6 Isotopes, Atomic Mass, and Mass Spectrometry (M2Q3)


This section explores isotopes. We’ll examine how we use mass spectrometry to precisely measure the mass and abundance of a given element’s isotopes. The section below provides more detailed description of these topics, worked examples, and practice problems.

Learning Objectives for Isotopes, Atomic Mass, and Mass Spectrometry

  • Recognize that elements are identified by the number of protons, but the number of neutrons may vary (isotopes).
    | Isotopes |
  • Calculate natural abundance and atomic mass from mass spectrometry data.
    | Natural Abundance |
  • Sketch a mass spectrometer and explain how one works.
    | Mass Spectrometer |
  • Use mass spectrometry data to predict the composition of a molecule; use a molecule’s composition to predict it’s hard and soft mass spectra.
    | Mass Spectrometry of Molecules |

| Key Concepts and Summary | Key Equations | Glossary | End of Section Exercises |


Although all atoms of an element exhibit similar behavior, they are not all the same. The symbol for a specific isotope of any element is written by placing the mass number as a superscript to the left of the element symbol (Figure 1). The atomic number is sometimes written as a subscript preceding the symbol, but since this number defines the element’s identity, as does its symbol, it is often omitted. For example, magnesium exists as a mixture of three isotopes, each with an atomic number of 12 and with mass numbers of 24, 25, and 26, respectively. These isotopes can be identified as 24Mg, 25Mg, and 26Mg. These isotope symbols are read as “element, mass number” and can be symbolized consistent with this reading. For instance, 24Mg is read as “magnesium 24,” and can be written as “magnesium-24” or “Mg-24.” 25Mg is read as “magnesium 25,” and can be written as “magnesium-25” or “Mg-25.” All magnesium atoms have 12 protons in their nucleus. They differ only because a 24Mg atom has 12 neutrons in its nucleus, a 25Mg atom has 13 neutrons, and a 26Mg has 14 neutrons.

This diagram shows the symbol for helium, “H e.” The number to the upper left of the symbol is the mass number, which is 4. The number to the upper right of the symbol is the charge which is positive 2. The number to the lower left of the symbol is the atomic number, which is 2. This number is often omitted. Also shown is “M g” which stands for magnesium It has a mass number of 24, a charge of positive 2, and an atomic number of 12.
Figure 1. The symbol for an atom indicates the element via its usual two-letter symbol, the mass number as a left superscript, the atomic number as a left subscript (sometimes omitted), and the charge as a right superscript.

Information about the naturally occurring isotopes of elements with atomic numbers 1 through 10 is given in Table 1. Note that in addition to standard names and symbols, the isotopes of hydrogen are often referred to using common names and accompanying symbols. Hydrogen-2, symbolized 2H, is also called deuterium and sometimes symbolized D. Hydrogen-3, symbolized 3H, is also called tritium and sometimes symbolized T.

Element Symbol Atomic Number Number of Protons Number of Neutrons Mass (amu) % Natural Abundance
hydrogen [latex]_1^1[/latex]H (protium) 1 1 0 1.0078 99.989
[latex]_1^2[/latex]H (deuterium) 1 1 1 2.0141 0.0115
[latex]_1^3[/latex]H (tritium) 1 1 2 3.01605 — (trace)
helium [latex]_2^3[/latex]He 2 2 1 3.01603 0.00013
[latex]_2^4[/latex]He 2 2 2 4.0026 100
lithium [latex]_3^6[/latex]Li 3 3 3 6.0151 7.59
[latex]_3^7[/latex]Li 3 3 4 7.0160 92.41
beryllium [latex]_4^9[/latex]Be 4 4 5 9.0122 100
boron [latex]_5^{10}[/latex]B 5 5 5 10.0129 19.9
[latex]_5^{11}[/latex]B 5 5 6 11.0093 80.1
carbon [latex]_6^{12}[/latex]C 6 6 6 12.0000 98.89
[latex]_6^{13}[/latex]C 6 6 7 13.0034 1.11
[latex]_6^{14}[/latex]C 6 6 8 14.0032 — (trace)
nitrogen [latex]_7^{14}[/latex]N 7 7 7 14.0031 99.63
[latex]_7^{15}[/latex]N 7 7 8 15.0001 0.37
oxygen [latex]_8^{16}[/latex]O 8 8 8 15.9949 99.757
[latex]_8^{17}[/latex]O 8 8 9 16.9991 0.038
[latex]_8^{18}[/latex]O 8 8 10 17.9992 0.205
fluorine [latex]_9^{19}[/latex]F 9 9 10 18.9984 100
neon [latex]_{10}^{20}[/latex]Ne 10 10 10 19.9924 90.48
[latex]_{10}^{21}[/latex]Ne 10 10 11 20.9938 0.27
[latex]_{10}^{22}[/latex]Ne 10 10 12 21.9914 9.25
Table 1. Nuclear Compositions of Atoms of the Very Light Elements

