DMPC and DHPC phospholipids can be purchased as dry powders or already prepared mixture at different phospholipids molar ratios from Avanti Polar Lipids Inc. and used without further purification. They can be stored in a freezer at -18 deg C.
A small amount of tetradecyltrimethylammonium bromide (TTAB) can be added to the sample to increase bicelle stability (it can be purchased from Sigma).
A 15% w/v (15 g of total lipids in 100 ml) solution of lipids with a DMPC/DHPC ratio of 3:1 (mol:mol), 2.4 mM of TTAB in a phosphate 10 mM, pH = 6.5, and 0.02% NaN3 buffer solution was prepared in the following way:
Warnings
The long term stability of bicelles is limited by the hydrolysis of the
ester bonds connecting the saturated fatty acid chains and the glycerol-phosphatidylcholine
headgroup.
This hydrolysis is catalised both by base and by acid, and is
therefore a strong function of the pH, within a minimum at 6.5-7.0, this
justifies the pH choice. At this latter pH the solution is stable for months
at lower or higher pH the bicelle stability makes the sample last for less
than one day.
There will be a slower decrease in the transition temperature
as the sample ages resulting from a more effective hydrolysis of DHPC relative
to DMPC.
Samples may be stored frozen, refrigerated or at room temperature with
no noticeable effect on the reproducibility of the liquid crystalline phase
once the sample are reheated at 38 deg C.
However frozen sample hydrolyses much more slowly so it is better to store
them at -80 deg C where they can last for months.
Diluite liquid crystalline NMR samples can be obtained by adding buffer
to the 15% stock solution followed by vortexing and a light centrifugation.
The deuterium solvent signal, normally used for field-frequency lock
purposes, provides a very convenient probe for monitoring the liquid crystalline
state. There is a microscopic phase separation as evidenced by the simultaneous
presence of a 2H singlet and a 2H doublet as the
temperature raises.
Above 38 deg C the 2H solvent signal shows
a well defined doublet splitting, with very narrow line widths as a consequence
of the rapid exchange of water molecules between partially aligned hydration
shell of oriented bicelles and the bulk solvent resulting in an incomplete
averaging of the large 2H quadrupole coupling.
Insertion of the sample into the heated probehead into the magnet makes
the 2H doublet appear within few seconds.
The 2H
splitting is, to a good approximation, proportional to the bicelles concentration.
Above a given threshold, there is no significant effect of the magnetic field strength on the degree of alignment and no difference in solvent 2H splitting or protein alignment is detected between measurements at 500 and 600 MHz.
The small degree of alignment which results from the protein's diamagnetic susceptibility, typically is negligible relative to the much larger alignment induced by the liquid crystal.
Besides density effect a small change in the temperature across the sample can effect the splitting width of 2H and this can influence when shimming the sample.
To test the system the deuterium splitting can measured after hours or monitored overnight.
If no meaningful change in both the magnitude and line widths of the splitting are observed no phase separation has occurred and bicelles are stable. The asymmetry in the doublet intensity observed after shimming can be used as a sensitive indicator for monitoring the homogeneity of the liquid crystal phase.
A concentration of bicelles of 3.5 % (w/v) produces a splitting of about 6 Hz in the deuterium line. This should give values for the magnitude of the molecular alignment tensor of about 0.001.
For alignment significantly larger than this value the observed 1H signals will increase considerably in line width as a result of the multitude of residual 1H-1H dipolar interactions. Therefore alignment values of 0.001 are optimal for the purpose of extracting heteronuclear couplings in fully protonated proteins.
Higher degree of alignment can also result in poor INEPT magnetisation transfer for spin pairs where the dipolar contribution is comparable in magnitude to the one-bond J coupling.