# Tune Particle Swarm Optimization Process

This example shows how to optimize using the `particleswarm`

solver. The particle swarm algorithm moves a population of particles called a swarm toward a minimum of an objective function. The velocity of each particle in the swarm changes according to three factors:

The effect of inertia (

`InertiaRange`

option)An attraction to the best location the particle has visited (

`SelfAdjustmentWeight`

option)An attraction to the best location among neighboring particles (

`SocialAdjustmentWeight`

option)

This example shows some effects of changing particle swarm options.

### When to Modify Options

Often, `particleswarm`

finds a good solution when using its default options. For example, it optimizes `rastriginsfcn`

well with the default options. This function has many local minima, and a global minimum of `0`

at the point `[0,0]`

.

rng default % for reproducibility [x,fval,exitflag,output] = particleswarm(@rastriginsfcn,2);

Optimization ended: relative change in the objective value over the last OPTIONS.MaxStallIterations iterations is less than OPTIONS.FunctionTolerance.

```
formatstring = 'particleswarm reached the value %f using %d function evaluations.\n';
fprintf(formatstring,fval,output.funccount)
```

particleswarm reached the value 0.000000 using 2560 function evaluations.

For this function, you know the optimal objective value, so you know that the solver found it. But what if you do not know the solution? One way to evaluate the solution quality is to rerun the solver.

[x,fval,exitflag,output] = particleswarm(@rastriginsfcn,2);

Optimization ended: relative change in the objective value over the last OPTIONS.MaxStallIterations iterations is less than OPTIONS.FunctionTolerance.

fprintf(formatstring,fval,output.funccount)

particleswarm reached the value 0.000000 using 1480 function evaluations.

Both the solution and the number of function evaluations are similar to the previous run. This suggests that the solver is not having difficulty arriving at a solution.

### Difficult Objective Function Using Default Parameters

The Rosenbrock function is well known to be a difficult function to optimize. This example uses a multidimensional version of the Rosenbrock function. The function has a minimum value of `0`

at the point `[1,1,1,...]`

.

rng default % for reproducibility nvars = 6; % choose any even value for nvars fun = @multirosenbrock; [x,fval,exitflag,output] = particleswarm(fun,nvars);

Optimization ended: relative change in the objective value over the last OPTIONS.MaxStallIterations iterations is less than OPTIONS.FunctionTolerance.

fprintf(formatstring,fval,output.funccount)

particleswarm reached the value 3106.436648 using 12960 function evaluations.

The solver did not find a very good solution.

### Bound the Search Space

Try bounding the space to help the solver locate a good point.

lb = -10*ones(1,nvars); ub = -lb; [xbounded,fvalbounded,exitflagbounded,outputbounded] = particleswarm(fun,nvars,lb,ub);

fprintf(formatstring,fvalbounded,outputbounded.funccount)

particleswarm reached the value 0.000006 using 71160 function evaluations.

The solver found a much better solution. But it took a very large number of function evaluations to do so.

### Change Options

Perhaps the solver would converge faster if it paid more attention to the best neighbor in the entire space, rather than some smaller neighborhood.

options = optimoptions('particleswarm','MinNeighborsFraction',1); [xn,fvaln,exitflagn,outputn] = particleswarm(fun,nvars,lb,ub,options);

fprintf(formatstring,fvaln,outputn.funccount)

particleswarm reached the value 0.000462 using 30180 function evaluations.

While the solver took fewer function evaluations, it is unclear if this was due to randomness or to a better option setting.

Perhaps you should raise the `SelfAdjustmentWeight`

option.

options.SelfAdjustmentWeight = 1.9; [xn2,fvaln2,exitflagn2,outputn2] = particleswarm(fun,nvars,lb,ub,options);

fprintf(formatstring,fvaln2,outputn2.funccount)

particleswarm reached the value 0.000074 using 18780 function evaluations.

This time `particleswarm`

took even fewer function evaluations. Is this improvement due to randomness, or are the option settings really worthwhile? Rerun the solver and look at the number of function evaluations.

[xn3,fvaln3,exitflagn3,outputn3] = particleswarm(fun,nvars,lb,ub,options);

fprintf(formatstring,fvaln3,outputn3.funccount)

particleswarm reached the value 0.157026 using 53040 function evaluations.

This time the number of function evaluations increased. Apparently, this `SelfAdjustmentWeight`

setting does not necessarily improve performance.

### Provide an Initial Point

Perhaps `particleswarm`

would do better if it started from a known point that is not too far from the solution. Try the origin. Give a few individuals at the same initial point. Their random velocities ensure that they do not remain together.

x0 = zeros(20,6); % set 20 individuals as row vectors options.InitialSwarmMatrix = x0; % the rest of the swarm is random [xn3,fvaln3,exitflagn3,outputn3] = particleswarm(fun,nvars,lb,ub,options);

fprintf(formatstring,fvaln3,outputn3.funccount)

particleswarm reached the value 0.039015 using 32100 function evaluations.

The number of function evaluations decreased again.

### Vectorize for Speed

The `multirosenbrock`

function allows for vectorized function evaluation. This means that it can simultaneously evaluate the objective function for all particles in the swarm. This usually speeds up the solver considerably.

rng default % do a fair comparison options.UseVectorized = true; tic [xv,fvalv,exitflagv,outputv] = particleswarm(fun,nvars,lb,ub,options);

toc

Elapsed time is 0.152962 seconds.

```
options.UseVectorized = false;
rng default
tic
[xnv,fvalnv,exitflagnv,outputnv] = particleswarm(fun,nvars,lb,ub,options);
```

toc

Elapsed time is 0.421945 seconds.

The vectorized calculation took about half the time of the serial calculation.

### Plot Function

You can view the progress of the solver using a plot function.

options = optimoptions(options,'PlotFcn',@pswplotbestf); rng default [x,fval,exitflag,output] = particleswarm(fun,nvars,lb,ub,options);

fprintf(formatstring,fval,output.funccount)

particleswarm reached the value 0.079755 using 24960 function evaluations.

### Use More Particles

Frequently, using more particles obtains a more accurate solution.

```
rng default
options.SwarmSize = 200;
[x,fval,exitflag,output] = particleswarm(fun,nvars,lb,ub,options);
```

fprintf(formatstring,fval,output.funccount)

particleswarm reached the value 0.000424 using 169400 function evaluations.

### Hybrid Function

`particleswarm`

can search through several basins of attraction to arrive at a good local solution. Sometimes, though, it does not arrive at a sufficiently accurate local minimum. Try improving the final answer by specifying a hybrid function that runs after the particle swarm algorithm stops. Reset the number of particles to their original value, 60, to see the difference the hybrid function makes.

```
rng default
options.HybridFcn = @fmincon;
options.SwarmSize = 60;
[x,fval,exitflag,output] = particleswarm(fun,nvars,lb,ub,options);
```

fprintf(formatstring,fval,output.funccount)

particleswarm reached the value 0.000000 using 25191 function evaluations.

disp(output.hybridflag)

1

While the hybrid function improved the result, the plot function shows the same final value as before. This is because the plot function shows only the particle swarm algorithm iterations, and not the hybrid function calculations. The hybrid function caused the final function value to be very close to the true minimum value of 0. The `output.hybridflag`

field shows that `fmincon`

stops with exit flag 1, indicating that `x`

is a true local minimum.