I wrote a code for ising model simulation which works but I want some help in optimizing it The Next CEO of Stack OverflowOptimizing code for UVAJ 573 The Snail

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I wrote a code for ising model simulation which works but I want some help in optimizing it



The Next CEO of Stack OverflowOptimizing code for UVAJ 573 The Snail










0












$begingroup$


I have written this code to simulate Ising Model at one particular temperature in presence of magnetic field to observe hysteresis effect using the metropolis algorithm.



While the code runs and gave me a desired output, it is a badly written code(I feel so) because of my lack of coding experience. Could you help me out as to how could I have written this in a better way? Or what can I do to optimize it next time I write such a code? Or are there any inbuilt functions I could have called instead of writing a block?



P.S. I borrowed the random number generator directly from someone's answer to a thread on this site. I cannot find the exact thread, apologies! (I will cite it once I do)



I hope this kind of a question is allowed on this thread. Any help or resources would be appreciated.



//function to assign random spins to the lattice



int spin(int r) 

int s;
if(r>5)

s=+1;

else

s=-1;


return s;



////////////////////////////////////////////////////////////////////////////



////////////////////////////////////////////////////////////////////////////
//random number generator



float prandom(int i,int N)

std::random_device rd; //Will be used to obtain a seed for the random number engine
std::mt19937 gen(rd()); //Standard mersenne_twister_engine seeded with rd()
std::uniform_real_distribution<> dis(i,N);
// Use dis to transform the random unsigned int generated by gen into a
// double in [1, 2). Each call to dis(gen) generates a new random double
int t = dis(gen);
return t;



////////////////////////////////////////////////////////////////////////////
//frunction to randomly flip the spins



I am selecting a random site and seeing how the total energy will change by calculating the energy dE for the neighbouring sites. If the energy is negative then I make the spin flip permanent if it is not negative then I gave a probability exp(-dE) by which it can flip the spin



std::vector< std::vector < int > > flip (int N,std::vector< std::vector < int > >lattice, float beta,int tab[],float H)

int a =prandom(0,N);
int b =prandom(0,N);
int s=lattice[a][b];
float dE=(2*s*H)+(2*s*(lattice[tab[a+2]][b]+lattice[tab[a]][b]+lattice[a][tab[b+2]]+lattice[a][tab[b]]));
//std::cout<<dE<<"t"<<a<<"t"<<b<<"n";
if(dE<0)

s=-1*s;

else

float k = 1.0*prandom(0.0,1000)/1000;
float H = exp(-beta*dE);
if(k<=H)

s=-1*s;

else

s = 1*s;


lattice[a][b]=s;
return lattice;



////////////////////////////////////////////////////////////////////////////



// main program///////
int main()

std::ofstream outdata;
outdata.open("ising_model_field_final2.txt");
int a,b,N=20,i,j,k,r,t,sweep=1500;
float M=0,M_sweep=0,H=-0.10;
int tab[N];
tab[0] = N-1;
tab[N+1] = 0;
for (i=1;i<=N;i++)

tab[i]=i-1; // this is the periodic boundary condition to make my lattice infinite (lattice site [x][0] is a neighbour of [x][N] and so on..)

float T, beta;
//beta=1.0/T; // boltzman constant is assumed to be 1.
//creating a 2d lattice and populating it
std::vector< std::vector < int > >lattice;

//populate the lattice
for (i=0; i<N; i++)

std::vector< int > row; //create a row of the lattice
for (j=0;j<N;j++)

row.push_back(-1); //populate the row vector

lattice.push_back(row); //populate the column vector

lattice=flip(N,lattice,beta, tab,H);
/* for(i=0;i<N;i++)

for(j=0;j<N;j++)

std::cout<<lattice[j][i]<<"t";

std::cout<<std::endl;
*/
///////////////////////////////////////////////////////////////////////////
//field control
for(int temp=1;temp<=30;temp++)

if(temp>15)

H=H-0.015;

else

H=H+0.015;

//M=0;
T=2.2;
beta=1.0/T;
///////////////////////////////////////////////////////////////////////////
//number of sweeps
std::cout<<beta<<"n";
for(i=0;i<=sweep;i++)

