabricated by sewing textile-structured electrodes onto casual fabrics such as cotton, silk, and felt, or paper, thereby forming core integrated DSSC structures with high energy-conversion efficiency (,5.8%). The fabricated textile-based DSSC devices showed high flexibility and high performance under 4-mm radius of curvature over thousands of deformation cycles. Considering the vast number of textile types, our textile-based DSSC devices offer a huge range of applications, including transparent, stretchable, wearable devices. T he demand for lightweight, highly flexible or bendable solar cells has grown rapidly as the application of photovoltaic electric power generation has widened to encompass urban life in the form of building- integrated photovoltaics (BIPV) or electronics-integrated photovoltaics (EIPV)1–5 . Until several years ago, most of the research effort had focused on techniques involving flexible plastic substrates onto which transparent conductive oxide (TCO) films were deposited6–8 . However, TCO films can be easily fractured, resulting in a loss of conductivity due to their brittle nature. More recently, there has been a renewed interest in traditional material- based flexible solar cells, such as those associated with paper, string/fiber, and textiles9–26 . Textile forms of solar cells possess special advantages over other types of solar cells, including their light weight, high flexibility, and mechanical robustness. Recent demand for wearable devices has promoted interest in the development of high-efficiency textile-based solar cells for energy suppliers. Based on these demands, several studies have investigated the fabrication of textile-based solar cells, using organic solar cells or dye-sensitized solar cells18–24 . However, these research efforts were basically aimed at producing wires or strings of solar cells, ignoring their condition during the weaving process. Generally, the weaving process occurs under high-friction, high- tension conditions that are not conducive to coated solar-cell active layers or electrodes deposited on the wire or strings. Additionally, current research results can only produce very short (tens of centimeters) strings, far less than the length required for actual weaving or textile-based applications. Therefore, a new approach is needed for the development of textile-based solar cells suitable for woven fabrics for wide-range application. Dye-sensitized solar cells (DSSCs) have attracted much interest, due to their low fabrication costs, relatively high, efficiency especially under weak illumination, and ability to incorporate the dye color employed1–5 . In terms of textile solar cells, DSSCs offer several advantages, including spatial separation of the photoanode and counter electrode via electrolyte insertion, which minimizes the possibility of a short circuit. By combining this approach with the concept of core-integrated DSSCs for paper-based TCO-free DSSC9 , we propose a new prototype for textile-based solar cells using DSSCs. In this report, we present a highly flexible, efficient DSSC, fabricated by sewing textile-structured electrodes onto casual fabrics such as cotton, silk, and felt, or paper, thereby forming core integrated DSSC structures. By carefully fabricating the woven electrodes, the sewing process, one of characteristics of textiles, can be applied to the fabrication of solar cells as well as to the process of weaving using a loom. OPEN SUBJECT AREAS: SOLAR CELLS DESIGN, SYNTHESIS AND PROCESSING Received 14 March 2014 Accepted 27 May 2014 Published 24 June 2014 Correspondence and requests for materials should be addressed to S.I.C. (sicha@keri.re. kr) SCIENTIFIC REPORTS | 4 : 5322 | DOI: 10.1038/srep05322 1
