Lecture 5: MD1 Flashcards

1
Q

What does statistical mechanics bridge?

A

Macroscopic and microscopic

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2
Q

What are the aims of Statistical mechanics?

A

-predict behaviour of bulk matter from knowledge of molecular properties
-extract microscopic properties from a knowledge of bulk behaviour

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3
Q

What is a macro state?

A

A particular set of values of energy, the number of particles and then volume of an isolated thermodynamic system

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4
Q

What is a Microstate?

A

Specific microscopic configuration of the system

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5
Q

are thermodynamic properties of individual micro states measureable?

A

No- we observe averages instead

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6
Q

What does movement that changed the arrangement or particles cause?

A

A new micro state

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7
Q

Are all micro states equally probable?

A

Yes

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8
Q

Are all macro states equally probable?

A

No- prob is directly proportional to number of associated micro states
The more ways a microstate can occur the more probable it is

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9
Q

How can classical systems of N particles be described?

A

In 6N-dimensional phase space

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10
Q

What’s the equation for 6N phase space?

A

X(r,p)
r=(x1,y1,z1…) position
p=(px1, py1, pz1…) momentum

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11
Q

What’s a good way to visualise phase space?

A

-Consider a ball bouncing in a box
-each frame is a microstate
-phase space is X=(x,y,z,px,py,pz)
-over time the ball bounces all over the box exploring the inside of the box

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12
Q

What is the ergodic hypothesis?

A

A system/microstate is equally likely to be found in any microstate, or, that over long periods of time all accessible micro states are equiprobable

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13
Q

What is the ergodic hypothesis simplified?

A

The time average is the same as the ensemble average

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14
Q

Is there proof of the ergodic hypothesis?

A

No but there is overwhelming practical evidence

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15
Q

What is an ensemble?

A

A system at equilibrium corresponding to different physical requirements

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16
Q

Describe the microscopic va macroscopic view of ensembles

A

Macroscopic view: looks unchanging
Microscopic view: different microstates

17
Q

What statistical ensemble would the coefficient of thermal expansion use?

A

Isobaric-isothermal NPT ensemble that allows for volume changes

18
Q

Describe the process of MD program

A
  1. Read in parameters (specify system conditions)
  2. Initialise system (initial positions and velocities)
  3. Compute forces on all properties
  4. Integrate through time (use Newtons equations of motions)
  5. Compute and print averages
19
Q

What is important to remember when picking the right approach

A

Is the simulation sensible?
What will it tell me?

20
Q

Why is it important to initialise the system?

A

-There is a large unfavourable potential energy of the system that leads to the system exploding/breaking
-there is particle-particle overlap
-there is unfavourable intramolecular interactions that can lead to poor initial choices eg long bonds

21
Q

How are positions assigned for a crystal?

A

Place molecules in desired position along a lattice

22
Q

How are positions assigned for a liquid?

A

Start from a crystal, run at very high temp, cool to desired temp
Place at random at a slightly lower density, run at constant pressure to get desired density

23
Q

How are positions assigned for a gas?

A

Randomly

24
Q

What are some options for assigning momentum?

A

-temp ramp from 0K
-assign velocities from a uniform distribution between two values and scales to produce target temp
-assign velocities from a Gaussian distribution with mean=0 and variance scaled to produce target temp

25
Q

How is force calculated in MD simulations?

A

F=-dU/dr

26
Q

What’s mathematically good about F and U?

A

(sigma/r)^6 can be calculated and then used for both calculations rather than calculating both from scratch

27
Q

What is the equation for energy in the Harmonic potential?

A

U(r) =1/2 k(r-r0)^2

28
Q

Why do we need to integrate through time?

A

To get the ensemble averages of our property of interest

29
Q

What is Newton’s second law?

A

F=ma

30
Q

Describe the method used for solving time integration

A

-the equations must be solved numerically rather than analytically
-time is quantised
-simulated time goes in time steps dt
-need to know positions and time derivatives

31
Q

What are two time integration errors?

A

-truncation errors (due to accuracy of finite difference method)
-round off errors (due to implementation of algorithm)

32
Q

How can time integration errors be reduced?

A

By reducing dt

33
Q

What is the Verdot algorithm?

A

-calculated both forward and backwards step
-more accurate than forward simple step time integration

34
Q

What does the verlet algorithm not generate?

A

Velocities needed for kinetic energy and temp

35
Q

Why is verlet algorithm computationally cheaper?

A

Lower data storage required

36
Q

What is the leapfrog algorithm

A

-modification of verlet algorithm
-allows velocities and positions to leap over one another ensuring velocities are accurately calculated

37
Q

What does leapfrog Algorithm not generate?

A

Velocities at time t
Instead need to take means from t+/-1/2 dt

38
Q

What is the velocity verlet algorithm

A

-more accurate trajectories and less drift in total energy
-increased computational cost

39
Q

Describe the velocity verlet algorithm

A

-calculate position at t+dt
-calculate half step velocities t+1/2 dt
-calculate acceleration at t+dt from forces using r(t+dt)
-calculate velocities at t+dt