Espectroscopia vibracional e propriedades estruturais das chalconas (3E)-4-[4-(dimetilamina) fenil]but-3-en-2-ona e (3R)-3-(4-clorofenil)-3-hidroxi-1-(2-hidroxifenil)propan-1-ona
| Ano de defesa: | 2022 |
|---|---|
| Autor(a) principal: | |
| Orientador(a): | |
| Banca de defesa: | |
| Tipo de documento: | Tese |
| Tipo de acesso: | Acesso aberto |
| Idioma: | por |
| Instituição de defesa: |
Não Informado pela instituição
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| Programa de Pós-Graduação: |
Não Informado pela instituição
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| Departamento: |
Não Informado pela instituição
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| País: |
Não Informado pela instituição
|
| Palavras-chave em Português: | |
| Link de acesso: | http://www.repositorio.ufc.br/handle/riufc/71072 |
Resumo: | In this work, a systematic study of the vibrational and structural properties of two chalcones, (3E)-4- [ 4- ( dimethylamino ) phenyl ] but-3-en-2-one, C12H15NO (DMAP) and 3-(4- chlorophenyl ) – 3 – hydroxy – 1 - (2-hydroxyphenyl) propano -1- one, C15H13ClO3 (DIHYDROCHAL), were done. The molecules were synthesized, crystallized and characterized by single crystal X-ray diffraction (XRD), Fourier transform Raman spectroscopy (FT-Raman), attenuated total reflection Fourier transform infrared spectroscopy (ATR-FTIR) and ultraviolet-visible (UV-Vis) spectroscopy. Theoretical quantum chemistry calculations were performed to obtain data on vibration normal modes, the dipole moment, border molecular orbitals, quantum chemical parameters (HOMO-LUMO, energy gap, ionization energy, electron affinity, chemical potential, among others), molecular electrostatic potential map, Hirshfeld surfaces and theoretical UV-vis spectrum. DMAP chalcone has only one aromatic ring, in contrast to most chalcones which are formed by two aromatic rings. The DMAP crystal, at T = 300 K, presents orthorhombic symmetry and space group P212121 with four molecules per unit cell and structural parameters: a = 6.2440(7) Å, b = 7.3723(8) Å, c = 23.627(3) Å. The crystalline structure of DMAP is stabilized by two short intermolecular contacts, both involving the dimethylamine group. The chalcone DIHYDROCHAL presents a monoclinic crystalline structure at room temperature with space group P21/c with four molecules per unit cell and with the following structural parameters: a = 9.8661(11) Å, b = 5.5235(6) Å, c = 24.930(3) Å and β =94.83°. In the direction of the crystallographic a axis, the molecules are arranged in such a way that they form layers. The crystalline structure of DIHYDROCHAL is stabilized by two intermolecular hydrogen bonds involving chloride and carbonyl (C2-H2...Cl and C8-H8...O1). It is also noted that in the crystallographic direction of the a axis, the molecules are arranged forming layers. Through first principle calculations, it was possible to identify most of the normal modes of vibration of the two chalcones. A study of the vibrational modes of DIHYDROCHAL as a function of hydrostatic pressure was also carried out, with changes in the external modes being observed – low-frequency region – which were interpreted as na indication of the occurrence of a structural phase transition between 0.47 and 0, 82 GPa. From the analysis of some of the internal modes, it was possible to infer that the phase transition involves the A ring, since the frequencies of modes associated with vibrations of atoms in this structure suffer discontinuity in the same pressure range. |
