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The crystals were prepared by a batch method similar to that of Baker et al, 1988 [1], modified as follows: 0.01g of insulin as a fine powder was placed in a clean test tube; 0.02M HCl was added to dissolve the protein; on addition of 0.15 mL of 0.15 M zinc acetate the solution became cloudy due to precipitation of the protein; 0.3 mL of acetone and then 0.5 mL of trisodium citrate together with 0.8 mL of water were added and the solution went clear; the pH was checked and increased with NaOH to a pH between 8 and 9 for different batches, thus ensuring complete dissolution. It was then adjusted to the required value of pH 6.3. If any slight turbidity occurred, it was removed by warming the solution. The solution was then filtered using a Millipore membrane/acetate cellulose acetate filter. This removes any nuclei which will encourage precipitation or formation of masses of small crystals.
The solution was then warmed to 50 deg C by surrounding the test tube with preheated water in a Dewar. This allowed the solution to cool slowly to room temperature. The test tube was lightly sealed with cling film; crystals formed within a few days and were of suitable size for X-ray diffraction within two weeks; the test tube containing crystals was kept at 4 degC prior to data collection. The crystal used for data collection was about 0.2 mm3.
Crystal Properties
Matthews coefficient
Solvent content
1.89
35
Crystal Data
Unit Cell
Length ( Å )
Angle ( ˚ )
a = 81.82
α = 90
b = 81.82
β = 90
c = 33.85
γ = 120
Symmetry
Space Group
H 3
Diffraction
Diffraction Experiment
ID #
Crystal ID
Scattering Type
Data Collection Temperature
Detector
Detector Type
Details
Collection Date
Monochromator
Protocol
1
1
x-ray
100
PIXEL
DECTRIS PILATUS 6M
Data were collected at 16000keV (0.77 Angstrom) and 100 deg K with the Pilatus 6M detector as close to the sample as possible (179.5mm). The EDNA strategy was used to obtain a start angle and 180 deg of data were collected with 0.1 deg oscillation and 0.1s exposure. The resolution of useful diffraction data achieved and used for structure analysis was 0.92 Angstrom.