# Preparation of a Textile-Based Dye-Sensitized Solar Cell

Authors: Klaus Opwis; Jochen Stefan Gutmann; Ana Rosa Lagunas Alonso; Maria Jesus Rodriguez Henche; Mikel Ezquer Mayo; Fanny Breuil; Enrico Leonardi; Luca Sorbello
Journal: International Journal of Photoenergy
 (2016)

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## Abstract

Solar energy conversion is an object of continuous research, focusing on improving the energy efficiency as well as the structure of photovoltaic cells. With efficiencies continuously increasing, state-of-the-art PV cells offer a good solution to harvest solar energy. However, they are still lacking the flexibility and conformability to be integrated into common objects or clothing. Moreover, many sun-exposed surface areas are textile-based such as garments, tents, truck coverings, boat sails, and home or outdoor textiles. Here, we present a new textile-based dye-sensitized solar cell (DSC) which takes advantage from the properties inherent to fabrics: flexibility, low weight, and mechanical robustness. Due to the necessary thermostability during manufacturing, our DSC design is based on heat-resistant glass-fiber fabrics. After applying all needed layers, the overall structure was covered by a transparent and simultaneously conductive protective film. The light and still flexible large-area devices (up to 6 cm2 per individual unit) are working with efficiencies up to 1.8% at 1/5 of the sun. Stability tests assure no loss of photovoltaic activity over a period of at least seven weeks. Therefore, our technology has paved the way for a new generation of flexible photovoltaic devices, which can be used for the generation of power in the mentioned applications as well as in modern textile architecture.


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## Body

## 1. Introduction

The conversion of sunlight into electric energy is the most environmentally friendly and nonhazardous alternative to fossil and fissionable resources. Along with the aim to increase the efficiency, former and present R&D focuses on the optimization of photovoltaic (PV) structures and the development of new photoactive materials.Currently, most photovoltaic devices are still fabricated for large-scale electric power generation either in centralized solar parks or as building integrated photovoltaics (BIPV). For these applications, rigid, weather-proof, and long-term stable devices are desired. The common material of choice is monocrystalline or multicrystalline silicon, which have high average energy-conversion efficiencies in the range of 18 to 26 percent. Besides silicon, other semiconducting alternative materials have been developed and tested within the previous decades, which differ strongly in terms of production costs on the one hand and the efficiency on the other hand. Well-described types are III–V (GaAs, InP, and GaInP), chalcogenide (CIGS, CdTe, and CZTS), and multijunction cells with up to five different p-n-junctions. Furthermore, in recent years organic, dye-sensitized, and perovskite solar cells have proven their large potential within the present and future photovoltaic market [1–3]. In particular, the dye-sensitized solar cell (DSC), which was introduced by O’Regan and Grätzel in the early 1990s, seems to be the most promising candidate for an enduring launch into several commercial products. Compared to other types of solar cells, DSC are much less sensitive to the angle of incidence of radiation, shadowing, and ambient temperature changes. They perform over the most extensive range of light conditions enabling the energy production even in the early morning, in the late afternoon, or on cloudy days. They combine high energy-conversion efficiencies and sufficient robustness towards environmental impact and, therefore, sufficient life-time. The base materials are comparatively inexpensive. In addition, the layer thickness of the used direct semiconductors can be reduced on micron or even nanoscale. This allows the use of cost-effective thin-layer and/or printing technologies and the integration of lightweight and flexible DSC structures into countless commercial products of our day-to-day life [3–8].Besides plastics and film applications [3, 9–11], which have already arrived to a commercial level, photovoltaic textiles have attracted increasing attention in recent years since they are often exposed directly to sunlight and represent ideal substrates for the conversion of solar energy into electricity. We refer to outdoor textiles such as blinds, tents, tarpaulins, sails, and last but not least the important increasing market of textile architecture, which has an outstanding potential to form the basis for flexible, lightweight, and robust PV structures.As a result, a large effort has been put into research activities focusing on innovative concepts for textile-based DSC. The major challenge is to combine properties and demands of the photovoltaic concept (and processing) with inherent properties of fibrous substrates (and typical textile processing).In literature, several successful DSC designs on fibrous materials such as paper, wires, fibers, strings, or textiles are listed [12–23]. However, in most cases these approaches are aimed at the production of single fibers or wires with photovoltaic activity, concealing the need of additional sensitive processing steps afterwards, for example, weaving, which could impair the cell performance dramatically. Furthermore, the length of those one-dimensional cells is limited to a certain extent. This impedes the (textile) processing additionally. On contrary to the most common single-fiber approaches, our investigations are focused on already woven textile structures taking advantage from the properties inherent to fabrics: flexibility, low weight, and mechanical robustness. We report on the preparation of a two-dimensional textile-based dye-sensitized solar cell and the used deposition techniques of all further needed conductive, photoactive, and protective layers to achieve flexible, light, mechanically strong, and comparatively large-area devices.


## 2. Experimental

### 2.1. Production of Textile-Based DSC

A commercial high flexible glass-fiber fabric (Interglas, Germany) with the following characteristics was used as basic substrate for the deposition of the DSC structure: mass per unit area 107 g/m2, thickness 0.09 mm, tensile strength (warp) 250 N/cm, tensile strength (weft) 235 N/cm, thermostability (short-time) 600°C, and thermostability (permanent) 500°C. Afterwards the glass-fiber fabric was covered with a thin polyamide film by roll-to-roll procedure followed by electron beam deposition or sputtering of a titanium layer. Titanium dioxide DSL-18NR-AO (Dyesol) was deposited by screen-printing. The cured material (500°C for 5 min) was sensitized by various ruthenium-based dyestuffs. As a transparent counter electrode, a commercial PEN + ITO film was selected (CPFilms). The film has a thickness of 125 μm with a transparency of 75% at 550 nm. The sheet resistance amounts to 15 Ω/sq. On the ITO side of the film, the catalyst layer was deposited by the chemical reduction of H2PtCl6 at room temperature resulting in homogeneous Pt clusters on the substrate surface. After the adding of the electrolyte (EL-HSE, Dyesol), the textile part (glass-fiber fabric + PA layer + Ti + dye-sensitized TiO2) was covered with the counter electrode part (PEN + ITO + Pt) yielding the flexible textile-based DSC. The overall structure was sealed by the use of special epoxy and thermoplastic foils (DuPont, Dyesol) to achieve the final textile-based DSC.