  • 2. Results The process used to create the textile-based flexible solar cells to be sewn onto cloth consisted of the following steps: weaving each elec- trode by loom, depositing the photoanode material (i.e., TiO2) and the counter-electrode material (Pt), administering heat treatment, sewing to form the core-integrated DSSC device, and dye loading; these steps are shown in Fig. 1(a). The photoanode and counter- electrode textiles consisted of two parts: (1) a woven structure of stainless steel ribbon with periodic holes of 70 mm as the wefts and Ti wire of 100 mm as the wraps, and (2) the woven structure of glass fiber yarn as the wefts and Ti wire as the wraps (Fig. 1 (b) and (c)). The former (stainless steel/Ti wire) was used as the collector and as a substrate for the device; additionally, the later part provided mech- anical support and robustness for sewing to the other textiles, as shown in Fig. 1(c). It should be noted that the textile electrodes consisted of heat-resistant materials, such as metal and glass fibers. Therefore, each electrode can be heat treated after the deposition of the TiO2 porous film and Pt, which is an important factor for high- efficiency DSSCs. The photoanode and counter-electrode textiles were woven using a 351 twill structure, providing relatively high flexibility and a flat woven surface. (See Supporting Information Fig. S1 for schematics of twill structured textile) Combined with stainless steel ribbon as the wefts, the textile structure photoanodes had quite flat structures compared with those expected in woven structures, as shown in Fig. 1(c). Therefore, the conventional doctor-blade process or screen-printing process was applied to deposit the electrode materi- als. The counter electrodes were prepared using two-step deposition of Pt. First, the Pt was deposited onto the counter-electrode textile using an electroplating method, and this was followed by the depos- ition of Pt-containing paste. The structure was then heat treated. Using this two-step deposition process, Pt thin flakes resembling flowers can be prepared (see Supporting Information Fig. S2 and S3 for images of the counter electrode and photoanode deposited). The prepared textile electrodes were assembled by sewing, placing each electrode on either side of the cloth, followed by electrolyte infiltration, as shown Fig. 1(d). The textile-structured electrodes were attached to the cloth (in this case, paper) using a sewing machine. As a result, core-integrated forms of DSSCs were fabricated; Figs. 1(e) and 1(f) show a cross-sectional schematics and a plane view, respect- ively. In the cross-sectional schematics, the DSSC prepared by the sewing process consisted of three layers, similar to conventional DSSCs; however, no TCO films or glass plates were employed, which is a particular feature of core-integrated DSSCs. The photovoltaic performance of the textile-based DSSC sewn on Hanji, a Korean traditional paper, is shown in Fig. 2(a). The rela- tionship between the current density and applied voltage shows a high short-circuit current (.17 mA cm22 ). However, the fill factor was low at only 0.37, which is the main limitation for energy con- version efficiency. The low fill factor can come from the low porosity of Hanji infiltrated with electrolyte and the evaporation of electrolyte on the surface of electrode due to lack of sealing during measure- Figure 1 | (a) Schematic illustration of the fabrication concept for textile-based dye-sensitized solar cells (DSSCs) made by sewing textile electrodes onto cloth or paper. (b) Photograph of the loom (inset) used to weave the textile electrodes, and (c) a woven electrode. The inset shows an image of the stainless steel ribbon with periodic holes. (d) Photograph of the sewing process to attach the woven electrodes to Hanji, a Korean traditional paper. (e) Schematic illustration showing the cross-sectional structure of the textile-based DSSC prepared by sewing and (f) photograph of a core-integrated textile-based DSSC fabricated by sewing textile electrodes onto Hanji. www.nature.com/scientificreports SCIENTIFIC REPORTS | 4 : 5322 | DOI: 10.1038/srep05322 2
  • 3. ment. The overall efficiency under 1-Sun illumination was ,4.3% despite the high current density, with 5.3% corresponding to the maximum conversion efficiency observed. The textile-based DSSC fabricated by sewing exhibited consid- erable bending ability, as shown in Fig. 2(b), where the prepared cell was wound around a rod of 0.4-cm radius of curvature. The cell underwent thousands of bending cycles of 90u. The photovoltaic performance under bending conditions was maintained at 80% of the flat cell value with bending to a 10-cm radius of curvature and 30% with a 4-mm radius of curvature, as shown in Fig. 2(c). Additionally, the photovoltaic