MDM Flashcards

1
Q

What is analytical spectroscopy?

A

Analytical spectroscopy is the science of determining how much of a substance is present by accurately measuring how much light is absorbed or emitted by atoms or molecules within it

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2
Q

What is an example of an instrument for analytical spectroscopy? What is its function?

A

Spectrophotometer - meausures the intensity of light absorbed by atoms or molecules
- can be double or single beam

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3
Q

What is needed for a spectrophotometer to function properly?

A
  • A source that generates a broad band of electromagnetic radiation
  • a dispersion device that selects from the broadband radiation of the source e.g a particular wavelength
  • a sample area
  • one or more detectors to measure the intensity of radiation
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4
Q

What are the 2 different light sources?

A
  • Tungsten lamp 350 to 2000nm suitable for colourimetry - halogen light (VISIBLE LIGHT - ONES IN KITCHEN E.G)
  • deuterium lamp 200 to 370nm, UV spectroscopy
    both light sources need to provide a constant intensity at all wavelengths with low noise and long-term stability
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5
Q

What is a monochromator?

A

monochromator is either a prism (triagle light pass through gives u a rainbow) or diffraction gratings, most quantitative measurments light must be monochromatic

SNGLE WAVELENGTH E.G LAZER

monochromators contain
- an enterance slit
- collimating mirrow (lens)
- a dispersing device (prism or grating)
- a focusing mirror (or lens)
- an exit slit

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6
Q

What is diffraction grating?

A

It is where,
polychromatic radiation enters through enterance slit
the beam is collimated (makes radiation parallel before hitting dispersing element) and strikes dispersing element at an angle
beam is split into component wavelength by frating
by moving the dispersing element or exit slit, radiation of a particluar wavelength leaves

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7
Q

what is a detector

A

a detector converts a light signal into an electrical signal
it should give a linear response over a wide range with low noise and high sensitivity
several different types, but usually photomultiplier tube or a photodiode array

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8
Q

What is a photomultiplier tube?

A

Approx 1000V connected across 16 dynodes each more positive than the last
avalanche of electrons giving a measurable current for a few photons

How does it work?
Light enters the tube anstrikesthephoto emissivecathode, thisreleases electrons which are attracted to the dynode,
morectrons ae released which are then attracted to the next dynode which is held move positive than the last, process repeats and generates a cascade of electrons at the anode and amplifies the signal.

window allows light to pass you, dynodes are held as a positive charge. electrons stike dynode more electrons are generated when they are given off they are m0re attracted to the dynodes because there are more positively charge. at the end when they hit the anode, 1x10-7 electrons for every photon of light - causes an avalanche effect

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9
Q

What is a photodiode array?

A

Some modern spectrophotometers contain an array of photodiode detectors positioned side by side on a silicon crystal
- single beam instrument
- meausres whole spectrum simultaneously
useful for uv/vis absorption of sampes rapidly passing through a sample flow cell e.g HPLC or CE detector
- only reolution of 1nm
- need more detectors to improve resolution

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10
Q

Summary - examples of spectrophotometer, light source, monochromator, detector?

A

Spectrophotometer - measures the intesnity of light absorbed or emitted by atoms or molecules
Light source - Tungsten and deuterium
Monochromator - either prism or diffraction grating
detector - PMT or photodiode array detector

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11
Q

Which light sources are used in absorption spectroscopy and why?

A
  1. Hollow Cathode Lamp (HCL): These lamps are commonly used in atomic absorption spectroscopy (AAS). They contain a cathode made of the element of interest, and when an electric current passes through the lamp, it generates a characteristic emission spectrum for that element. HCLs are particularly useful for the analysis of trace metal ions.
  2. Flame Emission Source: Flame atomic emission spectroscopy (FAES) employs a flame, typically an air-acetylene flame or a nitrous oxide-acetylene flame, as the light source. The atoms in the sample are vaporized and excited in the flame, producing characteristic emission lines that are detected and used for qualitative and quantitative analysis.
  3. Inductively Coupled Plasma (ICP): ICP is a high-temperature ionization source used in inductively coupled plasma atomic emission spectroscopy (ICP-AES) and inductively coupled plasma mass spectrometry (ICP-MS). It produces a high-temperature, ionized argon plasma that excites and ionizes atoms, making them emit characteristic wavelengths of light.
  4. Continuum Sources: For techniques like atomic absorption spectroscopy (AAS) or atomic fluorescence spectroscopy (AFS), continuum sources such as deuterium lamps and xenon lamps are used to provide a broad spectrum of light. This light is then passed through a monochromator to select the desired wavelength for analysis.
  5. Laser Sources: Laser-induced breakdown spectroscopy (LIBS) and laser ablation inductively coupled plasma mass spectrometry (LA-ICP-MS) use lasers, often in the form of pulsed lasers, to ablate and atomize solid samples. The light emitted during the process contains information about the elemental composition.
  6. X-ray Sources: X-ray fluorescence spectroscopy (XRF) uses X-ray sources to excite inner-shell electrons of atoms, leading to characteristic X-ray emissions that are detected for elemental analysis.
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12
Q

Do you understand how a monochromator works?

A

A monochromator is an optical device used to isolate and select a single, narrow range of wavelengths (or colors) from a broader spectrum of light. It’s a crucial component in many analytical instruments, such as spectrophotometers and spectrometers, where the separation and analysis of light by its constituent wavelengths are required.

Entrance Slit: The monochromator starts with an entrance slit that allows the incoming light to enter. The light is typically a mixture of different wavelengths.

Collimating Optics: After passing through the entrance slit, the light is directed through collimating optics, which may include lenses or mirrors. The collimating optics serve to make the light rays parallel.

Dispersive Element: The collimated light is then directed toward a dispersive element, which is often a diffraction grating or a prism. The dispersive element separates the different wavelengths of light based on their angles of diffraction or dispersion.

Diffraction Grating: In a grating monochromator, a diffraction grating is used. The grating has closely spaced lines that act as a series of slits. When light passes through the grating, it is diffracted, and the different wavelengths are spread out at different angles.
Prism: In a prism monochromator, a prism is used to disperse the light. The different wavelengths of light are bent by different amounts as they pass through the prism, causing them to spread out.
Selection of Wavelength: To select a specific wavelength from the dispersed light, a movable slit or aperture is placed at the desired angle. By adjusting the position of this slit, only light of the chosen wavelength is allowed to pass through.

Exit Slit: The selected wavelength, now isolated, passes through an exit slit. The exit slit can be adjusted in width to control the bandwidth or resolution of the monochromator.

Detector: Finally, the isolated wavelength is directed towards a detector, which measures the intensity of the light. This detector is connected to the analytical instrument to record the data.

By adjusting the angle of the dispersive element or the position of the entrance and exit slits, a monochromator can select different wavelengths of light for analysis

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13
Q

Can you describe how a PMT works?

A

Approx 1000V connected across up to 16 dynodes, each diode is more positive than the last,
it is an avalanche of electrons giving a measurable current for a few photons

A Photomultiplier Tube (PMT) is a highly sensitive photon detector used to measure low levels of light in various applications, including scientific research, medical instruments, and analytical equipment. PMTs work on the principle of photoemission and electron multiplication. Here’s how a PMT works:

Photon Detection: When a photon of light enters the PMT, it strikes the photocathode, which is typically a photosensitive material (e.g., cesium-antimony compounds). The energy from the incoming photon is absorbed by the photocathode, causing the emission of an electron through the photoelectric effect. This process converts the photon’s energy into an electron with kinetic energy.

Electron Emission: The emitted electron is then accelerated and focused by a series of electrodes within the PMT. These electrodes are designed to provide a voltage gradient that causes the electron to move toward the next electrode, typically referred to as the “dynode.”

Electron Multiplication: As the accelerated electron strikes the first dynode, it releases additional secondary electrons through a process known as secondary emission. Each secondary electron is accelerated and strikes the next dynode, releasing even more electrons. This cascade effect continues as the electrons are multiplied at each dynode stage.

