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Iniciação Científica I – F590
01/06/2009
Espectroscopia Atômica
Orientador: Prof. Dr. Carlos Alberto Luengo
([email protected]) Aluno: Danilo José de Lima, RA 032118 (djlima_fí[email protected])
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ÍNDICE
Introdução................................................................................................................... 3
Espectrômetro ótico .................................................................................................... 4
Calibração ................................................................................................................... 4
Experimental............................................................................................................... 6
Série de Balmer......................................................................................................... 7
Constante de Wien .................................................................................................. 11
Arco numa lâmpada ................................................................................................ 14
Conclusão .................................................................................................................. 18
Referências Bibliográficas ........................................................................................ 19
Apêndice A: Softwares.............................................................................................. 20
Apêndice B: Dados dos espectrômetros ................................................................... 21
Apêndice C: Criando Arco elétrico em casa ............................................................ 24
Apêndice D: Demais dados ....................................................................................... 26
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Introdução O uso de espectrômetro ótico eletrônico é atualmente comum para se retirar
informações a respeito do comportamento eletrônico dos átomos, porém compreender
corretamente os resultados obtidos, verificar conseqüências dos resultados além de
entender o funcionamento dos espectrômetros é uma tarefa que nem sempre os alunos
realizam. Como esse assunto é extremamente longo, foram feitas várias medidas e mais
sugestões que experimentos, incluindo sugestões de como aplicar este assunto no ensino
médio.
A primeira parte teria como objetivo familiarizar-se com o equipamento bem
como os conceitos básicos envolvidos, tais como entender o funcionamento do
espectrômetro ótico utilizado, obter alguns resultados já descritos na literatura tais como
a série de Balmer para o átomo de Hidrogênio, o valor da constante de Rydberg, estudar
o espectro de emissão de um corpo aquecido encontrando a constante de Wien entre
outras aplicações que possam surgir com o decorrer dos estudos. Além disso, dispõe-se
de um software para aquisição de dados dos espectrômetros capaz de realizar a
aquisição de dados dos espectrômetros também no tempo, desta forma pode-se estudar a
variação da intensidade das linhas com o tempo, o que pode ser usado para o estudo da
variação da temperatura de um corpo em função do tempo, entre outras possibilidades.
Uma outra característica que diferencia o equipamento a ser utilizado dos
espectrômetros óticos disponíveis nos laboratórios de ensino do IFGW é a resolução.
No laboratório de ensino de física moderna dispõe-se de um espectrômetro ótico com
2048 pixel de resolução na CCD que faz a captura do espectro de radiação visível, já
aqui iremos utilizar três espectrômetros, onde cada um varre uma região um pouco
maior do que um terço da região do visível, oferecendo ao todo uma resolução de quase
três vezes mais que no espectrômetro disponível no laboratório de ensino. Pesquisas
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financiadas pela FAPESP estão utilizando este equipamento bem como os softwares
aqui apresentados. Desta forma, o objetivo deste trabalho é, também, introduzir o
assunto ao estudante para que possa aplicar seus conhecimentos nas pesquisas a serem
realizadas.
A segunda parte do estudo, que está sugerida para a sequência desta disciplina,
em Iniciação Científica II, seria um estudo mais teórico, que poderia utilizar os dados
obtidos no trabalho anterior para estudar o espectro de vibração das moléculas. Não
entraremos em detalhe sobre este assunto aqui.
Espectrômetro ótico Três espectrômetros ópticos da Ocean Optics® de alta resolução modelo
HR2000+ cuja aquisição da intensidade da radiação eletromagnética é feita por uma
CCD. As características deles são idênticas, a menos da região de sensibilidade a
determinados comprimentos de onda. Dados específicos dos espectrômetros se
encontram no apêndice B.
Calibração Os equipamentos utilizados já estão calibrados, e para verificar isto foram feitos
alguns espectros e comparados com dados bibliográficos. O modelo de espectrômetro
utilizado permite que armazenemos os valores dos coeficientes da calibração, conforme
manual do equipamento4, no próprio equipamento. Para ilustrar isso, utilizamos um
espectrômetro do laboratório de física moderna, de outro modelo, no qual inserimos os
valores dos coeficientes obtidos no software da Ocean, utilizando o mesmo
procedimento que seria usado para calibrar os espectrômetros utilizados durante os
experimentos. Neste caso, como comentado na introdução, teríamos apenas um
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espectrômetro de resolução de 2048 pixels obtendo o espectro da figura 01 para uma
lâmpada de gás de Mercúrio e Argônio.
Figura 01 – Gráfico da contagem pelo canal do espectrômetro e valores esperados para os picos
Os valores esperados para cada um dos picos obtidos no experimento foram
obtidos também no site da Ocean4, que foi nossa principal referência. Com esses dados,
e seguindo o procedimento do manual, graficamos o valor esperado para determinado
pico vs a posição do pixel para o ponto e fizemos uma regressão para uma função
cúbica e obtivemos os coeficientes da equação. Estes são os coeficientes a serem
inseridos no software e, se fosse o caso, seriam os inseridos nos espectrômetros que
foram usados neste trabalho. O gráfico e os resultados da regressão encontram-se na
figura 02.
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Figura 02 – Resultado da calibração: coeficientes do polinômio da regressão
Experimental A montagem experimental é bem simples: posicionamos o espectrômetro diante
de nossa fonte e o software faz a aquisição. A figura 03 mostra um esboço desse
experimento: o espectrômetro possui em sua saída uma fibra óptica com uma pequena
abertura que é direcionada para nossa fonte. No caso, uma lâmpada de gás (esta
lâmpada é trocada conforme interesse podendo termos várias opções, dentre elas
lâmpadas de Hg-Ar, H2, entre outras) fica de frente à fibra óptica.
Também adquirimos espectros de uma lâmpada fluorescente e de um sistema
melhor explicado no apêndice C, no qual apresentamos uma montagem experimental
simples, que poder ser realizada em sala de aula. Neste caso, foi apresentado à uma
turma de Ensino de Jovens e Adultos (EJA) onde os alunos tiveram grande aceitação e
interesse por querer entender porque e o que estava acontecendo. Neste caso,
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procuramos determinar qual gás é utilizado em uma lâmpada incandescente comum.
Também utilizamos uma lâmpada incandescente como fonte de calor para verificarmos
determinarmos a constante de Wien.
Espectrômetro
Fig.: 03 – Esquema da montagem experimental: a) o espectrômetro à esquerda com a fibra ótica
apontada para a fonte à direita; e a lâmpada b) preenchida de H2 mostrando a região de estrangulamento.
A ponta de prova do Espectrômetro é apontada para essa região, onde concentra uma maior densidade de
corrente e o arco é mais intenso. A lâmpada não precisa ser aquecida para produzir o arco.
Série de Balmer
Na física clássica, um sistema mecânico pode possuir qualquer valor de energia,
podendo variá-la de quantidades infinitesimais, no entanto na física quântica isto não é
observado. Existem inúmeros indícios de que um sistema quântico possa adquirir
apenas quantidades definidas de energia, sendo um exemplo disso, seria um elétron
aprisionado em uma barreira de potencial. A quantização pode ser mais facilmente
entendida se compreendermos que no mundo quântico as partículas se comportam como
pacotes de onda e se pensarmos que um elétron aprisionado é uma onda estacionária
com nós nos contornos da caixa e que a frequência dessa onda determina a energia do
elétron, podemos entender que ele pode receber uma quantidade definida de energia
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exatamente suficiente para mudar de modo de vibração. Como vemos em ondas
estacionárias, que podem adquirir apenas determinadas freqüências de vibração, um
elétron aprisionado também pode adquirir determinadas freqüências, e se sua energia
estiver relacionada apenas com sua freqüência ( νhE = ), então ele pode receber apenas
certas quantidades de energia múltiplas inteiras de determinado valor.
Foi Max Karl Ernst Ludwig Planck, um físico alemão, quem postulou que um
sistema físico em movimento harmônico simples, poderia apresentar apenas
determinados valores múltiplos de uma constante1, chamada constante de Planck:
…,3,2,1,0, == nnhE ν
Figura 04 – Energias possíveis para um sistema clássico e valores discretos de energia, segundo postulado de Planck
Na prática, só é possível verificar a quantização quando levamos em conta
interações a nível atômico, pois como o valor da constante de Planck é extremamente
pequeno ( sJxh .10311069626,6 34−= ) se compararmos com as energias que estamos
acostumados a encontrar. Por isso, para verificar a quantização de energia, usamos o
espectrômetro e uma lâmpada de Hidrogênio. O Hidrogênio é excitado e os seus
elétrons absorvem energia que, ao retornarem para seu estado fundamental, emite um
fóton de energia bem definida e, portanto, com freqüência também definida.
