O objetivo do trabalho foi avaliar o desempenho do reflectômetro no domínio do tempo (TDR) comparativamente ao tensiômetro com manômetro de mercúrio (considerado como instrumento padrão), dando-se ênfase na sensibilidade de detecção de variações na umidade do solo sob condições de molhamento e secagem. Foi instalado um experimento em um solo classificado como Nitossolo Vermelho distrófico latossólico de textura muito argilosa, localizado próximo ao Posto Meteorológico do Departamento de Ciências Exatas, ESALQ/USP, Piracicaba (SP), Brasil, 22 o 42’ 30’’ de latitude sul e 47 o 38’ 00’’ de longitude oeste. Com dados de um ensaio de determinação da condutividade hidráulica do solo pelo Método do Perfil Instantâneo, de um período de secagem e de inundações intermitentes do solo, analisou-se a concordância entre a constante dielétrica obtido pelo TDR e o potencial matricial da água no solo obtido pelo tensiômetro, além dos valores de umidade volumétrica obtidos pelas mesmas técnicas. Concluiu-se que o desempenho do TDR foi superior ao do tensiômetro sob condições de secagem do solo e na detecção de variações de umidade. / The performance of a time domain-reflectometer (TDR) was compared with a mercury tensiometer (considered to be the norm), emphasizing the detection of variations in soil water content under wetting and drying conditions (as in instantaneous profile method to determine soil hydraulic conductivity). An experiment was performed in a Nitossolo Vermelho distrófico latossólico argiloso (Brazilian classification system), close to the meteorological observatory of the ESALQ/USP, Piracicaba (SP), Brazil, latitude 22 o 42’30’’ S, longitude 47 o 38’00’’ W. Data of matric potential, dieletric constant and water content during a dry period and water application were analyzed. The TDR cable tester was better than the tensiometer to detect the soil moisture variation.

Made available in DSpace on 2016-08-19T12:56:45Z (GMT). No. of bitstreams: 1 Dissertacao Darlan.pdf: 2834733 bytes, checksum: f7d35c098bddf8713fbdbe733565fdef (MD5) Previous issue date: 2013-07-12 / During several years, adulterated gasoline has been commercialized across all Brazil. Often such product has higher alcohol content, water traces or organic solvents insertion (e.g. paint thinner and/or turpentine). The use of nonconforming gasoline, in the short and long terms, has several problems for consumers, for the vehicle and the environment. Thus, this work aims to propose a low cost technique for analyzing gasoline blends, in relation to its oxygenated addition. Both capacitance and dielectric constant (relative permittivity) were determined by means of a high precision LCR-meter, using a metal concentric sensor. Therefore, gasoline blends were prepared by adding 16, 18, 20, 22, 24, 26, 28 and 30% of AEAF to the initial petroleum-based fuel and their dielectric constants were measured at frequencies of 0.3, 0.4, 0.5 and 0.6 kHz. The same samples were analyzed by the reference method, the Test Tube Test. According to statistical modeling, the frequency of 0.6 kHz showed the most significant results for all samples. The results show that at 95% confidence level, there is no significant difference between the two methods, indicating a good correlation between the proposed method and then standard one. However, when the density was used as evaluating parameter, instead of dielectric constant, for the same samples, a substantial discrepancy of the obtained values were observe, suggest a low sensibility of such methodology. / Vários são os casos de não conformidade da gasolina comercial, principalmente pelo excesso de etanol, ou ainda pela adição de água ou solventes leves como thinner e aguarrás. O uso de gasolina não conforme, a curto e longo prazo, traz diversos problemas para o consumidor, para o veículo e ao meio ambiente. No presente trabalho estudou-se a qualidade da gasolina tipo C, comercializada nos postos revendedores de combustível, no que diz respeito à concentração de álcool etílico anidro combustível (AEAC). Análises estas, realizadas através de medidas de constante dielétrica (permissividade relativa) utilizando sensor capacitivo. Misturas de gasolina A e AEAC foram preparadas nas concentrações de 16, 18, 20, 22, 24, 26, 28 e 30% de AEAC, sendo suas constantes dielétricas medidas nas frequências de 0,3; 0,4; 0,5 e 0,6 kHz. Utilizando tratamento estatístico verificou-se que a frequência de 0,6 kHz apresentou resultados mais significativos para leitura de AEAC das misturas preparadas. Nessa mesma frequência, amostras comerciais de gasolina e amostras de gasolinas não conformes contaminadas com gasolina A e AEAC foram submetidas à análise. As mesmas amostras foram submetidas à análise pelo método de referência, o Teste da Proveta. Os resultados obtidos mostram que, no nível de confiança de 95%, não há diferença significativa entre os dois métodos. Medidas de massas específicas também foram realizadas com as misturas gasolina A e AEAC (16 a 30%) para modelamento de curva de calibração com finalidade de determinar o teor de AEAC e posterior comparação com os resultados oriundos da constante dielétrica e do teste da proveta, entretanto, o método não se mostrou eficiente para análise das amostras de gasolina comercial e amostras de gasolinas não conformes analisadas.