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Romeu, Mairton CavalcanteFreire, Paulo de Tarso Cavalcante2023-03-02T19:35:51Z2023-03-02T19:35:51Z2022ROMEU, M. C. Espectroscopia vibracional e propriedades estruturais das chalconas (3E)-4-[4-(dimetilamina) fenil]but-3-en-2-ona e (3R)-3-(4-clorofenil)-3-hidroxi-1-(2-hidroxifenil)propan-1-ona. 2022. 132 f. Tese (Doutorado em Física: Física da Matéria Condensada) - Centro de Ciências, Universidade Federal do Ceará, Fortaleza, 2022.http://www.repositorio.ufc.br/handle/riufc/71072In this work, a systematic study of the vibrational and structural properties of two chalcones, (3E)-4- [ 4- ( dimethylamino ) phenyl ] but-3-en-2-one, C12H15NO (DMAP) and 3-(4- chlorophenyl ) – 3 – hydroxy – 1 - (2-hydroxyphenyl) propano -1- one, C15H13ClO3 (DIHYDROCHAL), were done. The molecules were synthesized, crystallized and characterized by single crystal X-ray diffraction (XRD), Fourier transform Raman spectroscopy (FT-Raman), attenuated total reflection Fourier transform infrared spectroscopy (ATR-FTIR) and ultraviolet-visible (UV-Vis) spectroscopy. Theoretical quantum chemistry calculations were performed to obtain data on vibration normal modes, the dipole moment, border molecular orbitals, quantum chemical parameters (HOMO-LUMO, energy gap, ionization energy, electron affinity, chemical potential, among others), molecular electrostatic potential map, Hirshfeld surfaces and theoretical UV-vis spectrum. DMAP chalcone has only one aromatic ring, in contrast to most chalcones which are formed by two aromatic rings. The DMAP crystal, at T = 300 K, presents orthorhombic symmetry and space group P212121 with four molecules per unit cell and structural parameters: a = 6.2440(7) Å, b = 7.3723(8) Å, c = 23.627(3) Å. The crystalline structure of DMAP is stabilized by two short intermolecular contacts, both involving the dimethylamine group. The chalcone DIHYDROCHAL presents a monoclinic crystalline structure at room temperature with space group P21/c with four molecules per unit cell and with the following structural parameters: a = 9.8661(11) Å, b = 5.5235(6) Å, c = 24.930(3) Å and β =94.83°. In the direction of the crystallographic a axis, the molecules are arranged in such a way that they form layers. The crystalline structure of DIHYDROCHAL is stabilized by two intermolecular hydrogen bonds involving chloride and carbonyl (C2-H2...Cl and C8-H8...O1). It is also noted that in the crystallographic direction of the a axis, the molecules are arranged forming layers. Through first principle calculations, it was possible to identify most of the normal modes of vibration of the two chalcones. A study of the vibrational modes of DIHYDROCHAL as a function of hydrostatic pressure was also carried out, with changes in the external modes being observed – low-frequency region – which were interpreted as na indication of the occurrence of a structural phase transition between 0.47 and 0, 82 GPa. From the analysis of some of the internal modes, it was possible to infer that the phase transition involves the A ring, since the frequencies of modes associated with vibrations of atoms in this structure suffer discontinuity in the same pressure range.Neste trabalho foi realizado um estudo sistemático das propriedades vibracionais e estruturais de duas chalconas, a (3E)-4-[4-(dimetilamina)fenil]but-3-en-2-ona, C12H15NO (DMAP) e a 3- (4-clorofenil) -3-hidroxi-1-(2-hidroxifenil) propan-1-ona, C15H13ClO3 (DIHIDROCHAL). As moléculas foram sintetizadas, cristalizadas e caracterizadas por difração de raios-X de monocristal (DRX), espectroscopia Raman por transformada de Fourier (FT-Raman), espectroscopia de infravermelho por transformada de Fourier de reflexão total atenuada (ATR- FTIR) e espectroscopia ultravioleta-visível (UV-Vis). Cálculos teóricos de química quântica foram realizados para se obter dados sobre os modos normais de vibração, o momento dipolar, orbitais moleculares de fronteira, parâmetros químicos quânticos (HOMO-LUMO, gap de energia, energia de ionização, afinidade eletrônica, potencial químico, entre outros), mapa de potencial eletrostático molecular, superfícies de Hirshfeld e espectro UV-vis teórico. A chalcona DMAP apresenta apenas um anel aromático, em contraste com a maioria das chalconas que são formadas por dois anéis aromáticos. O cristal da DMAP, a T = 300 K, apresenta simetria ortorrômbica e grupo espacial P212121 com quatro moléculas por célula unitária e parâmetros estruturais: a = 6,2440(7) Å, b = 7,3723(8) Å, c = 23,627(3) Å. A estrutura cristalina do DMAP é estabilizada por dois contatos intermoleculares curtos, ambos envolvendo o grupo dimetilamina. A chalcona DIHIDROCHAL