Para as regiões do Ultravioleta próximo e do visível, Johann Jakob Balmer, um
físico e matemático suíço, encontrou uma equação empírica que descreve o valor de λ
em função de um número inteiro n, com n>2 (n = 3, 4, 5, …). Utilizando a relação
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determinada por Balmer em 1985, obtemos o valor de λo, chamado de limite da série de
Balmer, quando n tende a infinito. A equação obtida por Balmer foi:
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2
−=
n
noλλ
Para obter o valor de λo utilizamos uma “lâmpada” que consiste de um bulbo
cilíndrico com uma região estrangula para concentrar o arco, representado também BA
figura 03, à direita. Em suas extremidades foi aplicada uma grande diferença de
potencial, da ordem de 10KV, capaz de excitar o elétron do átomo de Hidrogênio. O
espectro obtido está apresentado na (figura 05); a partir destes valores obtemos
λo = (365,1 ± 0,4) nm, cujo erro foi calculado com base no desvio padrão para os três
picos utilizados. O valor conhecido na época em que Balmer encontrou a relação da
série que levou seu nome era de 364,6nm1. Podemos obter, desse nosso resultado, o
valor da Constante de Rydberg reescrevendo a fórmula de Balmer:
Figura 05 – Valores discretos do espectro do Hidrogênio: Série de Balmer
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−=
−==
2222
1
2
141
2
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nonRk H
λλ
Sendo 2
.4
o
oRH
λ
δλδ
−= o erro da constante de Rydber e δλo o erro de λo. Assim,
temos: RH = (1096 ± 1).104 m-1. O valor com maior precisão medido até hoje1 foi de
RH = (10967757,6 ± 1,2) m-1 .
De nossos resultados, poderíamos prever outras séries para o hidrogênio. Assim,
obtemos o espectro do hidrogênio com maior tempo de integração para vermos as linhas
de menor comprimento de onda e comparamos os valores calculados com os valores
obtidos nesta medida. Os resultados são exibidos na figura 06. É possível verificar que o
valor medido sempre está acima do valor calculado, o que pode evidenciar um erro
sistemático na medida, no entanto não descobrimos sua causa. Observa-se também que
o menor ponto não está muito bem definido em relação a sua máxima intensidade, mas
acrescentamos esse valor mesmo assim apenas com o objetivo de comparação.
Figura 06 – Comprimentos de onda para a série de Balmer para o Hidrogênio: comparação entre comprimentos de onda medidos versus calculados com base na equação obtida anteriormente.
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Constante de Wien
Para medir a constante de Wien, precisa-se de uma fonte de calor muito intensa
(temperaturas acima de 700K). Como não dispomos de um pirômetro, ou outro
equipamento que pudesse ser utilizado para medir a temperatura do filamento da
lâmpada nos limitou apenas a estimar o valor da temperatura do filamento de tungstênio
de uma lâmpada de 100 w de potência. Utilizando um valor da literatura1 para a
constante de Wien ( KmxconstT .10898,2 3max
−==λ ), podemos obter para a temperatura
do filamento com a lâmpada em sua potência máxima o valor de 5431±1K, o que está
de acordo com dados experimentais para, por exemplo, a temperatura do Sol (5700K), o
que era de se esperar pois, é a faixa de luz visível.
Figura 07 – Filamento incandescente de tungstênio. A coloração avermelhada se deve pelo fato de ter sido tirada uma fotografia da projeção do filamento da lâmpada sobre uma parede, usando uma lente
divergente. Uma fotografia direta sem uso de filtro poderia danificar a máquina fotográfica se tirada foto com a lâmpada em sua potência máxima.
Figura 08 – Filamento da lâmpada desligada. É possível notar que o filamento se curva devido efeito de dilatação térmica.
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Figura 09 – Montagem experimental para medir a temperatura da lâmpada. Acima a lâmpada incandescente e abaixo a saída da fibra ótica dos espectrômetros.
Uma possibilidade avaliada seria determinar a temperatura da lâmpada em
função do tempo e estimar a condutividade térmica do gás no interior da lâmpada, pois
o software utilizado possibilita aquisição no tempo. Isso, porém não foi possível, pois a
queda de temperatura é muito rápida e mesmo utilizando a máxima capacidade de
aquisição (um espectro a cada 1 ms) não foi possível determinar essa queda. A figura 10
apresenta o gráfico obtido para o espectro da lâmpada em função do tempo, sendo a
lâmpada desligada algumas vezes durante a aquisição e a figura 11 apresenta uma
quatro medidas do espectro da lâmpada e média para valor máximo, bem como o erro
da medida.
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Figura 10 – Espectro da lâmpada em função do tempo. A reta vertical representa a contagem, a horizontal de 0 a 180 é o tempo e a outra é o comprimento de onda em nm.
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Figura 11 – Contagem nos espectrômetros em função do comprimento de onda em nm.
Arco numa lâmpada
Apresentamos algumas outras aplicações para a espectroscopia. A figura 12
apresenta o espectro de emissão de uma lâmpada de vapor de água em comparação com
a lâmpada de gás de Hidrogênio: nota-se que são praticamente iguais, evidenciando que
é possível determinar quais os átomos que compõe uma amostra de substância
desconhecida. Para comparar os resultados, selecionamos um tempo de integração de tal
forma que os valores dos picos para a água e para o Hidrogênio estejam próximos.
A figura 13 apresenta o espectro de uma lâmpada fria (de mercúrio) comercial.
Podemos notar que existe uma linha de comprimento de onda igual ao do comprimento
de onda do mercúrio. O revestimento branco da lâmpada é um composto de fósforo que
absorve a luz ultravioleta emitida pelo Mercúrio e a emite na região do visível.
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Figura 12 – Comparação entre os espectros de emissão de uma lâmpada de água e de uma de Hidrogênio
Figura 13 – Espectro de emissão de uma lâmpada de Mercúrio comercial (“lâmpada fria”)
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Figura 14 – Espectro de emissão de uma lâmpada de CO2
Outra medida realizada, que apresenta mais detalhe no apêndice C, foi do arco
produzido no interior de uma lâmpada incandescente, do mesmo tipo que a usada no
experimento para a lei de Wien. A seguir, os espectros obtidos e o arco produzido. Na
realidade não foi encontrado um gás que se coincidisse os valores de picos com os
obtidos neste experimento, assim comparamos visualmente com a bibliografia9. Neste
caso, não há rigor científico, mas só ousamos fazer isso, pois sabíamos previamente que
o gás contido na lâmpada é argônio. De fato, deve ser um gás inerte, que não reaja com
o filamento.
a) b) Figura 15 – (a) Arco elétrico obtido na lâmpada e (b) dado bibliográfico9.
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Conclusão Através de uma análise quantitativa, podemos verificar experimentalmente a
série de Balmer e o valor da constante de Rydberg, mostramos a utilidade de
espectrômetros óticos para determinar substâncias e uma forma possível de medirmos a
temperatura de materiais incandescente (que emitam radiação na frequência do visível).
Vimos que obter informações da matéria através do uso de técnicas de
espectroscopia é um método muito preciso e rápido. Dentre suas aplicações, podemos
citar a análise de materiais quando é preciso um resultado imediato, pois vimos que o
espectro de moléculas depende também dos átomos constituintes. Além disso, medimos
o espectro da água, do CO2, de uma lâmpada fria comercial e de uma lâmpada
incandescente.
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Referências Bibliográficas 1. Eisberg R., Resnick R., Física Quântica – Átomos, Moléculas, Sólidos, Núcleos e
Partículas, Editora Campus, 25ª tiragem, Rio de Janeiro, 1991. (pg. 23 – Lei de
Wien e constante de Wien; pg. 41 – fig. Comparando a quantização de energia
quântica com a correspondente contínua clássica; pg. 137 – constante de Rydberg
para o átomo de Hidrogênio)
2. Newton, I., Newton (Óptica), Nova Cultural, São Paulo, 2005.
3. N. M., Nusseinzveig, Curso de Física Básica, Vol. 4, Ed. Edgard Blücher, 1ª Ed.,
São Paulo, 1998. (pg. 245 – A hipótese de Planck; pg. 260 – Espectros atômicos –
Constante de Rydberg)
4. http://www.oceanoptics.com/, acessado em 22/02/2009. (Manual do equipamento
incluso e traduzido no apêndice B; Espectro da lâmpada usada para calibração do
espectrômetro. No manual, veja capítulo 1 e apêndices A e B)
5. http://www-rohan.sdsu.edu/staff/drjackm/chemistry/chemlink/analytic/analyt1.html,
acessado em 22/02/2009
6. Dalttrini, A. M., Estudo de arco a altas temperaturas por espectroscopia visível
e ultravioleta no vácuo, Tese de Doutorado, IFGW, Campinas, 2003.