performance remained over 70% of the initial value even after 1000 bending cycles over a 1-cm radius of curvature, as shown in Fig. 2(d). (See Supplementary Information Figure S5 and S6 for status of cell after repeated bending by pressing plunge). The energy conversion efficiency of the textile-based DSSC sewn on cloth was affected by several factors; some of these factors, to the best of our knowledge, have yet to be considered for textile-based DSSCs. One such factor is the contact between the metal wires in the woven electrodes. If the contact between the metal wrap and weft is lost, then an electrical open circuit forms within the cell that acts as a recombination site during operation. Under these conditions, the energy conversion efficiency can be degraded considerably by loss of contact between the woven electrodes. It is not totally clear when the contact becomes lost; however, tension maintained during the weaving process, as well as the pattern of the weave, could have an effect on the electrical contact of the woven electrode. Another factor that may affect photovoltaic performance of the textile-based DSSC is the cloth itself, which contains the electro- lyte and plays the role of a spacer to prevent electrical short circuits from forming between the electrodes. Hanji has very few pores for diffusion within the electrolyte, as shown in Fig. 3(a), which induces a low fill factor during photovoltaic operations. To investigate the effect of cloth on photovoltaic per- formance, other types of cloth including cotton and silk (both in the form of gauze) were used for the textile-based DSSC as a spacer. The woven electrodes were attached to either side of the cotton and silk gauze using a sewing machine, as shown in Fig. 3(b); note that a mechanically robust core-integrated DSSC can be fabricated using these cloth types. This is particularly useful and meaningful with respect to the application of wearable devices for energy supply. The microscopic structures of the cotton and silk gauze are shown in Figs. 3(c) and 3(d). Compared with Hanji, the gauze offers more space for electrolyte filling and diffusion. Figure 2 | (a) Relationship between current density and applied voltage (red circle) and specific power and applied voltage (blue line) of a textile-based DSSC prepared by sewing the woven electrode onto Hanji; measurements were obtained under 1-Sun, 1.5-AM conditions. (b) Photographs showing a textile-based DSSC wrapped around a rod with a 4-mm radius of curvature under cyclic bending deformation (inset). (c) Relative energy conversion efficiency of the flat-state textile-based DSSC and (d) relative efficiency after cyclical bending of 1000 and 2000 times. www.nature.com/scientificreports SCIENTIFIC REPORTS | 4 : 5322 | DOI: 10.1038/srep05322 3
  • 4. The open area of cotton gauze is measured as about 48%, while that of silk gauze is about 47%. The effect of cloth type on photovoltaic performance indicates that the inserted cloth considerably affects energy conversion efficiency and the relationship between current density and applied voltage, as shown in Fig. 4(a). High current densities for the textile electrodes can be expected as a result of light reflection from the metal and enhanced photon harvesting25,26 . The woven metal ribbon can reflect over 10% of incident light when it is oxidized. (See Figure S4 for light reflection from metal ribbon) It is also shown in wire-shaped solar cell that the light concentration by focusing light or luminescent concentrator could enhance energy conversion efficiency. In the case of cotton gauze, the current density decreased slightly, whereas the fill factor increased; hence, the energy conversion efficiency improved to 5%. When silk gauze is inserted between textile electro- des, the energy conversion efficiency was enhanced to 5.8%. For the champion cell, the efficiency is measured as nearly 7%; in this case, the current density increased to nearly 20 mA cm22 , which is a high value, even for conventional sandwich-structured DSSCs, as sum- marized in Table 1. The enhancement observed with cotton gauze compared with Hanji can be explained in terms of the ease of dif- fusion in the electrolyte due to the large free space; the chemical status of the cotton