2006
DOI: 10.1016/j.bpc.2006.03.012
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Topological and dynamical properties of Azurin anchored to a gold substrate as investigated by molecular dynamics simulation

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Cited by 21 publications
(31 citation statements)
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“…Accordingly, the outlined preservation of the shape of the emission spectrum upon AuNP addition in our experiments is an indication that Az molecules participating to the signal (and, thus, also the molecules bound to AuNP surface) remain presumably in their native configuration. This is in agreement with both experimental results [15,41] and molecular dynamics simulation of an Az molecule near a gold surface showing that the protein undergoes only small configurational changes even when it is covalently bound to the surface [42]. is obviously due to the sum of signal of quenched and not quenched sources.…”
supporting
confidence: 91%
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“…Accordingly, the outlined preservation of the shape of the emission spectrum upon AuNP addition in our experiments is an indication that Az molecules participating to the signal (and, thus, also the molecules bound to AuNP surface) remain presumably in their native configuration. This is in agreement with both experimental results [15,41] and molecular dynamics simulation of an Az molecule near a gold surface showing that the protein undergoes only small configurational changes even when it is covalently bound to the surface [42]. is obviously due to the sum of signal of quenched and not quenched sources.…”
supporting
confidence: 91%
“…Moreover, the hypothesis of aggregation caused by Az addition has link gold surfaces, as also theoretically described by means of molecular dynamics simulations [15,[40][41][42]. Whatever the link is, if a monolayer is formed, an estimate of the theoretical number of Az proteins (N Az ) that each spherical particle can accomodate on its surface may be derived from steric considerations using the following expression [43]:…”
mentioning
confidence: 99%
“…Along with well-known applications of metal surfaces, such as biosensors and implants (Liu et al 2004), metal surfaces are also used in bioelectronics as electrodes as they allow controlled exchange of electrons with metalloproteins immobilized on them (Alessandrini et al 2005;Andolfi et al 2004). The interactions of proteins with bare metal surfaces have been the subject of many computational studies, which cover a wide range of different elemental and alloy surfaces, such as Cu(100) (Chen & Wang, 2010), Au(111) (Bizzarri, 2006;Hoefling et al 2011;Siwko & Corni, 2013;Venkat et al 2007;Zanetti-Polzi et al 2014), Au(100) (Hagiwara et al 2009), Au nanoparticle (Todorova et al 2014), Fe (Zhang et al 2009b), Ni (Yang & Zhao, 2006), Pd (Coppage et al 2011), Pt (Kantarci et al 2005, Ag (Aliaga et al 2011;Ghosh et al 2012) and steel (Imamura et al 2003).…”
Section: Elemental Metals and Alloysmentioning
confidence: 99%
“…They provide two sets of parameters for metal atoms (Ag, Al, Au, Cu, Ni, Pb, Pd, Pt); one set suited for 12-6 Lennard-Jones functions to be used in AMBER, CHARMM, CVFF and OPLS-AA force-fields, and another for 9-6 Lennard-Jones functions to be used in the COMPASS (Sun, 1998) In addition to polarization, surface charges should be taken into account when modeling a surface. Bizzarri (2006) investigated the dynamics and electron transfer (ET) properties of the bacterial ET protein, azurin, anchored to neutral, positively and negatively charged gold surfaces using classical MD simulations. They calculated the ET rate between the azurin copper atom and the sulfur atom of the cysteine surface anchor using classical Marcus theory (Marcus & Sutin, 1985).…”
Section: Metal Surfacesmentioning
confidence: 99%
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