Mapa mental
Introduction to spectroscopy
Conteúdo do mapa
Introduction to spectroscopy
study of absorption & emission of electromagnetic radiation by atoms & molecules
Uses
- Determination of molecular structure
- Identification of unknown molecules
- Detection of known molecules
- Measurement of concentration
Electromagnetic radiation
- form of E produced by oscillating electric & magnetic disturbance
- electric & magnetic waves travel perpendicular to each other
- General properties
- travel through empty space
- speed of light always constant
- wavelength measured btw distance of crest & troughs
- Amplitude
- distance from the maximum vertical displacement of the wave to the middle of wave
- measure the magnitude of oscillation of a particular wave
- larger amplitude, larger energy
- Wavelength, λ
- distance of one full cycle of the oscillation
- shorter wavelength, higher frequency, greater energy,
- c = λv
- c = 3.0x10^8 m/s or 3.0x10^10cm/s
- v : 1/s
- Period, T
- amount of time a wave takes to travel one wavelength, in seconds
Photon
- quantum of electromagnetic E
- E = hv
- h: planck constant, 6.62607 x 10^-34 Js
Atomic Spectroscopy Techniques
- Atomic Emission Spectroscopy, AES
- require electrons to be excited b4 they emit
- selective excitation may occur
- Atomic Absorption Spectroscopy, AAS
- produce spectra whose lines reveal spacing btw E levels in electronic structure of atoms
- produce high level of noise
- maps the ground state, so there will always plenty of electrons available to absorb photons with right frequency
- Atomic Emission Spectroscopy, AES
Energy level & Transitions
- Energy level: internal E in atoms & molecules is quantized
- E(photon) = E(upper) - E(lower) = hv
- Absorption of photons
- upward transition to higher level
- increase in internal E
- Excitation
- Emission of photons
- downward transition to lower E level
- decrease in internal E
- Spontaneous emission
- electrons drop from excited state to lower E & photon released
- Stimulated emission
- emission triggered by incoming photon of same frequency
- Absorption of photons
Transition dipole moment, μ(fi)
- μ(fi) = ∫φ(f)μφ(i)d
- μ: electric dipole moment operator
- φ(f) & φ(i) : state level initial & final
- when μ ≠ 0, electric dipole is allowed
- when μ =0, electric dipole forbidden
- when a 1s electron become 2s electron, no net μ
- when a 1s electron become 2p electron , hv net μ
- μ(fi) = ∫φ(f)μφ(i)d
Selection Rules
- define which transition are allowed / forbidden
- Gross selection rules
- permanent electric dipole moment
- Specific selection rules
- quantum number changes
Intensity of spectral lines
- Factors
- Rate of transition
- more intense electromagnetic field, greater rate of transition induced, stronger absorption
- Population of initial E level
- Rate of transition
- Beer-Lambert Law
- Transmittance, T=I/I'
- I : Intensity of transmitted light
- I' : Intensity of incident light
- I=I_0 x 〖10〗^(-ε[J]L)
- ε : molar absorption coeficient
- depend on frequency of incidnet radiation & greatest when absorption is most intense
- L : length of sample
- [J] : molar concentration
- ε : molar absorption coeficient
- Absorbance, A =ε[J]L
- ε[J]L : optical of sample
- A =-log T
- Transmittance, T=I/I'
- Factors
Factors of broadening, ∆v
- Natural linewidth
- ∆E∆t = h/2π
- electrons in excited state remain for average time, ∆t b4 decay
- Collisional broadening
- ∆v(total) = ∆v + v(collision)/π
- at excited state, collision occur, loss E, larger at higher density
- Thermal broadening
- ∆v(D) = v_0/c x √(2kT/m)
- larger at higher T
- at excited, T increase, molecules decay, emitted E decrease
- Natural linewidth
absorption probability
- Intensity of incident radiation at absorption frequency
- square of magnitude of μ(fi)
Emission probability
- Intensity of emitted radiation
- square of magnitude of μ(fi)
Informações
- Descrição
- Mapa Mental sobre Introduction to spectroscopy, criado por Connie Leong em 05-04-2018.
- Criado por
- Connie Leong
- Visualizações
- 0
- Avaliação