and paper did not change significantly within the electrolyte under Fourier-transform infrared (FTIR) spectro- scopy analysis, as shown in Fig. 3(b). However, in the case of the silk gauze, the electrolyte changed the chemical status of the yarn, as shown in Fig. 3(b), where absorption near 3200–3500 and 1600 cm21 was observed after soaking the silk in the electrolyte for one day. The absorption that occurred was attributed to the forma- tion of hydroxyl groups, amide groups, and aromatic groups, which exist in protein molecules. The electrolyte and spacer, chemically modified in the silk gauze, enhanced the energy conversion effi- ciency. Thus, the potential exists for further improvement beyond the results presented here. Discussion However, questions remain regarding the determination of energy conversion efficiency in these devices. High current densities for the textile electrodes can be expected as a result of light reflection from the metal and enhanced photon harvesting. For electrochemical impedance spectroscopy (EIS) results under open-circuit conditions, as shown in Figs. 3(c) and 3(d), the cloth type appeared to affect the resistance during electrode reactions. Nyquist plots indicated that this effect was smallest in cotton gauze and highest in silk gauze in short circuit condition. The Bode plots showed that the resistance was related to the reaction near the 10–100 Hz range, which may correspond to recombination in the photoanode. In this case, the recombination rate was related to the ionic concentration near the photoanode, which can be affected by diffusion and the initial ionic concentration. To find the optimum operating conditions for textile- based solar cells, further research on the cloth material is needed. It should be noted that in this study, we used conventional commer- cially available materials, including TiO2 nanoparticle paste, com- mon electrolytes, and a Pt counter electrode. This suggests the possibility for considerable improvement in photovoltaic perform- ance of these structured DSSCs with suitable material optimization. The woven pattern is another critical factor that may allow further improvement in performance. As mentioned earlier, the woven structure and the applied tension in the wraps and wefts determine the electrical contact within the woven electrodes. By considering various forms of textiles developed, semi-transparent electrodes or stretchable electrodes could be fabricated by proper selection of the weave pattern. In this sense, the preparation of DSSCs by sewing textile electrodes on various types of cloth provides vast potential for possible application. In summary, highly bendable, mechanically robust DSSCs with high energy-conversion efficiency (,5.8%) can be fabricated by sew- ing textile electrodes prepared by loom weaving onto various types of cloth. The fabricated textile-based DSSC devices showed high flex- ibility and high performance under 4-mm radius of curvature over thousands of deformation cycles. Considering the vast number of textile types, our textile-based DSSC devices offer a huge range of applications, including transparent, stretchable, wearable devices. Mothods The etched mesh of 304 stainless steel (Tech-Etch MicroEtchH) and 50-mm-diameter Ti wire (iNexus) were used as the weft, and 100-mm-diameter Ti wire (iNexus) was Figure 3 | (a) Scanning electron microscopy (SEM) image of the Hanji surface. (b) Photograph of the process of sewing woven electrodes onto silk gauze using a sewing machine. SEM images of the surface of (c) cotton gauze and (d) silk gauze. Inset shows prepared textile-based DSSCs using (c) cotton gauze and (d) silk gauze. www.nature.com/scientificreports SCIENTIFIC REPORTS | 4 : 5322 | DOI: 10.1038/srep05322 4