Este trabalho de pesquisa apresenta a avaliação de uma sonda TDR helicoidal para estimar o teor de umidade dos solos, em diferentes profundidades, através da técnica da reflectometria no domínio do tempo (TDR). Essa sonda, desenvolvida especificamente para esse fim, foi devidamente calibrada em laboratório para diferentes tipos de solo. O processo de calibração consistiu na determinação da constante dielétrica aparente (Ka) e condutividade elétrica volumétrica (ECb) de um mesmo solo com diferentes teores de umidade. Posteriormente foram buscadas correlações entre Ka e o teor de umidade gravimétrico (w), obtido em estufa. São propostas correlações entre w e Ka, entre w e \'KA POT. 1/2\' e entre teor de umidade volumétrico (\'teta\') e Ka. Também foram consideradas as correlações propostas por Yu e Drnevich (2004), visando estimar também a massa específica seca dos solos. Foram realizados ensaios de campo para a validação das equações de calibração. Os valores dos teores de umidade estimados através da técnica da reflectometria no domínio do tempo, tanto em laboratório como em campo, foram comparados com os valores de teor de umidade obtidos com o método da estufa. Com base nos resultados foram determinados os erros referentes às calibrações. Nos ensaios de campo, os teores de umidade obtidos através da correlação entre w e \'KA POT. 1/2\' apresentaram melhores resultados, quando comparados com aqueles estimados com as outras correlações. Pelos resultados obtidos conclui-se que a técnica TDR é uma alternativa viável para a estimativa em campo do teor de umidade em grandes profundidades. / In this work is presented the evaluation of a recently developed helicoidal probe used for estimating the soil water content through the time domain technology (TDR). This probe has been calibrated in laboratory for different types of soils. The calibration process consisted in assessing the values of the apparent dielectric constant (Ka) and the bulk electric conductivity (ECb) of a specific soil at different levels of water content (w). Subsequently, correlations between the apparent dielectric constant and the water content have been established. The same has done with the bulk electric conductivity. Correlations between Ka and w, \'KA POT. 1/2\' and w, \'teta\' (volumetric water content) and Ka have been proposed. Also, the correlations proposed by Yu and Drnevich (2004) have been considered. To validate the proposed correlations, tests using the helicoidal probe were performed in the field. Estimated values of field water content, using the TDR technology have been compared to the correspondent oven water content values. Based on these comparisons, errors regarding the calibrations have been calculated. In the field tests, the correlations between \'KA POT. 1/2\' and w have presented more accurate results than those obtained with the other correlations. Experimental results have shown that the TDR technology for estimating water content at different depths in the field is feasible and expedite.

