Thermophoresis in Liquids and its Connection to...

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Master Thesis Defense Thermophoresis in Liquids and its Connection to Equilibrium Quantities Benjamin F. Maier 23 June 2014

Transcript of Thermophoresis in Liquids and its Connection to...

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Master Thesis Defense

Thermophoresis in Liquids and its Connection to Equilibrium Quantities

Benjamin F. Maier

23 June 2014

Page 2: Thermophoresis in Liquids and its Connection to ...people.physik.hu-berlin.de/~bfmaier/maier_defense.pdf · Master Thesis Defense Thermophoresis in Liquids and its Connection to Equilibrium

06/23/14 2

Thermophoresis

● directed movement of particles

● Induced by heat

● in gaseous or liquid systems

here: gas

● solute moves to cold

http://bit.ly/1qy7Gs7, 06/20/14

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Thermophoresis - Liquids

● Different picture for liquids

● Hot region sometimes preferred

● No coherent prediction possible

http://i.imgur.com/FKLjmUV.jpg, 06/20/14

?

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Thermophoresis – A Powerful Tool!

Powerful addition to electrophoresis

Braun, et. al. (2006)

Problem: Unpredictable!

DNA migration

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Thermophoresis in Formulae

phenomenological flux

diffusion thermal flux

Soret equilibrium

TemperatureDensityDiffusion coefficientThermal diffusive mobility

Soret coefficient

measured from Soret equilibrium density

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Soret Coefficient

● sign of dictates direction of movement

Piazza, et. al. (2008)

prefers cold region

prefers hot region

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Local Equilibrium

● assumptions

– length scale of solute-solvent interaction

– small heat flux

● Würger (2014)

● Braun/Dhont (2007)

force on solute

solvation free energy

solvation enthalpy

solvation entropy

Which one is true?

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Open Problems

● local equilibrium applicable?

● if yes, is driving force the entropy or the enthalpy?

● connection of and

● sign change of reproducible?

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Theory – Brownian Motion

● Overdamped Langevin equation (an SDE)

● interpretation: Ito or Stratonovich?

position change

external force interaction force

Gaussianstochastic process

local diffusion coefficient (not necessarily Einstein's relation)

ItoStratonovich

– friction

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Ideal Gas Soret Equilibrium Density

● ideal gas without external potential

● interpretation of

– Einstein's relation follows for spatially invariant diffusion coefficient

– may be wrong (Astumian, 2008)

– Will assume

ideal gasequation of state

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BD Simulation for 1D Ideal Gas

cold hotlinearreflective boundary conditions

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BD Simulation for 1D Ideal Gas

cold hotlinearreflective boundary conditions

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1D Ideal Gas with External Potential

cold hot

naïve Boltzmann expectation

−1.0 −0.5 0.0 0.5 1.00.0

0.2

0.4

0.6

0.8

1.0

T

−1.0 −0.5 0.0 0.5 1.00.0

0.2

0.4

0.6

0.8

1.0

T

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1D Ideal Gas with External Potential

cold hot

naïve Boltzmann expectation

−1.0 −0.5 0.0 0.5 1.00.0

0.2

0.4

0.6

0.8

1.0

T

−1.0 −0.5 0.0 0.5 1.00.0

0.2

0.4

0.6

0.8

1.0

T

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Dynamical Density Functional Theory (DDFT)

● local equilibrium assumption: use equilibrium functional

● traditional functional, dimensionless

● new scaling, adapted ideal gas functional

● interacting particles: how to scale excess functional?

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Interacting Particles – Solvent and Dilute Solute

two possibilities to scale the excess functional

solute densities

Soret coefficient

Würger, '14 Braun/Dhont, '07

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0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0 4.5

0.0

0.5

1.0

1.5

2.0

2.5

3.0

0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0 4.50.0

0.2

0.4

0.6

0.8

1.0

0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0 4.5

0.0

0.5

1.0

1.5

2.0

2.5

3.0

0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0 4.50.0

0.2

0.4

0.6

0.8

1.0

Gaussian Solute in Ideal Gas Solvent (1D)

equilibrium from thermodynamic integration

Significant difference in predictions from enthalpy and entropyapproaches

periodic boundary conditions

fit function

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Thermophoretic BD Sim. – Gaussian Solute

hotcold

looks like the prediction from the enthalpy

−0.5 0.0 0.5

0.6

0.8

1.0

1.2

−0.5 0.0 0.5

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0.8

1.0

1.2

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Thermophoretic BD Sim. – Gaussian Solute

hotcold

looks like the prediction from the enthalpy

−0.5 0.0 0.5

0.6

0.8

1.0

1.2

−0.5 0.0 0.5

0.6

0.8

1.0

1.2

0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0 4.5−1.0

−0.8

−0.6

−0.4

−0.2

0.0

0.2

0.4

0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0 4.5−1.0

−0.8

−0.6

−0.4

−0.2

0.0

0.2

0.4 Soret coefficient

Sign change!