### 2.2. Analytics/Characterization

After the Ti deposition, the samples were characterized by means of optical microscopy and mechanical profilometry. Surface resistances of the electrodes were measured via 4-point probe.The electrical characterization of the samples was performed at Standard Test Conditions (STC) in accordance with the standard IEC:60904-1-Ed.2:2006, under irradiation with a steady-state class A solar simulator according to IEC:60904-9-Ed.2:2007. TheIV-curves at STC (1000 W/m2, 25°C, AM 1.5G spectrum) and at various values of irradiance were measured. During the measurement, the samples were kept at a constant temperature using a vacuum chuck.The spectral mismatch, caused by the deviation of the simulator spectrum from the standard solar spectrum AM1.5G (IEC:60904-3-Ed.2:2008) in combination with the different spectral responses of reference cell and device under test, was calculated according to the standard IEC:60904-7-Ed.3:2008 and corrected consequently.For the spectral mismatch correction, the spectral distribution of the solar simulator was measured with a calibrated spectroradiometer, and the spectral response of the solar cell was measured with a filter monochromator according to IEC:60904-8-Ed.2:1998.In order to study the influence of the temperature on the electrical behavior of the cells, CENER carried outIV-curve measurements at different temperatures, maintaining the irradiance value constant at 830 W/m2.OutdoorIV-curve measurements were carried out on a sunny day, placing the PV cells on a solar tracker perfectly sun-oriented. The global irradiance was measured using a calibrated pyranometer, and the cell temperature was monitored with a calibrated thermocouple.The spectral response measurements were performed using a filter monochromator based system according to the procedure established in the IEC:60904-8:2008 standard. The frequency of the chopper was around 4 Hz, and the bias light used was a white light with an intensity value around 100 W/m2. For complementary information, the measurement of the spectral reflectance of the cells was carried out using a calibrated spectroradiometer and an integrating sphere.In the first part of the stability study, textile-based DSC were irradiated with a constant intensity of 830 W/m2, and the temperature of the cell was maintained almost constantly between 30°C and 31°C. In order to study the stability/durability of the electrical behavior of the cells over time,IV-curves (irradiance: 830 W/m2; temperature: 25°C) of the DSC cells were measured in 3 consecutive days and 45 days after the first measurement. The PV cells were stored in dark conditions between measurements. In addition, the open circuit voltage, the current density, and the fill factor of the DSC samples were measured over a period of 7 weeks.


## 2.1. Production of Textile-Based DSC

A commercial high flexible glass-fiber fabric (Interglas, Germany) with the following characteristics was used as basic substrate for the deposition of the DSC structure: mass per unit area 107 g/m2, thickness 0.09 mm, tensile strength (warp) 250 N/cm, tensile strength (weft) 235 N/cm, thermostability (short-time) 600°C, and thermostability (permanent) 500°C. Afterwards the glass-fiber fabric was covered with a thin polyamide film by roll-to-roll procedure followed by electron beam deposition or sputtering of a titanium layer. Titanium dioxide DSL-18NR-AO (Dyesol) was deposited by screen-printing. The cured material (500°C for 5 min) was sensitized by various ruthenium-based dyestuffs. As a transparent counter electrode, a commercial PEN + ITO film was selected (CPFilms). The film has a thickness of 125 μm with a transparency of 75% at 550 nm. The sheet resistance amounts to 15 Ω/sq. On the ITO side of the film, the catalyst layer was deposited by the chemical reduction of H2PtCl6 at room temperature resulting in homogeneous Pt clusters on the substrate surface. After the adding of the electrolyte (EL-HSE, Dyesol), the textile part (glass-fiber fabric + PA layer + Ti + dye-sensitized TiO2) was covered with the counter electrode part (PEN + ITO + Pt) yielding the flexible textile-based DSC. The overall structure was sealed by the use of special epoxy and thermoplastic foils (DuPont, Dyesol) to achieve the final textile-based DSC.


## 2.2. Analytics/Characterization

After the Ti deposition, the samples were characterized by means of optical microscopy and mechanical profilometry. Surface resistances of the electrodes were measured via 4-point probe.The electrical characterization of the samples was performed at Standard Test Conditions (STC) in accordance with the standard IEC:60904-1-Ed.2:2006, under irradiation with a steady-state class A solar simulator according to IEC:60904-9-Ed.2:2007. TheIV-curves at STC (1000 W/m2, 25°C, AM 1.5G spectrum) and at various values of irradiance were measured. During the measurement, the samples were kept at a constant temperature using a vacuum chuck.The spectral mismatch, caused by the deviation of the simulator spectrum from the standard solar spectrum AM1.5G (IEC:60904-3-Ed.2:2008) in combination with the different spectral responses of reference cell and device under test, was calculated according to the standard IEC:60904-7-Ed.3:2008 and corrected consequently.For the spectral mismatch correction, the spectral distribution of the solar simulator was measured with a calibrated spectroradiometer, and the spectral response of the solar cell was measured with a filter monochromator according to IEC:60904-8-Ed.2:1998.In order to study the influence of the temperature on the electrical behavior of the cells, CENER carried outIV-curve measurements at different temperatures, maintaining the irradiance value constant at 830 W/m2.OutdoorIV-curve measurements were carried out on a sunny day, placing the PV cells on a solar tracker perfectly sun-oriented. The global irradiance was measured using a calibrated pyranometer, and the cell temperature was monitored with a calibrated thermocouple.The spectral response measurements were performed using a filter monochromator based system according to the procedure established in the IEC:60904-8:2008 standard. The frequency of the chopper was around 4 Hz, and the bias light used was a white light with an intensity value around 100 W/m2. For complementary information, the measurement of the spectral reflectance of the cells was carried out using a calibrated spectroradiometer and an integrating sphere.In the first part of the stability study, textile-based DSC were irradiated with a constant intensity of 830 W/m2, and the temperature of the cell was maintained almost constantly between 30°C and 31°C. In order to study the stability/durability of the electrical behavior of the cells over time,IV-curves (irradiance: 830 W/m2; temperature: 25°C) of the DSC cells were measured in 3 consecutive days and 45 days after the first measurement. The PV cells were stored in dark conditions between measurements. In addition, the open circuit voltage, the current density, and the fill factor of the DSC samples were measured over a period of 7 weeks.