Organic photovoltaic (OPV) is a promising technology for renewable energy at low cost. Over the last five years, the power conversion efficiency (PCE) has doubled to 12%, which still is clearly lower than commercially available inorganic solar cells with a PCE around 20%. One approach to improve the PCE is to complement the conversion of light into electrical energy with the infrared (IR) part of the solar spectrum. However, the fundamental difference between organic and inorganic semiconductors is the exciton binding energy. Compared to inorganic semiconductors, in organic materials the exciton binding energy is more than 20 times higher, leading to strongly bound electron hole pairs, which are primarily generated upon photo-excitation. To dissociate these charges, in OPV, a donor-acceptor system is used. However, the energetics of this donor-acceptor system lowers the obtained open circuit voltage, representing one major loss of OPV as compared to inorganic solar cells. In the first part of this work, three benzannulated 4,4-difluoro-4-bora-3a,4a-diaza-s-indacene (aza-BODIPY) infrared absorbing donor dyes with methyl, methoxy, or without side-group attached are investigated. The solar cells with the highest PCE, i.e. the devices using the donor molecule without a side-group, exhibit a difference between the optical and the effective gap of 0.17 eV. It reflects the "driving force" for the electron to transfer from the donor to the acceptor, and is lowest for the best performing device, indicating that in the devices used efficient charge dissociation does not require large electron transfer energy loss. A - for OPV - relatively high open circuit voltage of 0.81 V is measured and when compared to the optical gap of the donor, a voltage loss of 0.74 V is obtained, reflecting the high voltage losses in OPV. In inorganic devices these voltage loss is around 0.4 V. One approach to lower this difference in the voltage loss is to lower the exciton binding energy of neat organic materials, leading to a larger exciton size. A saturation of the exciton size at about 1.2 nm is calculated by time dependent density functional method (TD-DFT) for one dimensional conjugated organic molecules with a size larger than 4nm. For the largest size of the exciton, provided by the poly(benzimidazobenzophenanthroline) (BBL), a Coulomb interaction of 0.4 eV between the electron and hole wave function is calculated, leading to an estimated exciton binding energy of about 0.2 eV, serving as a lower limit for the organic molecules investigated. The exciton binding energy can further be lowered by increasing the dielectric constant or by introducing a charge transfer (CT) state between two adjacent molecules. It is shown for the ladder polymer BBL that the dielectric function, including ionic and electronic contributions, can be calculated by a new method within the DFT and TD-DFT framework. In agreement with ellipsometry measurements, a highly anisotropic dielectric constant is obtained, which is 8.3 along the backbone of the polymer and around 3 perpendicular to the polymer. The high dielectric constant along the backbone originates from the strong delocalization of the electrons along the π-system. The ionic contribution increases the mean value of the dielectric constant from 3.6 to 4.2. In order to further increase the dielectric constant, different polar side-chains are attached to the ladder polymer BBL and their dielectric constant is calculated. A strong increase of the dielectric constant to about 17 is obtained by attaching a zwitterionic side-chain to the BBL monomer. In order to lower the exciton binding energy by a CT state, a charge transfer from a donor to an acceptor molecule must be introduced. The Coulomb binding energy of intermolecular CT states are calculated. It is shown that an intermolecular CT state of two π-stacked BBL oligomers does not exhibit a lower Coulomb binding energy as compared to the intramolecular binding energy. However, by a spatial separation of the donor and the acceptor molecule, in-line of the polymer backbone, the Coulomb binding energy is reduced from 0.40 eV to 0.24 eV. Combining such CT states with the high dielectric constant obtained by zwitterionic side-chains would lead to an exciton binding energy close to the thermal energy, resulting in spontaneous free carrier generation on neat materials. This could potentially reduce the voltage losses and increase the PCE in OPV devices significantly. / Die