Demonstration: Heavy water is more dense than regular water

Set up. As shown in the table above, hydrogen and oxygen each have three isotopes. Of these isotopes, hydrogen-1 and oxygen-16 are by far the most common isotopes. Therefore, water molecules typically consist of two hydrogen-1 atoms and an oxygen-16 atom, giving a molecular weight of ~18 amu. It is possible to form “heavy water”—water that is composed of two hydrogen-2 atoms and an oxygen-16 atom. This heavy water has a molecular weight of ~20 amu. In this demonstration, we compare the density of solid regular water (regular ice) and solid heavy water (“heavy water ice”) by placing each into a glass of liquid regular water.

Prediction. Before watching the video, make a prediction about whether the heavy water ice will float or sink in the glass of liquid water.

Explanation. In this video, the regular ice floats on the liquid regular water, as expected for an ice cube in a glass of water because the density of solid (regular) water is less than the density of liquid (regular) water. However, the heavy water ice cube sinks to the bottom of the glass because the extra mass causes the density of the heavy water ice to be greater than the density of the liquid regular water, and therefore it is unable to float.


Use this Build an Atom simulator to build atoms of the first 10 elements, see which isotopes exist, check nuclear stability, and gain experience with isotope symbols.

Natural Abundance

Because each proton and each neutron contribute approximately one amu to the mass of an atom, and each electron contributes far less, the atomic mass of a single atom is approximately equal to its mass number (a whole number). However, the average masses of atoms of most elements are not whole numbers because most elements exist naturally as mixtures of two or more isotopes.

The mass of an element shown in a periodic table or listed in a table of atomic masses is a weighted, average mass of all the isotopes present in a naturally occurring sample of that element. This is equal to the sum of each individual isotope’s mass multiplied by its fractional abundance.

average mass  =  ∑(fractional abundance × isotopic mass)i

For example, the element boron is composed of two isotopes: About 19.9% of all boron atoms are 10B with a mass of 10.0129 amu, and the remaining 80.1% are 11B with a mass of 11.0093 amu. The average atomic mass for boron is calculated to be:

boron average mass  =  (0.199 × 10.0129 amu) + (0.801 × 11.0093 amu)
=  1.99 amu + 8.82 amu
=  10.81 amu

It is important to understand that no single boron atom weighs exactly 10.8 amu; 10.8 amu is the average mass of all boron atoms, and individual boron atoms weigh either approximately 10 amu or 11 amu.

Example 1

Calculation of Average Atomic Mass
A meteorite found in central Indiana contains traces of the noble gas neon picked up from the solar wind during the meteorite’s trip through the solar system. Analysis of a sample of the gas showed that it consisted of 91.84% 20Ne (mass 19.9924 amu), 0.47% 21Ne (mass 20.9940 amu), and 7.69% 22Ne (mass 21.9914 amu). What is the average mass of the neon in the solar wind?


neon average mass  =  (0.9184 × 19.9924 amu) + (0.0047 × 20.9940 amu) + (0.0769 × 21.9914 amu)
=  (18.36 + 0.099 + 1.69) amu
=  20.15 amu

The average mass of a neon atom in the solar wind is 20.15 amu. (The average mass of a terrestrial neon atom is 20.1796 amu. This result demonstrates that we may find slight differences in the natural abundance of isotopes, depending on their origin.)