7. http://www.fsc.ufsc.br/ccef/port/02-1/artpdf/a5.pdf, acessado 30/05/2009. Este
artigo mostra como pode ser montado um espectrômetro caseiro para usá-lo no
ensino médio.
8. A Invenção de Quantum de Energia segundo Planck,
http://www.sbfisica.org.br/rbef/pdf/v22_523.pdf, acessado em 30/05/2009.
9. Imagens dos espectros mais comuns http://www.schaffrath.net/Spectra/, Acessado
em 01/02/2009. Usado para comparação visual com o espectro da lâmpada
incandescente quando é gerado um arco no seu interior.
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Apêndice A: Softwares O algoritmo não poderá ser inserido, mas abaixo se encontra a aparência da
interface final. Ele foi construído na plataforma Labview.
Fig. A1: Aparência do programa de aquisição de dados.
Fig. A2: Os resultados são apresentados em três gráficos separadamente, depois exportados automaticamente como imagem.
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Apêndice B: Dados dos espectrômetros Na tabela a seguir, apresentamos a faixa de comprimento de onda em que cada
modelo trabalha. As demais características são iguais para todos eles.
Tabela 01: Range de comprimento de onda que cada modelo de espectrômetro é capaz de ler. Modelo do Espectrômetro Range de comprimento de onda (nm)
HR+C0163 188,1 - 412,7
HR+C0162 392,4 - 601,5
HR+C0244 587,5 - 783,3
As características que podem ser alteradas de acordo com a necessidade de uso
estão descritas com mais detalhe nos itens a seguir (tabelas de 02 à 04 e figura B1). Os
três espectrômetros foram ligados ao PC utilizando-se o software LabView®. Esta rotina
foi criada para fazer a aquisição de dados do espectrômetro ótico em um intervalo de
tempo.
Fig. B1: Componentes internos dos Espectrômetros óticos. Na tabela 02 encontram-se as características de cada item
http://www.oceanoptics.com
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Fig. B2 – Detalhe para os três espectrômetros utilizados
Tabela 02: Identificação dos itens da figura 01. Descrição e nome dos itens Item Nome Descrição
1 Conector SMAFixa a entrada da fibra ótica ao espectrômetro. A luz da entrada da
fibra entra no sistema ótico por este conector.
2 Fenda
Uma peça de material escuro contendo uma abertura retangular,
montado diretamente sobre o conector SMA. O tamanho da
abertura regula a intensidade luminosa que entra no sistema otico
e controla a resolução espectral.
3 Filtro
Restringe a radiação para uma região pré-determinada de
comprimentos de onda. A luz passa pelo filtro antes de entrar no
sistema ótico. Filtros passa banda e passa alta são utilizados para
restringir o a faixa de comprimento de onda à certa região.
4 Espelho colimador
A luz não colimada que entra no sistema otico é então colimada
pelo espelho até a Grade. A luz que entra no espectrômetro, passa
pelo conector SMA, pelo Slit , e pelo filtro e é refletida pelo espelho
até a Grade.
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Tabela 03: Especificações do CCD dos espectrômetros Especificações Valores
Detector Sony ILX-511 arranjo linear de CCD de silício
nº de elementos 2048 pixels
75 fotons por contagem a 400 nm
41 fotons por contagem a 600 nm
Tamanho do Pixel 14 mm x 200 mm
Intensidade por Pixel 62.500 eletrons
Razão de sinal : ruído 250:1 (em sinal máximo)
Resolução A/D 14 bit
Ruído Dark 12 RMS counts
Correção de linearidade >99,8%
Taxa máxima de pixel Taxa com cada pixel digitalizado: 1MHz
Sensibilidade
Tabela 04: Características dos espectrômetros. Especificações Valores
Dimensões 148,6 mm x 104,8 mm x 45,1 mm
Massa 570 g
Consumo de Energia 220 mA à 5VDC
Detector Arranjo de 2048 elementos de CCD linear de silício
Range do detector 200 - 1100 nm
Grade 14 grades disponíveisAbertura de Entrada 5, 10, 25, 50, 100 ou 200 mm
Filtros Filtros instalados: passa-alta e passa-banda
Distância focal f/4, 101 mm
Resolução optica
Depende da grade e do tamanho da abertura de
entrada
Dispersão luminosa <0,05% a 600 nm; <0,10% a 435 nm
Range dinâmico 2 x 108 (sistema); 1300:1 para uma aquisição simples
Conector da fibra optica SMA 905 para cabo simples de fibra optica (0,22 NA)
Tranferência de dados:
USB 2.0 Leitura completa para a memória a cada 1 ms
Porta Serial Leitura completa para a memória a cada 100 ms
Tempo de integração De 1 ms à 65 s
Canal analógico
Uma entrada analógica de 13 bit e uma saída
analógica de 9 bit
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Apêndice C: Criando Arco elétrico em casa Neste item, incluímos um experimento simples, focado à aplicação no ensino de
física: pode-se criar arco em sala de aula. Para isso, utilizamos um acendedor de fogão
automático, conhecido comercialmente como “usininha” e que pode ser encontrado em
qualquer loja que trabalhe com manutenção de fogão ou até mesmo em casas de
ferramentas em geral. Os demais itens são mais comuns: um receptáculo (ou bocal) para
lâmpada, uma lâmpada incandescente (quanto maior sua potência melhor, pois menor
deverá ser a pressão no seu interior além de ter o bulbo maior, possibilitando maiores
arcos – neste exemplo, foi usada uma de 200 w), fios, tomada macho, interruptor de
campainha e um suporte (por exemplo, madeira).
A seguir, na figura C1, o resultado do trabalho. Deve-se ligar um dos fios que sai
da “usininha” ao receptáculo e outro pode ser fixado com fita adesiva na superfície da
lâmpada. Outros experimentos podem ser criados, dentre eles fazer uma chave de fenda
de teste ascender na mão sem ser necessário tocar na lâmpada.
Figura C1 – Montagem experimental para produzir arco em casa.
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Figura C2 – Montagem experimental com saída do espectrômetro.
Figura C3 Arco formado no filamento da lâmpada.
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Apêndice D: Demais dados
Mercury emission lines are <600 nm. Argon emission lines are >600 nm, and are shown here on an exaggerated amplitude scale.
Strong Hg Emission Lines by Wavelength (nm)
User's Tip: There are more emission lines published here than printed on the label on the HG-1 housing. The label is intended as a quick, convenient reference and does not list every Ar or Hg emission line that exists.
253.652 404.656
296.728 407.783*
302.150 435.833
313.155 546.074**
334.148 576.960
365.015 579.066
* This spectral line will not be evident with spectrometers configured with 300- or 600-lines/mm gratings.
** With spectrometers that have 1200-, 1800-, 2400- or 3600-lines/mm gratings, spectral lines will be evident at 576.96 nm and 579.07 nm.
Strong Ar Emission Lines by Wavelength (nm)
696.543 800.616*
706.722 811.531
710.748 826.452
727.294 842.465
738.398 852.144
750.387 866.794
763.511 912.297
27
772.376 922.450
794.818
* This spectral line will be evident only with spectrometers configured with 1800-, 2400-, or 3600-lines/mm gratings.
Parecer Parece me que o aluno tem se esforçado bastante e conseguido demonstrações notáveis. Professor C.A.Luengo
1.
HR2000+ High-speed Fiber Optic Spectrometer
Installation and Operation Manual Document Number 294-00000-000-02-0208
Offices: Ocean Optics, Inc. World Headquarters
830 Douglas Ave., Dunedin, FL, USA 34698
Phone 727.733.2447
Fax 727.733.3962
8 a.m.– 8 p.m. (Mon-Thu), 8 a.m.– 6 p.m. (Fri) EST
E-mail: [email protected] (General sales inquiries)
[email protected] (Questions about orders)
[email protected] (Technical support)
Additional
Offices:
Ocean Optics Asia
666 Gubei Road, Kirin Tower, Suite 601B, Changning District, Shanghai,
PRC. 200336
Phone 86.21.5206.8686
Fax 86.21.5206.8686
E-Mail [email protected]
Ocean Optics B.V. (Europe)
Geograaf 24, 6921 EW DUIVEN, The Netherlands
Phone 31-(0)26-3190500
Fax 31-(0)26-3190505
E -Mail [email protected]
Copyright © 2001-2008 Ocean Optics, Inc. All rights reserved. No part of this publication may be reproduced, stored in a retrieval system, or transmitted, by any means, electronic,
mechanical, photocopying, recording, or otherwise, without written permission from Ocean Optics, Inc.