## 3. Results and Discussion

### 3.1. Structure of Textile-Based DSC

In accordance to typical DSC, our textile-based DSC structure is a composite of several materials. The layer-by-layer structure (schematically shown in Table1) consists of the textile substrate (1), which serves as a flexible, lightweight but mechanically strong support for all the following layers. Each layer shows material-specific characteristics and must fulfill DSC requirements in terms of thermostability, roughness, adhesion, conductivity, photovoltaic activity, transparency, barrier properties, and flexibility. In addition, the overall structure must be liquid-proof to avoid leakage of the electrolyte.Table 1
Textile-based DSC device structure and essential requirements of the layers.
Sun light
8
Cover
Special epoxy and thermoplastic foils
Transparency and impermeability towards the electrolyte
7
Upper electrode
Thin PEN/ITO film
Conductivity and transparency
6
Catalyst
Pt
Good adhesion
5
Electrolyte
I
-/I
3
-
4
Active layer
T
i
O
2 and dyestuff
3
Bottom electrode
Ti
Conductivity, thermoresistance, high flexibility, and good adhesion
2
Smoothing layer
Polyamide coating
Thermoresistance, impermeability towards the electrolyte, high flexibility, and good adhesion
1
Substrate
Glass-fiber fabric
Thermoresistance, high flexibility, being light, and mechanical strength
Layer
Material used
Properties/requirementsTo achieve a flat, thermostable, and liquid-proof substrate, the glass-fiber fabric was covered with a thin polyamide film (2) by a simple roll-to-roll procedure (Figure1).Figure 1
Roll-to-roll technique used (a) to cover the glass-fiber fabric with a polyamide film (b).
(a)
(b)On this improved material, a titanium layer (3) was deposited to turn the fiber glass into a conductive substrate, which can act as the bottom electrode. The Ti films were grown by two different deposition techniques: electron beam (eBeam) and sputtering. After the Ti deposition, the samples were characterized by means of optical microscopy and mechanical profilometry. Exemplarily, Figure2 shows images of the materials after eBeam deposition of Ti. Independently from the Ti deposition technique used, the sample surfaces maintained the substrate topography. Moreover, both technologies lead to quite homogeneous films with good adherence to the substrate. Surface resistances lower than 3 Ω/sq were found indicating sufficient conductivity.Figure 2
Optical characterization of Ti layers deposited on the polyamide covered glass-fiber fabric by eBeam.In the following step, titanium dioxide DSL-18NR-AO was deposited by screen-printing and cured for 5 minutes at 500°C to achieve a nanoporous structure of the titania, which allows a high uptake of various ruthenium-based dyestuffs. The dye-sensitized titania forms the photoactive layer (4) that absorbs the sun light yielding electric charges. This short-term but high-temperature curing step clarifies the necessity of all previous layers to be thermostable in the range of 500°C for a certain time. In the field of conventional textile materials, only glass-fiber fabrics fulfill this essential requirement.A commercial PEN-ITO film (7) was selected as a transparent counter electrode. The film has a thickness of 125μm with a transparency of 75% at 550 nm. The sheet resistance of 15 Ω/sq is sufficient.On the ITO side of the film, the catalyst layer (6) was deposited by the chemical reduction of H2PtCl6 at room temperature resulting in homogeneous Pt clusters on the substrate surface. After adding the electrolyte (5), the textile part (glass-fiber fabric + PA layer + Ti + dye-sensitized TiO2) was covered with the counter electrode part (PEN + ITO + Pt) yielding the flexible textile-based DSC. The overall structure was sealed by a special epoxy and thermoplastic foils (8) to protect the structure from environmental conditions. Our textile-based DSC device with the size of nearly 6 cm2 is shown in Figure 3(a).Figure 3
Final textile-based DSC (a) and 4-point configuration used in theIV-curve measurement (b).
(a)
(b)