Check Your Learning
A sample of magnesium is found to contain 78.70% of 24Mg atoms (mass 23.98 amu), 10.13% of 25Mg atoms (mass 24.99 amu), and 11.17% of 26Mg atoms (mass 25.98 amu). Calculate the average mass of a Mg atom.


24.31 amu

We can also do variations of this type of calculation, as shown in the next example.

Example 2

Calculation of Percent Abundance
Naturally occurring chlorine consists of 35Cl (mass 34.96885 amu) and 37Cl (mass 36.96590 amu), with an average mass of 35.453 amu. What is the percent composition of Cl in terms of these two isotopes?

The average mass of chlorine is the fraction that is 35Cl times the mass of 35Cl plus the fraction that is 37Cl times the mass of 37Cl.

chlorine average mass  =  (fraction of 35Cl × mass of 35Cl) + (fraction of 37Cl × mass of 37Cl)

If we let x represent the fraction that is 35Cl, then the fraction that is 37Cl is represented by 1.00 − x.

(The fraction that is 35Cl + the fraction that is 37Cl must add up to 1, so the fraction of 37Cl must equal 1.00 − the fraction of 35Cl.)

Substituting this into the average mass equation, we have:

35.453 amu  =  (x × 34.96885 amu) + [(1.00 – x) × 36.96590 amu]
35.453  =  34.96885x + 36.96590 – 36.96590x
1.99705x  =  1.513
x  =  [latex]\frac{\text{1.513}}{\text{1.99705}}[/latex]  =  0.7576

So solving yields: x  =  0.7576, which means that 1.00 − 0.7576  =  0.2424. Therefore, chlorine consists of 75.76% 35Cl and 24.24% 37Cl.

Check Your Learning
Naturally occurring copper consists of 63Cu (mass 62.9296 amu) and 65Cu (mass 64.9278 amu), with an average mass of 63.546 amu. What is the percent composition of Cu in terms of these two isotopes?


69.15% Cu-63 and 30.85% Cu-65

Visit this site to make mixtures of the main isotopes of the first 18 elements, gain experience with average atomic mass, and check naturally occurring isotope ratios using the Isotopes and Atomic Mass simulation.

Mass Spectrometer

The occurrence and natural abundances of isotopes can be experimentally determined using an instrument called a mass spectrometer. Mass spectrometry (MS) is widely used in chemistry, forensics, medicine, environmental science, and many other fields to analyze and help identify the substances in a sample of material. There are many types of mass spectrometers, but we will concern ourselves with two styles: hard ionization and soft ionization mass spectrometers. In a hard-ionization mass spectrometer (Figure 2), the sample is vaporized and exposed to a high-energy plasma that causes any chemical bonds in the sample to be broken and the constituent atoms to become electrically charged, typically by losing one or more electrons. These cations then pass through a (variable) electric or magnetic field that deflects each cation’s path to an extent that depends on both its mass and charge (similar to how the path of a large steel ball bearing rolling past a magnet is deflected to a lesser extent that that of a small steel BB). The magnetic field deflects low mass ions more that high mass ions of the same charge. The ions are detected, and a plot of the relative number of ions generated versus their mass-to-charge ratios (a mass spectrum) is made. The height of each vertical feature or peak in a mass spectrum is proportional to the fraction of cations with the specified mass-to-charge ratio. Mass spectrometers can measure masses with very high resolution, on the order of 0.0001 amu. Thus, atoms with only slight differences in mass, such as isotopes, are readily detected and their relative abundances measured.