organische Photovoltaik stellt eine kostengünstige, erneuerbare und daher zukunftsgerichtete Energieversorgung dar. Die Umwandlungseffizienz organischer Solarzellen von Sonnenenergie in elektrische Energie konnte über die letzten fünf Jahre auf 12% verdoppelt werden. Kommerziell erhältliche anorganische Solarzellen weisen im Vergleich dazu eine Effizienz von ca. 20% auf. Eine Möglichkeit, die Effizienz organischer Solarzellen zu erhöhen, ist die Umwandlung von Licht in Elektrizität nicht nur im sichtbaren Bereich, sondern zusätzlich auch im infraroten Bereich des Sonnenspektrums. Der größte Unterschied zwischen den organischen und anorganischen Solarzellen liegt allerdings in der Exzitonbindungsenergie, welche in organischen Materialien ca. 20 Mal größer ist. Um das Exziton in freie Ladungsträger zu trennen, wird in organischen Solarzellen deshalb ein Donator-Akzeptor-Übergang benutzt, welcher unter anderem auch für den Spannungs- und damit für den Effizienzverlust von organischen Solarzellen verantwortlich ist. Im ersten Teil der Dissertation werden verschiedene funktionalisierte Donator-Moleküle, die infrarotes Licht absorbieren, untersucht. Die Donator-Moleküle ohne zusätzliche Funktionalisierungsgruppe weisen dabei die höchste Umwandlungseffizienz auf. In den besten Zellen kann ein Unterschied zwischen der optischen und effektiven \"Bandlücke\" von 0,17 eV gemessen werden. Dieser Unterschied stellt die treibende Kraft für den Übergang des Elektrons vom Donator zum Akzeptor dar. Da jedoch dieser Unterschied in der besten Solarzelle am geringsten ist, scheint die Dissoziation der Ladungsträger in den untersuchten Donator-Akzeptor-Systemem nicht vom ihm abzuhängen. Die gemessene relative hohe Leerlaufspannung von 0,81 V ist 0,74 V kleiner als die effektive Bandlücke und zeigt die hohen Spannungsverluste organischer Solarzellen. Die Spannungsverluste anorganischer Solarzellen liegen im Bereich von 0,4 V. Ein Ansatz, um die Spannungsverluste zu verkleinern, liegt in der Reduzierung der Exzitonbindungsenergie, woraus ein größeres Exziton erfolgt. Mit der zeitabhängigen Dichtefunktionaltheorie wird an einer Reihe organischer Moleküle gezeigt, dass die Exzitongröße bei einer Moleküllänge (oder Konjugationslänge) größer als 4nm bei 1,2nm sättigt. Für das größte Exziton, welches im Leiterpolymer Poly(benzimidazobenzophenanthroline) (BBL) vorhanden ist, wird eine Coulomb-Bindungsenergie von 0,4 eV berechnet und eine Exzitonbindungsenergie von 0,2 eV abgeschätzt. Die Exzitonbindungsenergie kann entweder durch Erhöhung der Dielektrizitätskonstante oder durch Erzeugung eines Ladungstransfer-Zustandes weiter verringert werden. Es wird gezeigt, dass mit einer neu entwickelten Methode auf Basis der Dichtefunktionaltheorie die ionischen und elektronischen Beiträge zur dielektrischen Funktion von BBL berechnet werden können. Die berechneten anisotropen Werte stimmen gut mit Werten aus Ellipsometriemessungen überein. Entlang der Polymerkette erhalten wir eine hohe Dielektrizitätskonstante von 8,3 und senkrecht dazu von ca. 3. Die hohe Dielektrizitätskonstante entlang der Polymerkette kann auf die starke Delokalisation der π-Elektronen zurückgeführt werden. Der Mittelwert der Dielektrizitätskonstante wird durch die ionischen Beiträge von 3,6 auf 4,2 erhöht. Um die Dielektrizitätskonstante weiter zu erhöhen, werden verschiedene polare Seitenketten am BBL-Polymer angebracht und die Dielektrizitätskonstante berechnet. Es wird gezeigt, dass die Anbringung einer zwitterionischen Seitenkette am BBL-Monomer die Dielektrizitätskonstante auf 17 erhöht. Um die Exzitonbindungsenergie durch einen Ladungstransfer-Zustand zu verringern, werden ein Donator- und ein Akzeptor-Molekül benötigt. Die Coulomb-Bindungsenergien der intermolekularen Ladungstransfer-Zustände werden berechnet. Es wird gezeigt, dass intermolekulare Ladungstransfer-Zustände zwischen zwei π-gestapelten BBL-Oligomeren keine Verringerung der Coulomb-Bindungsenergie bewirken. Bei einer räumlichen Trennung des Donator- und Akzeptor-Moleküls entlang der Polymerkette kann die Coulomb-Bindungsenergie von 0,40 eV auf 0,24 eV gesenkt werden. Eine Kombination aus diesem Ladungstransfer und der Erhöhung der Dielektirizitätskonstante durch zwitterionische Seitenketten kann zu einer niedrigen Exzitonbindungsenergie, nahe der thermischen Energie, und damit zu freien Ladungsträgern führen. Der damit verringerte Spannungsverlust kann die Umwandlungseffizienz organischer Solarzellen signifikant erhöhen.

