上海交通大學(xué)理論物理研究所馬紅孺.ppt

模擬物理導(dǎo)論,凝聚態(tài)物質(zhì)的數(shù)值模擬方法(V) 馬紅孺,,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子模型,Molecular systems:,In most cases the interaction part can be approximated by pair interactions:,One famous example is the Lennard-Jones potential,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子模型,A very important quantity in statistical mechanics is the pair correlation function g( r,r0 ), defined as,where,It may also be written as,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子模型,For a homogeneous system the pair correlation function depends only on the distance between r and r0 . In this case we denote it as g(r) .,The g( r,r0 ) is proportional to the probability that given a particle at point r and find another particle at point r0 . At large distance g(r) tends to 1, we may define the total correlation function,The Fourier transform of the above function gives the static structure function (or structure factor),2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子模型,The structure function is defined as the correlation function of Fourier component of density fluctuations, The density is defined as: , and the density fluctuation is: , and its Fourier component is: ,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子模型,當(dāng)體積趨于無限時, 紅顏色的部分可以略去.,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子模型,The structure factor can be measured directly by scattering experiments and can also be calculated by simulations.,Many physical quantities can be expressed in terms of the pair correlation functions, for example the energy in NVT ensemble is,The pressure is,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子模型,The compressibility,This expression can be derived from the fluctuations of particle numbers,Since so,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子模型,On the other hand, it can be proved that,We have the final result.,The time correlation function is the correlations of two physical quantities at different times,For systems at equilibrium the time correlation function is a function of the time difference only and can be written as,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子模型,The velocity auto correlation function of the ith particle is,This can be derived from the definition (we will back to this point),Which is related to the diffusion constant of the particle.,which holds for large t.,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子模型,In general, transport coefficient is defined in terms of the response of a system to a perturbation.,where is the transport coefficient, and A is a physical variable appearing in the perturbation Hamiltonian. There is also an Einstein relation associated with this kind of expression,which holds for large t , (t , where is the relaxation time of ).,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子模型,The shear viscosity is given by,or,Here,The negative of P is often called stress tensor.,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,Monte Carlo 模擬,Monte Carlo simulation of Particle Systems,粒子系統(tǒng)的Monte Carlo 模擬和自旋系統(tǒng)原則上是一樣的。Metropolis 算法為： 1，隨機(jī)或順序選取一個粒子，其位置矢量為 ，對此粒子做移動 2，計算前后的能量差，決定是否接受移動。 3，在達(dá)到平衡后，收集數(shù)據(jù)，計算物理量。,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子動力學(xué)模擬,Molecular dynamics simulations,MD method is essentially the integration of the equation of motion of the classical many-particle system in a period of time. The trajectories of the system in the phase space are thus obtained and averages of the trajectories give various physical properties. Since we work on real dynamics in MD simulations we can also study the dynamic properties of the system such as relaxation to equilibrium, transport etc.,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子動力學(xué)模擬,Consider a rectangular volume of L1 L2 L3, with N classical particles put in. The particles are interact with each other. In principle, the interaction include pair interactions, three body interactions as well as many body interactions. For simplicity we will consider here only pair interactions. In this case each particle feel a force by all other particles and we further assume the force is depend only on distances from other particles and for each pair the force directed along the line join the pair of particles. So the force on the ith particle is,where is an unit vector along rj-ri.,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子動力學(xué)模擬,Periodic boundary condition(PBC),where L are vectors along the edges of the rectangular system volume and the sum over n is with all integers n . Usually this sum is the most time consuming part in a simulation.,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子動力學(xué)模擬,General procedure of MD (NVE ensemble),1. Initialize; 2. Start simulation and let the system reach equilibrium; 3. Continue simulation and store results.,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子動力學(xué)模擬,Initialize: 1, Specify the number of particles and interaction; 2, Setup the simulation box; 3, Specify the total energy of the system; 4, Assign position and momenta of each particle. a, In many cases we assign particles in a FCC lattice,If we use cubic unit cell and cube BOX then the number of particles per unit cell is 4, and the total number of particles are a 4M3, M=1,2,3, . That is we may simulation systems with total number of particles N=108, 256, 500, 864, .,b, The velocities of particles are draw from a Maxwell distribution with the specified temperature.,This is accomplished by drawing the three components of the velocity from the Gaussian distribution.,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子動力學(xué)模擬,The distribution of the x-component of velocity is,Draw numbers from a Gaussian: Consider:,Then,where v2=vx2+vy2 and,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子動力學(xué)模擬,So the distribution of vx and vy may be obtained from v and . The distribution of v:,The distribution of is uniform in the interval 0,2 .,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子動力學(xué)模擬,Generate random numbers for a given distribution,For a given distribution P(y) we consider how to get a random number y draw from P(y) from a random number x draw from uniform 0,1, i.e., we are going to find a function f(x), from which for a series of random numbers x distributed uniformly in the interval 0,1, y=f(x) will distributed according to P(y).,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子動力學(xué)模擬,then,Since,Exponential distribution,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子動力學(xué)模擬,The distribution of v:,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子動力學(xué)模擬,Draw random numbers uniformly distributed in the interval 0,2.,Another method of draw random numbers in the Gaussian distribution is through the following empirical methods.,Consider the distribution,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子動力學(xué)模擬,According to the central limit theorem, if we draw uniform random numbers ri in interval 0,1, and define a variable,when n! 1 the distribution of is the Gaussian distribution,If we take n=12, we get,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子動力學(xué)模擬,After the generation of the velocity of each particle, we may shift the velocity so that the total momentum is zero.,The standard Verlet algorithm is the first successful method in history and still wide used today in different forms. It is,To start the integration we need r(h), given by,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子動力學(xué)模擬,Variations of this method are,and,Both of these variations are mathematically equivalent to the original one but more stable under finite precision arithmetic.,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子動力學(xué)模擬,The temperature of the system is given by the equal partition theorem, that is the average of kinetic energy of each degree of freedom is half kBT,The N-1 is due to the conservation of the total momentum which reduce the degree of freedom by 3.,To reach the desired temperature we may scale the velocity at every few steps of integration,2003-10-21,上海交通大學(xué)理論物理研究所 馬紅孺,分子動力學(xué)模擬,After the system reach to equilibrium the integration continue in the same method as above without scaling of velocity. The data are stored or accumulated for the calculating physical properties. The static properties of physical quantity A is given by time average,2003