Sequential Dynodes: A typical PMT consists of multiple dynodes arranged in a sequence. The number of dynodes can vary depending on the PMT model, and each dynode stage provides electron multiplication. This cascade amplification results in a significant increase in the number of electrons produced.

Anode and Current Amplification: At the final dynode, a large number of electrons are collected and focused onto an anode. The anode generates an electric current that is directly proportional to the number of incident photons, making it a measure of the light intensity. This electric current can be read and processed by external electronics.

Output Signal: The amplified electric current is the output signal of the PMT, which can be further processed and analyzed by external equipment, such as amplifiers, data acquisition systems, or other detectors.

PMTs are highly efficient at converting photons into measurable electrical signals, making them valuable in applications that require sensitive detection of light, such as in fluorescence spectroscopy, scintillation counting, particle physics experiments, and more.

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14
Q

What are the differences between a diode array and a single beam spectrometer?

A

Design:

Single-Beam Spectrophotometer: This is the traditional type of spectrophotometer. It consists of a single optical path where light from the source passes through a sample, and the intensity of transmitted or reflected light is measured at a single fixed wavelength at a time.
Diode Array Spectrophotometer: Diode array spectrophotometers use an array of photodetectors, such as charge-coupled devices (CCDs) or complementary metal-oxide-semiconductor (CMOS) detectors, to simultaneously measure the entire spectrum of wavelengths. They capture multiple data points across a wide range of wavelengths simultaneously.
Speed:

Single-Beam Spectrophotometer: Single-beam instruments measure one wavelength at a time and require manual adjustments when scanning across different wavelengths. This can be time-consuming when obtaining a full spectrum.
Diode Array Spectrophotometer: Diode array spectrophotometers are much faster because they capture the entire spectrum in a single measurement, making them suitable for rapid scanning and kinetic studies.
Wavelength Range:

Single-Beam Spectrophotometer: Single-beam instruments are typically designed for specific wavelength ranges, and they require the manual insertion of different filters or gratings to change the wavelength.
Diode Array Spectrophotometer: Diode array spectrophotometers cover a wide range of wavelengths without the need for manual adjustments or changing components. They can be versatile for various applications.
Accuracy and Precision:

Single-Beam Spectrophotometer: Single-beam instruments can offer high accuracy and precision when used within their specified wavelength range.
Diode Array Spectrophotometer: Diode array spectrophotometers can also provide high accuracy and precision, and their ability to capture a full spectrum in a single measurement can reduce potential errors associated with wavelength changes.
Applications:

Single-Beam Spectrophotometer: These are suitable for routine measurements at specific wavelengths, such as absorbance at a fixed wavelength. They are commonly used in teaching laboratories and for simple applications.
Diode Array Spectrophotometer: Diode array instruments are versatile and suitable for a wide range of applications, including quantitative analysis, kinetics, and applications where a full UV-Visible spectrum is needed.
In summary, diode array spectrophotometers offer the advantage of speed and the ability to capture full spectra simultaneously, making them more versatile and efficient for many applications. Single-beam spectrophotometers are simpler in design and are suitable for basic measurements at a single wavelength or when a full spectrum is not required. The choice between the two depends on the specific needs of the analysis and the available budget.

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15
Q

Why does polychromatic light passing through a substance decrease?

A
  • Reflection at phase boundaries - i.e. liquid/air, glass/liquid etc. This is caused by differences in the refractive index of the different materials through which the light is passing
  • scattering of light caused by non-homogeneity of the sample
    -absorbance by atoms or molecules in solution
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16
Q

What wavelength would you select?

A

Scan sample over region of interest and not wavelength at highest absorption
also use Brittish pharmacopeia to find max wavelength of a particluar drug
gives greatest sensitivity and peaks tend to be fairly flat depending on sample

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17
Q

What molecular orbitals are in single and double bonds?

A

Single and electrons
moelcular orbitals called sigma orbitals and sigma electrons
double bonds - 2 types
sigma orbital = pair of bonding electrons
and a pi

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18
Q

What are the energy levels? which transition will give an absorbance oeak between 200-750nm?

A
  1. bonding sigma
  2. bonding pi
  3. non bonding n
  4. antibonding pi star
    5 antibonding sigma star
    n to pi star and pi to pi star transitions will generate an absorption peak between 200-750nm
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19
Q

What is the equation for change in energy? what is the theory for energy and wavelength

A

chnage in energy = h x v
change in energy = h x c/wavelength

larger the energy the lower the waveelngth required

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20
Q

What is the A11 equation and what is A11?

A

£=A11 x Mr /10
A11 value is useful in pharmaceutical analysis where the molecular weight of the sample is unknown
- e.g when analysing a protein or DNA or
- where a mixture of several components is being analysed in the same sample ( ointment or suspension)

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21
Q

explain Beers law?

A

Beer’s Law, also known as the Beer-Lambert Law or Beer’s Law of Absorption, is a fundamental principle in analytical chemistry used to relate the concentration of a solute in a solution to the absorbance of light by that solution. It is a vital tool for quantitative analysis, particularly in spectrophotometry.

The basic equation for Beer’s Law is:

A=ε⋅b⋅c

Where:
A is the absorbance of the solution.

ε (epsilon) is the molar absorptivity or molar absorptivity coefficient (also called molar extinction coefficient), which is a constant specific to the substance being analyzed.

b is the path length of the sample through which the light passes (typically measured in centimeters).

c is the concentration of the solute in the solution, usually expressed in molarity (moles per liter).
Key points about Beer’s Law:

Direct Proportionality: Beer’s Law states that absorbance (A) is directly proportional to both the concentration of the solute (c) and the path length (b) of the sample. In other words, as the concentration or path length increases, so does the absorbance.

Molar Absorptivity (

ε): The molar absorptivity is a constant for a given substance at a specific wavelength of light. It depends on the nature of the solute, the solvent, and the wavelength of the incident light. It is a measure of how strongly the substance absorbs light at that wavelength.

Linearity: Beer’s Law holds true as long as the concentration range is within a linear region. Outside of this range, deviations may occur due to factors like non-linearity or the saturation of the absorbance.

Wavelength Specific: Beer’s Law is specific to a particular wavelength of light. The choice of wavelength depends on the absorption characteristics of the substance being analyzed.

Applications: Beer’s Law is widely used in spectrophotometry and colorimetry for quantitative analysis of various substances, including determining the concentration of analytes in solutions, such as in chemistry, biology, environmental science, and pharmaceuticals.

By measuring the absorbance of a sample and knowing the molar absorptivity and path length, you can use Beer’s Law to calculate the concentration of the solute in the solution. It’s a powerful tool for quantitative analysis in various scientific and industrial applications.

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22
Q

beers law with concentration

A

Low concentration directly proportional
high concentration curve

beers law describes the absorption behaviour of dilute solutions only
below 10mM conc effects not usually observed
above 10mM the close distance between absorbing molecules can alter ability to absorb a given wavelength

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23
Q

What can landa max show?

A

identification of drugs and unknown compounds
characteristic of a particular chromophore
should remain constant
be aware that when its ionised the position of landa max can change

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24
Q

What happens when the landa max becomes longer?

A

A shift in landa max towards longer wavelength is referred as a bathochromatic or RED shift

Occurs due to an action of an auxochrome
- this is a functional group attatched to a chromophore which does not absorb light energy itself, but influences the wavelengths of light absorbed by the chromophore
- examles include NH2, OH and SH groups
- possess long pairs of non-bonded electrons which can interact with the pi electrons of the chromophore and allow light of longer wavelength to eb absorbed.

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25
Q

What happens to aniline in acidic and alkaline conditions?

A

NH2 is an auxochrome
In pH>7 aniline is a base which is not ionised.
the landa max for benzene is 204nm compared to aniline 230nm. Due t the lone pair of electrons of NH2 interacting with the ring electrons it inc the electron density throughout the ring

In pH < 7 aniline in acidic solution reacts to form anilinium salt
lone pairs of electrons is now involved in bond formation to an H+ ion
no longer acts as a auxochroms
landa max returns to value of benzene
landa max =203nm

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26
Q

What is a hypsochromic effect?

