1D nOe Experiment
The 1D-nOe experiment measures the
distance-dependent nuclear Overhauser effect from one 1H
proton to other protons within 5Å. The idea is to irradiate one
peak and change the size of the peak(s) coupled through space relative
to a reference spectrum. One resonance in the spectrum is perturbed by
saturation. The net intensities of other resonance may change due to
spins close in space to those directly affected by the perturbation. A
measure of the change in amplitude can be used to determine the
geometry of the molecule.
In a 1H - 1H nOe the percent
change is small (2-10%), using the nOe difference experiment. 1H
- 1H nOe is used to determine the proximity of pairs of
protons. A 2-D NOESY experiment gives a measure of the through-space
coupling for all the protons at once.
Acquiring 1D nOe data
- Acquire a proton spectrum. Set the appropriate window. Type dgain
and record this value.
- Adjust the following parameters:
ss=2
pw = 1H 90° pulse width (listed on shim card)
tpwr = power for pw (listed on shim card)
d1 = 5*T1. If the T1
value is unknown then set d1 to 7.
il='y' This allows experiment interleaving.
dm='yyn'
dpwr=(see step #3 below)
homo='y'
bs=8
gain=(value from step one)
temp='n' su If your experiment is longer than
30 minutes then you should set temp=30 on the VT unit to avoid peak
shifting.
- Normally a dpwr value of 10 is a reasonable value. The
post-run spectrum should show the irradiated peaks to be about 10-20%
of the non-irradiated peaks. You can set dpwr=10 as a test, run a few
scans and then measure the delta of the irradiated peak and the
non-irradiated peaks. You can then adjust the dpwr value so that the
irradiated peak is no larger than 10% of its original height. NOTE:
the greater the dpwr value, the wider the irradiated band becomes and
could produce undesirable results by partially irradiating peaks next
to the main irradiated peak.
- Acquire a standard 1D-proton spectrum and then place the cursor
on the peak to be irradiated, type nl and then sd (this
sets the decoupler offset to the cursor position). This is the "on-resonance
decoupler frequency".
- Place the cursor in a blank region, near the end (downfield), of
the spectrum (at least 1/2 ppm away from any peaks) and type sda.
This adds the cursor value to the decoupler offset array. This
is the "off-resonance decoupler frequency" and is termed the sda-blank
in this document.
- If additional peaks are to be irradiated, you place the cursor on
the next peak, type nl and then sda again. Do this for
all of your peaks of interest. If you have more than 3 or 4 peaks that
you want to irradiate then you may want to set a second sda-blank
in your experiment to allow you to check the system stability. You could
set this at any blank space on your spectrum. Typing da will
display a list of the peaks and off-resonance frequencies you have
selected.
- nt should be set from 10 to 100 times the number
of transients normally collected for a 1H spectrum of this
sample. nt should be a multiple of 32. Quantitative nOe
measurements require excellent signal/noise while a qualitative nOe is
a little more lenient.
- You can type time to see how long your experiment will
take. This will help you in scheduling your time for the spectrometer.
- Type ai ga to set the absolute intensity mode and start
your acquisition. If you receive an ADC overflow error message, you
will want to reduce your gain setting and start the experiment again.
- At the end of your run be sure to save your data with the file
- save FID selection. All spectra can be saved in 1 file under 1 name
Processing nOe data
- Log on to a Sun data-station.
- Recall your nOe data like any other fid into any experimental
area except exp5.
- Set your lb (line broading) parameter between 1.0 and 5.0,
type ai and then wft. This increases the
signal-to-noise ratio of the spectrum (at the expense of resolution)
which is important for accuracy.
- Type ds(#) f full and aph to start
processing your first spectrum (NOTE: # is the peak you
irradiated).
- Type bc. This performs a baseline correction to your
spectrum.
- You reference your solvent peak next.
- Type ds(2) f full to process the second
spectrum (DO NOT phase. The phasing values from step #4 are used) NOTE: 2
is the sda-blank region you irradiated. You may have made the sda-blank
your third, fourth, or fifth irradiated region in which case you would
use ds(3), ds(4), or ds(5).
- Type bc. This is the same as step #5.
- NOTE: (see #1 in the last section below.) Type clradd ds(#)
spadd ds(2) addi. This will clear experimental 5 area,
add ds(#) to that area, and then place ds(2) there and subtract ds(2)
from ds(#) and show the results. Always use the sda-blank in the
second half of the above command statement.
- Select sub from the interactive menu.