This manual is sold as part of an order and subject to the condition that it shall not, by way of trade or otherwise, be lent, re-sold, hired out or
otherwise circulated without the prior consent of Ocean Optics, Inc. in any form of binding or cover other than that in which it is published.
Trademarks
All products and services herein are the trademarks, service marks, registered trademarks or registered service marks of their respective owners.
Limit of Liability
Every effort has been made to make this manual as complete and as accurate as possible, but no warranty or fitness is implied. The information
provided is on an “as is” basis. Ocean Optics, Inc. shall have neither liability nor responsibility to any person or entity with respect to any loss or
damages arising from the information contained in this manual.
Table of Contents
About This Manual .......................................................................................................... iii
Document Purpose and Intended Audience.............................................................................. iii What’s New in this Document ................................................................................................... iii Document Summary.................................................................................................................. iii
Product-Related Documentation ..................................................................................... iii
Upgrades......................................................................................................................... iv
Chapter 1: Introduction ......................................................................1
Product Overview ............................................................................................................ 1
System Requirements ..................................................................................................... 2 EEPROM Utilization .................................................................................................................. 2 About SpectraSuite.................................................................................................................... 2 Sampling System Overview....................................................................................................... 2
How Sampling Works............................................................................................................ 2 Modular Sampling Accessories............................................................................................. 3
Interface Options ............................................................................................................. 3 Breakout Box ............................................................................................................................. 3
Shipment Components.................................................................................................... 4
Chapter 2: Installing the HR2000+.....................................................5
Overview ......................................................................................................................... 5
HR2000+ Installation ....................................................................................................... 5
Configuring the HR2000+ with OOIBase32 .............................................................................. 6 Operator and Serial Number Dialog Box .............................................................................. 6 Default Spectrometer Configuration File............................................................................... 6 Configure Hardware Screen ................................................................................................. 6 Spectrometer Configuration Screen...................................................................................... 7
Connect Spectroscopic Accessories ............................................................................... 8
External Triggering Options............................................................................................. 8
294-00000-000-02-0208 i
Table of Contents
Chapter 3: Troubleshooting ...............................................................9
Overview ......................................................................................................................... 9
HR2000+ Connected to PC Prior to Software Installation............................................... 9 Windows Operating Systems .................................................................................................... 9
Remove the Unknown Device from Windows Device Manager ........................................... 10 Remove Improperly Installed Files........................................................................................ 10
Mac Operating Systems ............................................................................................................ 11 Linux Operating Systems .......................................................................................................... 11
Older Version of OOIBase32 Installed ............................................................................ 11
Appendix A: Calibrating the Wavelength of the HR2000+...............13
Overview ......................................................................................................................... 13
About Wavelength Calibration......................................................................................... 13
Calibrating the Spectrometer........................................................................................... 14 Preparing for Calibration............................................................................................................ 14 Calibrating the Wavelength of the Spectrometer ...................................................................... 14
Saving the New Calibration Coefficients: USB Mode ...................................................... 16
Saving the New Calibration Coefficients: Serial Mode .................................................... 17
Appendix B: Specifications................................................................19
Overview ......................................................................................................................... 19
How the HR2000+ Works................................................................................................ 19 HR2000+ Components Table.................................................................................................... 20
HR2000+ Specifications .................................................................................................. 21 CCD Detector Specifications..................................................................................................... 21 HR2000+ Spectrometer............................................................................................................. 21
System Compatibility ....................................................................................................... 22
Compatibility for Desktop or Notebook PCs.............................................................................. 22
30-Pin Accessory Connector Pinout................................................................................ 23 30-Pin Accessory Connector Pinout Diagram........................................................................... 23 30-Pin Accessory Connector – Pin Definitions and Descriptions.............................................. 23 30-Pin J2 Accessory Connector - Part Numbers ...................................................................... 25
HR2000+ 15-Pin Accessory Cable Pinout....................................................................... 26
Index.....................................................................................................27
ii 294-00000-000-02-0208
About This Manual
Document Purpose and Intended Audience
This document provides the user of HR2000+ Spectrometer with instructions for setting up, calibrating
and performing experiments with their spectrometer.
What’s New in this Document
This version of the HR2000+ High-speed Fiber Optic Spectrometer, Installation and Operation Manual
updates the power consumption specification.
Document Summary
Chapter Description
Chapter 1: Introduction Contains descriptive information about the HR2000+ Spectrometer and how sampling works. It also provides a list of system requirements, interface options, and shipment components.
Chapter 2: Installing the HR2000+ Provides installation and configuration instructions.
Chapter 3: Troubleshooting Contains recommended steps to isolate and correct common problems.
Appendix A: Calibrating the
Wavelength of the HR2000+
Provides instructions for calibrating the HR2000+ Spectrometers.
Appendix B: Specifications Contains technical specifications and connector pinouts for the HR2000+ Spectrometers.
Product-Related Documentation You can access documentation for Ocean Optics products by visiting our website at
http://www.oceanoptics.com. Select Technical ! Operating Instructions, then choose the appropriate
document from the available drop-down lists. Or, use the Search by Model Number field at the bottom
of the web page.
! Detailed instructions for SpectraSuite Spectrometer Operating Software are located at:
http://www.oceanoptics.com/technical/SpectraSuite.pdf.
! Detailed instructions for the OOIBase32 Spectrometer Operating Software are located at:
http://www.oceanoptics.com/technical/ooibase32.pdf
294-00000-000-02-0208 iii
About This Manual
! Detailed instructions for the Breakout Box are located at:
http://www.oceanoptics.com/technical/HR4_breakout.pdf.
! Detailed instructions for External Triggering are located at:
http://www.oceanoptics.com/technical/external-triggering.pdf.
Engineering-level documentation is located on our website at Technical ! Engineering Docs.
You can also access operating instructions for Ocean Optics products from the Software and Technical
Resources CD that ships with the product.
Upgrades Occasionally, you may find that you need Ocean Optics to make a change or an upgrade to your system.
To facilitate these changes, you must first contact Customer Support and obtain a Return Merchandise
Authorization (RMA) number. Please contact Ocean Optics for specific instructions when returning a
product.
iv 294-00000-000-02-0208
Chapter 1
Introduction
Product Overview The HR2000+ High-Speed Miniature Fiber Optic Spectrometer provides optical resolution as good as
0.035 nm (FWHM). The HR2000+ is responsive from 200-1100 nm, but the specific range and resolution
depends on your grating and entrance slit selections. With its capability of transferring 1ms spectra
continuously, the HR2000+ is the fastest spectrometer available from Ocean Optics.
The HR2000+ is perfect for applications where fast reactions need to be monitored and high resolution is
necessary, such as chemistry and biochemistry applications.
Data programmed into a memory chip on each HR2000+ includes wavelength calibration coefficients,
linearity coefficients, and the serial number unique to each spectrometer. Our spectrometer operating
software simply reads these values from the spectrometer — a feature that enables hot swapping of
spectrometers among PCs.
The HR2000+ Spectrometer connects to a notebook or desktop PC via USB port or serial port. When
connected to the USB port of a PC, the HR2000+ draws power from the host PC, eliminating the need for
an external power supply.
Ocean Optics HR2000+ High-speed Fiber Optic Spectrometer
294-00000-000-02-0208 1
1: Introduction
System Requirements You can use the HR2000+’s USB connectivity with any PC that meets the following requirements:
! Windows 98/Me/2000/XP operating system (or Windows CE 2.11 or later for handheld PCs)
! Ocean Optics SpectraSuite or OOIBase32 software application installed and configured for use
with the HR2000+. See Chapter 2: Installing the HR2000+ for specific configuration
instructions.
Alternately, the HR2000+ has serial port adaptability for connecting to PCs, PLCs, and other devices that
support the RS-232 communication protocol. However, this connection method requires an external
power supply to power the HR2000+, the Breakout Box (HR4-BREAKOUT), and a serial cable.