//T=0.1*i;
///////////////////////////////////////////////////////////////////////////
//Number of flips
//printf("Sweep = %dn",i);
for(j=1;j<=N*N;j++)

lattice=flip(N,lattice,beta, tab,H);

M_sweep=0;
for(t=0;t<N;t++)

for(int u=0;u<N;u++)

if(i>=500)
M_sweep=M_sweep+lattice[t][u];

//std::cout<<"Mag="<<M<<"t";

M=M+ M_sweep/(N*N);
//std::cout<<"Mag="<<M<<"t";

M=M/(sweep-1000);
std::cout<<T<<"n";
outdata << M <<"t"<< H <<"n";

////////////////////////////////////////////////////////////////////////////
//printing the output of 2d lattice
for(i=0;i<N;i++)

for(j=0;j<N;j++)

std::cout<<lattice[j][i]<<"t";

std::cout<<std::endl;

outdata.close();









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    0












    $begingroup$


    I have written this code to simulate Ising Model at one particular temperature in presence of magnetic field to observe hysteresis effect using the metropolis algorithm.



    While the code runs and gave me a desired output, it is a badly written code(I feel so) because of my lack of coding experience. Could you help me out as to how could I have written this in a better way? Or what can I do to optimize it next time I write such a code? Or are there any inbuilt functions I could have called instead of writing a block?



    P.S. I borrowed the random number generator directly from someone's answer to a thread on this site. I cannot find the exact thread, apologies! (I will cite it once I do)



    I hope this kind of a question is allowed on this thread. Any help or resources would be appreciated.



    //function to assign random spins to the lattice



    int spin(int r) 

    int s;
    if(r>5)

    s=+1;

    else

    s=-1;


    return s;



    ////////////////////////////////////////////////////////////////////////////



    ////////////////////////////////////////////////////////////////////////////
    //random number generator



    float prandom(int i,int N)

    std::random_device rd; //Will be used to obtain a seed for the random number engine
    std::mt19937 gen(rd()); //Standard mersenne_twister_engine seeded with rd()
    std::uniform_real_distribution<> dis(i,N);
    // Use dis to transform the random unsigned int generated by gen into a
    // double in [1, 2). Each call to dis(gen) generates a new random double
    int t = dis(gen);
    return t;



    ////////////////////////////////////////////////////////////////////////////
    //frunction to randomly flip the spins



    I am selecting a random site and seeing how the total energy will change by calculating the energy dE for the neighbouring sites. If the energy is negative then I make the spin flip permanent if it is not negative then I gave a probability exp(-dE) by which it can flip the spin



    std::vector< std::vector < int > > flip (int N,std::vector< std::vector < int > >lattice, float beta,int tab[],float H)

    int a =prandom(0,N);
    int b =prandom(0,N);
    int s=lattice[a][b];
    float dE=(2*s*H)+(2*s*(lattice[tab[a+2]][b]+lattice[tab[a]][b]+lattice[a][tab[b+2]]+lattice[a][tab[b]]));
    //std::cout<<dE<<"t"<<a<<"t"<<b<<"n";
    if(dE<0)

    s=-1*s;

    else

    float k = 1.0*prandom(0.0,1000)/1000;
    float H = exp(-beta*dE);
    if(k<=H)

    s=-1*s;

    else

    s = 1*s;


    lattice[a][b]=s;
    return lattice;



    ////////////////////////////////////////////////////////////////////////////



    // main program///////
    int main()

    std::ofstream outdata;
    outdata.open("ising_model_field_final2.txt");
    int a,b,N=20,i,j,k,r,t,sweep=1500;
    float M=0,M_sweep=0,H=-0.10;
    int tab[N];
    tab[0] = N-1;
    tab[N+1] = 0;
    for (i=1;i<=N;i++)

    tab[i]=i-1; // this is the periodic boundary condition to make my lattice infinite (lattice site [x][0] is a neighbour of [x][N] and so on..)

