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  <resource>
  <id>6561</id>
  <path>/www/nrich/html/content/id/6561/</path>
  <resourceTypeID>1</resourceTypeID>
  <last_published>2011-02-01T00:00:01</last_published>
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&lt;br&gt;&lt;/br&gt;
&lt;ul id=&quot;stemLinks&quot;&gt;
&lt;li&gt;&lt;a href=&quot;http://nrich.maths.org/920&quot;&gt;Warm-up&lt;/a&gt;&lt;/li&gt;
&lt;li&gt;&lt;a href=&quot;http://nrich.maths.org/6562&quot;&gt;Try this next&lt;/a&gt;&lt;/li&gt;
&lt;li&gt;&lt;a href=&quot;http://nrich.maths.org/6581&quot;&gt;Think higher&lt;/a&gt;&lt;/li&gt;
&lt;li&gt;&lt;a href=&quot;http://nrich.maths.org/5904&quot;&gt;Read: mathematics&lt;/a&gt;&lt;/li&gt;
&lt;li&gt;&lt;a href=&quot;http://en.wikipedia.org/wiki/Hydrocarbon&quot;&gt;Read: science&lt;/a&gt;&lt;/li&gt;
&lt;li&gt;&lt;a href=&quot;http://en.wikipedia.org/wiki/Isotope&quot;&gt;Explore further&lt;/a&gt;&lt;/li&gt;
&lt;/ul&gt;
&lt;div&gt; &lt;/div&gt;
&lt;br&gt;&lt;/br&gt;
&lt;p&gt;&lt;span style=&quot;font-style: italic;&quot;&gt;This problem consists of a series of questions concerning hydrocarbons made from the stable isotopes of hydrogen and carbon. Assume that the probability of the occurrence of unstable isotopes is effectively zero. Assume also that the mass of an isotope is equal to the mass number.&lt;/span&gt;&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
Carbon is found in two naturally occurring stable isotopic forms: Carbon-12, $^{12}$ C, accounts for $98.9\%$ of naturally occurring carbon, and Carbon-13, $^{13}$ C, accounts for $1.1\%$ of naturally occurring carbon.&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
Hydrogen also has two stable isotopes: $^1$H accounts for slightly more than $99.985\%$ of naturally occurring hydrogen. $^2$H, called deuterium, accounts for about $0.015\%$ of naturally occurring hydrogen.&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
What possibilities are there for the molecular mass of a stable molecule of methane CH$_4$? Which three are the most common? What is the probability that a randomly encountered methane molecule will be of each of these masses?&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
What would be the three most likely possibilities for the molecular masses of the next two alkanes: ethane, C$_2$H$_6$, and propane C$_3$H$_8$?&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
Am I likely to find a molecule of butane C$_4$H$_{10}$ of molecular mass $72$ in a litre of butane? (Avogadro&amp;#39;s constant is approximately $6.02\times 10^{23}$).&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
Are there any alkanes for which the most commonly found molecule is not the one made entirely from $^{12}$C and $^1$H?&lt;/p&gt;
&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
&lt;div class=&quot;framework&quot;&gt;&lt;br&gt;&lt;/br&gt;
NOTES AND BACKGROUND&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
Mass spectrometry allows chemists to determine the molecular masses of compounds. The frequency of occurrence of common isotopes of elements is an important factor in understanding such as analysis. Mass spectrometry is of great industrial and scientific importance, and in practice, the results of an analysis are determined by comparison with a database of experimental spectrometry
information.&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
For information on alkanes and hydrocarbons, see &lt;a href=&quot;http://en.wikipedia.org/wiki/Hydrocarbon&quot;&gt;http://en.wikipedia.org/wiki/Hydrocarbon&lt;/a&gt;&lt;/div&gt;
&lt;br&gt;&lt;/br&gt;

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Note that in actuality the masses of the different isotopologues of
$\text{CH}_4$ are slightly different. These differences may be
noted by a very sensitive mass spectrometer. Take for
example:&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
RMM $^{12}\text{CH}_3\text{D}$ = 12 + 3(1.007825) + 2.014102 =
17.037577 gmol$^{-1}$&lt;br&gt;&lt;/br&gt;
RMM $^{13}\text{CH}_4$ = 13.00335 + 4(1.007825) = 17.03465
gmol$^{-1}$&lt;br&gt;&lt;/br&gt;
where the calculation is limited by the degree of accuracy of the
given data.&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