A

also known as a blue shift is when a shift in landa max to a shorter wavelength.

Occurs when compounds with a basic auxochrome ionise and the lone pair is no longer able to interact with the electrons of the chromophore
- also been seen when different solvents or at elevated temperatures
- useful to identify amines, R_NH2

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27
Q

What is a bathochromic effect?

A

usually associated with increases in light absorption (hyperchromic effect)

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28
Q

What is a hypsochromic effect?

A

occurs with a decrease in absorbance (hypochromic effecect)

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29
Q

What do weak acids do to ionisation, give an example and what are the effects?

A

Example - Phenols - paracetamol (weak acids)
Ionisation causes;
an increase in the intensity of light absorption and
the position of landa max moves to longer wavelength

Effects
due to ionisationa nd loss of H atom as an H+ ion
- results in full negative charge on oxygen
- Interacts more effectively with ring than lone pair of electrons present in unionised form

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30
Q

What are the two methods of drug assay?

A

Comparative US
- a test/ a std
- advantage can be used if the drug undergoes a chemical reaction during assay
- disadv an authentic sampke of the drug in question must be available for comparison
Absolute EU
- absorbance meausred and BL equation used to calculate drug
- used in uk and in europe

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31
Q

How do you know if Beer’s law is obeyed?

A

when there is a colomn of numbers in an exam question - ALWAYS plot a graph - conc at bottom absorbance on the side

when absorbance is v concentration is plotted and a straight line is observed we can say beers law is obeyed for this drug at this particular wavelength.

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32
Q

How is A11 and E (molar absorbidity) calculated

A

Can be read of graph is axis are in %w/v or calculated using each data point and converting them into conc of g/ and taking average A=A11 x c x l

remember the concentration e.g if its 1%w (mg)/v you need to find conc 0.001 divided by 100 = 0.001%w/v

Molar absorbidity

A = E x c x l

c 1mg per 100ml = 0.01gL

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33
Q

What type of bonds will produce absorption in the UV and visible region?

A

Absorption of ultraviolet (UV) and visible light in molecules is primarily associated with electronic transitions within the molecule. The types of chemical bonds and electronic structures that can produce absorption in the UV and visible region are as follows:


π-


π

Transitions: These transitions involve the movement of electrons from a lower-energy

π (pi) orbital to a higher-energy


π

(pi-star) anti-bonding orbital. This type of transition is commonly associated with conjugated systems, such as those found in organic compounds like conjugated dienes and polyenes.

π-


π

transitions often result in absorption in the UV or visible region.

n-


π

Transitions: These transitions involve the movement of electrons from a non-bonding (n) orbital to a higher-energy


π

anti-bonding orbital. Molecules with lone pairs of electrons, like carbonyl compounds (e.g., ketones and aldehydes), can exhibit n-


π

transitions that result in UV or visible absorption.


σ-


σ

Transitions:

σ-


σ

transitions involve the movement of electrons from a lower-energy

σ (sigma) bonding orbital to a higher-energy


σ

(sigma-star) anti-bonding orbital. These transitions are less common and typically occur at shorter wavelengths in the vacuum UV region.

Metal-Ligand Transitions: In coordination compounds, transition metals can absorb visible light through metal-ligand charge transfer (MLCT) or ligand-field transitions. The specific transitions depend on the metal, ligands, and the coordination complex’s structure.

Conjugation: Extended conjugation of double bonds or delocalized

π electrons in a molecule can lead to absorption in the UV or visible region. Examples include aromatic compounds like benzene, which absorb in the UV region due to the resonance-stabilized

π electrons in the ring.

Halogenation: Halogens, such as chlorine, bromine, and iodine, in organic compounds can lead to UV absorption due to their lone pair electrons participating in n-


π

transitions. Halogenated organic compounds can show UV absorption bands.

Color Centers: In ionic solids, defects or impurities can create color centers. These arise from electron transitions associated with defects in the crystal lattice and can produce visible absorption.

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34
Q

What effect does have on different functional groups to its spectrum?

A

The pH of a solution can significantly affect the absorption spectrum of molecules with specific functional groups, particularly in the UV and visible region. Here are some examples of how pH can influence the absorption spectrum of different functional groups:

Amino Groups (NH2):

In a basic (high pH) solution, amino groups (-NH2) can become deprotonated, forming amine ions (-NH2⁻). This can shift the absorption spectrum to longer wavelengths, resulting in a bathochromic shift (redshift). This effect is observed in amino acids and amines.
In an acidic (low pH) solution, amino groups remain protonated, resulting in shorter-wavelength absorption and a hypsochromic shift (blueshift).
Carboxyl Groups (COOH):

In a basic solution, carboxyl groups (-COOH) can lose a proton, forming carboxylate ions (-COO⁻), leading to a bathochromic shift.
In an acidic solution, carboxyl groups remain protonated, resulting in a hypsochromic shift.
Phenolic Groups (ArOH):

In a basic solution, phenolic groups can lose a proton, forming phenolate ions (ArO⁻), which leads to a bathochromic shift.
In an acidic solution, phenolic groups remain protonated, resulting in a hypsochromic shift.
Imine Groups (C=N):

In a basic solution, imine groups can become deprotonated, forming imine ions (C=N⁻), leading to a bathochromic shift.
In an acidic solution, imine groups remain protonated, resulting in a hypsochromic shift.
Quinone Groups (C=O, C=O):

The absorption spectrum of quinone groups can be influenced by pH. Changes in pH can affect the equilibrium between the keto and enol tautomers, resulting in shifts in the absorption spectrum. These shifts can be bathochromic or hypsochromic.
Chromophores in Dyes and Indicators:

Many synthetic dyes and pH indicators contain specific functional groups that exhibit pH-dependent color changes due to changes in their electronic structure. For example, litmus paper changes color in response to pH changes.

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35
Q

What is the difference between comparative and absolute assay methods?

A

Comparative and absolute assay methods are two approaches used in analytical chemistry to determine the concentration or amount of a specific analyte (substance of interest) in a sample. Here are the key differences between these two methods:

Objective:

Comparative Assay: Comparative assays determine the concentration of an analyte by comparing it to a reference standard or a known substance of similar composition. The result is reported as a relative measurement, often in comparison to a standard or reference material.
Absolute Assay: Absolute assays aim to determine the exact, precise quantity or concentration of an analyte without comparison to a reference standard. The result is reported in quantitative terms (e.g., moles, mass, or concentration).
Calibration:

Comparative Assay: Comparative assays require calibration against a reference standard or a substance of known concentration. The sample’s properties are compared to those of the reference material.
Absolute Assay: Absolute assays do not require calibration against reference standards because they are intended to provide a direct quantitative measurement of the analyte.
Measurement Uncertainty:

Comparative Assay: Comparative methods are influenced by the accuracy and precision of the reference standard, and the measurement is subject to uncertainties related to both the sample and the reference material.
Absolute Assay: Absolute methods aim to minimize sources of uncertainty and provide a more direct measurement of the analyte’s quantity. Measurement uncertainty is typically lower.
Common Applications:

Comparative Assay: Comparative methods are often used for qualitative or semi-quantitative analyses, as well as for routine testing when high precision is not critical. Examples include colorimetric assays using color standards and some titration methods.
Absolute Assay: Absolute methods are essential for precise quantitative analysis, especially in research, quality control, and industries where accurate measurement of analyte concentration is crucial. Examples include gravimetry, electrochemical methods, and some advanced spectroscopic techniques.
Examples:

Comparative Assay: Colorimetric pH tests, titrations with color indicators, and some types of titrations using known volumes of reagents.
Absolute Assay: Gravimetric analysis, titrations with primary standard reagents, inductively coupled plasma mass spectrometry (ICP-MS), and gas chromatography with a thermal conductivity detector (TCD).
In summary, the main distinction between comparative and absolute assay methods lies in the use of reference standards and the reporting of results. Comparative assays rely on comparisons to known standards and provide relative measurements, while absolute assays aim to directly determine the quantity of the analyte in an absolute, quantitative manner, often without the need for reference standards. The choice of method depends on the specific requirements of the analysis and the level of accuracy and precision needed.