    float T, beta;
    //beta=1.0/T; // boltzman constant is assumed to be 1.
    //creating a 2d lattice and populating it
    std::vector< std::vector < int > >lattice;

    //populate the lattice
    for (i=0; i<N; i++)

    std::vector< int > row; //create a row of the lattice
    for (j=0;j<N;j++)

    row.push_back(-1); //populate the row vector

    lattice.push_back(row); //populate the column vector

    lattice=flip(N,lattice,beta, tab,H);
    /* for(i=0;i<N;i++)

    for(j=0;j<N;j++)

    std::cout<<lattice[j][i]<<"t";

    std::cout<<std::endl;
    */
    ///////////////////////////////////////////////////////////////////////////
    //field control
    for(int temp=1;temp<=30;temp++)

    if(temp>15)

    H=H-0.015;

    else

    H=H+0.015;

    //M=0;
    T=2.2;
    beta=1.0/T;
    ///////////////////////////////////////////////////////////////////////////
    //number of sweeps
    std::cout<<beta<<"n";
    for(i=0;i<=sweep;i++)

    //T=0.1*i;
    ///////////////////////////////////////////////////////////////////////////
    //Number of flips
    //printf("Sweep = %dn",i);
    for(j=1;j<=N*N;j++)

    lattice=flip(N,lattice,beta, tab,H);

    M_sweep=0;
    for(t=0;t<N;t++)

    for(int u=0;u<N;u++)

    if(i>=500)
    M_sweep=M_sweep+lattice[t][u];

    //std::cout<<"Mag="<<M<<"t";

    M=M+ M_sweep/(N*N);
    //std::cout<<"Mag="<<M<<"t";

    M=M/(sweep-1000);
    std::cout<<T<<"n";
    outdata << M <<"t"<< H <<"n";

    ////////////////////////////////////////////////////////////////////////////
    //printing the output of 2d lattice
    for(i=0;i<N;i++)

    for(j=0;j<N;j++)

    std::cout<<lattice[j][i]<<"t";

    std::cout<<std::endl;

    outdata.close();









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      0












      0








      0





      $begingroup$


      I have written this code to simulate Ising Model at one particular temperature in presence of magnetic field to observe hysteresis effect using the metropolis algorithm.



      While the code runs and gave me a desired output, it is a badly written code(I feel so) because of my lack of coding experience. Could you help me out as to how could I have written this in a better way? Or what can I do to optimize it next time I write such a code? Or are there any inbuilt functions I could have called instead of writing a block?



      P.S. I borrowed the random number generator directly from someone's answer to a thread on this site. I cannot find the exact thread, apologies! (I will cite it once I do)



      I hope this kind of a question is allowed on this thread. Any help or resources would be appreciated.



      //function to assign random spins to the lattice



      int spin(int r) 

      int s;
      if(r>5)

      s=+1;

      else

      s=-1;


      return s;



      ////////////////////////////////////////////////////////////////////////////



      ////////////////////////////////////////////////////////////////////////////
      //random number generator



      float prandom(int i,int N)

      std::random_device rd; //Will be used to obtain a seed for the random number engine
      std::mt19937 gen(rd()); //Standard mersenne_twister_engine seeded with rd()
      std::uniform_real_distribution<> dis(i,N);
      // Use dis to transform the random unsigned int generated by gen into a
      // double in [1, 2). Each call to dis(gen) generates a new random double
      int t = dis(gen);
      return t;



      ////////////////////////////////////////////////////////////////////////////
      //frunction to randomly flip the spins



      I am selecting a random site and seeing how the total energy will change by calculating the energy dE for the neighbouring sites. If the energy is negative then I make the spin flip permanent if it is not negative then I gave a probability exp(-dE) by which it can flip the spin



      std::vector< std::vector < int > > flip (int N,std::vector< std::vector < int > >lattice, float beta,int tab[],float H)

      int a =prandom(0,N);
      int b =prandom(0,N);
      int s=lattice[a][b];
      float dE=(2*s*H)+(2*s*(lattice[tab[a+2]][b]+lattice[tab[a]][b]+lattice[a][tab[b+2]]+lattice[a][tab[b]]));
      //std::cout<<dE<<"t"<<a<<"t"<<b<<"n";
      if(dE<0)

      s=-1*s;

      else

      float k = 1.0*prandom(0.0,1000)/1000;
      float H = exp(-beta*dE);
      if(k<=H)

      s=-1*s;

      else

      s = 1*s;


      lattice[a][b]=s;
      return lattice;



