Measuring Diffusion
Pertinent pulse sequences are “vpge1” and “vpge_cnvct”
Suggested literature reference is A.S. Atieri et al., JACS, 117:7566, 1995.
Currently only installed on 6001, because vpge_cnvct requires triple axis gradients
“vpge1” is used in most instances. “vpge_cnvct” should be used for temperatures above 30C.
For “vpge1”, two parameters are adjusted/arrayed to optimize the experiment and collect a series of data points for calculation of the diffusion coefficient. These are:
d3: typical values from 50 to 100ms
gt2: typical values from 1 to 4ms.
“d3” should be set with a larger value for smaller molecules.
The two parameters are optimized so that when “gt2” is arrayed, a series of spectra produces a linear decrease in observed signal approaching a null. An array of 10-12 points is usually sufficient for the calculation. The first and last points are typically discarded.
After collecting the data, two macros are used to process and analyse the data: “bca” and “idif”.
“bca” is a simple macro to adjust the baseline in the entire array of spectra.
“idif” integrates the peaks in the spectra and performs calculations to prepare the data to be graphed for linear regression analysis. “idif” queries the user for a file name for the data to be output in a comma separated table format that can be imported into a program such as MS Excel. The first column represents the experiment specific parameters in the equation: A(2t) = A(0) exp[-(gamma*delta*G)^2 * ( DELTA – delta/3)/Ds], where delta = PFG duration in s, G = gradient strength in Gauss/cm, and DELTA = time between PFG pulses. Further columns are the natural logarithm of A(2t)/A(0) for each peak of the spectra.
N.B. “idif” saves the text file in the experiment directory (i.e. vnmrsys/expX), neither in the user's default directory nor in the current working directory.
For the “vpge_cnvct” experiment, two gradients are employed to cancel out the effects of convection currents. These gradients (gt2 and gt3) MUST be arrayed simultaneously, not consecutively.