Abstract:We have explored the effects of percolation on the properties of supercapacitors with thin nanotube networks as electrodes. We find the equivalent series resistance, R(ESR), and volumetric capacitance, C(V), to be thickness independent for relatively thick electrodes. However, once the electrode thickness falls below a threshold thickness (∼100 nm for R(ESR) and ∼20 nm for C(V)), the properties of the electrode become thickness dependent. We show the thickness dependence of both R(ESR) and C(V) to be consisten… Show more
“…Moreover, high T simultaneously results in reduced CA, hence a reduction in the energy which can be stored by a device with a given footprint. 27,32 Quantifying these trade-offs using the described figures of merit will greatly assist with the development of high performance transparent SCs.…”
Section: mentioning
confidence: 99%
“…Whilst examples of the former are presently scarce, 16 significant efforts are underway to develop transparent/flexible SCs. [17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32][33][34][35] The electrode materials under investigation for this purpose are numerous, including carbon nanotubes, 27,[32][33] graphene, 21,29,34 transition metal oxides 17, 19-20, 23, 25 and conducting polymers. 17,22,30 In some transparent SC reports, the capacitive charge storage materials have been supported by an underlying transparent indium-tin oxide (ITO) layer to provide efficient current collection.…”
Section: Introductionmentioning
confidence: 99%
“…27 To characterise this behaviour the electrode sheet resistance, Rs, can be related to T via a similar expression as for the areal capacitance: …”
This work describes the potential
of thin, spray-deposited, large-area poly(3,4-ethylenedioxythiophene)/poly(styrene-4-sulfonate)
(PEDOT:PSS) conducting polymer films for use as transparent supercapacitor
electrodes. To facilitate this, we provide a detailed explanation
of the factors limiting the performance of such electrodes. These
films have a very low optical conductivity of σop = 24 S/cm (at 550 nm), crucial for this application, and a reasonable
volumetric capacitance of C
V = 41 F/cm3. Secondary doping with formic acid gives these films a DC
conductivity of σDC = 936 S/cm, allowing them to
perform both as a transparent conductor/current collector and transparent
supercapacitor electrode. Small-area films (A ∼
1 cm2) display measured areal capacitance as high as 1
mF/cm2, even for reasonably transparent electrodes (T ∼ 80%). However, in real devices, the absolute
capacitance will be maximized by increasing the device area. As such,
here, we measure the electrode performance as a function of its length
and width. We find that the measured areal capacitance falls dramatically
with scan rate and sample length but is independent of width. We show
that this is because the measured areal capacitance is limited by
the electrical resistance of the electrode. We have derived an equation
for the measured areal capacitance as a function of scan rate and
electrode lateral dimensions that fits the data extremely well up
to scan rates of ∼1000 mV/s (corresponding to charge/discharge
times > 0.6 s). These results are self-consistent with independent
analysis of the electrical and impedance properties of the electrodes.
These results can be used to find limiting combinations of electrode
length and scan rate, beyond which electrode performance falls dramatically.
We use these insights to build large-area (∼100 cm2) supercapacitors using electrodes that are 95% transparent, providing
a capacitance of ∼12 mF (at 50 mV/s), significantly higher
than that of any previously reported transparent supercapacitor.
“…Moreover, high T simultaneously results in reduced CA, hence a reduction in the energy which can be stored by a device with a given footprint. 27,32 Quantifying these trade-offs using the described figures of merit will greatly assist with the development of high performance transparent SCs.…”
Section: mentioning
confidence: 99%
“…Whilst examples of the former are presently scarce, 16 significant efforts are underway to develop transparent/flexible SCs. [17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32][33][34][35] The electrode materials under investigation for this purpose are numerous, including carbon nanotubes, 27,[32][33] graphene, 21,29,34 transition metal oxides 17, 19-20, 23, 25 and conducting polymers. 17,22,30 In some transparent SC reports, the capacitive charge storage materials have been supported by an underlying transparent indium-tin oxide (ITO) layer to provide efficient current collection.…”
Section: Introductionmentioning
confidence: 99%
“…27 To characterise this behaviour the electrode sheet resistance, Rs, can be related to T via a similar expression as for the areal capacitance: …”
This work describes the potential
of thin, spray-deposited, large-area poly(3,4-ethylenedioxythiophene)/poly(styrene-4-sulfonate)
(PEDOT:PSS) conducting polymer films for use as transparent supercapacitor
electrodes. To facilitate this, we provide a detailed explanation
of the factors limiting the performance of such electrodes. These
films have a very low optical conductivity of σop = 24 S/cm (at 550 nm), crucial for this application, and a reasonable
volumetric capacitance of C
V = 41 F/cm3. Secondary doping with formic acid gives these films a DC
conductivity of σDC = 936 S/cm, allowing them to
perform both as a transparent conductor/current collector and transparent
supercapacitor electrode. Small-area films (A ∼
1 cm2) display measured areal capacitance as high as 1
mF/cm2, even for reasonably transparent electrodes (T ∼ 80%). However, in real devices, the absolute
capacitance will be maximized by increasing the device area. As such,
here, we measure the electrode performance as a function of its length
and width. We find that the measured areal capacitance falls dramatically
with scan rate and sample length but is independent of width. We show
that this is because the measured areal capacitance is limited by
the electrical resistance of the electrode. We have derived an equation
for the measured areal capacitance as a function of scan rate and
electrode lateral dimensions that fits the data extremely well up
to scan rates of ∼1000 mV/s (corresponding to charge/discharge
times > 0.6 s). These results are self-consistent with independent
analysis of the electrical and impedance properties of the electrodes.