This diploma thesis is studing the possibilities of influencing the optoelectric properties of printed light emitting panels, which work on the principle of electroluminescence excited by alternating electric field. The aim of this worrk is to monitor the influence od dielectric properties of electroluminescent phosphor binder on the targeted electroluminescence. In the theoretical part of this thesis, there are described principles of electroluminescence, suitable materials methods of characterization and preparation of panels using printing techniques. Experiment part contains electrical characterization of selected binders to determine their dielectric constants. Subsequently, printing pastes were formulated in different weight ratios of binder electroluminescent phosphor and model light-emitting panels were prepared. Optoelectric characterization was used to determine the change in irradiance. It was found that the dielectric properties of the binder significantly affect the resulting irradinace. It has same irradiance for a smaller amount od phosphor than with the binder with a low dielectric constant. The finding of this work can be used to improve the luminosity at the electroluminescent panels.

Tato diplomová práce zkoumá flexibilní materiál k produkci elektřiny založený na piezoelektrickém polymeru Polyvinylidenfluorid (PVDF). Inkorporací piezoaktivní keramiky lze vlastnosti piezoelektrického polymeru PVDF významně zlepšit a převést na užitečnou elektrickou energii. PVDF byl vytvořen elektrostatickým zvlákňováním do vláken o tloušťce 1,5-0,3 µm a poté studován různými analytickými metodami. Tato práce nabízí popis elektrostatického zvlákňování, přípravu vzorků a teoretický úvod do analytických metod, kterým byly vzorky podrobeny. Morfologie a distribuce nanostrukturované keramiky do polymerní matrice PVDF byla pozorována použitím skenovací elektronové mikroskopie (SEM) a energiově disperzní spektroskopie (EDX). Pro tvorbu fáze a podrobné fázové složení byly vzorky charakterizovány infračervenou spektroskopií s Fourierovou transformací (FTIR). Práce také obsahuje analýzu s použitím Ramanovy spektroskopie, metody používané k identifikaci a porovnání chemických sloučenin. Elektrické vlastnosti byly studovány dielektrickou spektroskopií a je poskytnuta korelace se složením. Jednotlivé komponenty dotovaných vláken jsou charakterizovány a vyhodnocovány v souvislosti s jejich budoucím využitím v senzorech.

This thesis deals with problems of electrical insulation materials based on epoxy composites used in the electronics industry. This thesis is divided into theoretical part focused on composite materials, their technological processing and diagnostics. It also describes dielectric materials, their properties and events taking place in their structure. The experimental section describes the measurement of electrical properties of samples of electrical insulating materials with different types of fillers.

