MSE-561/MEAM-553 Homework 1 (due 09/23/21)
Notes: I will introduce the Lennard-Jones (L-J) pair potential for solid Argon in the next class.
You need to know this potential and the smooth cut-off to zero that is needed in modeling. Both the
potential and the cut-off are described in Prof. Vitek’s notes in a separate file titled the L-J
potential. Please read this before attempting the homework or wait until Tuesday’s class to know
more. In the meantime, you may look up or convince yourself what close-packed crystal structures
are in one, two and three dimensional space. You may search if you are not familiar with this
concept. If anybody needs a pointer, please email me and I can suggest some good websites. Once
you know what close-packed structure you should consider in two dimensions, please draw a rough
sketch by hand or make a plot using a code and identify how many neighbors an atom has and at
what distances given the lattice parameter. The pair potential only depends on the distance between
the atoms and not their orientation. Such potentials are called “central” potentials in physics.
With this background, you may proceed to do the homework. Please prepare your answers in the
form of a report where you explain your thinking and procedure in words briefly before solving the
problem. The numerical code or relaxation code in subsequent homework should be attached here
and also uploaded separately.
Consider a material in which atoms interact via the Lennard-Jones potential that is
smoothly cut-off at = 7.5Å, as explained in the description of the Lennard-Jones
potential (see Vitek’s notes). Do not forget that the potential has a different form for r
< and for .
1. Determine analytically the equilibrium lattice parameter for the two-dimensional
periodic close-packed structure with no surfaces. The L-J potential parameters given
in the notes are for three-dimensional face-centered cubic close-packed structure. In
this HW 1, you are asked to determine the equilibrium lattice parameter for a close-
packed lattice in two dimensions with the same L-J potential. Use the following
method:
Decide first geometrically the close-packed two-dimensional structure. Make a
sketch showing several tens of atoms.
Determine how many first, second, third etc. interacting neighbors are within
the cut-off radius. First, choose just the neighbors which are the closest to the central
atom which is chosen as the origin. Analytically, minimize the potential energy with
respect to the lattice parameter and obtain its value. Now check, if the second
neighbor shell atoms lie within the cut-off value of the potential. Repeat the
rcut
ro ro < r < rcut
2
minimization analytically by including the first and second neighbors. Obtain the
equilibrium lattice parameter. Now, check if the third neighbors lie within the cut-off
of the potential. If they do, repeat the procedure and find the two dimensional
equilibrium lattice parameter for your chosen close-packed lattice. Include more
neighboring shells if necessary and repeat.
2. In order to get the first training in coding solve this problem numerically.
Proceed as in the analytical case: build your 2D close-packed lattice and calculate the
radius of first, second, third and fourth neighbor shells. Determine the number of
neighbors in each shell. Evaluate the energy of the system as a function of the lattice
parameter and taking into account only the first shell, the first and second shell, etc.,
up the fourth shell of neighbors. Plot this dependence of the potential energy as a
function of the lattice parameter. The minimum of the potential energy determines the
equilibrium lattice parameter. In the computer code you have to make logical
decisions whether two atoms interact with each other or not, what is their separation
and what is the contribution of this interaction to the potential energy. Comment on
the agreement/disagreement between your analytical and numerical answers to the
first and second part of this homework respectively.
Please upload your homework with the numerical code, details of analytical method
and plot of the variation of energy with lattice parameter.
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