However in this question it is acceptable to take values to the
nearest gmol$^{-1}$, giving roughly equal molecular masses for
certain isotopes.&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$^{12}\text{CH}_4$ = 16 gmol$^{-1}$&lt;br&gt;&lt;/br&gt;
$^{12}\text{CH}_3\text{D}$, $^{13}\text{CH}_4$ = 17
gmol$^{-1}$&lt;br&gt;&lt;/br&gt;
$^{12}\text{CH}_2\text{D}_2$, $^{13}\text{CH}_3\text{D}$ = 18
gmol$^{-1}$&lt;br&gt;&lt;/br&gt;
$^{12}\text{CHD}_3$, $^{13}\text{CH}_2\text{D}_2$ = 19
gmol$^{-1}$&lt;br&gt;&lt;/br&gt;
$^{12}\text{CD}_4$, $^{13}\text{CHD}_3$ = 20 gmol$^{-1}$&lt;br&gt;&lt;/br&gt;
$^{13}\text{CD}_4$ = 21 gmol$^{-1}$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
The three most common species encountered would be
$^{12}\text{CH}_4$, $^{13}\text{CH}_4$ and
$^{12}\text{CH}_3\text{D}$ in order of likelihood. This can bee
seen intuitively as the probability of encountering a
$^{13}\text{C}$ more likely than encountering a single
$^{2}\text{H}$, and for a small molecule such as methane, it is far
more likely to obtain $^{12}\text{CH}_4$ than either of the other
possibilities. The three most likely molecular masses as 16, 17 and
18 gmol$^{-1}$ as the introduction of more $^{13}\text{C}$ and
$^{2}\text{H}$ to a small molecule reduces its likelihood more than
any combinatorial effects can compensate for.&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
The actual probabilities of encountering each of these molecular
masses of methane are:&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
&lt;span style=&quot;font-weight: bold;&quot;&gt;16 gmol$^{-1}$
[$^{12}\text{CH}_4$]&lt;/span&gt;&lt;br&gt;&lt;/br&gt;
$\textbf P(16 \text{gmol}^{-1}) = 0.989 \times (0.99985)^4 = 0.988$
(3sf)&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
&lt;span style=&quot;font-weight: bold;&quot;&gt;17 gmol$^{-1}$
[$^{12}\text{CH}_3\text{D}$, $^{13}\text{CH}_4$]&lt;/span&gt;&lt;br&gt;&lt;/br&gt;
 $\textbf P(17 \text{gmol}^{-1}) =
(0.989\times^4\textbf{C}_1(0.00015)\times (0.99985)^3&lt;br&gt;&lt;/br&gt;
) + (0.011 \times (0.99985)^4) = 0.0116$ (3sf)&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
&lt;span style=&quot;font-weight: bold;&quot;&gt;18 gmol$^{-1}$
[$^{12}\text{CH}_2\text{D}_2$,
$^{13}\text{CH}_3\text{D}$]&lt;/span&gt;&lt;br&gt;&lt;/br&gt;
$\textbf P(18 \text{gmol}^{-1}) =
(0.989\times^4\textbf{C}_2(0.00015)^2\times (0.99985)^2 ) +
(0.011\times^4\textbf{C}_1(0.00015)\times (0.99985)^3) =
6.73\times10^{-6}$ (3sf)&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
&lt;span style=&quot;font-weight: bold;&quot;&gt;19 gmol$^{-1}$
[$^{12}\text{CHD}_3$, $^{13}\text{CH}_2\text{D}_2$]&lt;/span&gt;&lt;br&gt;&lt;/br&gt;
$\textbf P(19 \text{gmol}^{-1}) =
(0.989\times^4\textbf{C}_3(0.00015)^3\times 0.99985 ) +
(0.011\times^4\textbf{C}_2(0.00015)^2\times (0.99985)^2) =
1.50\times10^{-9}$ (3sf)&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
&lt;span style=&quot;font-weight: bold;&quot;&gt;20 gmol$^{-1}$
[$^{12}\text{CD}_4$, $^{13}\text{CHD}_3$]&lt;/span&gt;&lt;br&gt;&lt;/br&gt;
$\textbf P(20 \text{gmol}^{-1}) =
(0.989\times^4\textbf{C}_4(0.00015)^4) +
(0.011\times^4\textbf{C}_3(0.00015)^3\times 0.99985) =
1.49\times10^{-13}$ (3sf)&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
&lt;span style=&quot;font-weight: bold;&quot;&gt;21 gmol$^{-1}$
[$^{13}\text{CD}_4$]&lt;/span&gt;&lt;br&gt;&lt;/br&gt;
$\textbf P(21 \text{gmol}^{-1}) =
(0.011\times^4\textbf{C}_4(0.00015)^4) = 5.57\times10^{-18}$
(3sf)&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
Following a similar principle to that above, the three most likely
possibilities for the molecular masses of ethane are 30, 31 and 32
gmol$^{-1}$ in order of likelihood.&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$^{12}\text{C}_2\text{H}_6$ = 30 gmol$^{-1}$&lt;br&gt;&lt;/br&gt;
$^{12}\text{CD}_2\text{H}_5$,
$^{12}\text{C}^{13}\text{C}\text{H}_6$ = 31 gmol$^{-1}$&lt;br&gt;&lt;/br&gt;
$^{12}\text{C}_2\text{H}_4\text{D}_2$,
$^{12}\text{C}^{13}\text{CD}\text{H}_5$,
$^{13}\text{C}_2\text{H}_6$ = 32 gmol$^{-1}$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$\textbf P(30 \text{gmol}^{-1}) = (0.989)^2 \times (0.99985)^6 =
