Time of Flight Mass Spectrometry (AQA A Level Chemistry): Revision Note

Exam code: 7405

Stewart Hird

Written by: Stewart Hird

Reviewed by: Philippa Platt

Updated on

Time of Flight (TOF) Mass Spectrometry

  • Mass spectrometry is a powerful analytical technique

  • It is the most useful instrument for the accurate determination of:

    • The relative atomic mass (Ar) of an element

    • The relative molecular mass (Mr) of a molecule

  • As a sample passes through the mass spectrometer, a spectrum is produced

    • The spectrum plots the abundance of ions against their mass-to-charge ratio (m/z)

  • The peak with the highest m/z value is often the molecular ion peak (M+)

  • The tallest peak in the spectrum is called the base peak

Principles of TOF mass spectrometry

  • The entire apparatus is kept under a high vacuum to prevent ions from colliding with air molecules.

  • There are 4 key stages:

    • Ionisation

    • Acceleration

    • Ion drift

    • Detection

Ionisation

  • The sample is converted into positive ions.

  • The two main methods are electron impact and electrospray ionisation

Electron impact:

  • This is used for elements and low-mass compounds

  • High-energy electrons bombard the vaporised sample from an electron gun

  • The high-energy electrons knock an electron off each particle to form a 1+ ion:

X (g) → X+ (g) + e-

  • The 1+ ions formed are called molecular ions (M+)

  • This high-energy process can also cause the M+ ion to break into smaller pieces, known as fragments

    • Fragment ions also pass through a TOF mass spectrometer and appear on the final mass spectrum

Electrospray ionisation (ESI):

  • This is used for higher-mass compounds (like proteins) to prevent fragmentation

  • This is a 'soft ionisation' technique

  • The sample is dissolved in a volatile solvent and injected through a high-voltage needle

  • This causes the particles to gain a proton (H+) from the solvent:

M (g) + H+ → MH+ (g)

Examiner Tips and Tricks

In electrospray ionisation, the mass of the detected ion will be the relative molecular mass of the sample + 1 (Mr + 1)

Flowchart showing ionisation: a sample in a volatile solvent forms an aerosol, becomes charged droplets, then ions in a high vacuum region.
Inside the time of flight mass spectrometer 

Acceleration

  • The positive ions are:

    • Attracted towards a negatively charged plate

    • Accelerated by an electric field

  • The key principle is that all ions are accelerated to have the same kinetic energy (KE)

  • Since KE = ½mv2:

    • Ions with a lower mass have a higher velocity

    • Ions with a higher mass have a lower velocity

Ion drift

  • The accelerated ions pass through a hole in the negatively charged plate and travel down a flight tube

    • The flight tube is a region with no electric field

  • The time it takes for an ion to travel this distance is its time of flight

  • Ions with a lower mass-to-charge ratio (m/z):

    • Travel faster

    • Have a shorter time of flight

Diagram of a process showing sample injection, ionisation, acceleration, ion drift and detection in a TOF mass spectrometer.
Lighter ions arrive at the detector first as they have higher velocities than heavier ions

Detection

  • The ions arrive at a detector (an electron multiplier)

  • When an ion hits the detector, it gains an electron, which generates a small electric current

  • The size of this current is directly proportional to the abundance of that specific ion

  • A computer records the time of flight and relative abundance for each ion to produce the mass spectrum

Example mass spectrum of boron

Graph showing isotopic abundance. Two bars at mass-to-charge ratios 10 and 11, with 19.9% and 80.1% abundance respectively. Arrows indicate axes.
The peak heights show the relative abundance of the boron isotopes: boron-10 has a relative abundance of 19.9% and boron-11 has a relative abundance of 80.1%

Key calculations for TOF mass spectrometry

  • TOF mass spectrometry uses two key equations:

  1. Kinetic energy:

KE = ½mv2

  • Where:

    • KE = kinetic energy of the particles (J)