apresenta estrutura cristalina monoclínica à temperatura ambiente com grupo espacial P21/c com quatro moléculas por célula unitária e com os seguintes parâmetros estruturais: a = 9,8661(11) Å, b = 5,5235(6) Å, c = 24,930(3) Å e β =94,83°. Na direção do eixo cristalográfico a, as moléculas são dispostas de tal maneira que formam camadas. Já a estrutura cristalina do DIHIDROCHAL é estabilizada por duas ligações de hidrogênio intermoleculares envolvendo cloreto e carbonila (C2-H2...Cl e C8-H8...O1). Nota-se também que na direção cristalográfica do eixo a, as moléculas estão dispostas formando camadas. Através de cálculos de primeiros princípios foi possível identificar a maioria dos modos normais de vibração das duas chalconas. Realizou-se também um estudo dos modos vibracionais da DIHIDROCHAL em função da pressão hidrostática, tendo sido observadas alterações nos modos externos – região de baixas frequências – que foram interpretadas como indício da ocorrência de uma transição de fase estrutural entre 0,47 e 0,82 GPa. Da análise de alguns dos modos internos foi possível inferir que a transição de fase envolve o anel A, uma vez que as frequências de modos associados a vibrações de átomos dessa estrutura sofrem descontinuidades no mesmo intervalo de pressão.ChalconasTeoria do Funcional da DensidadeEspectroscopia vibracional e propriedades estruturais das chalconas (3E)-4-[4-(dimetilamina) fenil]but-3-en-2-ona e (3R)-3-(4-clorofenil)-3-hidroxi-1-(2-hidroxifenil)propan-1-onainfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/doctoralThesisporreponame:Repositório Institucional da Universidade Federal do Ceará (UFC)instname:Universidade Federal do Ceará (UFC)instacron:UFCinfo:eu-repo/semantics/openAccessLICENSElicense.txtlicense.txttext/plain; charset=utf-81748http://repositorio.ufc.br/bitstream/riufc/71072/10/license.txt8a4605be74aa9ea9d79846c1fba20a33MD510ORIGINAL2022_tese_mcromeu.pdf2022_tese_mcromeu.pdfapplication/pdf9880000http://repositorio.ufc.br/bitstream/riufc/71072/11/2022_tese_mcromeu.pdf16527a2623406f056f256e4d619953c5MD511riufc/710722023-03-02 16:37:09.197oai:repositorio.ufc.br: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Repositório InstitucionalPUBhttp://www.repositorio.ufc.br/ri-oai/requestbu@ufc.br || repositorio@ufc.bropendoar:2023-03-02T19:37:09Repositório Institucional da Universidade Federal do Ceará (UFC) - Universidade Federal do Ceará (UFC)false |
| dc.title.pt_BR.fl_str_mv |
Espectroscopia vibracional e propriedades estruturais das chalconas (3E)-4-[4-(dimetilamina) fenil]but-3-en-2-ona e (3R)-3-(4-clorofenil)-3-hidroxi-1-(2-hidroxifenil)propan-1-ona |
| title |
Espectroscopia vibracional e propriedades estruturais das chalconas (3E)-4-[4-(dimetilamina) fenil]but-3-en-2-ona e (3R)-3-(4-clorofenil)-3-hidroxi-1-(2-hidroxifenil)propan-1-ona |
| spellingShingle |
Espectroscopia vibracional e propriedades estruturais das chalconas (3E)-4-[4-(dimetilamina) fenil]but-3-en-2-ona e (3R)-3-(4-clorofenil)-3-hidroxi-1-(2-hidroxifenil)propan-1-ona Romeu, Mairton Cavalcante Chalconas Teoria do Funcional da Densidade |
| title_short |
Espectroscopia vibracional e propriedades estruturais das chalconas (3E)-4-[4-(dimetilamina) fenil]but-3-en-2-ona e (3R)-3-(4-clorofenil)-3-hidroxi-1-(2-hidroxifenil)propan-1-ona |
| title_full |
Espectroscopia vibracional e propriedades estruturais das chalconas (3E)-4-[4-(dimetilamina) fenil]but-3-en-2-ona e (3R)-3-(4-clorofenil)-3-hidroxi-1-(2-hidroxifenil)propan-1-ona |
| title_fullStr |
Espectroscopia vibracional e propriedades estruturais das chalconas (3E)-4-[4-(dimetilamina) fenil]but-3-en-2-ona e (3R)-3-(4-clorofenil)-3-hidroxi-1-(2-hidroxifenil)propan-1-ona |
| title_full_unstemmed |
Espectroscopia vibracional e propriedades estruturais das chalconas (3E)-4-[4-(dimetilamina) fenil]but-3-en-2-ona e (3R)-3-(4-clorofenil)-3-hidroxi-1-(2-hidroxifenil)propan-1-ona |
| title_sort |
Espectroscopia vibracional e propriedades estruturais das chalconas (3E)-4-[4-(dimetilamina) fenil]but-3-en-2-ona e (3R)-3-(4-clorofenil)-3-hidroxi-1-(2-hidroxifenil)propan-1-ona |
| author |
Romeu, Mairton Cavalcante |