Organic photovoltaic (OPV) is a promising technology for renewable energy at low cost. Over the last five years, the power conversion efficiency (PCE) has doubled to 12%, which still is clearly lower than commercially available inorganic solar cells with a PCE around 20%. One approach to improve the PCE is to complement the conversion of light into electrical energy with the infrared (IR) part of the solar spectrum. However, the fundamental difference between organic and inorganic semiconductors is the exciton binding energy. Compared to inorganic semiconductors, in organic materials the exciton binding energy is more than 20 times higher, leading to strongly bound electron hole pairs, which are primarily generated upon photo-excitation. To dissociate these charges, in OPV, a donor-acceptor system is used. However, the energetics of this donor-acceptor system lowers the obtained open circuit voltage, representing one major loss of OPV as compared to inorganic solar cells. In the first part of this work, three benzannulated 4,4-difluoro-4-bora-3a,4a-diaza-s-indacene (aza-BODIPY) infrared absorbing donor dyes with methyl, methoxy, or without side-group attached are investigated. The solar cells with the highest PCE, i.e. the devices using the donor molecule without a side-group, exhibit a difference between the optical and the effective gap of 0.17 eV. It reflects the "driving force" for the electron to transfer from the donor to the acceptor, and is lowest for the best performing device, indicating that in the devices used efficient charge dissociation does not require large electron transfer energy loss. A - for OPV - relatively high open circuit voltage of 0.81 V is measured and when compared to the optical gap of the donor, a voltage loss of 0.74 V is obtained, reflecting the high voltage losses in OPV. In inorganic devices these voltage loss is around 0.4 V. One approach to lower this difference in the voltage loss is to lower the exciton binding energy of neat organic materials, leading to a larger exciton size. A saturation of the exciton size at about 1.2 nm is calculated by time dependent density functional method (TD-DFT) for one dimensional conjugated organic molecules with a size larger than 4nm. For the largest size of the exciton, provided by the poly(benzimidazobenzophenanthroline) (BBL), a Coulomb interaction of 0.4 eV between the electron and hole wave function is calculated, leading to an estimated exciton binding energy of about 0.2 eV, serving as a lower limit for the organic molecules investigated. The exciton binding energy can further be lowered by increasing the dielectric constant or by introducing a charge transfer (CT) state between two adjacent molecules. It is shown for the ladder polymer BBL that the dielectric function, including ionic and electronic contributions, can be calculated by a new method within the DFT and TD-DFT framework. In agreement with ellipsometry measurements, a highly anisotropic dielectric constant is obtained, which is 8.3 along the backbone of the polymer and around 3 perpendicular to the polymer. The high dielectric constant along the backbone originates from the strong delocalization of the electrons along the π-system. The ionic contribution increases the mean value of the dielectric constant from 3.6 to 4.2. In order to further increase the dielectric constant, different polar side-chains are attached to the ladder polymer BBL and their dielectric constant is calculated. A strong increase of the dielectric constant to about 17 is obtained by attaching a zwitterionic side-chain to the BBL monomer. In order to lower the exciton binding energy by a CT state, a charge transfer from a donor to an acceptor molecule must be introduced. The Coulomb binding energy of intermolecular CT states are calculated. It is shown that an intermolecular CT state of two π-stacked BBL oligomers does not exhibit a lower Coulomb binding energy as compared to the intramolecular binding energy. However, by a spatial separation of the donor and the acceptor molecule, in-line of the polymer backbone, the Coulomb binding energy is reduced from 0.40 eV to 0.24 eV. Combining such CT states with the high dielectric constant obtained by zwitterionic side-chains would lead to an exciton binding energy close to the thermal energy, resulting in spontaneous free carrier generation on neat materials. This could potentially reduce the voltage losses and increase the PCE in OPV devices significantly. / Die