    • m = mass of the particles (kg)

    • v = velocity of the particles (ms-1)

  1. Velocity:

v = straight d over straight t

  • Where:

    • v = velocity of the particles (ms-1)

    • d = the length of the flight tube (m)

    • t = time of flight of the particles (s)

  • The kinetic energy and velocity equations are often combined

  • KE = ½mv2 rearranges to:

v = square root of fraction numerator 2 KE over denominator straight m end fraction end root

  • v = straight d over straight t rearranges to:

t = straight d over straight v

  • Substituting v into the t = straight d over straight v equation gives:

t = dsquare root of fraction numerator straight m over denominator 2 KE end fraction end root

  • Unit conversions are crucial:

    • The mass (m) of the ion must be in kilograms (kg)

    • The length of the flight tube (d) must be in metres (m)

  • Calculating the mass of a single ion:

    • To convert the relative isotopic mass to the correct mass in kg:

      1. Divide the relative isotopic mass by the Avogadro constant (L) (6.022 x 1023)

      2. Divide the result by 1000 to convert it from grams to kilograms

Worked Example

In a TOF mass spectrometer, the time of flight, t, of an ion is shown by the

equation

t space equals space d square root of fraction numerator m over denominator 2 E end fraction end root

In this equation d is the length of the flight tube, m is the mass, in kg, of an ion, and E is the kinetic energy of the ions.

In this spectrometer, the kinetic energy of an ion in the flight tube is 1.013 × 10−13 J

The time of flight of a 49Ti+ ion is 9.816 × 10−7 s

Calculate the time of flight of the 47Ti+ ion.

Give your answer to the appropriate number of significant figures.

Answer

  • Rearrange the given expression,

d equals t square root of fraction numerator 2 E over denominator m end fraction end root

  • Substitute the known values,

d equals t to the power of 47 square root of fraction numerator 2 E over denominator 47 cross times 10 to the power of negative 3 end exponent divided by L end fraction end root equals t to the power of 49 square root of fraction numerator 2 E over denominator 49 cross times 10 to the power of negative 3 end exponent divided by L end fraction end root

  • Simplify,

fraction numerator t to the power of 47 over denominator square root of 47 end fraction equals fraction numerator t to the power of 49 over denominator square root of 49 end fraction

  • Find the TOF for 47Ti+,

t to the power of 47 equals fraction numerator t to the power of 49 cross times square root of 47 over denominator square root of 49 end fraction equals fraction numerator 9.816 cross times 10 to the power of negative 7 end exponent cross times square root of 47 over denominator square root of 49 end fraction

t to the power of 47 equals 9.6 cross times 10 to the power of negative 7 end exponent space s

Examiner Tips and Tricks

Remember: All particles are accelerated to the same kinetic energy

The time of flight is proportional to the square root of the mass of the ions

Lighter ions travel faster and have a shorter time of flight

Heavier ions travel more slowly and have a longer time of flight

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Stewart Hird

Author: Stewart Hird

Expertise: Chemistry Content Creator

Stewart has been an enthusiastic GCSE, IGCSE, A Level and IB teacher for more than 30 years in the UK as well as overseas, and has also been an examiner for IB and A Level. As a long-standing Head of Science, Stewart brings a wealth of experience to creating Topic Questions and revision materials for Save My Exams. Stewart specialises in Chemistry, but has also taught Physics and Environmental Systems and Societies.

Philippa Platt

Reviewer: Philippa Platt

Expertise: Chemistry Content Creator

Philippa has worked as a GCSE and A level chemistry teacher and tutor for over thirteen years. She studied chemistry and sport science at Loughborough University graduating in 2007 having also completed her PGCE in science. Throughout her time as a teacher she was incharge of a boarding house for five years and coached many teams in a variety of sports. When not producing resources with the chemistry team, Philippa enjoys being active outside with her young family and is a very keen gardener