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crc press - E-Lib FK UWKS

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Structure Prediction of CPPs and Iterative Development of Novel CPPs 191<br />

1<br />

0<br />

core core<br />

Water Interface Interface Water<br />

-18<br />

-13.5<br />

q 2 (-15.75Å)<br />

FIGURE 9.1 Model membrane of IMPALA.<br />

1<br />

13.5 18<br />

Monolayer 2 Monolayer 1<br />

q 1 (15.75Å)<br />

generally these interactions do not seem crucial for folding membrane proteins, as<br />

the proteins may refold in vitro under nonbiological conditions. 42 This assumption<br />

is also made for the crystallization of integrated membrane proteins (IMPs) in which<br />

lipids are replaced by detergents. Moreover, the description is so simple that it could<br />

be easily adapted to other interfaces (e.g., monolayer, spherical, or discoidal).<br />

9.2.2 ATOMIC SURFACE HYDROPHOBICITY (FIRST RESTRAINT)<br />

Z ( Å)<br />

To calculate the hydrophobic and hydrophilic restraints, we use atomic surface<br />

transfer energies, a concept relying on the assumption that the overall transfer energy<br />

of a molecule, H, can be calculated as<br />

N<br />

= ∑ i tr() i<br />

i=<br />

1<br />

H SE<br />

(9.2)<br />

where i is an index for the N atoms of the molecule, S (Å 2 ) the solvent-accessible<br />

surface calculated with Shrake and Rupley’s algorithm with 192 points, 43,44 and E tr<br />

(kJ/·mol·Å 2 ) is the transfer energy by surface of individual atoms (Table 9.1). A<br />

similar approach was successfully used on small molecules 45 by considering that<br />

N<br />

= ∑ ()<br />

i=<br />

1<br />

H E atr i<br />

(9.3)

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