This diagram illustrates how a mass spectrometer works. A yellow box at the top left is labeled “Sample (M)”. A blue dashed line indicating the path of the sample comes out of the sample box and enters into an elbow-shaped ionization chamber that curves downward and is attached to a vacuum pump. The first part of the path is labeled “Ionized sample (M+)” indicating that in this section the sample is ionized. The turn in the ionization chamber is lined with magnets on the inside and outside of the turn. The blue dashed line that entered the ionization chamber splits into three different colored dashed lines: a green dashed line continues to travel around the curve and hits a green box at the end of the ionization chamber labeled “Collector” approximately in the middle. A yellow dashed line labeled “High mass ion (low deflection)” is deflected around the curve and hits the outside wall of the ionization chamber. A pink dashed line labeled “Low mass ion (high deflection)” is deflected so that it hits the inside wall of the curve. The pink and yellow lines do not hit the collector. The collector is then connected to a computer that outputs a mass spectrum, which is a plot of abundance on the y-axis vs. m/z on the x-axis.
Figure 2. This diagram illustrates the design of a mass spectrometer. In a hard-ionization mass spectrometer the sample is ionized by a high temperature plasma that breaks any bonds between atoms and causes them to lose electrons to make atomic cations.

Mass spectra of elements reveal the isotopic composition of the elements. The hard-ionization mass spectrum of a sample of Mg exhibits three peaks at mass-to-charge ratios of 24, 25, and 26 amu (Figure 3) indicating that the element magnesium consists of three isotopes. Although it is Mg ions that arrive at the detector of the mass spectrometer and not Mg atoms, the numbers on the x-axis indicate the mass of each atom of the isotope because the mass of a Mg ion is almost the same as a Mg atom. The relative height of each peak, often expressed as a percentage value, are the natural abundance of each isotope 79%, 10%, and 11%, respectively, the sum of which is 100%. The element magnesium therefore has 79% of the isotope 24Mg with 12 neutrons and 12 protons for a total mass of 24 amu. Because all Mg atoms have 12 protons, the two less abundant isotopes have 13 and 14 neutrons.


The hard mass spectrum of Magnesium is shown. A mass spectrum has an x-axis labeled “m/z” and a y-axis labeled “relative abundance”. The signals on a mass spectrum look like vertical lines (or spikes) at different x values. In this spectrum, there are vertical lines at x=24, x=25, and x=26. The spike at x=24 is labeled “79%” indicating that Mg-24 is 79% abundant. The spike at x=25 is labeled “10%” and the spike at x=26 is labeled “11%”.
Figure 3. The mass spectrum of a sample of Mg that demonstrates the occurrence of three isotopes with A  =  24, 25, 26 amu and abundances of 79, 10, and 11%, respectively.


See an animation that explains mass spectrometry. Watch this video from the Royal Society for Chemistry for a brief description of the rudiments of mass spectrometry.

Mass Spectrometry of Molecules

We’ve learned in a previous module on atoms and molecules that a chemical formula uses symbols and subscripts to represent the identity and abundance of atoms in a compound. But, how do we know this information? The previous section discussed the general analysis of the natural abundance of isotopes. Here, we’ll discuss simplified analysis of molecules through hard and soft ionization of molecules.

When a molecule is subjected to hard ionization, all covalent bonds are broken to produce monatomic ions. In the mass spectrum of hard MS, the mass to charge ratio (m/Z ratio) on the x-axis tells the mass of the ion (i.e., amu) since all ions have a +1 charge. The identity of the ion can then be inferred using the periodic table and its relative abundance determined using the height of the peak on the y-axis. Unlike hard MSsoft MS does not break the covalent bonds of the molecule. Because the molecule remains intact, soft MS tells the molecular weight of the whole compound on the x-axis, and the relative abundance on the y-axis.

Figure 4 and Figure 5 illustrate the difference between hard and soft MS of carbon dioxide, CO2. When all atom-to-atom bonds are broken in CO2 during hard ionization, the result is one C+ ion and two O+ ions.

