Electrostatic Aggregation of â-Lactoglobulin Using Quasi-Electric Light Scattering by Malvern

Topics Covered

Background
Experimental
     Sample Preparation
     Determination of Particle Size
Results

Background

In 1934, Palmer first described the separation of ß-Lactoglobulin (ß-Lg) from the whey fraction of bovine milk. This discovery was made fifty years before the actual structure could be elucidated through X-ray crystallography.. The majority of these studies centre around heat induced aggregation since this is of great interest and importance to the processing of dairy products. Despite the years of research, the specific function of ß-Lactoglobulin is yet to be completely understood. The purpose of this work is to provide a study of ß-Lg electrostatic aggregation at low ionic strength (I) and at pH values below the isoelectric point (pI) where aggregation occurs at a rate slow enough to be evaluated by quasi-elastic light scattering (QELS).

Experimental

Sample Preparation

ß-Lg A&B, purchased from Sigma- Aldrich and used without further purification, was dissolved in 4.5mM NaCl prepared from Milli-Q water. The dissolved ß-Lg was then raised to pH 9 in order to disassociate the protein into its monomeric species. An equal volume of 4.5mM NaCl was prepared containing the appropriate amount of 0.1M HCl to bring the combined solutions to the target pH and concentration of 4.2 and 1mg/mL respectively. Both solutions were filtered (0.2 µm filters, Sartorius AG, Germany), and then mixed immediately prior to analysis.

Determination of Particle Size

Size distributions of the ß-Lg aggregates were determined using the Malvern Zetasizer Nano ZS. Correlation times were seven seconds per run and three runs per measurement. QELS was used to determine size distributions over fifty minutes.

Results

Figure 1 shows the intensity size distribution collected during the kinetic experiment at time (t) = 0. As evident here, the QELS results indicate that, ß-Lg aggregates in two distinct size populations almost immediately.

Figure 1. Intensity size distribution for 1mg/mL ß-Lg in 4.5mM NaCl at pH 4.2 at time = 0.

The smaller size population has a hydrodynamic diameter of circa 5.4nm. Using a known mass vs. size relationship for globular proteins, shown in Equation 1, the molecular weight of the 5.4nm protein is approximately 35 kDa, consistent with the dimeric form of the ß-Lg protein.

The kinetic trace for the experiment is shown in Figure 2, which shows the intensity and Z-Average diameter as a function of experimental time.

Figure 2. Kinetic trace of 1.0mg/mL ß-Lg in 4.5mM NaCl at pH 4.2.

The scattering intensity is roughly proportional to the concentration and the square of the molecular weight, and is hence quite sensitive to the formation of higher order aggregates. The Z-Average diameter is the mean diameter of the ensemble of particles, and is derived from the slope of the linearized form of the correlation function (Cumulants method). As seen in Figure 2, the formation of the higher order aggregate occurs in the first 20-25 minutes of the experiment. At longer times, the scattering intensity is relatively constant, suggesting that dimer-aggregate equilibrium has been achieved. Stabilization of the higher order aggregate at longer times is also evident in Figure 3, which shows selected intensity size distributions from the kinetic experiment.

Figure 3. Selected intensity size distributions from the ß-Lg kinetic experiment.

A decrease in the relative amount of dimer was also observed over the time course of the experiment. At the initial conditions, shown in Figure 1, the dimer concentration accounted for 80% of the scattering intensity. At the conclusion of the experimental run, the contribution to scattering intensity by the dimer had stabilized at roughly 10% of the total (see Figure 4). As seen in Figure 4, an increase in scattering intensity and size stabilization of the super aggregate could also be seen over time. The scattering intensity of the aggregate increased from 20% to 90% during the run, with the size of the aggregate ultimately stabilized at approximately 425nm.

Figure 4. Time dependent intensity size distributions for ß-Lg in 4.5mM NaCl at pH 4.2.

Note: A complete list of references is available by referring to the original document.

Source: "Aggregation of β-Lactoglobulin", Application Note by Malvern Instruments.

For more information on this source please visit Malvern Instruments Ltd (UK) or Malvern Instruments (USA).

Date Added: May 9, 2005 | Updated: Jun 11, 2013
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