Introductory Theory and Terminology
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3.2 Reference Compounds, Hertz, ppm
It has already been stated that NMR signals are analyzed with respect to two characteristics,
intensity  and  frequency.  Absolute  frequencies  are  measured  in  Hertz  (Hz  -  cycles  per
second)  or  Megahertz  (MHz).  Reporting  on  measured  signals  is  simplified  if  all  frequency
measurements  are  made  with  respect  to  a  reference.  For 
1
H  NMR  the  recommended
reference  is  a  chemical  called  tetramethylsilane  (TMS).  When  a 
1
H  or  a 
13
C  spectrum  is
acquired  the  presence  of  TMS  gives  rise  to  a  single,  easily  identifiable  peak.  This  peak  is
referenced to zero and the frequencies of all other peaks are given in terms of their frequency
relative to the TMS frequency.  Thus, we  can  talk of  a signal  being  2.5 kHz  above the  TMS
peak. This is preferable to quoting the absolute frequency of the signal which might look like
500.1325 MHz.
Referencing  signals  to  the  TMS  peak  clearly  cuts  down  the  number  of  digits  needed  to
describe the frequency of a signal. However, this can be even more simplified if the ppm unit
is used instead of  Hertz. The  ppm unit represents frequencies as  a fraction  of the  absolute
resonance frequency which will depend on the strength of the magnet. The advantage of the
ppm unit is that frequency  measurements are independent  of magnet  strength.  This greatly
simplifies the comparison of spectra acquired on different spectrometers.
The  conversion  factors  to  be  used  when  changing  from  Hertz  to  ppm  and  vice  versa  are
shown in the diagram below.
Figure3.5: Converting Hertz and ppm
1 Hertz 3 ppm
2 Divide by the carrier frequency
(SFO1) in MHz
4 Multiply by the carrier frequency
(SFO1) in MHz
The advantages of using the ppm unit are best illustrated with a practical example.
Suppose a 
1
H signal was observed at 2.5 kHz above TMS using a carrier frequency (SF01) of
500 MHz. The frequency of any emitted NMR signal is directly proportional to the strength of
the  magnet.  The  same  signal  would  appear  at  3.0  kHz  above  TMS  on  a  600  MHz
spectrometer and at 2.0 kHz above  TMS  on a 400  MHz machine. A  single  conversion may
not  be  a  great  inconvenience  but  it  must  be  done  for  every  peak  for  each  system.  Now
consider the same signal but quoted in the ppm unit.
Frequency in Hertz divided by SFO1 = Frequency in ppm
Examples:
2500 Hz / 500 MHz = 5 ppm
3000 Hz / 600 MHz = 5 ppm
2000 Hz / 400 MHz = 5 ppm
The 
1
H signal may now be described as being located at 5 ppm above, (i.e. downfield from)
the TMS peak regardless of the spectrometer frequency.