Hard ionization mass spectrum of CO2. The x-axis is labeled with "m/z" and there are three vertical lines at x=12, x=13, and x=16. The vertical line at 12 has a height of 50%, the line at 16 has a height of 100%, and the line at 13 is hardly registered. This indicates that there are twice as many O atoms (at x=16) as C atoms (at x=12). The small spike at x=13 is for the other common isotope of carbon, C-13.
Figure 4. Hard MS of carbon dioxide, CO2.

Note that there are three discrete peaks visible in the mass spectra of CO2: one major peak at 12 amu, one very small peak at 13 amu, and a major peak at 16 amu. (Remember that we are assuming that the charge, Z, is equal to +1. This means that if the peak is at m/Z  =  12, then m must be 12 amu.) The peaks at 12 and 13 amu correspond to the two major isotopes of the element carbon, carbon-12 (98.9%) and carbon-13 (1.1% ). No peak is detected for carbon-14 as its natural abundance is extremely low. Separate analysis shows that the element oxygen is composed of mainly the isotope oxygen-16 (99.76%) with just trace amounts of two other isotopes, oxygen-17 and oxygen-18. Like carbon-14, these are not detected by this mass spectrometer due to their low natural abundance. The abundance of the peak at 16 amu has relative units of 100. Thus, if we compare the heights of the two major peaks at 12 and 16 amu, the ratio of carbon atoms to oxygen atoms is 1:2. This is also the ratio in the formula of carbon dioxide, CO2.

When subjected to soft ionization, the CO2 molecule remains intact, and ionization results in one CO2+ ion. Figure 5 shows that there are two discrete peaks visible in the mass spectra of CO2+ ion: one major peak at 44 amu and one very small peak at 45 amu. The abundance of the peak at 44 amu has relative units of 100, while the abundance of the peak at 45 amu is very small.

The soft mass spectrum of CO2 has an x-axis labeled as "m/z" and has two spikes: one at x=44, and another at x=45. The one at x=44 has a height of 100% and the one at x=45 is barely registered.
Figure 5. Soft MS of carbon dioxide, CO2.

Processing the data from the hard MS and soft MS provides different information. From the hard MS, we can calculate the molar mass of the lowest ratio of atoms, also called the empirical formula. If there is one copy of carbon and two copies of oxygen, then the molecule has a molar mass of 44 or 45 amu, depending on the isotope of carbon in the molecule. Since the molecule is not broken into its constituent parts in soft MS, the soft MS spectrum tells us the molecular weight of the molecule and therefore its molecular formula. The empirical formula from hard MS is the same value as the two peaks in the soft MS, which tells us that the molecular formula of the compound is CO2 (the same as the empirical formula in this instance). The CO2+ ion at 44 amu contains one carbon-12 atom plus two oxygen-16 atoms, while the CO2+ ion at 45 amu contains one carbon-13 atom plus two oxygen-16 atoms. As the abundance of carbon-12 is significantly greater than that of carbon-13, we expect the abundance of the ion at 44 amu to be much greater than that of the ion at 45 amu. Separate analysis shows the abundance to be 989 : 11 like that of the isotopes of the element carbon.

Example 3

More Complicated Mass Spectra

Use these mass spectra data to determine the chemical formula of an unknown compound.  Assume your sample contains only the predominant isotopes of the atoms.

Two mass spectrum are shown, a hard and soft. The hard mass spectrum shows two signals at x=1 and x=12 that are both at a height of 3. The soft mass spectrum shows a single signal at x=78 at a height of 7.

The hard MS has peaks at 1 amu and 12 amu, and they are approximately the same height.  Hydrogen has mass of 1 amu and carbon has mass of 12 amu, and they are in a 1:1 ratio.

The soft MS has a single peak at 78 amu.  If there was one hydrogen atom and one carbon atom in the molecule, then the mass of the compound would be 13 amu.  However, there is no peak at 13 amu.  There must be multiple copies of the CH-unit in the molecule.  Dividing the molecular weight (78 amu) by the empirical formula’s molecular weight (13 amu) gives the number of copies. There are 78/13 or six copies of the CH unit.  Thus, the unknown compound has a formula of C6H6.

