Application of electroosmotically-driven solution displacement for on-chip probing and characterization of protein adsorption
Source: Appl. Phys. Lett. 97, 043704 (2010); doi:10.1063/1.3459688
Published 28 July 2010
An alternative strategy for realizing on-chip characterization of protein adsorption is demonstrated using solution displacement with electro-osmotic flow in microchannels. The idea is illustrated by studying adsorption of bovine serum albumin (BSA) on polydimethylsiloxane surfaces. Through tracking the zeta potential change using the current monitoring technique, we quantify how the surface coverage of BSA varies with time and the BSA concentration. The Langmuir kinetic model is employed to capture the transient behavior of the adsorption and to determine both the adsorption and desorption rate constants. The Langmuir isotherm is also established in line to account for the sorption equilibrium.
©2010 American Institute of Physics
| History: | Received 16 April 2010; accepted 3 June 2010; published 28 July 2010 |
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http://link.aip.org/link/?APPLAB/97/043704/1 |
REFERENCES (14)
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The reported formula is - The actual current changes are not strictly linear in time, which is attributed to the O((1−
2/
1)2) terms neglected in Eq. (2). We also use the unsimplified equation to determine the zeta potential. The result merely has a few percent of difference compared to that using Eq. (2) because of this small nonlinear effect. - K. S. Phillips and Q. Cheng,
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Polym. Int. 54, 304 (2005) . - In principle, both
and
can be determined solely by the kinetic study, as they can be obtained by plotting k against C if sufficient data of k are available in a wide range of C. At high C(>10 ppm), however, an accurate kinetic study would hardly be attainable, since the adsorption rate would become so fast that the system would have already reached an equilibrium by the time we measure the zeta potential. In other words, because the surface concentration now changes very rapidly, it is impossible in practice to rinse the channel and to load the solutions in time while still keeping the surface not changed significantly prior to the zeta-potential measurement. At the other extreme, too low C such as 1 ppm will not give enough data showing discernable zeta potential changes (<3 mV) for determining k.
(in mV)=6.75–29.75pC for 6.5<pH<7. With pC
1.48 for the 20 mM buffer, the estimated
is −37.3 mV.
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