### 3.2. Photovoltaic Performance of Textile-Based DSC

#### 3.2.1.IV-Curve Measurement under Standard and Nonstandard Test Conditions

In order to characterize the textile-based DSC electrically in terms of its photovoltaic performance, we started withIV-curve measurement under Standard Test Conditions (STC) using the configuration shown in Figure 3(b) providing the results summarized in Figure 4. The DSC devices show a significant photovoltaic activity with an average efficiency of nearly 1.0%.Figure 4
IV-curves of two samples of textile-based DSC under STC.Solar cells normally present a different electrical behavior depending on the irradiance level, and the photovoltaic efficiency of the cells can change significantly depending on the irradiance value. As a consequence of this and in addition to the STC measurements, we measured theIV-curve of the DSC-1 cell at different irradiance values, maintaining the AM1.5G spectrum and the 25°C temperature. As an example, in Figure 5, theIV-curves obtained for 3 representative levels of irradiance (1000 W/m2, 500 W/m2, and 200 W/m2) are shown to have joined to the electrical parameters extracted from them. The representedIV-curves were obtained by applying the correction value due to the spectral mismatch factor.Figure 5
IV-curves at 3 different irradiance levels for DSC-1.As can be seen in Figure5, the electrical behavior of the cell presents a clear dependency with the irradiance level. The efficiency of the cell improves significantly when the irradiance decreases, mainly due to the significant increase of the Fill Factor (FF) at low irradiance levels.Figure6 shows the variation of the main electrical parameters (V
oc, I
sc, FF, and efficiency) as a function of the irradiance level. All the represented values are extracted from theIV-curves measured at different irradiances, taking into account the spectral mismatch factor.Figure 6
Variation of the main electrical parameters of DSC-1 with the irradiance level.The value of theI
sc increases linearly with the irradiance level. This fact is completely reasonable because, normally, the I
sc value is directly proportional to the irradiance value. In addition, V
oc increases with the irradiance level due to the increasing electron injection into titania at higher illumination, which pushes the Fermi level up.The most important data, extracted from these measurements, is the large improvement of the fill factor when the irradiance value decreases. Apparently, the dependency of the FF with the irradiance level follows a linear tendency. The slope of said tendency is so considerable that, as an example, the value of the FF at 200 W/m2 is practically double compared to the value at 1000 W/m2.Finally, despite theI
sc and V
oc tendency, the electrical efficiency of the cell improves notably when irradiance decreases, due to the significant improvement of the FF at low irradiance levels. Under 1/5 of sun conditions, the efficiency increases to a remarkable 1.8%. As demonstrated here, DSC devices are known to perform well under difficult light conditions such as low illumination or diffuse/indirect illumination, under which 1st- and 2nd-generation PV technologies tend to suffer a loss of performance.


#### 3.2.2. Temperature Coefficients of the Main Electrical Parameters

In order to study the influence of the temperature on the electrical behavior of the textile-based DSC, we carried out someIV-curve measurements at different temperatures, maintaining the irradiance value constant at 830 W/m2. Figure 7 shows theIV-curves measured at 6 different temperatures at constant irradiance level (830 W/m2) for DSC-1.Figure 7
DSC-1IV-curves measured at 6 different temperatures at an irradiance value of 830 W/m2.As presented in Figure7,IV-curve shape changes significantly with temperature variation. Figure 8 shows the variation of I
sc, V
oc, FF, and P
max
⁡ with the cell temperature for the case of the DSC-1. The keys of the figure show the value of the temperature coefficients for I
sc, V
oc, and P
max
⁡ parameters.Figure 8
Variation of the main electrical parameters of DSC-1 with the temperature, at an irradiance value of 830 W/m2.As can be seen in Figure8, I
sc and V
oc parameters show a negative variation with temperature, meaning that their value decreases when temperature increases. Nevertheless, the most important information extracted from this data is the improvement of the FF parameter when temperature increases. Simultaneously as I
sc and V
oc decrease, the maximum power (P
max
⁡) remains practically constant with the temperature variation. This represents a very important advantage for these types of cells in comparison to other PV technologies as crystalline silicon based solar cells, which suffer significant P
max
⁡ reduction with increasing temperature.


#### 3.2.3. OutdoorIV-Curve Measurement

As a complementary study of the measurements carried out in the solar simulator,IV-curve measurements were also performed outdoors to test the electrical behavior of the cell under real conditions. The main advantage of the outdoor measurement is that the data does not require any spectral mismatch correction, but the disadvantage is the inability to control the irradiance level. Both irradiance and cell temperature were also measured during the test.TheIV-curves were measured on a sunny day by placing the PV cells on a solar tracker, perfectly adjusted to the sun. The global irradiance during theIV-curve measurements varied between 1010 W/m2 and 1020 W/m2, and the cell temperature fluctuated between 37°C and 39°C. The measurements obtained for both DSC samples are shown in Figure 9. As shown from Figure 9, the results of the outdoor measurements are quite similar to the results obtained in the solar simulator.Figure 9
OutdoorIV-curves of DSC-1 and DSC-2 (38°C, 1015 W/m2).


#### 3.2.4. Spectral Response and Global Reflectance Measurement

The measurement of the spectral response of dye-sensitized solar cells is not a trivial matter. The time response of these cells is quite slow compared to other technologies and, as a consequence, very low frequencies must be used in the chopping process of the light during the spectral response measurement. Besides this fact, the spectral response of the cells presents a clear dependence with the bias light intensity used to polarize the cell during the measurement.Figure10 shows the relative External Quantum Efficiency (EQE) measured for both cells (DSC-1 and DSC-2). The global reflectance as a function of the wavelength is also included in the graph. Finally, as a comparison, the EQE measurement of a similar dye-sensitized cell (deposited on glass) is also included.Figure 10
Relative External Quantum Efficiency (EQE) and global reflectance of DSC-1 and DSC-2 and EQE measurement of a reference dye-sensitized cell.As can be seen in Figure10, the relative spectral response of both cells (DSC-1 and DSC-2) is quite similar. The photogeneration wavelength range of these cells goes from 400 nm to 750 nm and shows a maximum around 550 nm. Comparing these results with the EQE values extracted from the bibliography for similar dye-sensitized solar cells (deposited on glass), it can be said that the spectral response is quite similar, with a slight worse performance, especially in the short wavelength range (<550 nm).