      ////////////////////////////////////////////////////////////////////////////



      // main program///////
      int main()

      std::ofstream outdata;
      outdata.open("ising_model_field_final2.txt");
      int a,b,N=20,i,j,k,r,t,sweep=1500;
      float M=0,M_sweep=0,H=-0.10;
      int tab[N];
      tab[0] = N-1;
      tab[N+1] = 0;
      for (i=1;i<=N;i++)

      tab[i]=i-1; // this is the periodic boundary condition to make my lattice infinite (lattice site [x][0] is a neighbour of [x][N] and so on..)

      float T, beta;
      //beta=1.0/T; // boltzman constant is assumed to be 1.
      //creating a 2d lattice and populating it
      std::vector< std::vector < int > >lattice;

      //populate the lattice
      for (i=0; i<N; i++)

      std::vector< int > row; //create a row of the lattice
      for (j=0;j<N;j++)

      row.push_back(-1); //populate the row vector

      lattice.push_back(row); //populate the column vector

      lattice=flip(N,lattice,beta, tab,H);
      /* for(i=0;i<N;i++)

      for(j=0;j<N;j++)

      std::cout<<lattice[j][i]<<"t";

      std::cout<<std::endl;
      */
      ///////////////////////////////////////////////////////////////////////////
      //field control
      for(int temp=1;temp<=30;temp++)

      if(temp>15)

      H=H-0.015;

      else

      H=H+0.015;

      //M=0;
      T=2.2;
      beta=1.0/T;
      ///////////////////////////////////////////////////////////////////////////
      //number of sweeps
      std::cout<<beta<<"n";
      for(i=0;i<=sweep;i++)

      //T=0.1*i;
      ///////////////////////////////////////////////////////////////////////////
      //Number of flips
      //printf("Sweep = %dn",i);
      for(j=1;j<=N*N;j++)

      lattice=flip(N,lattice,beta, tab,H);

      M_sweep=0;
      for(t=0;t<N;t++)

      for(int u=0;u<N;u++)

      if(i>=500)
      M_sweep=M_sweep+lattice[t][u];

      //std::cout<<"Mag="<<M<<"t";

      M=M+ M_sweep/(N*N);
      //std::cout<<"Mag="<<M<<"t";

      M=M/(sweep-1000);
      std::cout<<T<<"n";
      outdata << M <<"t"<< H <<"n";

      ////////////////////////////////////////////////////////////////////////////
      //printing the output of 2d lattice
      for(i=0;i<N;i++)

      for(j=0;j<N;j++)

      std::cout<<lattice[j][i]<<"t";

      std::cout<<std::endl;

      outdata.close();









      share







      New contributor




      aargiee is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
      Check out our Code of Conduct.







      $endgroup$




      I have written this code to simulate Ising Model at one particular temperature in presence of magnetic field to observe hysteresis effect using the metropolis algorithm.



      While the code runs and gave me a desired output, it is a badly written code(I feel so) because of my lack of coding experience. Could you help me out as to how could I have written this in a better way? Or what can I do to optimize it next time I write such a code? Or are there any inbuilt functions I could have called instead of writing a block?



      P.S. I borrowed the random number generator directly from someone's answer to a thread on this site. I cannot find the exact thread, apologies! (I will cite it once I do)



      I hope this kind of a question is allowed on this thread. Any help or resources would be appreciated.