organische Photovoltaik stellt eine kostengünstige, erneuerbare und daher zukunftsgerichtete Energieversorgung dar. Die Umwandlungseffizienz organischer Solarzellen von Sonnenenergie in elektrische Energie konnte über die letzten fünf Jahre auf 12% verdoppelt werden. Kommerziell erhältliche anorganische Solarzellen weisen im Vergleich dazu eine Effizienz von ca. 20% auf. Eine Möglichkeit, die Effizienz organischer Solarzellen zu erhöhen, ist die Umwandlung von Licht in Elektrizität nicht nur im sichtbaren Bereich, sondern zusätzlich auch im infraroten Bereich des Sonnenspektrums. Der größte Unterschied zwischen den organischen und anorganischen Solarzellen liegt allerdings in der Exzitonbindungsenergie, welche in organischen Materialien ca. 20 Mal größer ist. Um das Exziton in freie Ladungsträger zu trennen, wird in organischen Solarzellen deshalb ein Donator-Akzeptor-Übergang benutzt, welcher unter anderem auch für den Spannungs- und damit für den Effizienzverlust von organischen Solarzellen verantwortlich ist. Im ersten Teil der Dissertation werden verschiedene funktionalisierte Donator-Moleküle, die infrarotes Licht absorbieren, untersucht. Die Donator-Moleküle ohne zusätzliche Funktionalisierungsgruppe weisen dabei die höchste Umwandlungseffizienz auf. In den besten Zellen kann ein Unterschied zwischen der optischen und effektiven \"Bandlücke\" von 0,17 eV gemessen werden. Dieser Unterschied stellt die treibende Kraft für den Übergang des Elektrons vom Donator zum Akzeptor dar. Da jedoch dieser Unterschied in der besten Solarzelle am geringsten ist, scheint die Dissoziation der Ladungsträger in den untersuchten Donator-Akzeptor-Systemem nicht vom ihm abzuhängen. Die gemessene relative hohe Leerlaufspannung von 0,81 V ist 0,74 V kleiner als die effektive Bandlücke und zeigt die hohen Spannungsverluste organischer Solarzellen. Die Spannungsverluste anorganischer Solarzellen liegen im Bereich von 0,4 V. Ein Ansatz, um die Spannungsverluste zu verkleinern, liegt in der Reduzierung der Exzitonbindungsenergie, woraus ein größeres Exziton erfolgt. Mit der zeitabhängigen Dichtefunktionaltheorie wird an einer Reihe organischer Moleküle gezeigt, dass die Exzitongröße bei einer Moleküllänge (oder Konjugationslänge) größer als 4nm bei 1,2nm sättigt. Für das größte Exziton, welches im Leiterpolymer Poly(benzimidazobenzophenanthroline) (BBL) vorhanden ist, wird eine Coulomb-Bindungsenergie von 0,4 eV berechnet und eine Exzitonbindungsenergie von 0,2 eV abgeschätzt. Die Exzitonbindungsenergie kann entweder durch Erhöhung der Dielektrizitätskonstante oder durch Erzeugung eines Ladungstransfer-Zustandes weiter verringert werden. Es wird gezeigt, dass mit einer neu entwickelten Methode auf Basis der Dichtefunktionaltheorie die ionischen und elektronischen Beiträge zur dielektrischen Funktion von BBL berechnet werden können. Die berechneten anisotropen Werte stimmen gut mit Werten aus Ellipsometriemessungen überein. Entlang der Polymerkette erhalten wir eine hohe Dielektrizitätskonstante von 8,3 und senkrecht dazu von ca. 3. Die hohe Dielektrizitätskonstante entlang der Polymerkette kann auf die starke Delokalisation der π-Elektronen zurückgeführt werden. Der Mittelwert der Dielektrizitätskonstante wird durch die ionischen Beiträge von 3,6 auf 4,2 erhöht. Um die Dielektrizitätskonstante weiter zu erhöhen, werden verschiedene polare Seitenketten am BBL-Polymer angebracht und die Dielektrizitätskonstante berechnet. Es wird gezeigt, dass die Anbringung einer zwitterionischen Seitenkette am BBL-Monomer die Dielektrizitätskonstante auf 17 erhöht. Um die Exzitonbindungsenergie durch einen Ladungstransfer-Zustand zu verringern, werden ein Donator- und ein Akzeptor-Molekül benötigt. Die Coulomb-Bindungsenergien der intermolekularen Ladungstransfer-Zustände werden berechnet. Es wird gezeigt, dass intermolekulare Ladungstransfer-Zustände zwischen zwei π-gestapelten BBL-Oligomeren keine Verringerung der Coulomb-Bindungsenergie bewirken. Bei einer räumlichen Trennung des Donator- und Akzeptor-Moleküls entlang der Polymerkette kann die Coulomb-Bindungsenergie von 0,40 eV auf 0,24 eV gesenkt werden. Eine Kombination aus diesem Ladungstransfer und der Erhöhung der Dielektirizitätskonstante durch zwitterionische Seitenketten kann zu einer niedrigen Exzitonbindungsenergie, nahe der thermischen Energie, und damit zu freien Ladungsträgern führen. Der damit verringerte Spannungsverlust kann die Umwandlungseffizienz organischer Solarzellen signifikant erhöhen.