EEPROM Utilization
An EEPROM memory chip in each HR2000+ contains wavelength calibration coefficients, linearity
coefficients, and a serial number unique to each individual spectrometer. The software application reads
these values directly from the spectrometer, enabling the ability to “hot-swap” spectrometers between PCs
without entering the spectrometer coefficients manually on each PC.
About SpectraSuite
SpectraSuite is the latest generation of operating software for all Ocean Optics spectrometers. It is a
completely modular, Java-based spectroscopy software platform that operates on Windows, Macintosh
and Linux operating systems. The software can control any Ocean Optics USB spectrometer and device,
as well as any other manufacturer’s USB instrumentation using the appropriate drivers.
SpectraSuite is a user-customizable, advanced acquisition and display program that provides a real-time
interface to a variety of signal-processing functions. With SpectraSuite, you have the ability to perform
spectroscopic measurements (such as absorbance, reflectance, and emission), control all system
parameters, collect and display data in real time, and perform reference monitoring and time acquisition
experiments. Consult the SpectraSuite manual for hardware requirements when using SpectraSuite (see
Product-Related Documentation).
Sampling System Overview
How Sampling Works
Ocean Optics components function in a sampling system as follows:
1. The user stores reference and dark measurements to correct for instrument response variables.
2. The light transmits through an optical fiber to the sample.
3. The light interacts with the sample.
4. Another optical fiber collects and transmits the result of the interaction to the spectrometer.
5. The spectrometer measures the amount of light and transforms the data collected by the
spectrometer into digital information.
2 294-00000-000-02-0208
1: Introduction
6. The spectrometer passes the sample information to SpectraSuite.
7. SpectraSuite compares the sample to the reference measurement and displays processed spectral
information.
Modular Sampling Accessories
Ocean Optics offers a complete line of spectroscopic accessories for use with the HR2000+. Most of our
spectroscopic accessories have SMA connectors for application flexibility. Accordingly, changing the
sampling system components is as easy as unscrewing a connector and replacing an accessory.
Interface Options The HR2000+ has both USB and serial port connectors (with the use of an adapter), enabling you to
connect the spectrometer to a desktop or notebook PC via a USB port.
Computer Interface
Operating System Requirements
Part Needed Description of Part
Desktop or Notebook PC via USB Port
Windows 98/Me/ 2000/XP
USB-CBL-1 (included)
Cable that connects from USB port on HR2000+ to USB port on desktop or notebook PC
Desktop or Notebook PC via Serial Port
Any 32-bit Windows operating system
HR4-BREAKOUT (not included)
Adapter block that enables connection from serial port on HR2000+ to serial port on desktop or notebook PC; comes with 5 VDC power supply (required when connecting to serial port). User must supply own software.
Breakout Box
Ocean Optics also offers the Breakout Box (HR4-BREAKOUT), a passive module that separates the
signals from their 30-pin port to an array of standard connectors and headers, enabling easy access to a
variety of features found in Ocean Optics’ HR2000+ Spectrometer. In addition to the accessory
connector, the breakout box features a circuit board based on a neutral breadboard pattern that allows
custom circuitry to be prototyped on the board itself.
294-00000-000-02-0208 3
1: Introduction
Shipment Components The following information and documentation ships with the HR2000+ Spectrometer:
! Packing List
The packing list is inside a plastic bag attached to the outside of the shipment box (the invoice
arrives separately). It lists all items in the order, including customized components in the
spectrometer (such as the grating, detector collection lens, and slit). The packing list also includes
the shipping and billing addresses, as well as any items on back order.
! Spectrometer Installation Instructions
A sheet of paper that contains the information that you need to get your spectrometer system up
and running. Further information can be found on the Ocean Optics Software and Resources
Library CD (see below).
! Wavelength Calibration Data Sheet
Each spectrometer is shipped with a Wavelength Calibration Data Sheet that contains information
unique to your spectrometer. SpectraSuite reads this calibration data from your spectrometer
when it interfaces to a PC via the USB port. Any other interface requires that you manually enter
the calibration data in OOIBase32 (select Spectrometer | Configure | Wavelength Calibration
tab). See the OOIBase32 documentation for more information (refer to Product-Related
Documentation for instructions on accessing OOIBase32 documentation).
Note
Please save the Wavelength Calibration Data Sheet for future reference.
! Software and Technical Resources CD
Each order ships with the Ocean Optics Software and Technical Resources CD. This disc
contains software, operating instructions, and product information for all Ocean Optics software,
spectrometers, and spectroscopic accessories. You must have Adobe Acrobat Reader version 6.0
or higher to view these files. Ocean Optics includes the Adobe Acrobat Reader on the Software
and Technical Resources CD.
Ocean Optics software requires a password during the installation process. You can locate
passwords for the other software applications on the back of the Software and Resources Library
CD package.
4 294-00000-000-02-0208
Chapter 2
Installing the HR2000+
Overview You must install the software application prior to connecting the HR2000+ Spectrometer to the PC. The
software installation installs the drivers required for HR2000+ installation. If you do not install the
software first, the system will not properly recognize the HR2000+.
If you have already connected the HR2000+ to the PC prior to installing the software, consult Chapter 3:
Troubleshooting for information on correcting a corrupt HR2000+ installation.
HR2000+ Installation To connect the HR2000+ to a PC via the USB port, the PC must be running the Windows
98/ME/2000/XP operating system.
Note
The USB port on a PC can power up to five HR2000+ spectrometer channels. Systems
with more than five channels require a powered USB hub.
! Procedure
Follow the steps below to connect the HR2000+ to a PC via the USB port:
1. Install SpectraSuite on the destination computer.
2. Locate the USB cable (USB-CBL-1) provided with the HR2000+.
3. Insert the square end of the cable into the side of the HR2000+.
4. Insert the rectangular end of the cable into the USB port of the PC.
If you installed SpectraSuite prior to connecting the HR2000+, SpectraSuite installs the HR2000+ drivers.
If the drivers do not successfully install (or if you connected the HR2000+ to the PC before installing
SpectraSuite), consult Chapter 3: Troubleshooting.
If you have followed the previous steps and started SpectraSuite, the spectrometer is already acquiring
data. Even with no light in the spectrometer, there should be a dynamic trace displayed in the bottom of
the graph. If you allow light into the spectrometer, the graph trace should rise with increasing light
intensity. This means the software and hardware are correctly installed.
Note the spectrometer(s) that you have installed are listed in the Data Sources pane.
294-00000-000-02-0208 5
2: Installing the HR2000+
Once you install the SpectraSuite software and the hardware, and establish your sampling system, you are
ready to take measurements.
Configuring the HR2000+ with OOIBase32
Once you install the HR2000+ with OOIBase32 software, you must configure OOIBase32’s Configure
Spectrometer options so that OOIBase32 recognizes the HR2000+ Spectrometer. Consult the
OOIBase32 Spectrometer Operating Software Operating Instructions for detailed instructions on
configuring the spectrometer in OOIBase32 (see Product-Related Documentation).
The following sections contain instructions on initially configuring the HR2000+ the first time you start
OOIBase32. Additional features are available for this spectrometer. See the OOIBase32 Spectrometer
Operating Software Operating Instructions for detailed information on these HR2000+ features.
Operator and Serial Number Dialog Box
The Operator and Serial Number screen prompts you to enter a user name and software serial number
into OOIBase32. Some data files created by OOIBase32 during sampling procedures use this information
in the file headers.
Default Spectrometer Configuration File
The Default Spectrometer Configuration File screen prompts you to select a spectrometer configuration
(.SPEC) file for use with the HR2000+. The unique serial number of the HR2000+ precedes the file
extension (for example, HR2A0162.SPEC).
Navigate to the OOIBase32 installation directory and select the spectrometer configuration file.
Configure Hardware Screen
The Configure Hardware screen prompts you to enter spectrometer-specific information into
OOIBase32 the first time you run the program. Typically, you need only enter this information the first
time you run OOIBase32. However, you can alter the hardware configuration at any time using the
Spectrometer Configuration screen. Select Spectrometer | Configure from the OOIBase32 menu bar
to access the Spectrometer Configuration screen.
6 294-00000-000-02-0208
2: Installing the HR2000+
! Procedure
To configure hardware in USB Mode:
1. Specify S2000 in the Spectrometer Type drop-down menu.
2. Specify HR2000+ in the A/D Converter Type drop-down menu.
3. Specify the serial number of the HR2000+ under the USB Serial Number drop-down menu.
Note
The system pre-fills this drop-down menu with the serial numbers of all discovered
HR2000+ Spectrometers.