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Homogeneous 1D System of Gaussian Particles

Soret equilibrium density from enthalpy connected to equation of state

hotcold

const.pressuresecond order

virial eq. of state

second virial coefficient

−0.5 0.0 0.5

20

25

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40

45

−0.5 0.0 0.5

20

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30

35

40

45

T

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Homogeneous 1D System of Gaussian Particles

Soret equilibrium density from enthalpy connected to equation of state

hotcold

const.pressuresecond order

virial eq. of state

second virial coefficient

−0.5 0.0 0.5

20

25

30

35

40

45

−0.5 0.0 0.5

20

25

30

35

40

45

T

Thermophoretic system seems to follow the equation of state!

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Summary So Far

● achieved

– local equilibrium assumption seems to be appropriate

– Soret coefficient connected to enthalpy

– sign change of reproducible

– crucial assumption:

● open

– does it describe real systems?

– choice of and its origin

MD simulations

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MD Setup

● modified SPC/E thermostats (Nosé-Hoover)

● SPC/E solvent● Lennard-Jones noble gas solute

● periodic boundary conditions in z● reflective boundary conditions in xy

● NPT equilibration● NVT runs● measuring the Soret equilibrium

density

● SPC/E: water model(extended simple point charge)

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First: Solvation Free Energy

fit function

300 350 400 450 500

T / K300 350 400 450 500

T / K

Method: Widom Insertion in thermodynamic equilibrium bulk SPC/E for Ar, Kr and Xe

example: xenon

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Thermophoretic simulations - Solvent

● 7 simulations of Ar, Xe, Kr with run times t > 200 ns in temperature range 300 K < T < 450 K● measured the Soret equilibrium density and temperature profile of solvent and solute

example: krypton solvent density

following the equation of state!

linear profile

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Thermophoretic simulations - Solute

● 7 simulations of Ar, Xe, Kr with run times t > 200 ns in temperature range 300 K < T < 450 K● measured the Soret equilibrium density and temperature profile of solvent and solute

example: krypton solute density

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Soret Coefficient from Density – Krypton

Calculate Soret coefficient as

derivative – how to model ?

Soret eq. density Soret coefficient

Kr, 300 K < T < 350 K

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Soret Coefficient from Density – Krypton

Calculate Soret coefficient as

derivative – how to model ?

Soret eq. density Soret coefficient

Kr, 300 K < T < 350 K

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Soret Coefficient from Density – Argon

Calculate Soret coefficient as

Soret eq. density Soret coefficient

Ar, 300 K < T < 350 K

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Soret Coefficient from Density – Argon

Calculate Soret coefficient as

Soret eq. density Soret coefficient

Ar, 300 K < T < 350 K

For every simulation: Soret coefficient isregion where all fits coincide

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Soret Coefficient from all Simulations

no significant agreement/results in MD simulations

no sign change

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Summary & Outlook

● theoretical derivation of Soret equilibrium density for various systems via DDFT

● connection between Soret coefficient and solvation enthalpy/equation of state found in BD simulations

● no significant agreement between Soret coefficient and solvation enthalpy in MD simulations

● agreement between Soret eq. density and eq. of state in MD simulations

● Ito/Stratonovich

● more realistic BD simulations / difference between BD and MD, extract meaningful data from MD

● connection between local diffusion coefficient and local temperature

● consideration of electrostatics and hydrodynamics

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1D Hard Rods

equation of state

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2D Ideal Gas in Harmonic Potential

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2D Ideal Gas in Harmonic Potential

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Soret Coefficient

● sign of dictates direction of movement

Piazza, et. al. (2008)

prefers cold region

prefers hot region Solute size

dependenceBraun, et. al. (2006)

Polystyrene beads

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Hypothetical Influence of Friction

Stokes' law consider SPC/E viscosityadditional factor in densityadditional term in Soret coeff.

● 8 hypotheses● sign change in