MAAC: Analytical Spectrophometry 5 Flashcards

1
Q

Pharmaceutical aplications of atomic absorbation

A

Determination of metal residues remaining from the manufacturing process in drugs

Used to measure:

–Zn content of insulin

–Fe in blood or tablets

–Heavy metals (Hg, Cd, etc.) in drinking water

–Cu or Mn in tonics.

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2
Q

What is the basic mechanism of atomic Absorption?

A
  • Measures absorbance of light by ground state atoms or ions.
  • Highly specific method useful in some aspects of quality control
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3
Q

What is the difference in flame use in AE and AA?

A
  • In AE – a flame is used to excite electrons from ground state to excited state (Boltzmann Law)
  • In AA – flame is only used to atomise the sample.
    • Absorption is carried out using a hollow cathode lamp
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4
Q
A
  • Hollow cathode lamp – made of same metal as sample – emits light of exactly the same wavelength as absorbed by sample.
  • Flame – 10 cm acetylene flame, acts as absorbance cell. Should not excite sample.
  • Modulator – provides lamp with AC current to overcome small number of excited atoms emitting light.
    • Only amplifies light from the lamp and not from the flame (see later)
  • Modern instruments use graphite furnace.
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5
Q

Describe how the intrumentation of AA works

A

you’ll see very similar to the flame photometer method we covered before the sample, again, has to be in solution. We have a nebuliser, there’s a fuel, gas and oxidant, those gases are going to pass in front of the capillary that’s gone into the sample. That’s going to create a pressure differential between one end of the capillary to the other. And that’s going to cause the sample to be pulled up into the nebuliser. Once that liquid comes into the nebuliser, it’s going to be broken down into droplets. The larger droplets will be too heavy and will fall down the drain. So only about 10 percent of the actual sample will carry on with the flame gases and head up to the burner. From there, the flame will be used to remove any solvent, the sample, but not cause it to be excited. Instead will now have our light source. The hollow cathode lamp, passing the light of a very specific wavelength through the flame. And that’s going to give us an atomic absorption. reading dependent on how much atoms are in the sample. The rest of the system, is then very similar, a monochromator to pick our wavelength and the detector. Probably a PMT being used and a PC for the readout

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6
Q

Describe the make of the hollow cathode lamp

A
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7
Q

Describe how the hollow cathode light generates light emission

A

Highly energetic electrons emitted by cathode

  • Ar ionised by collision with electrons (Ar + e- —> Ar+ + 2e-)
  • Ar+ accelerated to cathode causing sputtering of metal atoms (M(s) —–> M(g))
    • This is when there is phase change directluy from solid to gas
  • Metal atoms are excited by collisions with e- and ions (M(g)) —> M*(g))
  • The excited metal atoms relax then emit the excess energy in the form of a photon of light which produces the characteristic atomic emission lines (M*(g) —–> M(g) + hν)
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8
Q

Describe the temperature and pressure of the gas in emission region

What does this mean?

A

Temperature of gas in emission region is only a few hundred oC and is at low pressure

–Little Doppler broadening

–Little pressure broadening

–i.e. very narrow lines

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9
Q

What are the limitations of a hollow cathode lamp?

A

Limitations:

  • One lamp required for each element
  • Not good for volatile elements e.g. As, Se
    • Use electrodeless discharge lamp
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10
Q

Disuss the need for a monochromator

A

Several emission lines both from atoms and filler gas for each lamp so a monochromator is still required

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11
Q

What are the requirements for the atom cell (flame)

A
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12
Q

The flame itself also generates spectral emission as it is generating a light source. It also has lots of free readicals inside of the flame gases and these will produce different emissions.

How methods can this be used to resolve/ correct this?

A
  • Amplifier
  • Back ground correction light source
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13
Q

Describe the process of amplification

A

Both modulated current and using a chopper will produce the same effect ie a pulsed signal generated by the lamp.

