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Essentials of Computational Chemistry

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12.6 CASE STUDY: BINDING OF BIOTIN ANALOGS TO AVIDIN 453<br />

O<br />

HN 1<br />

2<br />

3<br />

HN<br />

S 4<br />

O<br />

S<br />

NH<br />

5<br />

NH<br />

6<br />

F<br />

7<br />

8<br />

CO2<br />

9<br />

∆GS(1→2)<br />

CO 2<br />

∆Gbind,1<br />

+ avidin E•S1<br />

∆Gbind,2<br />

+ avidin E•S2<br />

∆GE•S(1→2)<br />

Figure 12.6 Free-energy cycle associated with the binding <strong>of</strong> biotin and fluorobiotin analogs<br />

to avidin. What issues arise in choosing a force field for explicit simulation <strong>of</strong> these systems?<br />

What methods are better suited to computing the vertical legs <strong>of</strong> the cycle and what methods<br />

the horizontal ones?<br />

Note that since the free energies <strong>of</strong> the isolated components are computed using the<br />

same geometries as are employed in computing the free energy <strong>of</strong> the complex, the internal<br />

force-field energies cancel in computing a free energy <strong>of</strong> binding as<br />

〈G〉bind =〈G〉complex −〈G〉biotin −〈G〉avidin<br />

(12.33)<br />

Only the force-field energy term associated with interactions between the biotin and avidin<br />

fragments remains. This is added to the differential solvation free energies and differential<br />

thermal terms to determine the full binding free energy.<br />

To avoid the cost <strong>of</strong> multiple MD simulations, Eqs. (12.32) and (12.33) for fluorosubstituted<br />

biotin analogs are also evaluated using geometries from the original MD<br />

trajectory. The relevant hydrogen is simply replaced by a fluorine atom having the appropriate<br />

bond length oriented along the original C–H bond axis. Thus, there is no relaxation<br />

<strong>of</strong> the complex to relieve steric clashes if they are introduced. Again, the only forcefield<br />

energy terms that survive in computing the free energy <strong>of</strong> binding are the interaction<br />

energies between the biotin analog and the avidin. It is further assumed that the<br />

entropy change computed for complexation with biotin remains the same for a fluorinated<br />

biotin.<br />

The results <strong>of</strong> this rapid fluorine scanning are that substitution at positions pro-R 6and<br />

9andpro-S 7, 8, and 9 are all predicted to decrease binding by more than 4 kcal mol −1 ,<br />

substitution at position pro-S 6 is predicted to decrease binding by about 2 kcal mol −1 ,<br />

substitution at position pro-R 7 is predicted to have only a small unfavorable effect,<br />

and substitution at position pro-R 8 is predicted to increase binding by a little less than<br />

1 kcal mol −1 . The absolute free energy <strong>of</strong> binding for biotin itself with this method is<br />

computed to be −18.8 kcal mol −1 , although the fluctuations in the ensemble average and

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