rotational spectroscopy Flashcards

(43 cards)

1
Q

what type of spectroscopy is rotational spectroscopy?

A

transmission

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2
Q

how does transmission spectroscopy work?

A

light source passes through a molecule which absorbs certain wavelengths / colours, and transmits others

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3
Q

what kind of EM radiation is used in rotational spectroscopy?

A

microwave, as ΔE is ~1-10 cm-1, quite small

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4
Q

is a molecules moves in a direction x, y or z, what does this imply?

A

means the molecule has kinetic energy

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5
Q

how is speed of rotation determined, and why is speed specifically used?

A

speed = distance / rotation time
where distance = circumference = 2πr

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6
Q

angular velocity, ω definition

A

angular velocity is = for all points of a rigid rotating body, defined in terms of distance from the centre and translational velocity: v = rω

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7
Q

adapt the kinetic energy equation for angular velocity

A

E = 1/2mv^2
= 1/2m(rω)^2
= 1/2mr^2*ω^2

now E = kinetic energy of a single particle rotating around a fixed axis

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8
Q

how is angular momentum conserved?

A

it is conserved when no net force is acting to slow the rotation - once rotation starts energy is constant, but velocity can change so it can increase if resistance forces are minimised

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9
Q

give the equation for moment of inertia, I

A

I = Σmr^2 or better I = μr^2
where m = mass, μ = reduced mass and r = distance

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10
Q

moment of inertia, I definition

A

energy of rotation in a certain direction

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11
Q

how many moments of inertia do molecules have?

A

3, one for each axis
- however these moments of inertia are only deemed significant if atoms change position during rotation

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12
Q

what 3 factors does rotational energy depend on?

A

atomic mass, distance between atoms, angular velocity

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13
Q

what is the purpose of reduced mass, μ?

A

in most molecules, mass is not evenly distributed, so reduced mass is used to simplify a 2 body system into a 1 body system

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14
Q

outline the rigid motor model

A

using reduced mass, the molecule/diatomic/bond has been simplified to a single point mass, where the centre of the molecule = the centre of the bond, closer to the heavier atom
when the bond is rotated, the heavier atom hardly moves, the smaller atom spins around it - as its a rigid rotor, this assumes bond length doesn’t change with rotation

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15
Q

forbidden transition definition

A

when transitions between energy levels have a 0% chance of occurring, based on quantum mechanical calculation

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16
Q

what is the purpose of selection rules?

A

to inform us about which transitions are allowed and which aren’t

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17
Q

what are the 2 types of selection rule?

A

gross and specific

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18
Q

outline the purpose of the gross selection rules for rotational spectroscopy

A

they tell us if a molecules will have a rotational spectra, in terms of molecular properties for particular types of absorption

19
Q

outline the purpose of the specific selection rules for rotational spectroscopy

A

they tell us which transitions are allowed, in terms of levels between which transitions can take place

20
Q

what molecules can undergo rotational spectroscopy?

A

the molecule must possess an electric dipole that can oscillate at the frequency of the radiation, in order to interact with the EM radiation used
- this is an example of a gross selection rule

21
Q

can homonuclear diatomics undergo rotational spectroscopy?

A

no, they have no permanent dipole

22
Q

can heteronuclear diatomics undergo rotational spectroscopy?

A

yes, they do have permanent dipoles

23
Q

what transitions are allowed in rotational spectroscopy?

A

only transitions between adjacent energy levels (ΔJ = +/-1) - where J = energy levels
- this is an example of a specific selection rule

24
Q

what is B?

A

rotational constant, takes 3 forms:
- energy = h^2/(8π^2I), units J
- wavenumber = h/(8π^2Ic), units cm^-1
- frequency = h/(8π^2I), units Hz

necessary to calculate the energy of rotational levels

25
what happens to energy levels as B changes?
they will also change, as their related to molecular mass and bond length - therefore all molecules have unique energy levels, like a signature/fingerprint
26
what kind of photon will be absorbed?
the photon must match the difference between energy levels - this means energy of photons absorbed is related to bond length and molecular mass
27
what is on the x and y axes of a spectra?
y-axis = intensity/absorption x-axis = energy
28
when E = 0, what do we expect to see on a spectra and why?
when E=0, no energy is present, meaning there is no light, so no absorption or activity at all will be recorded
29
what do we expect to see on a spectra as wavelength of light is changed?
as energy/wavelength of light changes, some will be absorbed if it matches with the energy needed for available transitions - this is what peaks show
30
how does the difference between photon energies change on the spectra?
it doesn't, photon energy/peaks will increase in equal steps because ΔE increases in equal steps (ΔE - ΔE = 2B)
31
how does isotopic substitution affect the spectra produced?
it doesn't affect electronic binding, but it does affect mass - change in mass means change in moment of inertia, which means change in B which changes ΔE - on a spectra this could appear as a series of many slightly overlapping, differently spaced lines per isotope present, intensity depending on abundance
32
how does isotopic substitution affect diatomics?
for heterodiatomics, one atom is larger than the other - there is a much larger impact if the lighter element is substituted with an isotope, as this has a larger impact on the mass ratio - e.g. if hydrogen were swapped with dueterium, μ woudl change a lot
33
give the limitations of rigid rotor model
we assume through the rigid rotor model that bond lengths are fixed, whereas in real life this isn't the case faster rotation causes bonds to stretch, which increases J values so 2B is not longer the distance between 2 peaks, the gap decreases as bonds are stretched
34
how do we account for the stretching of bonds during rotation?
centrifugal distortion constant D
35
what are the 4 types of polyatomic molecules?
linear molecules symmetric tops spherical tops asymmetric rotors
36
give an example of linear polyatomics and describe their moments of inertia
e,g, CO2. C2H2 these have 2 moments of inertia where one = 0: Ib = Ic, Ia ~ 0 - treated just like 2 body molecules
37
give an example of symmetric top polyatomics and describe their moments of inertia
e.g. NH3, CH3F overall 3 moments of inertia Ib = Ic =/= Ia, but Ia =/= 0
38
give an example of spherical top polyatomics and describe their moments of inertia
e.g. CH4 3 moments of inertia Ia = Ib = Ic - however these have no dipoles, so usually have no rotational spectra anyway
39
give an example of asymmetric rotors and describe their moments of inertia
e.g. H2O, NO2 have 3 moments of inertia, most complex Ia =/= Ib =/= Ic, also have different B depending on axis of rotation - introducing more axis of rotation requires more quantum numbers, very complicated)
40
why do peaks have different intensities?
this depends on population and degeneracy: - absorption is related to the number of molecules in that rotational state which can be promoted to the next state via photon absorption, so greater population of a state of excitation means greater number of molecules that can absorb radiation, means greater intensity - degeneracy of higher energy orbitals means there are more pathways into these orbitals so its possible for more molecules to absorb photos and excite themselves into that state, so greater intensity
41
how can degeneracy be calculated for rotational levels?
formula 2J +1
42
how does degeneracy affect population of rotational energy levels?
as J increases, degeneracy increases, and so does ΔE, so eventually ΔE>>KbT so population ratio becomes ~ 1 at high J values
43
explain the boltzmann-like shape of rotational spectra
at lower J, when ΔE is small, the exponential tends to 1, so degeneracy has a greater impact and dominates, so we see linear increase on graph whereas at higher J, ΔE is larger and so the exponential term dominated, tending towards 0, so we see exponential decrease