36
Q

What effect does incraesing the light source intesnsity have on absorption?

A

Increasing the intensity of the light source in a spectrophotometer or other absorption spectroscopy instruments can have several effects on the absorption measurement:

Increased Absorbance: Higher light intensity can result in increased absorbance (A) values. This is because a greater number of photons are being absorbed by the sample. According to Beer’s Law, absorbance is directly proportional to the concentration of the absorbing species and the path length of the sample, and it is also directly proportional to the intensity of the incident light.

Improved Sensitivity: Greater light intensity can enhance the sensitivity of the instrument, allowing it to measure lower concentrations of the analyte. This is particularly useful when analyzing samples with low analyte concentrations.

Reduced Noise: When measuring samples with low absorbance, increasing the light source intensity can help reduce the effects of electronic noise in the detector. A stronger signal-to-noise ratio results in more accurate measurements.

Wider Linear Range: Increasing light intensity can extend the linear range of the instrument. It allows for the measurement of higher concentrations without signal saturation, where the instrument’s response is no longer linear.

Faster Scanning: Higher light intensity can lead to faster scan times, which is advantageous in applications requiring rapid data acquisition, such as kinetic studies or process monitoring.

Risk of Photodegradation: In some cases, very high light intensity can lead to photodegradation of the sample, where the sample molecules are chemically altered by exposure to excessive light. It is essential to strike a balance between using sufficient light for accurate measurements and avoiding photodegradation, which may require using neutral density filters or adjusting instrument settings.

Heating Effects: Intense light sources, particularly those with high energy, can generate heat in the sample. Temperature changes may affect the absorption properties of the sample, especially for temperature-sensitive compounds.

Instrument Limitations: The effect of increasing light intensity can also depend on the design and specifications of the specific instrument being used. Some instruments may have limitations on the maximum light intensity they can provide.

It’s important to note that while increasing light source intensity can have several advantages, it should be done within the limits of the instrument and the sample’s tolerance to avoid potential issues like photodegradation or heating effects. Adjusting the light intensity to an optimal level based on the specific analytical requirements is crucial for obtaining accurate and reliable absorption measurements.

37
Q

What is the difference between absorption and fluoresecnce?

A

Absorption:

Process: Absorption is the process where a molecule absorbs photons of light, transitioning from a lower energy state to a higher energy state. This energy is typically used to promote an electron to a higher energy level.
Direction: During absorption, the molecule takes in energy from the incident light, and the absorbed light is not re-emitted in the same form.
Result: Absorption results in a decrease in the intensity of the incident light at specific wavelengths, leading to the formation of an absorption spectrum. The absorbed energy may be converted into heat or other forms of energy.
Fluorescence:

Process: Fluorescence is the process where a molecule in an excited state (due to previous absorption) returns to its ground state by emitting a photon. This is often accompanied by the release of excess energy in the form of fluorescence.
Direction: Fluorescence involves the emission of light. The emitted light has a longer wavelength and lower energy than the absorbed light, causing it to be of a different color.
Result: Fluorescence results in an increase in emitted light at specific wavelengths, creating a fluorescence spectrum. The emitted light occurs after a delay (nanoseconds to microseconds) following the absorption of the incident light.
Spectra:

Absorption Spectrum: An absorption spectrum shows the wavelengths at which a molecule absorbs light. It appears as dark lines or bands on a light background, representing the energy transitions that occur upon absorption.
Fluorescence Spectrum: A fluorescence spectrum shows the wavelengths of light emitted during the fluorescence process. It appears as bright lines or bands on a dark background, representing the specific wavelengths of the fluorescence.
Stokes Shift:

Absorption: Absorption is associated with the absorption peak in the UV or visible region.
Fluorescence: Fluorescence is associated with the emission peak in the visible or longer-wavelength region. The difference in wavelength between the absorption and emission peaks is called the Stokes shift.
Time Scale:

Absorption: The absorption process is essentially instantaneous when light interacts with the molecule.
Fluorescence: The fluorescence process occurs with a time delay, usually in the nanoseconds to microseconds range, depending on the specific molecule and conditions.

38
Q

What are the mechanisms of fluorescence?

A

There are two states?
1. Singlet states (s) - the spin of the e- is paired (opposite) to that of the ground state e- always opposite arrows
2. Triplet state (T) is the spins are unpaired and parallel arrows facing BOth up or down

39
Q

what is fluorimetry?

A

An analytical technique which relies on the emission of electromagnetic energy by molecules
- sample absorbs light in uv region of ems
-sample emits light is Visble region
the light emitted by the sample is always longer in wavelength (lower energy) than the light absorbed by the molecule
- called stokes law

40
Q

What is internal conversion?

A

Internal conversion is a transition between states of the same multiplicity

in solution this process is followed by a vibrational relaxation towards the lowest vibrational level of the final electronic state
excess energy can be transferred to the solvent during collisions of excited molecules and solvent molecules
very fast process
can get internal conversion back to the ground state but energy gap is much bigger - less efficient
the loss of energy accounts for the stokes shift in wavelength from excitation to emission

41
Q

What is inter- system crossing?

A

Is when the spin of an excited e- is reversed (singlet-triplet transition)

Loss of energy from triplet state to ground state is spectroscopically forbidden
- triplet state has long lifetime
if this occurs radiatively it is known as phosphorescence

42
Q

What is the stokes shift?

A

the gap between the maximum of the first absorption band and the max of fluorescence

43
Q

what is the mirror image rule?

A

in general the differences between the vibrationak levels are similar in the ground and excited states so that fluorescence spectrum resemble the first absorption band. excitation is the absorbance and the emission is fluorecence

44
Q

what are the differences between absorption and fluorescence instrumentation

A

Light Source:

Absorption: Absorption spectroscopy typically uses a continuous and broad-spectrum light source, such as a tungsten lamp or a deuterium-halogen lamp. These sources cover a wide range of wavelengths.
Fluorescence: Fluorescence spectroscopy uses a high-intensity, monochromatic light source, such as a xenon arc lamp or a laser. The excitation source emits light at a specific wavelength to selectively excite the fluorophores.
2. Excitation and Emission Monochromators:

Absorption: Absorption instruments often have a single monochromator to select a specific wavelength of light for absorption measurements.
Fluorescence: Fluorescence instruments typically have two monochromators, one for selecting the excitation wavelength (excitation monochromator) and another for selecting the emission wavelength (emission monochromator). This dual-monochromator setup allows for the isolation of the emitted fluorescence signal.
3. Sample Path:

Absorption: In absorption spectroscopy, the sample path typically involves a single cuvette or sample compartment. The light intensity is measured before and after it passes through the sample.
Fluorescence: In fluorescence spectroscopy, the sample path includes a cuvette or sample compartment where the sample is excited by the monochromatic light. The emitted fluorescence is collected at right angles to the excitation beam to minimize scattered excitation light and other interference.
4. Detector:

Absorption: Absorption spectroscopy commonly uses a photodetector, such as a photodiode or photomultiplier tube (PMT), to measure the transmitted light intensity.
Fluorescence: Fluorescence instruments often use a PMT or a photomultiplier tube as a detector to measure the emitted fluorescence signal. The detector is sensitive to low-intensity light and operates at specific wavelengths.
5. Signal Measurement:

Absorption: In absorption spectroscopy, the measurement involves comparing the intensity of the incident light to that of the transmitted light, and the result is reported as the absorbance (A).
Fluorescence: In fluorescence spectroscopy, the measurement involves quantifying the emitted fluorescence intensity at a specific wavelength, and the result is typically reported as the fluorescence intensity.
6. Purpose:

Absorption: Absorption spectroscopy is primarily used to measure the absorption of light by the sample, providing information about the sample’s composition and concentration.
Fluorescence: Fluorescence spectroscopy is used to study fluorescent compounds and their properties, such as quantifying their concentration, investigating their environment, and monitoring dynamic processes like binding interactions.
In summary, while both absorption and fluorescence spectroscopy involve the interaction of light with matter, they differ in terms of their light sources, monochromators, sample path, detectors, measurement principles, and applications. These differences are designed to suit the specific requirements of each technique and provide valuable information for different types of analyses.

