Water molecule bond length: Difference between revisions

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=== Potential Function ===
=== Potential Function ===


[https://en.wikipedia.org/wiki/Lennard-Jones_potential Lennard--Jones potential] with parameters for [https://en.wikipedia.org/wiki/Water_model TIPS] model:  
[https://en.wikipedia.org/wiki/Lennard-Jones_potential Lennard--Jones potential] with dimensionless parameters for [https://en.wikipedia.org/wiki/Water_model TIPS] model:  


<math>
<math>
V(x) = 4\epsilon \left[ \left( \frac\sigma x\right)^{12} - \left( \frac \sigma x\right)^6 \right]
V(x) = 4 \left[ \left( \frac1x\right)^{12} - \left( \frac1 x\right)^6 \right]
</math>
</math>


 
where the distance <math>x</math> is given in Ångstroms.
<math>
\begin{align}
A &= 580.0 \times 10^3 kcal A^{12}/mol \\
B &= 525.0 kcal A^6/mol
\end{align}
</math>
where <math>A</math> is Ångströms.


=== Integration ===
=== Integration ===

Revision as of 22:00, 12 October 2020

Introduction

Classical Mechanics

Newton Equations

where Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle F = - \nabla V} . The system is 1D, thus gradient will be differential, and Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle F= - \frac{d V}{dx}} .

Potential Function

Lennard--Jones potential with dimensionless parameters for TIPS model:

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle V(x) = 4 \left[ \left( \frac1x\right)^{12} - \left( \frac1 x\right)^6 \right] }

where the distance Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle x} is given in Ångstroms.

Integration

The finite differences (Euler method) are

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \begin{align} v(t) &= \frac{x(t+\Delta t) - x(t)}{\Delta t} \\ a(t) &= \frac{v(t+\Delta t) - v(t)}{\Delta t} \end{align} } and

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle a(t) = -\frac{\frac{d}{dx}(V(x(t)))}{m} }


Velocity Verlet Algorithm

A very good and easy to implement integration method is velocity Verlet:

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \begin{align} x(t + \Delta t) &= x(t) + v(t) \Delta t + \frac12 a \Delta t^2 \\ v(t + \Delta t) &= v(t) + \frac12\left( a(t) + a(t+\Delta t) \right) \Delta t \end{align} }

Temperature/ Initial distribution

The initial velocity of the hydrogen atom is chosen randomly from the Maxwell-Boltzmann distribution at given temperature Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle T}

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle p(v) = \left( \frac{m}{2\pi k_B T} \right)^{1/2} \exp\left[- \frac12 \frac{mv^2}{k_B T} \right] }

Results

Issues

1D statement