Check Your Learning
Draw both the hard MS and soft MS of water.


Two mass spectrum are shown, a hard and soft. The hard mass spectrum shows two signals at x=1 and x=16. The signal at x=1 has a height of 8, and the signal at x=16 has a height of 4. The soft mass spectrum shows a single signal at x=18 and a heights of 8.

The formula for water is H2O.

In the hard MS, the signal at 1 amu represents H+ ion, and the signal at 16 amu represents O+ ion.  The ratio of the abundance of H+ ion to O+ ion is 2:1. Note that as long as the two peaks in the hard MS are represented in a 2:1 ratio it would be correct, e.g., drawing a 6:3 H:O ratio would be equally acceptable.

In the soft MS, there is a single peak at 18 amu for the H2O+ ion (1 + 1 + 16 amu). The single peak can be drawn at any height.



Example 4

Mass Spectra of a Molecule Containing Bromine

Use these mass spectra data to determine the chemical formula of an unknown compound.  The element bromine consists of two isotopes, 79Br (50.7%) and 81Br (49.3%).

This hard mass spectrum of an unknown compound has signals at x=1, x=12, x=79, and x=81. The spike at x=1 has a height of 60%, the spike at x=12 has a height of 20%, and the spikes at x=79 and x=81 each have a height of 10%.               This soft mass spectrum of an unknown compound has signals at x=94 and x=96. These spikes are the same height.

The hard MS has peaks at 1 amu, 12 amu, 79 amu and 81 amu. Hydrogen has mass of 1 amu and carbon has mass of 12 amu, and they are in a 3:1 ratio. The two peaks at 79 and 81 amu correspond to the single element, Br, that exists as two isotopes in very nearly equal abundances. Considered as a single element the sum of the two percentages needs to be calculated for comparison with the C and H. This indicates a C:H:Br ratio of 20:60:20 or 1:3:1. and an empirical formula of CH3Br.

The soft MS has two peaks at 94 and 96 corresponding to the molecular weights 94 amu and 96 amu of the two molecules CH379Br and CH381Br respectively. The empirical formula and actual formula are therefore the same for this molecule, i.e., CH3Br.

Key Concepts and Summary

Isotopes of an element are atoms with the same atomic number but different mass numbers; isotopes of an element, therefore, differ from each other only in the number of neutrons within the nucleus. When a naturally occurring element is composed of several isotopes, the atomic mass of the element represents the average of the masses of the isotopes involved.

Mass spectrometry is a powerful tool to identify elements by their mass. We can use hard MS to break apart the molecule and determine the identity of the constituent atoms (based on the location of the peaks) and the empirical formula of the compound (based on the ratio of atoms). We use soft MS to determine the molecular formula of a molecule since soft MS does not break the molecule apart into its constituent atoms.

Key Equations

  • average mass  =  ∑(fractional abundance × isotopic mass)i


atomic mass
average mass of atoms of an element, expressed in amu
empirical formula
formula showing the composition of a compound given as the simplest whole-number ratio of atoms
atoms that contain the same number of protons but a different number of neutrons
molecular formula
formula indicating the composition of a molecule of a compound and giving the actual number of atoms of each element in a molecule of the compound

Chemistry End of Section Exercises


  1. Visit the PhET Isotopes and Atomic Mass simulation site and select the “Mix Isotopes” tab, hide the “Percent Composition” and “Average Atomic Mass” boxes, and then select the element boron.
    1. Write the symbols of the isotopes of boron that are shown as naturally occurring in significant amounts.
    2. Predict the relative amounts (percentages) of these boron isotopes found in nature. Explain the reasoning behind your choice.
    3. Add isotopes to the black box to make a mixture that matches your prediction in (b). You may drag isotopes from their bins or click on “More” and then move the sliders to the appropriate amounts.
    4. Reveal the “Percent Composition” and “Average Atomic Mass” boxes. How well does your mixture match with your prediction? If necessary, adjust the isotope amounts to match your prediction.
    5. Select “Nature’s mix” of isotopes and compare it to your prediction. How well does your prediction compare with the naturally occurring mixture? Explain. If necessary, adjust your amounts to make them match “Nature’s” amounts as closely as possible.
  2. Pick an element from this list of isotope abundances that has three naturally occurring isotopes, and find the average mass of the element given the abundances of its isotopes.

