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The Electronic Structure-Based Explicit Polarization X-Pol Potential

The Electronic Structure-Based Explicit Polarization (X-Pol) Potential [Pg.86]

Za (/) is the nucleus charge of atom a and 2M is the number of electrons in molecule /, V) ( P/) is the electrostatic potential of molecular J at either the electronic (t = i) or nuclear (t = a) positions of molecule I. The electrostatic potential due to molecule J is defined as follows  [Pg.87]

Consequently, we introduce the second approximation which is to use an approximate electrostatic potential in Eq.(4-21) to determine inter-fragment electronic interaction energies. Thus, the electronic integrals in Eq. (4-21) are expressed as a multipole expansion on molecule J, whose formalisms are not detailed here. If we only use the monopole term, i.e., partial atomic charges, the interaction Hamiltonian is simply given as follows  [Pg.88]

For proteins, the fragment is defined by the peptide unit convention as recommended by the International Union of Pure and Applied Chemistry, although the [Pg.88]




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Based Electronics

Electron polarization

Electronic potentials

Electronic structure-based explicit polarization

Electronic-based

Explicitness

Polar structure

Polarization electronic

Polarization potential

Polarization structural

Polarized potential

Polarized structure

Polarizing potential

Potential structure

Structural polarity

The electronic polarization

X electron

X potential

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