#### 3.2.5. Stability Study

In order to complete the electrical characterization of the textile-based DSC, a study of the stability of their electrical response with the increase of the exposition time was carried out. In the first part of this stability study, DSC-2 was irradiated with a constant intensity of 830 W/m2, and the temperature of the cell was maintained practically constant between 30°C and 31°C. DifferentIV-curves were measured during the exposition time. Figure 11 shows the evolution of the electrical parameters (I
sc, V
oc, FF, and P
max
⁡) as a function of the exposure time.Figure 11
Evolution of the main electrical parameters with exposure time at 830 W/m2 at 30-31°C.All electrical parameters show a slight variation with the exposure time:I
sc and V
oc exhibit a slight improvement with exposure time. The behavior of the FF is just the opposite of its value decreasing with the exposure time. The variation of the FF provokes that the maximum power (P
max
⁡) of the cell also decreases when exposure time increases. Independently of the tendency, the progress of the 4 parameters is quite similar. They show a rapid change in the first minutes of exposure (≈15 minutes) and, after this period of time, the variation with time slows down. After 2 hours of exposure, the efficiency remains almost stable.Finally, we studied the stability/durability of the textile-based DSC over time. Figure12 shows theIV-curves of DSC-2 obtained after 3 consecutive days and 45 days after the first experiment, and the electrical parameters were extracted from them. The figure demonstrates the stability of the electrical behavior of our DSC, at least in dark-stored conditions.Figure 12
IV-curves measured in 4 different days for DSC-2. (Irradiance: 830 W/m2, Temperature: 25°C.)In addition, the open circuit voltage, the current density, and the fill factor of the DSC samples were measured over a period of 7 weeks. All parameters show no significant loss of cell performance over the investigated period (data forV
oc exemplarily shown in Figure 13).Figure 13
Characterization ofV
oc over a period of 7 weeks.


## 3.1. Structure of Textile-Based DSC

In accordance to typical DSC, our textile-based DSC structure is a composite of several materials. The layer-by-layer structure (schematically shown in Table1) consists of the textile substrate (1), which serves as a flexible, lightweight but mechanically strong support for all the following layers. Each layer shows material-specific characteristics and must fulfill DSC requirements in terms of thermostability, roughness, adhesion, conductivity, photovoltaic activity, transparency, barrier properties, and flexibility. In addition, the overall structure must be liquid-proof to avoid leakage of the electrolyte.Table 1
Textile-based DSC device structure and essential requirements of the layers.
Sun light
8
Cover
Special epoxy and thermoplastic foils
Transparency and impermeability towards the electrolyte
7
Upper electrode
Thin PEN/ITO film
Conductivity and transparency
6
Catalyst
Pt
Good adhesion
5
Electrolyte
I
-/I
3
-
4
Active layer
T
i
O
2 and dyestuff
3
Bottom electrode
Ti
Conductivity, thermoresistance, high flexibility, and good adhesion
2
Smoothing layer
Polyamide coating
Thermoresistance, impermeability towards the electrolyte, high flexibility, and good adhesion
1
Substrate
Glass-fiber fabric
Thermoresistance, high flexibility, being light, and mechanical strength
Layer
Material used
Properties/requirementsTo achieve a flat, thermostable, and liquid-proof substrate, the glass-fiber fabric was covered with a thin polyamide film (2) by a simple roll-to-roll procedure (Figure1).Figure 1
Roll-to-roll technique used (a) to cover the glass-fiber fabric with a polyamide film (b).
(a)
(b)On this improved material, a titanium layer (3) was deposited to turn the fiber glass into a conductive substrate, which can act as the bottom electrode. The Ti films were grown by two different deposition techniques: electron beam (eBeam) and sputtering. After the Ti deposition, the samples were characterized by means of optical microscopy and mechanical profilometry. Exemplarily, Figure2 shows images of the materials after eBeam deposition of Ti. Independently from the Ti deposition technique used, the sample surfaces maintained the substrate topography. Moreover, both technologies lead to quite homogeneous films with good adherence to the substrate. Surface resistances lower than 3 Ω/sq were found indicating sufficient conductivity.Figure 2
Optical characterization of Ti layers deposited on the polyamide covered glass-fiber fabric by eBeam.In the following step, titanium dioxide DSL-18NR-AO was deposited by screen-printing and cured for 5 minutes at 500°C to achieve a nanoporous structure of the titania, which allows a high uptake of various ruthenium-based dyestuffs. The dye-sensitized titania forms the photoactive layer (4) that absorbs the sun light yielding electric charges. This short-term but high-temperature curing step clarifies the necessity of all previous layers to be thermostable in the range of 500°C for a certain time. In the field of conventional textile materials, only glass-fiber fabrics fulfill this essential requirement.A commercial PEN-ITO film (7) was selected as a transparent counter electrode. The film has a thickness of 125μm with a transparency of 75% at 550 nm. The sheet resistance of 15 Ω/sq is sufficient.On the ITO side of the film, the catalyst layer (6) was deposited by the chemical reduction of H2PtCl6 at room temperature resulting in homogeneous Pt clusters on the substrate surface. After adding the electrolyte (5), the textile part (glass-fiber fabric + PA layer + Ti + dye-sensitized TiO2) was covered with the counter electrode part (PEN + ITO + Pt) yielding the flexible textile-based DSC. The overall structure was sealed by a special epoxy and thermoplastic foils (8) to protect the structure from environmental conditions. Our textile-based DSC device with the size of nearly 6 cm2 is shown in Figure 3(a).Figure 3
Final textile-based DSC (a) and 4-point configuration used in theIV-curve measurement (b).
(a)
(b)