These results can be used to find limiting combinations of electrode
length and scan rate, beyond which electrode performance falls dramatically.
We use these insights to build large-area (∼100 cm2) supercapacitors using electrodes that are 95% transparent, providing
a capacitance of ∼12 mF (at 50 mV/s), significantly higher
than that of any previously reported transparent supercapacitor.
“…We believe the current study is the first demonstration of percolation of capacitance in composite supercapacitor electrodes (although percolation scaling of capacitance has been observed in single-component nanotube networks). 79 Understanding the nature of such percolation will be critical for the optimisation of capacitive composites.…”
Section: Percolation Of Capacitance In Composite Filmsmentioning
Here we demonstrate significant improvements in the performance of supercapacitor electrodes based on 2D MnO2 nano-platelets by the addition of carbon nanotubes. Electrodes based on MnO2 nano-platelets do not display high areal capacitance because the electrical properties of such films are poor, limiting the transport of charge between redox sites and the external circuit.In addition, the mechanical strength is low, limiting the achievable electrode thickness, even in the presence of binders. By adding carbon nanotubes to the MnO2-based electrodes, we have increased the conductivity by up to eight orders of magnitude, in line with percolation theory.The nanotube network facilitates charge transport, resulting in large increases in capacitance, especially at high rates, around 1 V/s. The increase in MnO2 specific capacitance scaled with nanotube content in a manner fully consistent with percolation theory. Importantly, the mechanical robustness was significantly enhanced, allowing the fabrication of electrodes that were 10 times thicker than could be achieved in MnO2-only films. This resulted in composite films with areal capacitances up to 40 times higher than could be achieved with MnO2-only electrodes.
“…18 These materials have been used as electrodes in a range of applications including light emitting diodes, solar cells and transparent capacitors. 19,20 However, more recently, attention has turned to using nanostructured transparent conductors as transparent heaters. [21][22][23][24][25][26][27][28][29][30] Transparent heaters are simply conducting films which are thin enough to be transparent but can be heated up on application of a voltage.…”
Transparent heaters are important for many applications and in the future are likely to be fabricated from thin, conducting, nanostructured networks. However, the electrical properties of such networks are almost always controlled by percolative effects.The impact of percolation on heating effects has not been considered and the material parameter combinations which lead to efficient performance are not known. In fact, figures of merit for transparent heaters have not been elucidated, either in bulk-like or percolative systems. Here, we develop a simple yet comprehensive model describing the operation of transparent heaters. By considering the balance of Joule heating versus power dissipated by both convection and radiation, we derive an expression for the time-dependent heater temperature as a function of both electrical and thermal parameters. This equation can be modified to describe the relationship between temperature, optical transmittance and electrical/thermal parameters in both bulk-like and percolative systems. By performing experiments on silver nanowire networks, systems known to display both bulk-like and percolative regimes, we show the model to describe real systems extremely well. This work shows the performance of transparent heaters in the percolative regime to be significantly less efficient compared to the bulk-like regime, implying the diameter of the nanowires making up the network to be critical. The model allows the identification of figures of merit for networks in both bulk-like and percolative regimes. We show that metallic nanowire networks are most promising, closely followed by CVD graphene with networks of solutionprocessed graphene and carbon nanotubes being much less efficient.
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