0.977$ (3sf)&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$\textbf P(31 \text{gmol}^{-1}) = ((0.989)^2 \times
^6\textbf{C}_10.00015 \times (0.99985)^ 5) +
((0.989)\times^2\textbf{C}_1(0.011)\times(0.99985)^ 6) = 0.0226$
(3sf)&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$\textbf P(32 \text{gmol}^{-1}) = ((0.989)^2 \times
^6\textbf{C}_2(0.00015)^2 \times (0.99985)^ 4) +
((0.989)\times^2\textbf{C}_1(0.011)\times^6\textbf{C}_1(0.00015)\times(0.99985)^
5)$&lt;br&gt;&lt;/br&gt;
$+ (^2\textbf{C}_2(0.011)^2 \times (0.99985)^6) = 1.41 \times
10^{-4} \text{ (3sf)}$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
The three most likely possibilities for the molecular mass of
propane are 44, 45 and 46 gmol$^{-1}$ in order of likelihood.&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$^{12}\text{C}_3\text{H}_8$ = 44 gmol$^{-1}$&lt;br&gt;&lt;/br&gt;
$^{12}\text{C}_2{}^{13}\text{C}\text{H}_8$,
$^{12}\text{C}_3\text{D}\text{H}_7 = 45\text {gmol}^{-1}$&lt;br&gt;&lt;/br&gt;
$^{12}\text{C}^{13}\text{C}_2\text{H}_8$,
$^{12}\text{C}_2^{13}\text{C}\text{D}\text{H}_7,
^{12}\text{C}_3\text{D}_2\text{H}_ 6 = 46\text {gmol}^{-1}$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$\textbf P(44 \text{gmol}^{-1}) = (0.989)^3 \times (0.99985)^8 =
0.966$ (3sf)&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$\textbf P(45 \text{gmol}^{-1}) = (^3\textbf{C}_1 \times 0.011
\times (0.989)^2 \times (0.99985)^ 8) +
((0.989)^3\times^8\textbf{C}_1(0.00015)\times(0.99985)^ 7) =
0.0334$ (3sf)&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$\textbf P(46 \text{gmol}^{-1}) = (^3\textbf{C}_2 \times (0.011)^2
\times 0.989 \times (0.99985)^ 8) + (^3\textbf{C}_1 \times 0.011
\times (0.989)^2 \times^8\textbf{C}_1(0.00015)\times(0.99985)^
7)$&lt;br&gt;&lt;/br&gt;
 $+ ((0.989)^3\times^8\textbf{C}_2(0.00015)^2\times(0.99985)^ 6) =
3.98 \times 10^{-4}$ (3sf)&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
A molecule of butane with molecular mass 72 is the isotopologue
$^{13}\text{C}_4\text{D}_{10}$. The probability of any butane
molecule being this isotopologue is:&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$\textbf{P}(^{13}\text{C}_4\text{D}_{10}) = 0.011^4 \times
0.00015^{10} = 8.44 \times 10^{-47}$ (3sf)&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
24dm$^3$ of butane corresponds to roughly 1 mole of butane
molecules. Thus, as 1 dm$^3$ is equivalent to a litre, the number
of moles in the required volume is $\frac{1}{24}$.&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
The number of molecules in the sample is given by multiplying the
number of moles, by the number of molecules in a mole (the &lt;span style=&quot;font-weight: bold;&quot;&gt;Avogadro's constant&lt;/span&gt;):&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
Number of molecules $= \frac{N_A}{24} = 2.51 \times 10^{22}$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
So the likelihood can be found by multiplying the probability for
one molecule by the total number of molecules in the sample.&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$\therefore\text{E}(^{13}\text{C}_4\text{D}_{10}) = 2.51 \times
10^{22} \times 8.44 \times 10^{-47} = 2.12 \times 10^{-24}$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
This question requires a little more algebraic appreciation of the
calculations thusfar.&lt;br&gt;&lt;/br&gt;
The probability of encountering a generic alkane
$^{12}\text{C}_n{}^1\text{H}_{2n + 2}$ is given by:&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$\textbf{P} = 0.989^n \times (0.99985)^{2n + 2}$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
The probability of encountering an isotopologue containing
deuterium $^{12}\text{C}_n^{\ 1}\text{H}_{2n + 1}\text{D}$ is given
by:&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$\textbf{P} = 0.989^n \times ^{2n + 2}\textbf{C}_1(0.99985)^{2n +
1}\times 0.00015$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
The probability of encountering this isotopologue must be greater
than the likelihood of finding the butane molecule consisting
entirely of $^{12}\text{C}$ and H.&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$0.989^n \times ^{2n + 2}\textbf{C}_1 \times (0.99985)^{2n +