4. Click the OK button to accept the selected options.
5. The spectrometer should now be able to acquire data and respond to light. Exit and restart
OOIBase32 to save configuration data to disk.
Spectrometer Configuration Screen
The Spectrometer Configuration screen prompts you to configure specific channel-level spectrometer
information, if necessary.
! Procedure
1. Select Spectrometer | Configure from the menu and set system parameters.
2. Select the Wavelength Calibration tab. OOIBase32 pre-fills the coefficients for the HR2000+
from information on a memory chip in the spectrometer.
294-00000-000-02-0208 7
2: Installing the HR2000+
3. Verify that the calibration coefficients match the coefficients from the Wavelength Calibration
Data Sheet that accompanied the spectrometer. If necessary, modify these values using the USB
Programmer utility.
4. Additionally, ensure that you select both the Master and Channel Enabled boxes.
5. In the A/D Interface tab, enter the same values as in the Configure Hardware screen.
OOIBase32 stores this information for future use once you close the program.
Connect Spectroscopic Accessories To find operating instructions for HR2000+-compatible products (such as light sources, sampling
chambers, and probes), consult the Software and Technical Resources CD or the Ocean Optics website at
http://www.oceanoptics.com/technical/operatinginstructions.asp.
External Triggering Options You can trigger the HR2000+ using a variety of External Triggering options through the 30-pin
Accessory Connector on the spectrometer. See the External Triggering Options document located at
http://www.oceanoptics.com/technical/external-triggering.pdf. This document contains instructions
for configuring External Triggering options for the HR2000+.
8 294-00000-000-02-0208
Chapter 3
Troubleshooting
Overview The following sections contain information on troubleshooting issues you may encounter when using the
HR2000+ Spectrometer.
HR2000+ Connected to PC Prior to Software Installation
Windows Operating Systems
If you connected your Ocean Optics USB device to the computer prior to installing your Ocean Optics
software application, you may encounter installation issues that you must correct before your Ocean
Optics device will operate properly.
Follow the applicable steps below to remove the incorrectly installed device, device driver, and
installation files.
Note
If these procedures do not correct your device driver problem, you must obtain the
Correcting Device Driver Issues document from the Ocean Optics website:
http://www.oceanoptics.com/technical/engineering/correctingdevicedriverissues.pdf.
294-00000-000-02-0208 9
3: Troubleshooting
Remove the Unknown Device from Windows Device Manager
! Procedure
1. Open Windows Device Manager. Consult the Windows operating instructions for your computer
for directions, if needed.
2. Locate the Other Devices option and expand the Other Devices selection by clicking on the "+"
sign to the immediate left.
Note
Improperly installed USB devices can also appear under the Universal Serial Bus
Controller option. Be sure to check this location if you cannot locate the unknown device.
3. Locate the unknown device (marked with a large question mark). Right-click on the Unknown
Device listing and select the Uninstall or Remove option.
4. Click the OK button to continue. A warning box appears confirming the removal of the Unknown
Device. Click the OK button to confirm the device removal.
5. Disconnect the HR2000+ from your computer.
6. Locate the section in this chapter that is appropriate to your operating system and perform the
steps in the following Remove Improperly Installed Files section.
Remove Improperly Installed Files
! Procedure
1. Open Windows Explorer.
2. Navigate to the Windows | INF directory.
Note
If the INF directory is not visible, you must disable the Hide System Files and Folders
and Hide File Extensions for Known File Types options in Windows Folder Options.
Access Windows Folder Options from Windows Explorer, under the Tools | Folder
Options menu selection.
3. Delete the OOI_USB.INF in the INF directory. If your computer is running either the Windows
2000 or XP operating system, you must also delete the OOI_USB.PNF file in the INF directory.
4. Navigate to the Windows | System32 | Drivers directory.
5. Delete the EZUSB.SYS file.
6. Reinstall your Ocean Optics application and reboot the system when prompted.
10 294-00000-000-02-0208
3: Troubleshooting
7. Plug in the USB device.
The system is now able to locate and install the correct drivers for the USB device.
Mac Operating Systems
Since there are no device files for the USB2000-FLG Spectrometer in a Mac operating system, you
should not encounter any problems if you installed the spectrometer before the SpectraSuite software.
Linux Operating Systems
For Linux operating systems, all you need to do is install the SpectraSuite software, then unplug and
replug in the spectrometer. Technically, the driver files for Linux simply give nonprivileged users
permission to use newly connected hardware. There isn’t any long-term harm to plugging in the device
before installing the software.
Older Version of OOIBase32 Installed If the PC to be used to interface to your HR2000+ already has an older version of OOIBase32 software
installed, you must install the latest version of OOIBase32. You can download the latest version of
OOIBase32 from the Ocean Optics website at
http://www.oceanoptics.com/technical/softwaredownloads.asp.
You do not need to uninstall previous versions of OOIBase32 when upgrading to the latest version.
294-00000-000-02-0208 11
Appendix A
Calibrating the Wavelength of the HR2000+
Overview This appendix describes how to calibrate the wavelength of your spectrometer. Though each spectrometer
is calibrated before it leaves Ocean Optics, the wavelength for all spectrometers will drift slightly as a
function of time and environmental conditions. Ocean Optics recommends periodically recalibrating the
HR2000+.
About Wavelength Calibration You are going to be solving the following equation, which shows that the relationship between pixel
number and wavelength is a third-order polynomial:
"p = I + C1 p + C2 p2 + C3 p
3
Where:
" = the wavelength of pixel p
I = the wavelength of pixel 0#
C1 = the first coefficient (nm/pixel)
C2 = the second coefficient (nm/pixel2)
C3 = the third coefficient (nm/pixel3)
R" = the reference intensity at wavelength "
You will be calculating the value for I and the three Cs.
294-00000-000-02-0208 13
A: Calibrating the Wavelength of the HR2000+
Calibrating the Spectrometer
Preparing for Calibration
To recalibrate the wavelength of your spectrometer, you need the following components:
! A light source capable of producing spectral lines
Note
Ocean Optics’ HG-1 Mercury-Argon lamp is ideal for recalibration. If you do not have an
HG-1, you need a light source that produces several (at least 4-6) spectral lines in the
wavelength region of your spectrometer.
! An HR2000+ spectrometer
! An optical fiber (for spectrometers without a built-in slit, a 50-$m fiber works best)
! A spreadsheet program (Excel or Quattro Pro, for example) or a calculator that performs third-
order linear regressions
Note
If you are using Microsoft Excel, choose Tools | Add-Ins and check AnalysisToolPak
and AnalysisTookPak-VBA.
Calibrating the Wavelength of the Spectrometer
! Procedure
Perform the steps below to calibrate the wavelength of the spectrometer:
1. Place the software into Scope mode and take a spectrum of your light source. Adjust the
integration time (or the A/D conversion frequency) until there are several peaks on the screen that
are not off-scale.
2. Move the cursor to one of the peaks and position the cursor so that it is at the point of maximum
intensity.
3. Record the pixel number that is displayed in the status bar or legend (located beneath the graph).
Repeat this step for all of the peaks in your spectrum.
4. Use the spreadsheet program or calculator to create a table like the one shown in the following
figure. In the first column, place the exact or true wavelength of the spectral lines that you used.
In the second column of this worksheet, place the observed pixel number. In the third column,
calculate the pixel number squared, and in the fourth column, calculate the pixel number cubed.
14 294-00000-000-02-0208
A: Calibrating the Wavelength of the HR2000+
True Wavelength (nm) Pixel # Pixel # 2 Pixel # 3 Predicted
Wavelength Difference
Dependent
Variables
Independent
Variable
Values Computed
from the Regression
Output
253.65
296.73
302.15
313.16
334.15
365.02
404.66
407.78
435.84
546.07
576.96
579.07
696.54
706.72
727.29
738.40
751.47
175
296
312
342
402
490
604
613
694
1022
1116
1122
1491
1523
1590
1627
1669
30625
87616
97344
116964
161604
240100
364816
375769
481636
1044484
1245456
1258884
2223081
2319529
2528100
2647129
2785561
5359375
25934336
30371328
40001688
64964808
117649000
220348864
230346397
334255384
1067462648
1389928896
1412467848
3314613771
3532642667
4019679000
4306878883
4649101309
253.56
296.72
302.40
313.02
334.19
365.05
404.67
407.78
435.65
546.13
577.05
579.01
696.70
706.62
727.24
738.53
751.27
0.09
0.01
-0.25
0.13
-0.05
-0.04
-0.01
0.00
0.19
-0.06
-0.09
0.06
-0.15
0.10
0.06
-0.13
0.19
5. Use the spreadsheet or calculator to calculate the wavelength calibration coefficients. In the
spreadsheet program, find the functions to perform linear regressions.
