Spectroscopy 1 Flashcards

1
Q

Interaction of Light and Matter (1)

A

Light is made of photons.

We treat light as a wave, therefore electromagnetic radiation has both a frequency and a wavelength.

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2
Q

Frequency

A

Frequency (v) is defined as the number of waves produced by a source each second. It is measured in Hz or s(^-1).

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3
Q

Wavelength

A

Wavelength (λ) is defined as the distance between a point on one wave, and the same point on the next. It is usually measured in metres.

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4
Q

Equations

A

Frequency (v) = Velocity (c)/Wavelength(λ)

Wavelength (λ) = Velocity (c)/Frequency (v)

c = speed of light in a vacuum = 3 x10(^8)

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5
Q

Interaction of Light and Matter (2)

A

For infrared and Raman spectroscopy, the wavelength will be in the range of 400-100,000nm.

This covers the visible and infrared regions of the EM spectrum.

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6
Q

Motion in Molecules (1)

A

There are different ways in which a molecule can move:
Translation - movement in 3 dimensions.
Rotation - movement about an axis.
Vibration - movement on a bond.

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7
Q

Motion in Molecules (2)

A

All molecules have 3N degrees of freedom (dof), where N is the number of atoms.

Translation uses 3 dof.
Rotation uses 2 or 3 dof.
Vibration uses the remaining dof.

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8
Q

Vibrational Modes

A

Linear molecules have 3N - 5 vibrational modes.

Non-linear molecules have 3N - 6 vibrational modes.

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9
Q

Motion

A

Motion requires energy.
Translation requires the least amount of energy, it is purely kinetic.
Rotation requires more energy than translation, roughly equivalent to microwave wavelength.

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10
Q

Vibration in Molecules (1)

A

Absorption of infrared radiation causes covalent bones within molecules to vibrate.

A molecule is only able to absorb radiation whose energy corresponds to the energy difference.

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11
Q

Vibration in Molecules (2)

A

Most molecules have many covalent bonds, hence infrared and Raman spectra proving detailed information on molecular structure.

Bond vibrations that result in absorption of infrared radiation are either stretching or bending vibrations.

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12
Q

Modes of Vibration in Molecules

A

Symmetric stretch
Asymmetric stretch
Twisting
Wagging
Scissoring
Rocking

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13
Q

IR Active/Inactive (1)

A

Not all vibrations can be seen by IR spectroscopy, only those deemed “IR active” will be visible.

Gross selection rule:
A vibration must result in a change in the molecular dipole moment.

Specific selection rule:
The change in vibrational energy level must be Δν = ±1

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14
Q

IR Active/Inactive (2)

A

Large changes in the dipole moment results in an intense absorption.

Small changes in the dipole moment results in a weaker absorption.

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15
Q

Hooke’s Law (1)

A

By imagining a chemical bond to be a spring with a mass at each end, we can calculate the frequency of vibration using Hooke’s Law.

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16
Q

Hooke’s Law (2)

A

The strength of a bond is given by k, while μ is the reduced mass.

Reduced mass is the mass at the centre of gravity, which is made up of a combination of the two masses at either end of the spring.

17
Q

IR Spectroscopy - Benefits

A

Generally little sample prep is required.
Can handle any state of sample.
Identifies functional groups.

18
Q

IR Spectroscopy - Limitations

A

Not usually quantitative.
Low sensitivity.
Cannot detect IR inactive impurities.