1}\times 0.00015$ &amp;gt; $0.989^n \times (0.99985)^{2n + 2}$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$0.00015 (2n + 2)$ &amp;gt; 0.99985&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
2n + 2 &amp;gt; 6665.666667&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
n &amp;gt; 3331.833333&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
n = 3332&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
&lt;span style=&quot;font-style: italic;&quot;&gt;Is this long chain alkane likely
to exist in a real sample?&lt;/span&gt;&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
The probability of encountering an isotopologue containing
$^{13}\text{C}$ is given by:&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$\textbf{P} = ^n\textbf{C}_1\times 0.011 \times 0.989^{n-1} \times
(0.99985)^{2n + 2}$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
This probability must be greater than the likelihood of finding the
alkane molecule consisting entirely of $^{12}\text{C}$ and H.
So:&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$^n\textbf{C}_1\times 0.011 \times (0.989)^{n-1} \times
(0.99985)^{2n + 2}$ &amp;gt; $0.989^n \times (0.99985)^{2n + 2}$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$ \text{n} \times (0.989)^{n-1} \times 0.011$ &amp;gt; 
$(0.989)^{n}$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$0.011\text{n}$ &amp;gt; 0.989&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$\text{n}$ &amp;gt; 89.90909091&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
n = 90&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
&lt;span style=&quot;font-style: italic;&quot;&gt;Consider the likelihood of the
existence of this molecule&lt;/span&gt;.&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
&lt;span style=&quot;font-style: italic;&quot;&gt;As an extension, does the
probability of the existence of such molecules change if the
molecule is produced via a method which involves polymerisation?
Try to construct an algebraic test.&lt;/span&gt;&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
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&lt;br&gt;&lt;/br&gt;
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&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
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&lt;mdoxml version=&quot;1.0&quot;&gt;&lt;a href=&quot;http://nrich.maths.org/6561&quot;&gt;This activity&lt;/a&gt; makes a good homework or individual task.&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
It uses GCSE probability and A-level chemistry ideas, and gives a good exercise in combinatorics in an interesting context.&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;&lt;/mdoxml&gt;</noteXML>
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&lt;mdoxml version=&quot;1.0&quot;&gt;&lt;br&gt;&lt;/br&gt;
Remember that molecules with more than one hydrogen and carbon atom
can have isotopes at different places. For example, in ethane, a
carbon-13 could occur at either of the carbon sites!&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;&lt;/mdoxml&gt;</clueXML>
  <canonXML>&lt;?xml version=&quot;1.0&quot; encoding=&quot;UTF-8&quot;?&gt;
&lt;mdoxml version=&quot;1.0&quot;&gt;Carbon the ratios are almost exactly 90:1&lt;br&gt;&lt;/br&gt;
 &lt;br&gt;&lt;/br&gt;
Hydrogen, the ratios are almost 5500:1&lt;br&gt;&lt;/br&gt;
 &lt;br&gt;&lt;/br&gt;
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  <end_user_role>2</end_user_role>
  <difficulty>3</difficulty>
  <keystage1>0</keystage1>
  <keystage2>0</keystage2>
  <keystage3>0</keystage3>
  <keystage4>1</keystage4>
  <keystage4plus>0</keystage4plus>
  <title>Heavy hydrocarbons</title>
  <description>Explore the distribution of molecular masses for various hydrocarbons</description>
  <spec_group>Probability
    <specifier>Combining probabilities</specifier>
  </spec_group>
  <spec_group>Applications
    <specifier>chemistry</specifier>
  </spec_group>
  <spec_group>Probability
    <specifier>Probability</specifier>
  </spec_group>
  <spec_group>Applications
    <specifier>chemistry</specifier>
  </spec_group>
  <spec_group>Admin
    <specifier>Individual</specifier>
  </spec_group>
  <spec_group>Applications
    <specifier>STEM - physical world</specifier>
  </spec_group>
</resource>