## 3.2. Photovoltaic Performance of Textile-Based DSC

### 3.2.1.IV-Curve Measurement under Standard and Nonstandard Test Conditions

In order to characterize the textile-based DSC electrically in terms of its photovoltaic performance, we started withIV-curve measurement under Standard Test Conditions (STC) using the configuration shown in Figure 3(b) providing the results summarized in Figure 4. The DSC devices show a significant photovoltaic activity with an average efficiency of nearly 1.0%.Figure 4
IV-curves of two samples of textile-based DSC under STC.Solar cells normally present a different electrical behavior depending on the irradiance level, and the photovoltaic efficiency of the cells can change significantly depending on the irradiance value. As a consequence of this and in addition to the STC measurements, we measured theIV-curve of the DSC-1 cell at different irradiance values, maintaining the AM1.5G spectrum and the 25°C temperature. As an example, in Figure 5, theIV-curves obtained for 3 representative levels of irradiance (1000 W/m2, 500 W/m2, and 200 W/m2) are shown to have joined to the electrical parameters extracted from them. The representedIV-curves were obtained by applying the correction value due to the spectral mismatch factor.Figure 5
IV-curves at 3 different irradiance levels for DSC-1.As can be seen in Figure5, the electrical behavior of the cell presents a clear dependency with the irradiance level. The efficiency of the cell improves significantly when the irradiance decreases, mainly due to the significant increase of the Fill Factor (FF) at low irradiance levels.Figure6 shows the variation of the main electrical parameters (V
oc, I
sc, FF, and efficiency) as a function of the irradiance level. All the represented values are extracted from theIV-curves measured at different irradiances, taking into account the spectral mismatch factor.Figure 6
Variation of the main electrical parameters of DSC-1 with the irradiance level.The value of theI
sc increases linearly with the irradiance level. This fact is completely reasonable because, normally, the I
sc value is directly proportional to the irradiance value. In addition, V
oc increases with the irradiance level due to the increasing electron injection into titania at higher illumination, which pushes the Fermi level up.The most important data, extracted from these measurements, is the large improvement of the fill factor when the irradiance value decreases. Apparently, the dependency of the FF with the irradiance level follows a linear tendency. The slope of said tendency is so considerable that, as an example, the value of the FF at 200 W/m2 is practically double compared to the value at 1000 W/m2.Finally, despite theI
sc and V
oc tendency, the electrical efficiency of the cell improves notably when irradiance decreases, due to the significant improvement of the FF at low irradiance levels. Under 1/5 of sun conditions, the efficiency increases to a remarkable 1.8%. As demonstrated here, DSC devices are known to perform well under difficult light conditions such as low illumination or diffuse/indirect illumination, under which 1st- and 2nd-generation PV technologies tend to suffer a loss of performance.


### 3.2.2. Temperature Coefficients of the Main Electrical Parameters

In order to study the influence of the temperature on the electrical behavior of the textile-based DSC, we carried out someIV-curve measurements at different temperatures, maintaining the irradiance value constant at 830 W/m2. Figure 7 shows theIV-curves measured at 6 different temperatures at constant irradiance level (830 W/m2) for DSC-1.Figure 7
DSC-1IV-curves measured at 6 different temperatures at an irradiance value of 830 W/m2.As presented in Figure7,IV-curve shape changes significantly with temperature variation. Figure 8 shows the variation of I
sc, V
oc, FF, and P
max
⁡ with the cell temperature for the case of the DSC-1. The keys of the figure show the value of the temperature coefficients for I
sc, V
oc, and P
max
⁡ parameters.Figure 8
Variation of the main electrical parameters of DSC-1 with the temperature, at an irradiance value of 830 W/m2.As can be seen in Figure8, I
sc and V
oc parameters show a negative variation with temperature, meaning that their value decreases when temperature increases. Nevertheless, the most important information extracted from this data is the improvement of the FF parameter when temperature increases. Simultaneously as I
sc and V
oc decrease, the maximum power (P
max
⁡) remains practically constant with the temperature variation. This represents a very important advantage for these types of cells in comparison to other PV technologies as crystalline silicon based solar cells, which suffer significant P
max
⁡ reduction with increasing temperature.


### 3.2.3. OutdoorIV-Curve Measurement

As a complementary study of the measurements carried out in the solar simulator,IV-curve measurements were also performed outdoors to test the electrical behavior of the cell under real conditions. The main advantage of the outdoor measurement is that the data does not require any spectral mismatch correction, but the disadvantage is the inability to control the irradiance level. Both irradiance and cell temperature were also measured during the test.TheIV-curves were measured on a sunny day by placing the PV cells on a solar tracker, perfectly adjusted to the sun. The global irradiance during theIV-curve measurements varied between 1010 W/m2 and 1020 W/m2, and the cell temperature fluctuated between 37°C and 39°C. The measurements obtained for both DSC samples are shown in Figure 9. As shown from Figure 9, the results of the outdoor measurements are quite similar to the results obtained in the solar simulator.Figure 9
OutdoorIV-curves of DSC-1 and DSC-2 (38°C, 1015 W/m2).


### 3.2.4. Spectral Response and Global Reflectance Measurement

The measurement of the spectral response of dye-sensitized solar cells is not a trivial matter. The time response of these cells is quite slow compared to other technologies and, as a consequence, very low frequencies must be used in the chopping process of the light during the spectral response measurement. Besides this fact, the spectral response of the cells presents a clear dependence with the bias light intensity used to polarize the cell during the measurement.Figure10 shows the relative External Quantum Efficiency (EQE) measured for both cells (DSC-1 and DSC-2). The global reflectance as a function of the wavelength is also included in the graph. Finally, as a comparison, the EQE measurement of a similar dye-sensitized cell (deposited on glass) is also included.Figure 10
Relative External Quantum Efficiency (EQE) and global reflectance of DSC-1 and DSC-2 and EQE measurement of a reference dye-sensitized cell.As can be seen in Figure10, the relative spectral response of both cells (DSC-1 and DSC-2) is quite similar. The photogeneration wavelength range of these cells goes from 400 nm to 750 nm and shows a maximum around 550 nm. Comparing these results with the EQE values extracted from the bibliography for similar dye-sensitized solar cells (deposited on glass), it can be said that the spectral response is quite similar, with a slight worse performance, especially in the short wavelength range (<550 nm).


