Module 3: ES Flashcards
1
Q
Long-Range Electrostatics
(Problems)
A
- electrostatic potential converges slowly (1/r )
- dipole term is conditionally convergent, depending on whether one does periodic summation or shell summation
- Boundary conditions:
2
Q
Direct Summation
A
- compute potential using pbc
- requires large ncut
- bad scaling O(N2)
- number of cells scales with n3cut
3
Q
Ewald Summation
A
- separate into short-range and long-range by “adding zero” with Gaussian covering point charge
- short-range in real space
- long-range in k-space
- both terms now converge relatively quickly
- scaling O(N3/2)
- requires rcut, kcut
- minimum image convention → rcut < L/2
4
Q
Ewald Summation and P3M Errors
A
- rms force error depends on choice of Gaussian width α (and cut-offs)
- there exists methods to choose α based on desired accuracy
5
Q
P3M Method
(Overview)
A
- replace long-range contribution k-space sum with FFT on mesh grid
- scales O(NlogN)
6
Q
P3M Method
(Algorithm)
A
- Interpolate charges onto lattice charge density
- FFT transform lattice charge density to k-space
- Get potential by solving Poisson equation by multiplication of optimal influence function
- Get field iva k-space differentiation
- Inverse FFT transform back to real space
- Extrapolate field to position of charges
- Calculate force
7
Q
ELC + P3M
A
- P3M assumes 3D pbc
- ELC allows for “post-processing” correction for modelling 2D periodic systems using P3M
- requires charge neutral “buffer space” in non-periodic dimension
8
Q
Poiseuille Flow
A
Flow of incompressible, Newtonian fluid in channel is highest at the center
9
Q
Electro-Osmotic Flow
A
Flow of liquid in microchannel due to applied voltage
10
Q
Electrophoresis
A
motion of dispersed particles relative to a fluid under the influence of a spatially uniform electric field
11
Q
Rouse Model
(Overview)
A
- conformational dynamics of ideal chain
- no excluded volume interaction
- each monomer subject to Langevin Dynamics
- no hydrodynamic interactions
- usually assocaited with free-draining
12
Q
Rouse Model
(Good Performance)
A
- correctly predicts long-time diffusion for chains shorter than entanglement length
13
Q
Zimm Model
(Overview)
A
- extension of Rouse model to include hydrodynamic interactions
- uses Oseen matrix
14
Q
Zimm Model
(Good Performance)
A
- predicts diffusion relative to N -ν
- consistent with experiment