45
Q

Why is a high power light source used in fluorescence but not in absorption?

A

In fluorescence the emitted is much higher than the absorbance therfore a stronger light source is needed.

46
Q

What instruments are used in fluorescence?

A

Spectrofluorimeter
- high energy light source (xenon lamp)
-2 monochromators excitation and emission, gives loperator choice of wavelngth for both ex=ityation and emisi[[ssion
detector is aligned 9- degreed to lamp to minimise high energy light reaching detector that has nit passed through the sample
- a photomultiplier used as a detectopr and amplifier

47
Q

what are the advantages of fluorimetruc analysis?

A

fluorimetry is more specific than ordinary UV spectroscopy bc it has 2 monochromators and not all molecules with a chromophore fluorescence detection limit approx 100 times lower than uv/vis absorption spectroscopy
- ideal; for the analysis of a very small amounts of potent drugs (e.g contraceptive pill, 30 nanograms of active steroid or drug metablism studies)
- intrinsically easier to measure a small signal (fluorescence intensity) than the difference between two large signals (I and I0) in absorbance
- fluorescence intensity may be increased by increasing I0 (taking care to avoid photodecomposition)

47
Q

what is quenching?

A

a reduction in the intensity of light emitted during fluorescence
can be as much as 100%
there are 2 types
- self or conc quenching
- chemical quenching by other, non-fluorescent agents

47
Q

What factors affect fluorescence intesnity?

A
  • source intensity
  • fluorescence efficiency
  • concentration
  • pathlength
    in practice
  • quenching
    -self absorption
    -avoidance of matrix effects
48
Q

what is self quenching?

A
  • high conc
  • collects fluorescence emitted only from the central parts of the exciting beam
  • when conc is large a significant part of incidence light is absorbed before reaching the central part of the cuvette
  • emitted light conc at face of cell rather than through body of solution
    can cause calibration to curve and may be solved by further dilution of sample
48
Q

what is chemical quenching?

A

quenching involved the removal of the energy from an excited molecule by another molecule usually as the result of a collision
- this can be improtant in analysis - fluorescence of the analyte might be quenched by the moelcules of some compound present in sample known as matrix effect
- can produce a collision or a complex formation

48
Q

What causes chemical quenching?

A

prescence of heavy atoms e.g F, Cl, Br or I results in fluorescence quenching
internal heavy atom effect
- due to inc probability of intersystem crossing
size of effect F<Cl<Br<I
the size is also depends on teh atomic number

49
Q

Summary points of fluorescence

A

Fluorescence relies on the emission of light

λ emitted is always longer than λ absorbed (Stokes shift)

Uses a xenon lamp, 2 monochromators and PMT

More specific and lower detection limit than absorbance

Can be problems with quenching (concentration, self absorption or chemical)
Quenching reduces intensity

50
Q

What is the difference between atomic and molecular absorption?

A

Atomic and molecular absorption spectroscopy are two related techniques used to study the interaction of light with atoms and molecules. They have distinct differences in terms of the species they analyze and the principles underlying their measurements. Here are the key differences between atomic and molecular absorption spectroscopy:

  1. Analyte Species:

Atomic Absorption Spectroscopy (AAS): AAS is used to analyze the concentration of individual atomic species, typically metal ions (e.g., iron, calcium, sodium) in a sample. It focuses on the absorption of light by free atoms in the gas phase or after atomization of a sample solution.
Molecular Absorption Spectroscopy: Molecular absorption spectroscopy is used to analyze molecules, particularly organic compounds and gases. It investigates the absorption of light by the chemical bonds and electronic transitions within molecules.
2. Wavelength Range:

Atomic Absorption Spectroscopy: AAS typically operates in the ultraviolet (UV) and visible (VIS) regions of the electromagnetic spectrum, measuring the absorption of light by atomic transitions.
Molecular Absorption Spectroscopy: Molecular absorption spectroscopy covers a broader range, extending from the UV and VIS to the near-infrared (NIR) region, depending on the type of molecules and transitions being studied.
3. Technique:

Atomic Absorption Spectroscopy: AAS is typically used for quantitative analysis, measuring the concentration of specific metal ions in a sample. It relies on the atomization of the sample and detects atomic absorption lines.
Molecular Absorption Spectroscopy: Molecular absorption spectroscopy is used for various purposes, including quantitative analysis, identification, and qualitative analysis. It detects characteristic molecular absorption bands or lines associated with specific functional groups or chemical bonds within the molecules.
4. Flame or Graphite Furnace Atomization:

Atomic Absorption Spectroscopy: AAS often employs flame atomization or graphite furnace atomization to generate free atoms from the sample for measurement. This is critical for analyzing metal ions.
Molecular Absorption Spectroscopy: Molecular absorption can be measured directly from liquid samples or gases without the need for atomization.
5. Sample State:

Atomic Absorption Spectroscopy: AAS typically requires the sample to be in a gaseous state (e.g., after atomization) or as a solution, where the target metal ions can be atomized in a flame or graphite furnace.
Molecular Absorption Spectroscopy: Molecular absorption can be measured in various sample states, including liquid, gas, and solid. It is versatile for a wide range of sample types.
6. Application Focus:

Atomic Absorption Spectroscopy: AAS is commonly used in applications related to environmental analysis, clinical chemistry, and metal content analysis in various industries, such as metallurgy and pharmaceuticals.
Molecular Absorption Spectroscopy: Molecular absorption spectroscopy is used in applications ranging from organic compound identification and quantification to gas analysis, food chemistry, and many other fields.
In summary, atomic absorption spectroscopy is specialized for the analysis of metal ions, focusing on atomic transitions, whereas molecular absorption spectroscopy covers a broader range of molecules and functional groups, examining electronic transitions within molecules. The choice between the two techniques depends on the specific analyte of interest and the type of sample being analyzed.

51
Q

WHy do you not get any molecular information from atomic spectrocopy?

A

Atomic spectroscopy, including techniques like Atomic Absorption Spectroscopy (AAS) and Atomic Emission Spectroscopy (AES), primarily provides information about the elemental composition and concentration of a sample. This is because atomic spectroscopy focuses on the energy transitions and electronic structure of individual atoms, particularly those in the gas phase or in atomic form after atomization.

Here are the key reasons why atomic spectroscopy does not provide molecular information:

Species of Interest: Atomic spectroscopy is specifically designed to analyze the absorption or emission of light by individual atoms, typically metal ions. It targets elements, not molecules. The analysis involves measuring transitions within the electronic energy levels of atoms.

Gas Phase or Atomization: In atomic spectroscopy, the sample is often atomized, which converts molecules (if present) into their constituent atoms. This process breaks chemical bonds, and the resulting atoms are the ones subjected to analysis. Any information about molecular species is effectively lost during this atomization step.

Transitions in Isolated Atoms: The spectral lines observed in atomic spectroscopy correspond to transitions between energy levels in isolated atoms. These energy levels are specific to the atom itself and are not directly related to the bonds or molecular structure of the original sample.

Sensitivity to Atomic Species: The sensitivity of atomic spectroscopy to molecular species is limited. Even if a sample contains both atomic and molecular species, the primary focus is on the atomic transitions. The spectral lines associated with molecules may not be as prominent or may be overshadowed by atomic lines.

In contrast, molecular spectroscopy techniques, such as Infrared (IR) spectroscopy, Raman spectroscopy, or Ultraviolet-Visible (UV-Vis) spectroscopy, are specifically designed to study the interactions of light with the chemical bonds, electronic transitions, and vibrational modes within molecules. These techniques provide information about molecular structure, functional groups, and chemical composition.