### 3.2.5. Stability Study

In order to complete the electrical characterization of the textile-based DSC, a study of the stability of their electrical response with the increase of the exposition time was carried out. In the first part of this stability study, DSC-2 was irradiated with a constant intensity of 830 W/m2, and the temperature of the cell was maintained practically constant between 30°C and 31°C. DifferentIV-curves were measured during the exposition time. Figure 11 shows the evolution of the electrical parameters (I
sc, V
oc, FF, and P
max
⁡) as a function of the exposure time.Figure 11
Evolution of the main electrical parameters with exposure time at 830 W/m2 at 30-31°C.All electrical parameters show a slight variation with the exposure time:I
sc and V
oc exhibit a slight improvement with exposure time. The behavior of the FF is just the opposite of its value decreasing with the exposure time. The variation of the FF provokes that the maximum power (P
max
⁡) of the cell also decreases when exposure time increases. Independently of the tendency, the progress of the 4 parameters is quite similar. They show a rapid change in the first minutes of exposure (≈15 minutes) and, after this period of time, the variation with time slows down. After 2 hours of exposure, the efficiency remains almost stable.Finally, we studied the stability/durability of the textile-based DSC over time. Figure12 shows theIV-curves of DSC-2 obtained after 3 consecutive days and 45 days after the first experiment, and the electrical parameters were extracted from them. The figure demonstrates the stability of the electrical behavior of our DSC, at least in dark-stored conditions.Figure 12
IV-curves measured in 4 different days for DSC-2. (Irradiance: 830 W/m2, Temperature: 25°C.)In addition, the open circuit voltage, the current density, and the fill factor of the DSC samples were measured over a period of 7 weeks. All parameters show no significant loss of cell performance over the investigated period (data forV
oc exemplarily shown in Figure 13).Figure 13
Characterization ofV
oc over a period of 7 weeks.


## 3.2.1.IV-Curve Measurement under Standard and Nonstandard Test Conditions

In order to characterize the textile-based DSC electrically in terms of its photovoltaic performance, we started withIV-curve measurement under Standard Test Conditions (STC) using the configuration shown in Figure 3(b) providing the results summarized in Figure 4. The DSC devices show a significant photovoltaic activity with an average efficiency of nearly 1.0%.Figure 4
IV-curves of two samples of textile-based DSC under STC.Solar cells normally present a different electrical behavior depending on the irradiance level, and the photovoltaic efficiency of the cells can change significantly depending on the irradiance value. As a consequence of this and in addition to the STC measurements, we measured theIV-curve of the DSC-1 cell at different irradiance values, maintaining the AM1.5G spectrum and the 25°C temperature. As an example, in Figure 5, theIV-curves obtained for 3 representative levels of irradiance (1000 W/m2, 500 W/m2, and 200 W/m2) are shown to have joined to the electrical parameters extracted from them. The representedIV-curves were obtained by applying the correction value due to the spectral mismatch factor.Figure 5
IV-curves at 3 different irradiance levels for DSC-1.As can be seen in Figure5, the electrical behavior of the cell presents a clear dependency with the irradiance level. The efficiency of the cell improves significantly when the irradiance decreases, mainly due to the significant increase of the Fill Factor (FF) at low irradiance levels.Figure6 shows the variation of the main electrical parameters (V
oc, I
sc, FF, and efficiency) as a function of the irradiance level. All the represented values are extracted from theIV-curves measured at different irradiances, taking into account the spectral mismatch factor.Figure 6
Variation of the main electrical parameters of DSC-1 with the irradiance level.The value of theI
sc increases linearly with the irradiance level. This fact is completely reasonable because, normally, the I
sc value is directly proportional to the irradiance value. In addition, V
oc increases with the irradiance level due to the increasing electron injection into titania at higher illumination, which pushes the Fermi level up.The most important data, extracted from these measurements, is the large improvement of the fill factor when the irradiance value decreases. Apparently, the dependency of the FF with the irradiance level follows a linear tendency. The slope of said tendency is so considerable that, as an example, the value of the FF at 200 W/m2 is practically double compared to the value at 1000 W/m2.Finally, despite theI
sc and V
oc tendency, the electrical efficiency of the cell improves notably when irradiance decreases, due to the significant improvement of the FF at low irradiance levels. Under 1/5 of sun conditions, the efficiency increases to a remarkable 1.8%. As demonstrated here, DSC devices are known to perform well under difficult light conditions such as low illumination or diffuse/indirect illumination, under which 1st- and 2nd-generation PV technologies tend to suffer a loss of performance.


## 3.2.2. Temperature Coefficients of the Main Electrical Parameters

In order to study the influence of the temperature on the electrical behavior of the textile-based DSC, we carried out someIV-curve measurements at different temperatures, maintaining the irradiance value constant at 830 W/m2. Figure 7 shows theIV-curves measured at 6 different temperatures at constant irradiance level (830 W/m2) for DSC-1.Figure 7
DSC-1IV-curves measured at 6 different temperatures at an irradiance value of 830 W/m2.As presented in Figure7,IV-curve shape changes significantly with temperature variation. Figure 8 shows the variation of I
sc, V
oc, FF, and P
max
⁡ with the cell temperature for the case of the DSC-1. The keys of the figure show the value of the temperature coefficients for I
sc, V
oc, and P
max
⁡ parameters.Figure 8
Variation of the main electrical parameters of DSC-1 with the temperature, at an irradiance value of 830 W/m2.As can be seen in Figure8, I
sc and V
oc parameters show a negative variation with temperature, meaning that their value decreases when temperature increases. Nevertheless, the most important information extracted from this data is the improvement of the FF parameter when temperature increases. Simultaneously as I
sc and V
oc decrease, the maximum power (P
max
⁡) remains practically constant with the temperature variation. This represents a very important advantage for these types of cells in comparison to other PV technologies as crystalline silicon based solar cells, which suffer significant P
max
⁡ reduction with increasing temperature.


## 3.2.3. OutdoorIV-Curve Measurement

As a complementary study of the measurements carried out in the solar simulator,IV-curve measurements were also performed outdoors to test the electrical behavior of the cell under real conditions. The main advantage of the outdoor measurement is that the data does not require any spectral mismatch correction, but the disadvantage is the inability to control the irradiance level. Both irradiance and cell temperature were also measured during the test.TheIV-curves were measured on a sunny day by placing the PV cells on a solar tracker, perfectly adjusted to the sun. The global irradiance during theIV-curve measurements varied between 1010 W/m2 and 1020 W/m2, and the cell temperature fluctuated between 37°C and 39°C. The measurements obtained for both DSC samples are shown in Figure 9. As shown from Figure 9, the results of the outdoor measurements are quite similar to the results obtained in the solar simulator.Figure 9
OutdoorIV-curves of DSC-1 and DSC-2 (38°C, 1015 W/m2).


