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One micron magnetic beads optimised for automated immunoassays

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I mmunodiagnostics<br />

As Published in CLI April 2005<br />

Figure 2. Hysteresis curve <strong>for</strong> the bead plat<strong>for</strong>m: magnetisation as a function<br />

of <strong>magnetic</strong> field strength. The magnetisation curves are overlapping<br />

both when increasing and decreasing the <strong>magnetic</strong> field, and the <strong>beads</strong><br />

show superpara<strong>magnetic</strong> behaviour.<br />

Figure 3. Sedimentation of 1.0 µm and 2.8 µm <strong>beads</strong> in aqueous solution<br />

measured as relative absorbance at 450 nm as a function of settling<br />

time (minutes).<br />

urement is dependent on bead diameter since the volume of the<br />

bead is proportional to the cube of the radius.<br />

Magnetic properties<br />

The <strong>magnetic</strong> properties of <strong>beads</strong> used as the solid phase in<br />

<strong>automated</strong> systems are clearly of great importance, both during<br />

the manufacture of the immunoassay and in its application. To<br />

ensure that the <strong>beads</strong> are collected efficiently on the magnet the<br />

iron oxide content must be high. However, total resuspension of<br />

the pellet during washing steps is equally important as rapid,<br />

effective washing steps reduce assay time and there<strong>for</strong>e increase<br />

overall throughput. To satisfy these requirements the <strong>beads</strong><br />

must be truly superpara<strong>magnetic</strong> and there should be no remanence<br />

after removing the <strong>magnetic</strong> field.<br />

The iron oxide content of Dyna<strong>beads</strong> My<strong>One</strong> <strong>beads</strong> is 37%. The<br />

<strong>magnetic</strong> material is evenly distributed throughout the <strong>beads</strong> as<br />

nanosized iron oxide crystals. This results in superpara<strong>magnetic</strong><br />

behaviour, as shown by the hysteresis curve in Figure 2, where<br />

the magnetisation is nearly identical with both increasing and<br />

decreasing <strong>magnetic</strong> fields. The <strong>beads</strong> show no remanence<br />

when the <strong>magnetic</strong> field is zero.<br />

Surface characteristics<br />

Hydrophobicity and the charge on the bead surface are important<br />

parameters when coating <strong>beads</strong> with antibodies or similar<br />

proteins generally needed in <strong>immunoassays</strong>. The initial driving<br />

Table 1. Relative contact angle and isoelectric point measured with Zeta potential.<br />

<strong>for</strong>ce when immobilising antibodies on hydrophobic <strong>beads</strong>,<br />

such as the tosylactivated <strong>beads</strong>, is hydrophobic adsorption to<br />

the bead surface. The chemical covalent bonds between the<br />

tosylactivated groups on the bead surface and the protein are<br />

only created after this initial contact. For hydrophilic bead surfaces<br />

the initial contact between the antibody and the surface<br />

of the bead is electrostatic or via random interactions, or it<br />

may occur following activation of functional groups on the<br />

bead surface.<br />

The degree of hydrophobicity of the tosylactivated <strong>beads</strong> as well<br />

as the carboxylic acid version of the <strong>beads</strong> was determined by<br />

measuring the contact angle of water droplets deposited on a<br />

layer of dry <strong>beads</strong> using a Fibro Dat 1120 instrument (Thwing-<br />

Albert Instrument Company, USA). The higher the contact<br />

angle observed, the more hydrophobic the bead surface.<br />

The isoelectric point <strong>for</strong> each of the bead types was also determined<br />

using the Zetasizer 2000-3000 HS (Malvern<br />

Instruments, UK) to measure the Zeta potential. These measurements<br />

were per<strong>for</strong>med on uncoated <strong>beads</strong> as well as on<br />

<strong>beads</strong> coated with antibody or streptavidin, to assess whether<br />

the surface properties of the <strong>beads</strong> are affected by the immobilised<br />

protein. The results are shown in Table 1.<br />

The hydrophobicity of the tosylactivated <strong>beads</strong> is very comparable,<br />

whereas the carboxylic acid <strong>beads</strong> are, in contrast, very<br />

hydrophilic due to their high negative<br />

net charge at neutral pH. Zeta potential<br />

measurements were per<strong>for</strong>med on three<br />

different types of <strong>beads</strong> (two sizes of<br />

tosylactivated <strong>beads</strong> and carboxylic acid<br />

<strong>beads</strong>) after coating with monoclonal<br />

mouse IgG1 antibody and streptavidin<br />

[Table 1]. These results show that the<br />

isoelectric point of the <strong>beads</strong> is principally<br />

determined by the nature of the<br />

immobilised protein. For example, after<br />

coating the originally negatively charged<br />

carboxylic acid <strong>beads</strong> with antibody,<br />

their isoelectric point is similar to the<br />

more neutral tosylactivated <strong>beads</strong> coated<br />

with the same antibody.

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