      //function to assign random spins to the lattice



      int spin(int r) 

      int s;
      if(r>5)

      s=+1;

      else

      s=-1;


      return s;



      ////////////////////////////////////////////////////////////////////////////



      ////////////////////////////////////////////////////////////////////////////
      //random number generator



      float prandom(int i,int N)

      std::random_device rd; //Will be used to obtain a seed for the random number engine
      std::mt19937 gen(rd()); //Standard mersenne_twister_engine seeded with rd()
      std::uniform_real_distribution<> dis(i,N);
      // Use dis to transform the random unsigned int generated by gen into a
      // double in [1, 2). Each call to dis(gen) generates a new random double
      int t = dis(gen);
      return t;



      ////////////////////////////////////////////////////////////////////////////
      //frunction to randomly flip the spins



      I am selecting a random site and seeing how the total energy will change by calculating the energy dE for the neighbouring sites. If the energy is negative then I make the spin flip permanent if it is not negative then I gave a probability exp(-dE) by which it can flip the spin



      std::vector< std::vector < int > > flip (int N,std::vector< std::vector < int > >lattice, float beta,int tab[],float H)

      int a =prandom(0,N);
      int b =prandom(0,N);
      int s=lattice[a][b];
      float dE=(2*s*H)+(2*s*(lattice[tab[a+2]][b]+lattice[tab[a]][b]+lattice[a][tab[b+2]]+lattice[a][tab[b]]));
      //std::cout<<dE<<"t"<<a<<"t"<<b<<"n";
      if(dE<0)

      s=-1*s;

      else

      float k = 1.0*prandom(0.0,1000)/1000;
      float H = exp(-beta*dE);
      if(k<=H)

      s=-1*s;

      else

      s = 1*s;


      lattice[a][b]=s;
      return lattice;



      ////////////////////////////////////////////////////////////////////////////



      // main program///////
      int main()

      std::ofstream outdata;
      outdata.open("ising_model_field_final2.txt");
      int a,b,N=20,i,j,k,r,t,sweep=1500;
      float M=0,M_sweep=0,H=-0.10;
      int tab[N];
      tab[0] = N-1;
      tab[N+1] = 0;
      for (i=1;i<=N;i++)

      tab[i]=i-1; // this is the periodic boundary condition to make my lattice infinite (lattice site [x][0] is a neighbour of [x][N] and so on..)

      float T, beta;
      //beta=1.0/T; // boltzman constant is assumed to be 1.
      //creating a 2d lattice and populating it
      std::vector< std::vector < int > >lattice;

      //populate the lattice
      for (i=0; i<N; i++)

      std::vector< int > row; //create a row of the lattice
      for (j=0;j<N;j++)

      row.push_back(-1); //populate the row vector

      lattice.push_back(row); //populate the column vector

      lattice=flip(N,lattice,beta, tab,H);
      /* for(i=0;i<N;i++)

      for(j=0;j<N;j++)

      std::cout<<lattice[j][i]<<"t";

      std::cout<<std::endl;
      */
      ///////////////////////////////////////////////////////////////////////////
      //field control
      for(int temp=1;temp<=30;temp++)

      if(temp>15)

      H=H-0.015;

      else

      H=H+0.015;

      //M=0;
      T=2.2;
      beta=1.0/T;
      ///////////////////////////////////////////////////////////////////////////
      //number of sweeps
      std::cout<<beta<<"n";
      for(i=0;i<=sweep;i++)

      //T=0.1*i;
      ///////////////////////////////////////////////////////////////////////////
      //Number of flips
      //printf("Sweep = %dn",i);
      for(j=1;j<=N*N;j++)

      lattice=flip(N,lattice,beta, tab,H);

      M_sweep=0;
      for(t=0;t<N;t++)

      for(int u=0;u<N;u++)

      if(i>=500)
      M_sweep=M_sweep+lattice[t][u];

      //std::cout<<"Mag="<<M<<"t";

      M=M+ M_sweep/(N*N);
      //std::cout<<"Mag="<<M<<"t";

      M=M/(sweep-1000);
      std::cout<<T<<"n";
      outdata << M <<"t"<< H <<"n";

      ////////////////////////////////////////////////////////////////////////////
      //printing the output of 2d lattice
      for(i=0;i<N;i++)

      for(j=0;j<N;j++)

      std::cout<<lattice[j][i]<<"t";

      std::cout<<std::endl;

      outdata.close();







      c++





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