## 3.2.4. Spectral Response and Global Reflectance Measurement

The measurement of the spectral response of dye-sensitized solar cells is not a trivial matter. The time response of these cells is quite slow compared to other technologies and, as a consequence, very low frequencies must be used in the chopping process of the light during the spectral response measurement. Besides this fact, the spectral response of the cells presents a clear dependence with the bias light intensity used to polarize the cell during the measurement.Figure10 shows the relative External Quantum Efficiency (EQE) measured for both cells (DSC-1 and DSC-2). The global reflectance as a function of the wavelength is also included in the graph. Finally, as a comparison, the EQE measurement of a similar dye-sensitized cell (deposited on glass) is also included.Figure 10
Relative External Quantum Efficiency (EQE) and global reflectance of DSC-1 and DSC-2 and EQE measurement of a reference dye-sensitized cell.As can be seen in Figure10, the relative spectral response of both cells (DSC-1 and DSC-2) is quite similar. The photogeneration wavelength range of these cells goes from 400 nm to 750 nm and shows a maximum around 550 nm. Comparing these results with the EQE values extracted from the bibliography for similar dye-sensitized solar cells (deposited on glass), it can be said that the spectral response is quite similar, with a slight worse performance, especially in the short wavelength range (<550 nm).


## 3.2.5. Stability Study

In order to complete the electrical characterization of the textile-based DSC, a study of the stability of their electrical response with the increase of the exposition time was carried out. In the first part of this stability study, DSC-2 was irradiated with a constant intensity of 830 W/m2, and the temperature of the cell was maintained practically constant between 30°C and 31°C. DifferentIV-curves were measured during the exposition time. Figure 11 shows the evolution of the electrical parameters (I
sc, V
oc, FF, and P
max
⁡) as a function of the exposure time.Figure 11
Evolution of the main electrical parameters with exposure time at 830 W/m2 at 30-31°C.All electrical parameters show a slight variation with the exposure time:I
sc and V
oc exhibit a slight improvement with exposure time. The behavior of the FF is just the opposite of its value decreasing with the exposure time. The variation of the FF provokes that the maximum power (P
max
⁡) of the cell also decreases when exposure time increases. Independently of the tendency, the progress of the 4 parameters is quite similar. They show a rapid change in the first minutes of exposure (≈15 minutes) and, after this period of time, the variation with time slows down. After 2 hours of exposure, the efficiency remains almost stable.Finally, we studied the stability/durability of the textile-based DSC over time. Figure12 shows theIV-curves of DSC-2 obtained after 3 consecutive days and 45 days after the first experiment, and the electrical parameters were extracted from them. The figure demonstrates the stability of the electrical behavior of our DSC, at least in dark-stored conditions.Figure 12
IV-curves measured in 4 different days for DSC-2. (Irradiance: 830 W/m2, Temperature: 25°C.)In addition, the open circuit voltage, the current density, and the fill factor of the DSC samples were measured over a period of 7 weeks. All parameters show no significant loss of cell performance over the investigated period (data forV
oc exemplarily shown in Figure 13).Figure 13
Characterization ofV
oc over a period of 7 weeks.


## 4. Conclusions

Solar energy conversion is an object of continuous research, focusing on improving the energy efficiency as well as the structure of photovoltaic cells. With efficiencies continuously increasing, state-of-the-art PV cells offer a good solution to harvest solar energy. However, it is important to understand that available, inflexible PV structures cannot be integrated in many common products, and especially textiles, although they are often directly exposed to sunlight and represent ideal substrates for the conversion of solar energy. Outdoor textiles such as blinds, tents, tarpaulins, and sails, and finally the increasing market of textile architecture, exhibit an outstanding potential to form the basis for flexible, lightweight, and robust PV structures.Compared to conventional silicon based photovoltaic technology, DSC technology promises a lower cost in manufacture. Because of greatly reduced sensitivity to angle of incidence of radiation and shadowing, DSC produces electricity more efficiently, including low light conditions. In addition, they can be directly incorporated into buildings by replacing conventional glass panels rather than taking up roof or extra land area. Moreover, advantages include not necessitating the use of high-priced raw materials, a manufacturing process that does not produce toxic emissions, and the potential for a rapid efficiency enhancement.We demonstrated successfully the development of a new two-dimensional textile-based dye-sensitized solar cell, which exploits the typical inherent properties of fabrics such as flexibility, low weight, and mechanical robustness. We apply our DSC design on a heat-resistant glass-fiber fabric due to the necessity of high-temperature processes during the manufacture and report on all further needed conductive, photoactive, and protective materials and their deposition techniques to achieve flexible, light, and mechanically strong textile-based DSC. Our produced large-area devices (up to 6 cm2 per individual unit) show efficiencies up to 1.8% at 1/5 of the sun. Stability tests assure no loss of photovoltaic activity of the noncorrosive and liquid-proof devices over a period of at least seven weeks.Therefore, our technology has paved the way for a new generation of flexible photovoltaic devices, which can be used for the generation of power in the mentioned applications as well as in modern textile architecture. This can be considered as a “breakthrough” in textile DSC technology and will promise a quick launch into market after some aspects on the durability in the day-to-day life are assured by various stress tests and the efficiency is improved to a level of >3%. In the near future, further research should be focused on the development of new titanium inks, low temperature curing processes, and the implementation of solid-state or quasi-solid-state electrolytes, which enables the use of other typical fiber forming polymers such as polyesters and polyamides as textile substrates for textile-based DSC.



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*Source: 3796074-2016-08-14.xml*