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:
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2
Q

Direct Summation

A
  • compute potential using pbc
  • requires large ncut
  • bad scaling O(N2)
    • number of cells scales with n3cut
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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
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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
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5
Q

P3M Method

(Overview)

A
  • replace long-range contribution k-space sum with FFT on mesh grid
  • scales O(NlogN)
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6
Q

P3M Method

(Algorithm)

A
  1. Interpolate charges onto lattice charge density
  2. FFT transform lattice charge density to k-space
  3. Get potential by solving Poisson equation by multiplication of optimal influence function
  4. Get field iva k-space differentiation
  5. Inverse FFT transform back to real space
  6. Extrapolate field to position of charges
  7. Calculate force
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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
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8
Q

Poiseuille Flow

A

Flow of incompressible, Newtonian fluid in channel is highest at the center

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9
Q

Electro-Osmotic Flow

A

Flow of liquid in microchannel due to applied voltage

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10
Q

Electrophoresis

A

motion of dispersed particles relative to a fluid under the influence of a spatially uniform electric field

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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
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12
Q

Rouse Model

(Good Performance)

A
  • correctly predicts long-time diffusion for chains shorter than entanglement length
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13
Q

Zimm Model

(Overview)

A
  • extension of Rouse model to include hydrodynamic interactions
    • uses Oseen matrix
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14
Q

Zimm Model

(Good Performance)

A
  • predicts diffusion relative to N -ν
    • consistent with experiment
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