Natural Abundance

  1. Average atomic masses listed by IUPAC are based on a study of experimental results. Bromine has two isotopes 79Br and 81Br, whose masses (78.9183 and 80.9163 amu) and abundances (50.69% and 49.31%) were determined in earlier experiments. Calculate the average atomic mass of bromine based on these experiments.
  2. Variations in average atomic mass may be observed for elements obtained from different sources. Lithium provides an example of this. The isotopic composition of lithium from naturally occurring minerals is 7.5% 6Li and 92.5% 7Li, which have masses of 6.01512 amu and 7.01600 amu, respectively. A commercial source of lithium, recycled from a military source, was 3.75% 6Li (and the rest 7Li). Calculate the average atomic mass values for each of these two sources.
  3. The 18O:16O abundance ratio in some meteorites is greater than that used to calculate the average atomic mass of oxygen on earth. Is the average mass of an oxygen atom in these meteorites greater than, less than, or equal to that of a terrestrial oxygen atom?

Mass Spectrometry

  1. Deduce the empirical formula (element ratio) from the following hard ionization mass spectrum:This hard mass spectrum of an unknown compound has spikes at x=1, x=12, x=79, and x=81. The spike at x=1 has a height of 40%, and at x=12, x=79, and x=81, the heights are all 20%.Given that the empirical formula for the compound is the same as the actual molecular formula, draw a representation of the soft ionization mass spectrum for this compound.
  2. Draw both the hard and soft mass spectrum for phosphorus trifluoride. Both P and F are monotopic, i.e., exist as single isotopes.

Answers to Chemistry End of Section Exercises

  1. (a) 10B and 11B; (b) Boron has an average atomic mass of that is closer to 11 amu than 10 amu, so there should be more 11B than 10B. For example, we can estimate 65% 11B and 35% 10B; (c) check; (d) Average atomic mass of the example estimation is 10.661 amu; (e) the example estimation is off; nature’s mix is 80.1% 11B and 19.9% 10B with average atomic mass of 10.811 amu.
  2. Let us use neon as an example. Since there are three isotopes, there is no way to be sure to accurately predict the abundances to make the total of 20.18 amu average atomic mass. Let us guess that the abundances are 9% Ne-22, 91% Ne-20, and only a trace of Ne-21. The average mass would be 20.18 amu. Checking the nature’s mix of isotopes shows that the abundances are 90.48% Ne-20, 9.25% Ne-22, and 0.27% Ne-21, so our guessed amounts have to be slightly adjusted.
  3. 79.90 amu
  4. From natural source: 6.94 amu; from commercial source: 6.98 amu
  5. The average mass of an oxygen atom in meteroites is greater than the average mass of a terrestrial oxygen atom because there is more O-18 that occurs in a meterorite than does on earth.
  6. CH2Br2. With two isotopes of Br and two Br atoms in each molecule there are four possible molecules: CH279Br79Br, CH279Br81Br, CH281Br79Br, and CH281Br81Br with masses of 172, 174, 174, and 176 amu respectively. The soft mass spectrum will therefore exhibit three peaks in a 1:2:1 ratio as two of the molecules have the same mass, which is twice as likely to occur as the other two possibilities:
    This soft mass spectrum of CH2Br2 has spikes at x=172, x=174, and x=176. The spikes at x=172 and x=176 are the same height and half the height of the spikes at x=174.
  7. For hard MS, 1:3 relative abundance of P:F with peaks at m/Z = 19 (F) and m/Z = 31 (P). For soft MS, peak at m/Z = 88 (PF3) with 100% abundance.


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