- Click on the select button twice (the visible yellow
spectrum is active now). Increase the scale of the yellow spectrum with
the middle mouse button. DO NOT touch the green or blue
spectrum.
- Select the Save button to save your worked-up data at this
point.
- Join exp5 (jexp5) to view and analyze this different
spectrum. NOTE: If you receive an error message to the effect
that experimental 5 area can't load the processed data then load the
FID and WFT the data. Next join another experimental area and start at
step #2 again.
Printing nOe data
You will type the following commands to print your
nOe spectrum.
- text('name') This will place a name on your
printout.
- ds(#) vsadj vs=vs/2 vp=12 pl pltext pscale NOTE:
# is the irradiated peak of interest, also, record the
vsadj value.
- ds(2) vp=60 pl NOTE: ds(2) is the irradiated blank
area (sda-blank) in this write-up. Do not change vertical scale here
- NOTE: If you want to plot out more than two spectrums on one
page, please refer to "How do I print Several Different Spectra
onto one page?" in the online IUNMR Users Guide.
- jexp5 ds vp=120 Adjust your vertical scale to the value
obtained above (step #2).
- pl page This sends your plot to the printer.
nOe Quantitative Process
A simplified way to quantitate your nOe data is as
follows:
- Follow the instructions above (the Processing nOe data section) up
to but not including step number 9.
- Print out a spectrum so you can write and place remarks on it.
- Zoom in on your area of interest on the spectra.
- Type vsadj to set the vertical adjustment of your
displayed spectra. You should write this value down. This is the
only time you will issue this command. All other views of
this or other spectra needs to have this vertical scale value in order
for you to obtain meaningful data.
- Place the cursor on a peak and type nl. You will
be given a value for the height of the peak. Write this value on your
printout by the peak. Also annotate whether this value is from an
irradiated peak or non-irradiated peak. You repeat this step for all
peaks of interest.
- Type ds(x) where x is
the next irradiated peak or sda-blank (irradiated blank region). You
repeat step number 5 for this spectrum and write down all values on
your printout (You may want to print out a fresh spectrum to write
your next set of values on). REMEMBER: DO NOT typevsadj
at anytime other than the first time you typed it in step number 4. This
would cause you to change the vertical scale in the middle of your data
gathering and would makes the data worthless. Repeat step 6 until all
irradiated peaks and the irradiated blank area (sda-blank) have been
measured and recorded. You should be able to produce a nice table with
these values. (See Table 1.)
- With this set of data you can now do the following calculations:
- To estimate the amount of saturation by the irradiation on your
peaks of interest: Starting with your irradiated peak, divide the
height value of the irradiated peak by the height value of the same
peak in the sda-blank spectrum. You will obtain a numerical value of Y.
Subtract Y from 1 to obtain a value Z where Z is the
saturation efficiency value. i.e. (1-Y = Z).
- For all other peaks, you subtract the value of a non-irradiated
peak measured in the sda-blank spectrum from the value of this same
peak measured in the irradiated peak column. You then divide that
answer with the non-irradiated peak value measured in the sda-blank
again. With this semi-final value you divide with the Z value
from the above step. Multiply by 100 and you now have the percentage
enhancement value for the peak.
- A descent nOe will have a value of around 5%, very strong will
be 10%, and a weak one is less than 2%. A positive value or a negative
value can be obtained.
This is an example table you create to help in
correlating your peak interactions. These calculations can be
done with an online calculator found on our server at:
http://nmr3.chem.indiana.edu/noecalc.php.
|
Irradiated peaks are in this row
>>>>
Non-irradiated peaks are in this
column
|
Peak-1
Irradiation on Peak-1
|
Peak-2
Irradiation on Peak-2
|
Peak-3
Irradiation on Peak-3
|
Peak-4
Irradiation on Peak-4
|
Sda-blank
Irradiation in Blank Area
|
|
Peak-1
|
34
|
349
|
336
|
322
|
320
|
|
Peak-2
|
282
|
40
|
260
|
266
|
260
|
|
Peak-3
|
304
|
292
|
21
|
287
|
290
|
|
Peak-4
|
274
|
282
|
273
|
36
|
275
|
|
Sda-blank
|
0
|
0
|
0
|
0
|
0
|
The following is an example of a calculation for the
nOe on Peak #2 when Peak #1 is irradiated.
nOe = 
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Last updated: Oct 11, 1999
URL: http://nmr.chem.indiana.edu/NMRguide/1dexpt/1dnoe.html
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Trustees of Indiana University