how to incorporate boundary conditions as constraints in fmincon optimization?
7 Ansichten (letzte 30 Tage)
Ältere Kommentare anzeigen
Saurav Parmar
am 7 Dez. 2023
Bearbeitet: Torsten
am 7 Dez. 2023
Trying to optimize the six parameters in a trial non-linear wavefunction for particle in a box to get the minimum energy. I trying to use fmincon. but i am getting an error that says - "Unrecognized function or variable 'variational_pi1DB_fun'." Somehow I am not able to incorporate non-linear constarints in the optimization problem. Can someone help me please! Pleas let me know if other methods of optimization is more helpful!
clear
clc
%defining optimization variables and an optimization problem object.
a = optimvar('a','LowerBound',30,"UpperBound",30);
b = optimvar('b','LowerBound',30,"UpperBound",30);
c = optimvar('c','LowerBound',30,"UpperBound",30);
d = optimvar('d','LowerBound',30,"UpperBound",30);
e = optimvar('e','LowerBound',30,"UpperBound",30);
f = optimvar('f','LowerBound',30,"UpperBound",30);
prob = optimproblem;
L = 5;
% w=1;
% v=1.5;
% constraints
% wavefunction zero @ x = 0 and x = L;
cons1 = double(subs(variational_pi1DB_fun,x,0)) == 0;
cons2 = double(subs(variational_pi1DB_fun,x,L)) == 0;
prob.Constraints.cons1 = cons1;
prob.Constraints.cons2 = cons2;
x0.a = -0.00006;
x0.b = -19;
x0.c = -9;
x0.d = 6;
x0.e = -0.90;
x0.f = 0.043;
%new variables
t_pi1DB = a + b*x + c*x^2 + d*x^3 + e*x^4 + f*x^5;
% equation 4.2 nominator
t_pi1DB_D1 = diff(t_pi1DB,x); % 1st derivative
t_pi1DB_D2 = diff(t_pi1DB_D1,x); % 2nd derivative
t_pi1DB_DD = ((-hbar^2)./(2*m)).*t_pi1DB_D2; % applying the hamiltonian to trial wfn Psi
t_pi1DB_c = (t_pi1DB)'; % conjugate of psi
t_pi1DB_prod = t_pi1DB_c.*t_pi1DB_DD; % multiplying the Psi* from left side
% equation 4.2 denominator
t_pi1DB_prod2 = t_pi1DB_c.*t_pi1DB; % hamiltonian not applied
% integration in nominator % ground state
probability1 = int(real(t_pi1DB_prod),x,0,L); % integrate from 0 to L
disp('probability = '),disp(probability1)
probability1 = subs(probability1,{hbar,m,L},{1,1,5}); % evaluate the probability at n = 1
disp('probability1 = '),disp(probability1)
% integration in denominator
probability2 = int(real(t_pi1DB_prod2),x,0,L);
probability2 = subs(probability2,L,5); % evaluate the probability at n = 1
disp('probability2 = '),disp(probability2)
norm_cons = sqrt(probability2);
variational_pi1DB_fun = t_pi1DB/norm_cons;
% application of equation 4.2
variational_Energy = probability1/probability2;
%objective function as an expression in the optimization variables.
P = variational_Energy;
%the objective function in prob.
prob.Objective = P;
show(prob)
sol = solve(prob,x0);
disp('sol = '),disp(sol)
3 Kommentare
Torsten
am 7 Dez. 2023
But you can't use a variable before you define it.
In the constraint section
% constraints
% wavefunction zero @ x = 0 and x = L;
cons1 = double(subs(variational_pi1DB_fun,x,0)) == 0;
cons2 = double(subs(variational_pi1DB_fun,x,L)) == 0;
variational_pi1DB_fun is not yet defined.
Akzeptierte Antwort
Torsten
am 7 Dez. 2023
Bearbeitet: Torsten
am 7 Dez. 2023
I think with the mixture of numerical, symbolic and optimization variables it is easier to set up the problem directly.
x0 = [ -0.00006; -19; -9; 6; -0.90; 0.043];
L = 5;
hbar = 1;
m = 1;
sol = fmincon(@(x)obj(x,L,hbar,m),x0,[],[],[],[],[],[],@(x)nonlcon(x,L,hbar,m))
function variational_Energy = obj(xnum,L,hbar,m)
a = xnum(1);
b = xnum(2);
c = xnum(3);
d = xnum(4);
e = xnum(5);
f = xnum(6);
syms x
%new variables
t_pi1DB = a + b*x + c*x^2 + d*x^3 + e*x^4 + f*x^5;
% equation 4.2 nominator
t_pi1DB_D1 = diff(t_pi1DB,x); % 1st derivative
t_pi1DB_D2 = diff(t_pi1DB_D1,x); % 2nd derivative
t_pi1DB_DD = ((-hbar^2)./(2*m)).*t_pi1DB_D2; % applying the hamiltonian to trial wfn Psi
t_pi1DB_c = (t_pi1DB)'; % conjugate of psi
t_pi1DB_prod = t_pi1DB_c.*t_pi1DB_DD; % multiplying the Psi* from left side
% equation 4.2 denominator
t_pi1DB_prod2 = t_pi1DB_c.*t_pi1DB; % hamiltonian not applied
% integration in nominator % ground state
probability1 = int(real(t_pi1DB_prod),x,0,L); % integrate from 0 to L
% integration in denominator
probability2 = int(real(t_pi1DB_prod2),x,0,L);
% application of equation 4.2
variational_Energy = probability1/probability2;
variational_Energy = double(variational_Energy);
end
function [C,Ceq] = nonlcon(xnum,L,hbar,m)
a = xnum(1);
b = xnum(2);
c = xnum(3);
d = xnum(4);
e = xnum(5);
f = xnum(6);
syms x
%new variables
t_pi1DB = a + b*x + c*x^2 + d*x^3 + e*x^4 + f*x^5;
t_pi1DB_c = (t_pi1DB)'; % conjugate of psi
% equation 4.2 denominator
t_pi1DB_prod2 = t_pi1DB_c.*t_pi1DB; % hamiltonian not applied
% integration in denominator
probability2 = int(real(t_pi1DB_prod2),x,0,L);
% constraints
% wavefunction zero @ x = 0 and x = L;
norm_cons = sqrt(probability2);
variational_pi1DB_fun = t_pi1DB/norm_cons;
Ceq(1) = double(subs(variational_pi1DB_fun,x,0));
Ceq(2) = double(subs(variational_pi1DB_fun,x,L));
C = [];
end
Weitere Antworten (1)
Siehe auch
Kategorien
Mehr zu Quantum Mechanics finden Sie in Help Center und File Exchange
Community Treasure Hunt
Find the treasures in MATLAB Central and discover how the community can help you!
Start Hunting!