! If using Quattro Pro, look under Tools | Advanced Math
! If using Excel, look under Analysis ToolPak
6. Select the true wavelength as the dependent variable (Y). Select the pixel number, pixel number
squared, and the pixel number cubed as the independent variables (X). After executing the
regression, you will obtain an output similar to the one shown below. Numbers of importance are
noted.
Regression Statistics
Multiple R 0.999999831
R Square 0.999999663 R Squared
Adjusted R Square 0.999999607
Standard Error 0.125540214
Observations 22
Intercept
Coefficients Standard Error
Intercept 190.473993 0.369047536 First coefficient
X Variable 1 0.36263983 0.001684745
X Variable 2-1.174416E-05 8.35279E-07
X Variable 3-2.523787E-09 2.656608E-10 Second coefficient
Third coefficient
294-00000-000-02-0208 15
A: Calibrating the Wavelength of the HR2000+
7. Record the Intercept, as well as the First, Second, and Third Coefficients. Additionally, look at
the value for R squared. It should be very close to 1. If not, you have most likely assigned one of
your wavelengths incorrectly.
Keep these values at hand.
Saving the New Calibration Coefficients: USB Mode Ocean Optics programs wavelength calibration coefficients unique to each HR2000+ onto an EEPROM
memory chip in the HR2000+.
You can overwrite old calibration coefficients on the EEPROM if you are using the HR2000+ via the
USB port. If you are using the HR2000+ via the serial port, consult the Saving the New Calibration
Coefficients: Serial Mode section later in this appendix.
! Procedure
To save wavelength calibration coefficients using the USB mode, perform the following steps:
1. Ensure that the HR2000+ is connected to the PC and that you have closed all other applications.
2. Point your browser to http://www.oceanoptics.com/technical/softwaredownloads.asp and
scroll down to Microcode. Select USB EEPROM Programmer.
3. Save the setup file to your computer.
4. Run the Setup.exe file to install the software. The Welcome screen appears.
5. Click the Next button. The Destination Location screen appears.
6. Accept the default installation location, or click the Browse button to specify a directory. Then,
click the Next button. The Program Manager Group screen appears.
7. Click the Next button. The Start Installation screen appears.
8. Click the Next button to begin the installation. Once the installation finishes, the Installation
Complete screen appears.
9. Click the Finish button and reboot the computer when prompted.
10. Navigate to the USB EEPROM Programmer from the Start menu and run the software.
11. Click on the desired HR2000+ device displayed in the left pane of the USB Programmer screen.
12. Double-click on each of the calibration coefficients displayed in the right pane of the USB
Programmer screen and enter the new values acquired in Steps 5 and 6 of the Calibrating the
Wavelength of the Spectrometer section in this appendix.
13. Repeat Step 12 for all of the new values.
14. Click on the Save All Values button to save the information, and then Exit the USB Programmer
software.
The new wavelength calibration coefficients are now loaded onto the EEPROM memory chip on the
HR2000+.
16 294-00000-000-02-0208
A: Calibrating the Wavelength of the HR2000+
Saving the New Calibration Coefficients: Serial Mode If you are connecting the HR2000+ Spectrometer to the serial port of the PC, you need to save the new
wavelength calibration coefficients to the .SPEC file that OOIBase32 accesses when opened.
Note
You cannot save the calibration coefficients to the EEPROM memory chip on the
HR2000+ when using the serial mode.
! Procedure
To save Wavelength Calibration Coefficients using the Serial mode, perform the following steps:
1. Open the OOIBase32 application.
2. Select Spectrometer | Configure from the OOIBase32 menu bar. The Configure Spectrometer
screen appears.
3. Select the Wavelength Calibration tab to update the wavelength coefficients within OOIBase32.
4. Enter in the new values acquired from Steps 5 and 6 of the Calibrating the Wavelength of the
Spectrometer section in this appendix.
5. Click the OK button to save the information in OOIBase32.
294-00000-000-02-0208 17
Appendix B
Specifications
Overview This appendix contains information on spectrometer operation, specifications, and system compatibility.
It also includes accessory connector pinout diagrams and pin-specific information.
How the HR2000+ Works Below is a diagram of how light moves through the optical bench of an HR2000+ Spectrometer. The
optical bench has no moving parts that can wear or break; all the components are fixed in place at the time
of manufacture. Items with an asterisk (*) are user-specified.
HR2000+ Spectrometer with Components
See HR2000+ Components Table on the following page for an explanation of the function of each
numbered component in the HR2000+ Spectrometer in this diagram.
294-00000-000-02-0208 19
B: HR2000+ Specifications
HR2000+ Components Table
Ocean Optics permanently secures all components in the HR2000+ at the time of manufacture. Only
Ocean Optics technicians can replace interchangeable components, where noted.
Item Name Description
1 SMA Connector
Secures the input fiber to the spectrometer. Light from the input fiber enters the optical bench through this connector.
2 Slit
A dark piece of material containing a rectangular aperture, which is mounted directly behind the SMA Connector. The size of the aperture regulates the amount of light that enters the optical bench and controls spectral resolution.
You can also use the HR2000+ without a Slit. In this configuration, the diameter of the fiber connected to the HR2000+ determines the size of the entrance aperture.
Only Ocean Optics technicians can change the Slit.
3 Filter
Restricts optical radiation to pre-determined wavelength regions. Light passes through the Filter before entering the optical bench. Both bandpass and longpass filters are available to restrict radiation to certain wavelength regions.
Only Ocean Optics technicians can change the Filter.
4 Collimating Mirror
Focuses light entering the optical bench towards the Grating of the spectrometer.
Light enters the spectrometer, passes through the SMA Connector, Slit, and Filter, and then reflects off the Collimating Mirror onto the Grating.
5 Grating
Diffracts light from the Collimating Mirror and directs the diffracted light onto the Focusing Mirror. Gratings are available in different groove densities, allowing you to specify wavelength coverage and resolution in the spectrometer.
Only Ocean Optics technicians can change the Grating.
6 Focusing Mirror
Receives light reflected from the Grating and focuses the light onto the CCD Detector or L2 Detector Collection Lens (depending on the spectrometer configuration).
7 L2 Detector Collection Lens
An optional component that attaches to the CCD Detector. It focuses light from a tall slit onto the shorter CCD Detector elements.
The L2 Detector Collection Lens should be used with large diameter slits or in applications with low light levels. It also improves efficiency by reducing the effects of stray light.
Only Ocean Optics technicians can add or remove the L2 Detection Collection Lens.
8 CCD Detector (UV or VIS)
Collects the light received from the Focusing Mirror or L2 Detector Collection Lens and converts the optical signal to a digital signal.
Each pixel on the CCD Detector responds to the wavelength of light that strikes it, creating a digital response. The spectrometer then transmits the digital signal to the OOIBase32 application.
20 294-00000-000-02-0208
B: HR2000+ Specifications
HR2000+ Specifications The following sections provide specification information for the CCD detector in the HR2000+, as well
as the HR2000+ Spectrometer itself. HR2000+CG-UV-NIR specifications are listed in Appendix C:
Error! Reference source not found..
CCD Detector Specifications
Specification Value
Detector Sony ILX-511 linear silicon CCD array
No. of elements 2048 pixels
Sensitivity 75 photons per count at 400 nm 41 photons per count at 600 nm
Pixel size 14 µm x 200 µm
Pixel well depth 62,500 electrons
Signal-to-noise ratio 250:1 (at full signal)
A/D resolution 14 bit
Dark noise 12 RMS counts
Corrected linearity >99.8%
Maximum pixel rate Rate at which pixels are digitized is 1 MHz
HR2000+ Spectrometer
Specification Value
Dimensions 148.6 mm x 104.8 mm x 45.1 mm
Weight 570 g
Power consumption 220 mA @ 5 VDC
Detector 2048-element linear silicon CCD array
Detector range 200-1100 nm
Gratings 14 gratings available
294-00000-000-02-0208 21
B: HR2000+ Specifications
294-00000-000-02-0208
Specification Value
Entrance aperture 5, 10, 25, 50, 100 or 200 µm wide slits
Order-sorting filters Installed longpass and bandpass filters
Focal length f/4, 101 mm
Optical resolution Depends on grating and size of entrance aperture
Stray light <0.05% at 600 nm; <0.10% at 435 nm
Dynamic range 2 x 108 (system); 1300:1 for a single acquisition
Fiber optic connector SMA 905 to single-strand optical fiber (0.22 NA)
Data transfer rate:
USB 2.0 Port
Serial Port
Full scans into memory every 1 millisecond
Full scans into memory every 600 milliseconds
Integration time 1 millisecond to 65 seconds
Interfaces USB 2.0, 480 Mbps (USB 1.1 compatible); RS-232 (2-wire); SPI (3-wire); I
2C
Inter-Integrated Circuit 2-wire serial bus
Operating systems:
USB Port
Serial Port
Windows 98/Me/2000/XP, Mac OS X, and Linux
Any 32-bit Windows operating system
Onboard GPIO 10 user-programmable digital I/Os
Analog channels One 13-bit analog input and one 9-bit analog output
System Compatibility The following sections provide information on hardware and software requirements for the HR2000+.