So, while atomic spectroscopy is a powerful tool for elemental analysis, it does not provide information about the molecular composition or structure of a sample, as it is not designed to do so. To obtain molecular information, other spectroscopic methods that focus on the characteristics of molecules themselves should be used.

52
Q

What is a flame photometer and waht does it do?

A

A flame photometer, also known as a flame atomic emission spectrometer (FAES), is an analytical instrument used for the quantitative analysis of certain metal ions, particularly alkali and alkaline earth metals, in a variety of sample types. It is based on the principles of atomic emission spectroscopy. Here’s how a flame photometer works and what it does:

Principle of Operation:

A flame photometer operates by atomizing a sample solution into a flame, where the atoms of the target metal ions are excited to higher energy levels by the heat of the flame. As the excited atoms return to their ground state, they emit characteristic wavelengths of light.
The emitted light, which is specific to each element, is then passed through a monochromator to isolate the wavelength of interest, and the intensity of the emitted light is measured using a photodetector.
Key Components:

Flame Source: The sample solution is introduced into a flame, typically a hydrogen-oxygen flame or an air-acetylene flame, where atomization and excitation occur.

Monochromator: The monochromator is used to select a specific wavelength of light corresponding to the characteristic emission line of the metal being analyzed.

Photodetector: A photodetector, such as a photomultiplier tube (PMT), measures the intensity of the emitted light at the selected wavelength.

Readout and Data Analysis: The instrument provides a readout of the emission intensity, which is then used to calculate the concentration of the target metal ion in the sample based on the relationship between emission intensity and concentration.

What a Flame Photometer Does:

A flame photometer is used for the quantitative determination of metal ions in various sample types, including aqueous solutions, biological fluids, geological samples, and environmental samples.
It is particularly useful for the analysis of alkali metals (e.g., sodium, potassium, lithium) and alkaline earth metals (e.g., calcium, magnesium) due to their characteristic emission lines.
Flame photometry is widely employed in clinical laboratories for the measurement of electrolytes in blood and urine, environmental analysis for the detection of metals in water and soil, and industrial applications where the concentration of specific metal ions needs to be determined.
Flame photometry is known for its simplicity, speed, and accuracy in measuring metal ion concentrations. It provides a direct and selective method for metal analysis.
However, it’s important to note that flame photometry is limited to the analysis of specific metal ions and is not suitable for compounds containing multiple elements or other types of analytes. In such cases, more versatile techniques like atomic absorption spectroscopy (AAS) or inductively coupled plasma atomic emission spectroscopy (ICP-AES) are employed.

53
Q

What are the principles of the ICP torch?

A
54
Q

What are the sources of interference in atomic emission?

A

In atomic emission spectroscopy, interference can arise from various sources that affect the accuracy and precision of the analysis. Identifying and mitigating these interferences is crucial to obtaining reliable results. Some common sources of interference in atomic emission spectroscopy include:

Chemical Interferences:

Ionization Interference: Some elements or compounds can be ionized more easily than others in the high-temperature environment of the plasma, leading to interference. For example, alkali metals are prone to ionization interference.
Formation of Compounds: Chemical reactions between the sample and the plasma can lead to the formation of compounds that affect the emission spectrum. For example, oxides, hydrides, and chlorides can interfere with the analysis.
Spectral Interferences:

Line Overlaps: Spectral interferences occur when the emission lines of different elements or ions overlap in the spectrum, making it challenging to distinguish and quantify individual elements. For example, the lines of adjacent elements in the periodic table may overlap.
Continuum Emission: The presence of a continuum emission background can obscure weaker atomic lines, making them difficult to detect and quantitate.
Matrix Effects:

Matrix Interference: The matrix of the sample can affect the emission intensity of the analyte. For example, the presence of complex matrices, high salt content, or high viscosity can lead to matrix effects, affecting the analyte’s atomization and excitation.
Polyatomic Interferences:

Polyatomic Ions: The presence of polyatomic ions or molecules in the sample can emit lines that overlap with the lines of the analyte. For example, the presence of carbon-containing compounds can lead to carbon-based molecular bands that interfere with the analysis.
Background Emission:

Continuum Background: The presence of a high continuum background emission can interfere with the detection of weak atomic lines.
Plasma-Related Interferences:

Ionization and Excitation Temperature: Variations in the temperature and conditions of the plasma can affect the ionization and excitation processes, leading to interferences. These variations can be caused by changes in gas flow rates, power settings, or instrument drift.
Spectrometer-Related Interferences:

Instrumental Drift: Drift in the spectrometer’s optical components, such as the diffraction grating or photodetector, can result in baseline shifts or fluctuations in signal intensity.

55
Q

How do standard additions work and how to use them to find the prescemce of interferences?

A

Standard additions are a common technique used in analytical chemistry to determine the concentration of an analyte in a sample, particularly when interferences may be present. The method is based on adding a known amount of a standard solution of the analyte to the sample and measuring the resulting change in the analytical signal. Here’s how standard additions work and how to use them to find the presence of interferences:

Principle of Standard Additions:

Prepare the Sample: Start with a sample of unknown concentration that you suspect may contain interferences.

Add Standard Solutions: Prepare a series of standard solutions with known concentrations of the analyte. These standards are added to the sample in equal volumes.

Measure the Signal: Measure the analytical signal (e.g., absorbance, fluorescence intensity, emission intensity) for each standard addition as well as for the sample without any added standard. This gives you a series of measurements.

Plot the Data: Create a plot (commonly a calibration curve) of the measured signal against the concentration of the added standard. Typically, a linear relationship is expected if there are no interferences.

Using Standard Additions to Find Interferences:

Interferences can manifest in various ways, affecting the signal in different manners. Standard additions can help identify the presence of interferences in the following ways:

Signal Suppression: If an interference causes signal suppression, you’ll observe a decrease in the signal as the concentration of the added standard increases. The plot will show a negative slope.

Signal Enhancement: If an interference enhances the signal, you’ll observe an increase in the signal as the concentration of the added standard increases. The plot will show a positive slope.

No Effect: In an ideal case with no interferences, the signal should increase linearly with the added standard concentration, forming a straight line with a positive slope.

By analyzing the relationship between the added standard concentration and the signal, you can identify interferences. In cases of suppression or enhancement, it’s important to investigate the source of the interference and take appropriate corrective measures. These measures may include using matrix-matched standards, using different sample preparation techniques, or considering alternative analytical methods.

The standard additions technique provides a way to correct for interferences and accurately determine the analyte concentration in the presence of potential interfering substances. It is particularly useful when you cannot easily remove or separate the interfering components from the sample.

56
Q

What are the priciples of the ICP torch?

A

The Inductively Coupled Plasma (ICP) torch is a crucial component of ICP-AES (Inductively Coupled Plasma Atomic Emission Spectroscopy) and ICP-MS (Inductively Coupled Plasma Mass Spectrometry). It plays a central role in the atomization and excitation/ionization of the sample for subsequent analysis. The principles of the ICP torch are as follows:

Generation of Plasma:

Introduction of Argon Gas: A flow of inert argon (Ar) gas is introduced into the torch. This gas serves several key functions:

It carries the sample into the torch for atomization and excitation/ionization.
It provides a cooling effect to maintain the stability of the high-temperature plasma.
It ensures a continuous flow of analyte atoms and ions for further analysis.
RF Coil Induction: Surrounding the torch chamber is an RF (radiofrequency) coil, typically made of copper. This RF coil generates an oscillating magnetic field, which induces an electric field within the torch chamber. This is where the “inductively coupled” part of the name comes from.

Ionization and Atomization:

Plasma Formation: The oscillating magnetic field generated by the RF coil induces an electric field within the torch chamber, leading to the creation of a high-temperature plasma. This plasma consists of ions, electrons, and neutral atoms. It operates at extremely high temperatures (around 6,000-10,000°C).