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Many electronic products of today utilize some form of touch technology. Looking at everything from smartphone screens to ticket vending machines, it is obvious that the number of applications is big and the demand is huge. Touch technologies generally require no force to use, which reduces mechanical wear-and-tear and thus increases their lifespan. In this thesis, a touch system was constructed to control RGB LEDs. The sensor surface was made from a white, semi-clear plastic, through which the LEDs’ light should be visible. Since the plastic both needed to transmit visible light and act as a touch surface, a problem arose: how do you construct a transparent touch sensor that can control RGB LEDs in a reliable way? Firstly, this thesis describes and discusses many of the different available touch technologies and their strengths and weaknesses. From this information, a specific sensor technology was chosen, from which a prototype of the transparent touch sensor was built. The sensor prototype was a capacitive sensor, made from a thin metallic mesh, placed on the back of the plastic surface. Using an embedded system, based on a differential capacitance touch IC and a microcontroller, the capacitance of the sensor was measured and converted into signals which controlled the LEDs. In order to ensure the sensor’s reliability, the environmental factors which affected the sensor had to be determined and handled. To do this, measurements were performed on the sensor to see how its capacitance changed with environmental changes. It was concluded that moisture, temperature and frequency had negligible effect on the sensor’s dielectric properties. However, it was discovered that proximity to ground greatly affected the sensor and that the sensor was significantly dependent on its enclosure and grounding. / Många av de elektronikprodukter som produceras idag använder någon form av touchteknik. Då den används i allt från skärmar på smartphones till biljettautomater är det tydligt att användningsområdena är många och att efterfrågan är stor. Touchtekniker kräver i regel ingen kraft för att användas, vilket minskar mekaniskt slitage och därför ökar dess livslängd. I detta arbete skulle en touchstyrning till en uppsättning RGB-lysdioder byggas. Problemet var att sensorytan skulle vara en vit, halvgenomskinlig plast, genom vilken lysdioderna skulle lysa. Eftersom plasten både skulle släppa igenom ljus och agera touchyta uppstod problemet: hur konstruerar man en genomskinlig touchsensor som kan styra RGBlysdioder på ett pålitligt sätt? Denna rapport inleds med att beskriva och diskutera många av de touchtekniker som finns idag samt vilka föroch nackdelar de har. Utifrån denna information valdes en specifik sensorteknik, varifrån en prototyp på den genomskinliga touchsensorn byggdes. Sensorprototypen var en kapacitiv sensor uppbyggd av ett tunt metallnät placerat bakom plastpanelen. Med ett inbyggt system, bestående av en integrerad touchkrets för differentiell kapacitansmätning och en mikrokontroller, mättes sensorns kapacitans och en styrning till lysdioderna implementerades. För att säkerställa sensorns pålitlighet var det viktigt att analysera vilka miljöfaktorer som påverkade sensorn och hur de kunde hanteras. Mätningar utfördes därför på sensorn för att se hur dess kapacitans förändrades med avseende på dessa. Det kunde konstateras att fukt, temperatur och frekvens hade försumbar påverkan på sensorns dielektrum. Däremot kunde det visas att närhet till jordplan påverkade sensorn avsevärt och att sensorns tillförlitlighet berodde signifikant på dess inkapsling och jordning.