  • 5. used as the warp of the woven electrode. The sewn part of the electrode, a glass fiber (D450 1/2, Hyunmin Fiber), was used as weft. A Daesung Hi-tech loom (Daesung Hi- Tech Co., Ltd., Korea) was used for weaving. The woven electrode was rinsed with acetone, ethanol, and deionized water by sonication and dried with nitrogen gas. After cleaning, the woven textile for the working electrode was heat treated at 480uC for 1 h in air for oxidation of the metal surface. After oxidation, a coating of TiO2 paste containing 20-nm TiO2 nanoparticles (EnB Korea) was applied using a 3M tape mask and the doctor blade method; the sample was then heat treated at 480uC for 1 h in air. For measurements, the active area size was 8 3 3 mm. The other woven electrode for the counter electrode was elec- troplated for deposition of Pt. Electrodeposition was carried out using an aqueous solution of 50 mM H2PtCl6 6H2O (Sigma Aldrich) at room temperature under 2 V direct current (DC) power for 5 min and then calcined at 180uC for 1 h. After calcination, Pt paste (Solaronix) was applied using the doctor blade method, followed by heat treatment at 400uC for 30 min. The two electrodes and spacer were attached using a Toyota sewing machine. After sewing, the thickness of the devices is ranged from 0.7 mm to 0.8 mm. The prepared cell after sewing process was immersed in 0.3 mM ethanol solution of cis-di(thio- cyanato)- N,N’-bis(2,2’-bipyridyl-4-carboxylic acid-4’-tetrabutylammoniumcarbox- ylate ruthenium(II) dye (N719 dye, Solaronix) for 20 hours to load dye on the nanoporous TiO2 electrode at room temperature. An acetonitrile-based electrolyte containing 50 mM tri-iodide (Solaronix SA, Iodolyte-AN50) was used for the elec- trolyte. (See Supplementary Information, Figure S7 for experimental procedures) Field-emission scanning electron microscopy (FE-SEM, Hitachi S4800) was per- formed to observe the sample surface. The energy conversion performance of the DSSCs was evaluated using a solar simulator (Abet Technologies, model Sun 2000, 1000 W Xe source, Keithley 2400 source meter) under 1.5-AM 1-Sun conditions, calibrated by a KG-3 filter and NREL-certified reference cell without a mask. The electrochemical characterizations were performed using a BioLogic SP-300 poten- tiostat. The impedance spectra were acquired under open-circuit voltage, 1 Sun conditions. 1. O’Regan, B. & Gra¨tzel, M. A low-cost, high-efficiency solar cell based on dye- sensitized colloidal TiO2 films. Nature 353, 737–740 (1991). 2. Bach, U. et al. Solid-state dye-sensitized mesoporous TiO2 solar cells with high photon-to-electron conversion efficiencies. Nature 395, 583–585 (1998). 3. Snaith, H. J. & Schmidt-Mende, L. Advances in liquid-electrolyte and solid-state dye-sensitized solar cells. Adv Mater 19, 3187–3200 (2007). 4. Lenzmann, F. & Kroon, J. Recent advances in dye-sensitized solar cells. Advances in OptoElectronics 2007, article ID 65073 , 1–10 (2007). 5. Ito, S. et al. High-efficiency (7.2%) flexible dye-sensitized solar cells with Ti-metal substrate for nanocrystalline-TiO2 photoanode. Chem. Comm. 4004–4006 (2006). 6. Uchida, S., Tomiha, M., Takizawa, H. & Kawaraya, M. Flexible dye-sensitized solar cells by 28 GHz microwave irradiation. J. Photochem. Photobiol. A. 164, 93–96 (2004). 7. Lindstro¨m, H. et al. A new method for manufacturing nanostructured electrodes on plastic substrates. Nano Letters 1, 97–100 (2001). 8. Zhang, D., Yoshida, T., Oekermann, T., Furuta, K. & Minoura, H. Room- Temperature Synthesis of Porous Nanoparticulate TiO2 Films for Flexible Dye- Sensitized Solar Cells. Adv. Funct. Mater. 16, 1228–1234 (2006). 9. Cha, S. I. et al. Dye-sensitized solar cells on glass paper: TCO-free highly bendable dye-sensitized solar cells inspired by the traditional Korean door structure. Energy Environ. Sci. 5, 6071–6075 (2012). Figure 4 | (a) Relationship between current density, specific power, and applied voltage according to the cloth used: Hanji (blue circle), cotton gauze (black triangle), and silk gauze (red triangle). (b) Fourier-transform infrared (FTIR) spectra of Hanji, cotton gauze, and silk gauze before (black line) and after (red line) soaking in the electrolyte for one day. (c) Nyquist plot and (d) Bode plot of textile-based DSSCs using Hanji, cotton gauze, and silk gauze under open-circuit conditions and 1-Sun, 1.5-AM illumination. Table 1 | Photovoltaic performance of textile-based dye-sensitized solar cells (DSSCs) prepared by sewing textile electrodes onto Hanji, cotton gauze, and silk gauze Spacer Voc (V) Jsc (mA) FF g(%) Paper 0.69 17.20 0.37 4.36 Cotton 0.67 15.59 0.47 5.00 Silk 0.69 19.70 0.43 5.83 www.nature.com/scientificreports SCIENTIFIC REPORTS | 4 : 5322 | DOI: 10.1038/srep05322 5
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