Sample Introduction: The sample, typically in liquid form, is introduced into the high-temperature plasma as an aerosol. This aerosol is created using a nebulizer, which converts the liquid sample into tiny droplets. The high temperature of the plasma causes these droplets to evaporate, atomize, and eventually become excited or ionized.

Emission or Ionization:

Emission (ICP-AES): In ICP-AES, the high-temperature plasma excites the analyte atoms, causing them to transition to higher energy levels. As these atoms return to their ground state, they emit characteristic wavelengths of light. The emitted light is collected and passed through a spectrometer, which disperses the light and measures its intensity. The resulting spectrum is used to identify and quantify the elements in the sample.

Ionization (ICP-MS): In ICP-MS, the high-temperature plasma efficiently ionizes the sample atoms, typically forming positively charged ions. These ions are then directed into a mass spectrometer, where their mass-to-charge ratios are measured, allowing for precise quantification and isotopic analysis.

The ICP torch creates a stable, high-temperature environment suitable for the efficient atomization, excitation, and ionization of a wide range of elements. This makes ICP-AES and ICP-MS powerful techniques for elemental analysis, providing high sensitivity and the ability to analyze a wide range of elements across various applications.

57
Q

How do you calculate the difference in energy levels?

A

difference in E = hv = hc/wavelength
There are a number of higher energy unfilled orbitals therefore a number of observed absorption/emission lines for each element
each element has its own characteristics absorption/ emission wavelength in UV/ visible region e.g na the most intense line is wavelength = 589nm (yellow-orange)

58
Q

what is ionisation

A

when energies more than 5.2 eV cause the electron to be removed altogether from the atom.

59
Q

What is flame photometry?

A

Na yellow
Ca brick red
K lilac
ground state atoms are thermally excited then emit light of charcteristic wavelength as they return to ground state.
calcium is also measured

60
Q

what is the flame used for in flame photometry?

A

volatilise the solution containing metals
use compressed gas or natural air for the flame at 2000 degrees
higher temp required for other ,etals such as mg which would use a air/acetylene flame at 2500 degrees

61
Q

what are the features of detection?

A

flame photometers are very simple, cheap instruments
use photosensitive detectors similar to PMT but not necessarily as sensitive
light emitted from sample is detected and converted into an electrical signal which is then displayed

62
Q

Inductively coupled plasma optical emission spectroscopy (ICP-OES)

A

an icp torch is a device which produces plasma - a fireball of atoms, ions and elctorns interacting at very high energies with temperatured up to 10,000K
- very efficient atomisation source
- exposing a sample to high temperatur plasma converts a very large proportion of its constituents atoms to an excited state
- ICP- OES can identify and determine simultaneously up to 40 elements with detection limits of parts per billion

63
Q

What is ICP?

A

alternative atom cells for AE, inductively coupled plasma

fuel and oxidant of flame replaced by Ar
powerful ratio-frequency rf applied to Cu load coil (induction coil) - Ar gas swirls through

the rf current has as associated magnetic field with lines of force passing along the axis of a quartz tube placed in the coil - Rf energy applied to induction coil

a spark is applied which ionises a dew Ar atoms - Spark causes some Ar to ionise and form free e

the e formed are rapidly accelerated to and drom in circular orbits by rapidly alternating electric field

collisions cause gas to heat up to high temperature forming - flow from the nebuliser, caarrying the sample drives a channel through the plasma

64
Q

what are the advantages of ICP-OES

A

-offers simultaneous analysis capability
- high T of plama gives large choice of emission lines for wide range of elements
- good detection limits
- long linear calibration ranges
- good precision (1 or 2%)

65
Q

What are different sources of interferences?

A

Ionisation
- at high temperature atoms such as K can loose an electron and therefore reduce the observed emission from the sample K-K+
- must add more readily ionised element to the sample to compensate
- e.g. strontium chloride solution is added to suppress ionisation of K in the BP assay of effervescent KCL

Spectral
- two overlapping spectral lines
- must select a different non - overlapping emission line
- there are more than 50,000 ICP - OES spectral lines documented

Chemical
-Presence of low volatility compounds not readily atomised
- sulphate and phosphate form involatile salts with metals abd reduce sample reading
- remove by adding lanthanum chlorise which precipitated them out and replaces them with chloride anions

calibration graph non - linear at high concentrations
- due to reabsorption of emitted light by ground state atoms/ ionis in flame

  • matrix effects i.e effects due to excipients (physical effects)
  • density, surface tension and viscocity all affect rates of aspiration and nebulisation
  • alters the rate of aspiration relative to the standard solutions therby producing different results
  • e.g sugar ion syrups inc viscocity, formation of less volatile salts
66
Q

What are standard additions?

A

used to eliminate matrix effects i.e. interference due to excipients in sample

increasing volumes of standard solution added to sample (spiked)

Amount of drug in sample found by extrapolation of graph to x axis

increases accuracu and precision of assay

67
Q

summary of atomic emission
flame photometry
ICP-OES
Standard additions

A

flame photometry - Atomic elements, simple, cheap, alkali metals only
change in energy is characteristic of each element, makes atomic spectroscopy very specific

ICP-OES - more expensive but more applications and lower detection limits

Standard additions - used to eliminate matrix effects
- increases accuracy and precision of assay

68
Q

What is the method of standard additions?

A

if interference (error in analytical result) is presnt which reduces samples absorbance then low concentration will result if use a normal caliobration graph

if we add the standard in incremental amounts to our sample and plot the readings against concentration of added standard - standard addition graph

69
Q

what is the difference betwen atomic absorption and atomic emission?

A

Measurement Principle:

Atomic Absorption Spectroscopy (AAS): AAS measures the concentration of specific elements by analyzing the absorption of light at the characteristic wavelength(s) of the element. It quantifies the number of ground-state atoms that absorb light energy to move to an excited state. The absorbance is directly proportional to the analyte concentration.

Atomic Emission Spectroscopy (AES): AES measures the concentration of elements by analyzing the emission of light at characteristic wavelengths when atoms in the sample are excited to higher energy states and then return to lower energy states. In AES, the intensity of emitted light is directly proportional to the analyte concentration.

  1. Analyte State:

AAS: AAS focuses on the analysis of ground-state atoms in the sample. It measures the absorption of light by atoms transitioning from the ground state to an excited state.

AES: AES focuses on the analysis of excited-state atoms. It measures the emission of light by atoms transitioning from excited states back to the ground state.

  1. Spectral Information:

AAS: AAS provides information about the absorption lines of elements. It shows dark lines or absorption bands in the spectrum at the characteristic wavelengths of the elements being analyzed.

AES: AES provides information about the emission lines of elements. It shows bright lines or emission bands in the spectrum at the characteristic wavelengths of the elements being analyzed.

  1. Sensitivity:

AAS: AAS is generally less sensitive than AES. It is well-suited for trace element analysis but may not be as sensitive as AES in some cases.

AES: AES is highly sensitive and is often used for trace element analysis, especially in applications where lower detection limits are required.

  1. Selectivity:

AAS: AAS is selective because it only measures the absorption of light by the specific element being analyzed, and the characteristic wavelength is used for identification.

AES: AES can be selective but may require additional measures (e.g., using a monochromator) to isolate and measure specific emission lines, especially in complex matrices.

70
Q

How does the light source used in AA work?

A

Hollow Cathode Lamp (HCL): The most common type of light source used in AAS is the hollow cathode lamp (HCL). Inside the HCL, there is a hollow cathode, typically made of the same metal as the analyte of interest. For example, if you are analyzing calcium (Ca), the hollow cathode will be made of calcium metal.

Cathode and Anode: The hollow cathode lamp has an anode and a cathode. The cathode is the metal target and is hollow to allow for the passage of gas. The anode is typically a metal rod positioned in the center of the cathode.

Gas Filling: The hollow cathode lamp is filled with a noble gas, such as argon (Ar) or neon (Ne). The noble gas serves to initiate and sustain a discharge when an electric current is applied.

Electrical Discharge: When an electric current is passed through the lamp, a low-pressure discharge is created within the lamp. This discharge produces a small, high-temperature, and high-energy plasma in the vicinity of the hollow cathode.