Compatibility for Desktop or Notebook PCs To use the HR2000+, you must have a PC that meets the following minimum requirements:
! Operating systems: Windows 98/Me/2000/XP, Mac OS X, or Linux with USB port; any 32-bit
Windows OS with serial port
! Computer interfaces: USB 2.0 @ 480 Mbps; RS-232 (2-wire) @ 115.2 K baud
! Peripheral interfaces: SPI (3-wire), I2C inter-integrated circuit
22
B: HR2000+ Specifications
30-Pin Accessory Connector Pinout The HR2000+ features a 30-pin Accessory Connector, located on the side of the unit as shown:
30-Pin Connector
Location of HR2000+ 30-Pin Accessory Connector
30-Pin Accessory Connector Pinout Diagram
When facing the 30-pin Accessory Connector on the front of the vertical wall of the HR2000+, pin
numbering is as follows:
2 4 6 8 10 12 14 16 18 20 22 24 26 28 30 USB
Port 1 3 5 7 9 11 13 15 17 19 21 23 25 27 29
30-Pin Accessory Connector Pinout Diagram
30-Pin Accessory Connector – Pin Definitions and Descriptions
The following table contains information regarding the function of each pin in the HR2000+’s 30-Pin
Accessory Connector:
Pin #
Function Input/Output Description
1 RS232 Rx Input RS232 receive signal – Communicates with a PC over DB9 Pin 3
2 RS232 Tx Output RS232 transmit signal – Communicates with a PC over DB9 Pin 2
3 GPIO (2) Input/Output General purpose software-programmable, digital input/output (channel number)
4 V5_SW Output Regulated 5 Volt power pin – Supplies 50 mA (maximum)
5 Ground Input/Output Ground
294-00000-000-02-0208 23
B: HR2000+ Specifications
294-00000-000-02-0208
Pin #
Function Input/Output Description
6 I2C SCL Input/Output I
2C clock signal for communication to other I
2C peripherals
7 GPIO (0) Input/Output General purpose software-programmable, digital input/output (channel number)
8 I2C SDA Input/Output I
2C data signal for communication to other I
2C peripherals
9 GPIO (1) Input/Output General purpose software-programmable, digital input/output (channel number)
10 Ext. Trigger In
Input TTL input trigger signal – See External Triggering Options document for information.
11 GPIO (3) Input/Output General purpose software-programmable, digital input/output (channel number)
12 VCC, VUSB, or 5VIN
Input or Output Input power pin for HR2000+ – When operating via USB, this pin can power other peripherals – Ensure that peripherals comply with USB specifications
13 SPI Data Out
Output SPI Master Out Slave In (MOSI) signal for communication to other SPI peripherals
14 VCC, VUSB, or 5VIN
Input or Output Input power pin for HR2000+ – When operating via USB, this pin can power other peripherals – Ensure that peripherals comply with USB specifications
15 SPI Data In Input SPI Master In Slave Out (MISO) signal for communication to other SPI peripherals
16 GPIO (4) Input /Output General purpose software-programmable, digital input/output (channel number)
17 Single Strobe
Output TTL output pulse used as a strobe signal – Has a programmable delay relative to the beginning of the spectrometer integration period
18 GPIO (5) Input/Output General purpose software-programmable, digital input/output (channel number)
19 SPI Clock Output SPI clock signal for communication to other SPI peripherals
20 Continuous Strobe
Output TTL output signal used to pulse a strobe – Divided down from the master clock signal
21 SPI Chip Select
Output SPI Chip/Device Select signal for communication to other SPI peripherals
24
B: HR2000+ Specifications
Pin #
Function Input/Output Description
22 GPIO (6) Input/Output General purpose software-programmable, digital input/output (channel number)
23 Analog In (0-5V)
Input 13-bit analog-to-digital input with a 0-5V range
24 Analog Out (0-5V)
Output 9-bit programmable output voltage with a 0-5V range
25 Lamp Enable
Output TTL signal driven Active HIGH when the Lamp Enable command is sent to the spectrometer
26 GPIO (7) Input/Output General purpose software-programmable, digital input/output (channel number)
27 Ground Input/Output Ground
28 GPIO (8) Input/Output General purpose software-programmable, digital input/output (channel number)
29 Ground Input/Output Ground
30 GPIO (9) Input/Output General purpose software-programmable, digital input/output (channel number)
30-Pin J2 Accessory Connector - Part Numbers
The part numbers for the 30-pin accessory connector on the HR2000+ Spectrometer are as follows:
! The connector is Pak50™ model from 3M Corp. Headed Connector – Part Number
P50–030P1–RR1–TG.
! The mating connector is Part Number P50–030S–TGF.
! Mating the two components requires two 1.27 mm (50 mil) flat ribbon cables (3M 3365 Series is
recommended).
If you are customizing your HR2000+ Spectrometer system or configuring External Triggering, you may
need these part numbers to complete your setup.
294-00000-000-02-0208 25
B: HR2000+ Specifications
HR2000+ 15-Pin Accessory Cable Pinout
Pin # Description Pin # Description
1 Single_strobe 9 GPIO-9
2 ContStrobe 10 GND_SIGNAL
3 V5_SW 11 SDA
4 ExtTrigIn 12 SCL
5 ExtTrigIn 13 LampEnable
6 GPIO-8 14 A_IN
7 A_OUT 15 GPIO-7
8 ExtTrigIn
26 294-00000-000-02-0208
Index
Numbers
15-pin accessory cable
pinouts, 26
30-pin accessory connector
diagram, 23
part numbers, 25
pin definitions, 23
A
accessories, 8
Accessories, 3
accessory connector
pinout, 23
Adobe Acrobat Reader, 4
B
breakout box, 3
C
Calibrating, iii, 13
calibration, 13
preparing for, 14
procedure, 14
calibration coefficients
saving in Serial mode, 17
saving in USB mode, 16
CCD, 21
CCD Detector, 20
collimating mirror, 20
compatibility, 22
Desktop or Notebook PCs, 22
Components Table, 20
Configure Hardware, 6
configuring, 6
D
Default Spectrometer Configuration File, 6
detector, 21
Detector Collection Lens, 20
document
audience, iii
purpose, iii
summary, iii
E
EEPROM, 2
External Triggering, 8
F
filter, 20
focusing mirror, 20
G
grating, 20
I
Installation, 5
USB mode, 5
installed filter, 20
Interface, 3
L
L2 Detector Collection Lens, 20
Lens, 20
294-00000-000-02-0208 27
Index
M
memory chip, 2
mirror, 20
O
OOIBase32
configuring, 6
Options
Interface, 3
P
packing list, 4
passwords, 4
power supply (external), 2
product-related documentation, iii
S
Sampling
Accessories, 3
System, 2
serial number, 6
setup, 5
shipment components, 4
slit, 20
SMA Connector, 20
Software and Resources Library CD, 4
specifications, 19, 21
detector, 21
spectrometer, 21
SpectraSuite, 2
Spectrometer Configuration Screen, 7
spectrometer operation, 19
spectroscopic accessories, 8
System Requirements, 2
T
Triggering, 8
troubleshooting
Linux systems, 11
Mac systems, 11
OOIBase32, 11
Windows systems, 9
Troubleshooting, 9
U
upgrades, iv
USB mode, 5
USB-ADP-PC, 3
USB-CBL-1, 3
W
Wavelength Calibration
about, 13
Wavelength Calibration Data File, 4
Wavelength Calibration Data Sheet, 4
what's new, iii
28 294-00000-000-02-0208
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