| author_facet |
Romeu, Mairton Cavalcante |
| author_role |
author |
| dc.contributor.author.fl_str_mv |
Romeu, Mairton Cavalcante |
| dc.contributor.advisor1.fl_str_mv |
Freire, Paulo de Tarso Cavalcante |
| contributor_str_mv |
Freire, Paulo de Tarso Cavalcante |
| dc.subject.por.fl_str_mv |
Chalconas Teoria do Funcional da Densidade |
| topic |
Chalconas Teoria do Funcional da Densidade |
| description |
In this work, a systematic study of the vibrational and structural properties of two chalcones, (3E)-4- [ 4- ( dimethylamino ) phenyl ] but-3-en-2-one, C12H15NO (DMAP) and 3-(4- chlorophenyl ) – 3 – hydroxy – 1 - (2-hydroxyphenyl) propano -1- one, C15H13ClO3 (DIHYDROCHAL), were done. The molecules were synthesized, crystallized and characterized by single crystal X-ray diffraction (XRD), Fourier transform Raman spectroscopy (FT-Raman), attenuated total reflection Fourier transform infrared spectroscopy (ATR-FTIR) and ultraviolet-visible (UV-Vis) spectroscopy. Theoretical quantum chemistry calculations were performed to obtain data on vibration normal modes, the dipole moment, border molecular orbitals, quantum chemical parameters (HOMO-LUMO, energy gap, ionization energy, electron affinity, chemical potential, among others), molecular electrostatic potential map, Hirshfeld surfaces and theoretical UV-vis spectrum. DMAP chalcone has only one aromatic ring, in contrast to most chalcones which are formed by two aromatic rings. The DMAP crystal, at T = 300 K, presents orthorhombic symmetry and space group P212121 with four molecules per unit cell and structural parameters: a = 6.2440(7) Å, b = 7.3723(8) Å, c = 23.627(3) Å. The crystalline structure of DMAP is stabilized by two short intermolecular contacts, both involving the dimethylamine group. The chalcone DIHYDROCHAL presents a monoclinic crystalline structure at room temperature with space group P21/c with four molecules per unit cell and with the following structural parameters: a = 9.8661(11) Å, b = 5.5235(6) Å, c = 24.930(3) Å and β =94.83°. In the direction of the crystallographic a axis, the molecules are arranged in such a way that they form layers. The crystalline structure of DIHYDROCHAL is stabilized by two intermolecular hydrogen bonds involving chloride and carbonyl (C2-H2...Cl and C8-H8...O1). It is also noted that in the crystallographic direction of the a axis, the molecules are arranged forming layers. Through first principle calculations, it was possible to identify most of the normal modes of vibration of the two chalcones. A study of the vibrational modes of DIHYDROCHAL as a function of hydrostatic pressure was also carried out, with changes in the external modes being observed – low-frequency region – which were interpreted as na indication of the occurrence of a structural phase transition between 0.47 and 0, 82 GPa. From the analysis of some of the internal modes, it was possible to infer that the phase transition involves the A ring, since the frequencies of modes associated with vibrations of atoms in this structure suffer discontinuity in the same pressure range. |
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2022 |
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2022 |
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2023-03-02T19:35:51Z |
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ROMEU, M. C. Espectroscopia vibracional e propriedades estruturais das chalconas (3E)-4-[4-(dimetilamina) fenil]but-3-en-2-ona e (3R)-3-(4-clorofenil)-3-hidroxi-1-(2-hidroxifenil)propan-1-ona. 2022. 132 f. Tese (Doutorado em Física: Física da Matéria Condensada) - Centro de Ciências, Universidade Federal do Ceará, Fortaleza, 2022. |
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ROMEU, M. C. Espectroscopia vibracional e propriedades estruturais das chalconas (3E)-4-[4-(dimetilamina) fenil]but-3-en-2-ona e (3R)-3-(4-clorofenil)-3-hidroxi-1-(2-hidroxifenil)propan-1-ona. 2022. 132 f. Tese (Doutorado em Física: Física da Matéria Condensada) - Centro de Ciências, Universidade Federal do Ceará, Fortaleza, 2022. |
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