Line Emission: The high-energy plasma in the hollow cathode lamp causes the metal atoms from the cathode to be excited to higher energy states. As these excited atoms return to their ground state, they emit light at characteristic wavelengths (emission lines) that are unique to the element of the hollow cathode material. These emitted wavelengths correspond to the resonance lines of the element.

Broad Spectrum: Although the lamp is designed for a specific element (e.g., a calcium hollow cathode lamp for Ca analysis), it often emits a range of wavelengths, covering a portion of the electromagnetic spectrum that includes the resonance line of interest. This broad spectrum is used to account for any variations in the atomization and excitation conditions of the sample.

Light Source Stability: The HCL provides a stable and consistent source of light over time, which is essential for accurate and reliable AAS measurements.

71
Q

What is background correction and what is its uses?

A

Background correction is a technique used in analytical spectroscopy to improve the accuracy and precision of measurements by compensating for interference or noise caused by sources other than the analyte of interest. It helps to enhance the signal-to-noise ratio and correct for baseline variations in the analytical signal. Background correction is commonly employed in various spectroscopic methods, including atomic absorption spectroscopy (AAS), atomic emission spectroscopy (AES), and UV-Vis spectroscopy, among others.

The main purposes of background correction are as follows:

Minimizing Interference: Background correction helps to reduce the influence of interfering species or spectral features that may overlap with the absorption or emission lines of the analyte. Interference can lead to inaccurate quantification.

Enhancing Sensitivity: By reducing noise and interference, background correction improves the sensitivity of the analytical method, allowing for the accurate detection of lower concentrations of the analyte.

Correcting Baseline Drift: Spectroscopic instruments may exhibit baseline drift, where the signal intensity varies with time due to factors like instrument instability or changes in the sample matrix. Background correction compensates for this drift and maintains a stable baseline.

Improving Precision: Background correction enhances the precision of measurements by providing a more consistent and reliable baseline, reducing random errors, and minimizing the impact of non-analyte-related variations.

There are several methods for background correction in spectroscopy, including:

Deuterium Lamp Correction: In UV-Vis spectroscopy, a deuterium lamp is often used as a light source to correct for baseline drift, as it emits a continuous spectrum with no spectral features.

Continuum Source Correction: In AAS and AES, a continuum source, such as a xenon lamp, can be used to correct for background variations, allowing for more accurate determination of the analyte’s absorbance or emission lines.

Zeeman Effect Correction: In AAS, the Zeeman effect is utilized for background correction. By applying a magnetic field, the atomic absorption lines split into multiple components, and background correction is achieved by measuring the absorbance at a specific component.

Method of Standard Additions: In situations where chemical interference is suspected, the method of standard additions can be employed. This involves adding known amounts of the analyte to the sample to correct for interference.

Chemometric Techniques: Advanced statistical methods, such as baseline correction algorithms, can be applied to spectroscopic data to remove baseline variations and enhance the accuracy of measurements.

72
Q

What are the advantages of using a graphite furnance?

A

A graphite furnace, also known as a graphite tube furnace, is a key component in techniques like graphite furnace atomic absorption spectroscopy (GFAAS) and graphite furnace atomic absorption spectrometry (GF-AAS). It offers several advantages for the analysis of trace elements and is particularly useful in situations where high sensitivity and precision are required. Some of the advantages of a graphite furnace include:

  • sample applied directly to furnace so no need for nebuliser - all sample participates in measurement process
  • detection limits are 100-1000 x better than flame
  • the atoms are presnt in atom cell for long time
    -furnace working range for real samples is 1-100ppb
  • only small amounts of sample material required
  • elements with resonance lines near 200 nm can be measured becayse of absence of flame gases
  • potential for direct analysis of solids

Enhanced Sensitivity: The use of a graphite furnace allows for significantly enhanced sensitivity compared to flame atomic absorption spectroscopy (FAAS). This is particularly important when analyzing samples with very low concentrations of trace elements.

Reduced Interference: Graphite furnaces can reduce spectral and chemical interferences, leading to more accurate and precise measurements. The high-temperature environment of the furnace can effectively remove chemical matrices that could interfere with the analysis.

Small Sample Volume: GFAAS requires only a small sample volume, making it suitable for applications where the sample quantity is limited, such as clinical, biological, and environmental analyses.

Improved Detection Limits: The enhanced sensitivity of a graphite furnace allows for lower detection limits, making it suitable for trace and ultratrace element analysis.

Improved Precision: The controlled temperature and heating profile of the graphite furnace provide better precision in the atomization process, leading to consistent and reproducible results.

Wide Element Range: While GFAAS is often associated with the analysis of nonmetals like arsenic, selenium, and antimony, it can also be used for the analysis of a wide range of elements. Different analytical lines and conditions can be established for various elements.

Single-Element Analysis: Graphite furnaces are particularly suitable for single-element analysis, ensuring that the analyte of interest is specifically measured without interference from other elements.

Variable Heating Programs: GFAAS instruments allow for the application of complex heating programs, which can be optimized for specific analytes, further improving precision and sensitivity.

Sample Matrix Tolerance: Graphite furnaces are less affected by the sample matrix, which can make them more robust and versatile in handling various sample types.

Automated Samplers: Many modern GFAAS instruments feature automated samplers that can process multiple samples sequentially, improving sample throughput and laboratory efficiency.

73
Q

summary
- atomic absorption
graphite furnace

A

atomic absorbance
newer, much more metals analysed, higher T flame than flame photometry
Graphite furnace
- removes flame and replaces with fraphite furnace
-heated electrically so removes flame interferences
able to use solid samples
- greater sensitivity than flame due to longer resonance times
- incorporates a L’vov platfform to help remove temp gradients in the cekk.

74
Q

What happens in AE?

A

A flame is used to excite electrons from ground state to an excited state Boltzmann law

75
Q

What happens in AA?

A

flame is only used to atomise the sample. Absorption is carried out using a hollow cathode lamp

76
Q

What instruments are used in Atomic absorption?

A

Hollow cathode lamp - made of same metal as sample - emits light of exacvtly the same wavelength as abosprbed by sample

Flame - 10cm acetylene flame, acts as absorbance cell should not excite the sample

Modulator - provides lamp with AXC current to overcome small number of excited atoms emitting light
- only amplifies light from the lamp and not the flame

  • modern instruments use graphite furnace
77
Q

What is the MAIN light source in atomic absorption?

A

Hollow cathode lamp
The cathode is made up of element that is being analysed
several hundred V applied between electrodes
Highly energetic electrons emitted by cathode
- Ar ionised by collison
Ar+ accelerated to cathode causing sputtering m solid to m gas
- metal atoms are excited by collisions with electrons and - the excited metal atoms then emit charesteristic atomic emission lines M star g to M g + hv
- temperature of gas in emission region is only a few hundrd degrees and is at low pressure
- little doppler broadnening
- little pressure broadnening
- i.e very narrow lines

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

LIMITATIONS
- one lmap required for each elem,eny
Not good for volatile elements e/g As, Se
use elctrodeless discahrge lamp.

78
Q

What is the difference between AA and FP?

A

AA has a wider application than FP (40 metals vs 4)
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 sortage

79
Q

What are the disadvantages of AA?

A

Only determins one metal at a time
have to change lamps for multi-component assays
useful for many assay of same metal, but poor for multi - component analysisn of single sample
does not determine non-metals
expensive comoared to FP

80
Q

what is the L’vov platform for?

A

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

81
Q

GFAAS procedure

A

Procedure
Sample (1-100 μl) injected by micropipette via injection hole in top of tube
Tube is heated rapidly by electric current (300 A) to volatilise and atomise sample (graphite material resists the passage of electric current and converts electrical energy into heat)
Inert gas flow (Ar) used to flush tube and prevent formation of refractory oxides and prevent tube incineration
Atoms take several seconds to diffuse down tube giving rise to transient absorption signal

82
Q
A