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14
Q

Describe how background correction works

A
  • If molecular absorption / scattering is due to a component of the sample
    • e.g. measurement of Ba in the presence of Ca (forms CaOH+)
    • then problem finding AA when HCL will measure AA + BK
  • Solved using Background Correction.
  • Most common method is deuterium (D2) lamp
  • Broad spectral output Io from D2
  • Any atomic absorption has little effect on I
  • Molecular absorption or scattering will be broad and cover whole width of monochromator
    • Thus reduces D2 lamp intensity
    • D2 lamp only measures unwanted broad absorption
  • Thus may be subtracted from AA absorption to give true reading

Summary:

Deuterium lamp emits broad spectrum of light. Light passing the sample in the flame is alternated between the HCL and the deuterium lamp. Broad spectrum not affected by narrow absorbance of atom = background. Whilst HCL is affected by absorbance by atoms = signal. Able to subtract the two to leave just the AA signal.

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15
Q

Describe the use of the monochromator in both AA and AE

A

•In AA

–Used to isolate the AA line from other lines emitted from the HCL

•In AE

–Used to isolate the AE line from other lines due either to element of interest or other elements in the sample matrix

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16
Q

What detector is used in AA and AE?

A

PMT

17
Q

Advantages of AA to Flame photometry

A
  • AA has wider application than FP (40 metals vs. 4).
    • FP - have to excite atoms which is limited by temp of flame and how many atoms you can cause exciation
    • In AA don’t want to excite therefore can use low temp flame and particular light source that will give absorption
  • AA has a lower limit of detection
    • AA uses ground state atoms vs. FP using excited state atoms.
  • AA is more reproducible
    • Does not rely on temp of flame or flow rate of gas.
  • Can be interfaced with pc for data storage.
18
Q

Disadvantages of AA compared to FP

A
  • Only determines one metal at a time.
  • Have to change lamps for multi-component assays.
  • Useful for many assays of same metal, but poor for multi-component analysis of single sample.
  • Does not determine non-metals.
  • Much more expensive technique than FP.
19
Q

How is AA turned into AE?

A
  • Flame photometers were designed for a limited application (alkali metals)
  • Able to adapt current AA instrument for AE analysis

–Remove light source

–Rotate burner head

•Reduces self-absorption

–Reduce monochromator to lowest setting

•More emission lines than absorption lines

20
Q

GRAPHITE FURNANCE ATOMIC ABSORPTION SPECTROMETRY

A
21
Q

What is the difference between GFAAS amd FAAS?

Advantages?

A

The main alternative to FAAS is graphite furnace atomic absorption spectrometry (GFAAS)

  • Removes the flame and replaces with a graphite furnace (flame gases cause background interference so this is good)
    • Safer than FAAS
      • Doesn’t need volatile gases so can be left to opperate on own
    • No need for a nebuliser
      • With neb only 10% of sample reached flame so 90% wasted. More sample can now go through
  • •Able to analyse solids

22
Q

Describe the use of L’VOV platmform

A

Normally the tube heats up due to the graphite restricting the passage of electrical conduction through it. This leads to hot spots where the sample is at the bottom. Part of this sample becomes atomised, but due to the gas not being heated consitantly all around condensation occcurs. L’vov platform used to prevent this:

  • Platform not heated directly by electric current but indirectly by radiation and convection from furnace walls
  • Delays atomisation until gas is heated up sufficiently to prevent condensation
23
Q

How is GFAAS carried out?

A
24
Q

Advantages of GFAAS

A

•Advantages

–Sample applied directly to furnace so no need for nebuliser

•All sample participates in measurement process

–Detection limits are 100-1000x better than flame

Flame AA: 10-1000 ppb Furnace AA: 0.01-10 ppb

–The atoms are present in the atom cell for a relatively long time

–Furnace working range for real samples 1 – 100 ppb

–Only small amounts of sample material required

–Elements with resonance lines near 200 nm can be measured because of absence of flame gases

–Potential for direct analysis of solids