I have a lot of points on the surface of the sphere. How can I calculate the area/spot of the sphere that has the largest point density? I need this to be done very fast. If
There is in fact no real reason to partition the sphere into a regular non-overlapping mesh, try this:
partition your sphere into semi-overlapping circles
see here for generating uniformly distributed points (your circle centers)
Dispersing n points uniformly on a sphere
you can identify the points in each circle very fast by a simple dot product..it really doesn't matter if some points are double counted, the circle with the most points still represents the highest density
this takes 12 seconds to analyze 5000 points. (and took about 10 minutes to write )
testcircles = { RandomReal[ {0, 1}, {3}] // Normalize};
Do[While[ (test = RandomReal[ {-1, 1}, {3}] // Normalize ;
Select[testcircles , #.test > .9 & , 1] ) == {} ];
AppendTo[testcircles, test];, {2000}];
vmax = testcircles[[First@
Ordering[-Table[
Count[ (testcircles[[i]].#) & /@ points , x_ /; x > .98 ] ,
{i, Length[testcircles]}], 1]]];
You can use the Peters projection, which preserves the areas.
This will allow you to efficiently count the points in a grid, but also in a sliding window (box Parzen window) by using the integral image trick.
This is really just an inverse of this answer of mine
just invert the equations of equidistant sphere surface vertexes to surface cell index. Don't even try to visualize the cell different then circle or you go mad. But if someone actually do it then please post the result here (and let me now)
Now just create 2D cell map and do the density computation in O(N)
(like histograms are done) similar to what Darren Engwirda propose in his answer
This is how the code looks like in C++
//---------------------------------------------------------------------------
const int na=16; // sphere slices
int nb[na]; // cells per slice
const int na2=na<<1;
int map[na][na2]; // surface cells
const double da=M_PI/double(na-1); // latitude angle step
double db[na]; // longitude angle step per slice
// sherical -> orthonormal
void abr2xyz(double &x,double &y,double &z,double a,double b,double R)
{
double r;
r=R*cos(a);
z=R*sin(a);
y=r*sin(b);
x=r*cos(b);
}
// sherical -> surface cell
void ab2ij(int &i,int &j,double a,double b)
{
i=double(((a+(0.5*M_PI))/da)+0.5);
if (i>=na) i=na-1;
if (i< 0) i=0;
j=double(( b /db[i])+0.5);
while (j< 0) j+=nb[i];
while (j>=nb[i]) j-=nb[i];
}
// sherical <- surface cell
void ij2ab(double &a,double &b,int i,int j)
{
if (i>=na) i=na-1;
if (i< 0) i=0;
a=-(0.5*M_PI)+(double(i)*da);
b= double(j)*db[i];
}
// init variables and clear map
void ij_init()
{
int i,j;
double a;
for (a=-0.5*M_PI,i=0;i<na;i++,a+=da)
{
nb[i]=ceil(2.0*M_PI*cos(a)/da); // compute actual circle cell count
if (nb[i]<=0) nb[i]=1;
db[i]=2.0*M_PI/double(nb[i]); // longitude angle step
if ((i==0)||(i==na-1)) { nb[i]=1; db[i]=1.0; }
for (j=0;j<na2;j++) map[i][j]=0; // clear cell map
}
}
//---------------------------------------------------------------------------
// this just draws circle from point x0,y0,z0 with normal nx,ny,nz and radius r
// need some vector stuff of mine so i did not copy the body here (it is not important)
void glCircle3D(double x0,double y0,double z0,double nx,double ny,double nz,double r,bool _fill);
//---------------------------------------------------------------------------
void analyse()
{
// n is number of points and r is just visual radius of sphere for rendering
int i,j,ii,jj,n=1000;
double x,y,z,a,b,c,cm=1.0/10.0,r=1.0;
// init
ij_init(); // init variables and map[][]
RandSeed=10; // just to have the same random points generated every frame (do not need to store them)
// generate draw and process some random surface points
for (i=0;i<n;i++)
{
a=M_PI*(Random()-0.5);
b=M_PI* Random()*2.0 ;
ab2ij(ii,jj,a,b); // cell corrds
abr2xyz(x,y,z,a,b,r); // 3D orthonormal coords
map[ii][jj]++; // update cell density
// this just draw the point (x,y,z) as line in OpenGL so you can ignore this
double w=1.1; // w-1.0 is rendered line size factor
glBegin(GL_LINES);
glColor3f(1.0,1.0,1.0); glVertex3d(x,y,z);
glColor3f(0.0,0.0,0.0); glVertex3d(w*x,w*y,w*z);
glEnd();
}
// draw cell grid (color is function of density)
for (i=0;i<na;i++)
for (j=0;j<nb[i];j++)
{
ij2ab(a,b,i,j); abr2xyz(x,y,z,a,b,r);
c=map[i][j]; c=0.1+(c*cm); if (c>1.0) c=1.0;
glColor3f(0.2,0.2,0.2); glCircle3D(x,y,z,x,y,z,0.45*da,0); // outline
glColor3f(0.1,0.1,c ); glCircle3D(x,y,z,x,y,z,0.45*da,1); // filled by bluish color the more dense the cell the more bright it is
}
}
//---------------------------------------------------------------------------
The result looks like this:
so now just see what is in the map[][]
array you can find the global/local min/max of density or whatever you need... Just do not forget that the size is map[na][nb[i]]
where i
is the first index in array. The grid size is controlled by na
constant and cm
is just density to color scale ...
[edit1] got the Quad grid which is far more accurate representation of used mapping
this is with na=16
the worst rounding errors are on poles. If you want to be precise then you can weight density by cell surface size. For all non pole cells it is simple quad. For poles its triangle fan (regular polygon)
This is the grid draw code:
// draw cell quad grid (color is function of density)
int i,j,ii,jj;
double x,y,z,a,b,c,cm=1.0/10.0,mm=0.49,r=1.0;
double dx=mm*da,dy;
for (i=1;i<na-1;i++) // ignore poles
for (j=0;j<nb[i];j++)
{
dy=mm*db[i];
ij2ab(a,b,i,j);
c=map[i][j]; c=0.1+(c*cm); if (c>1.0) c=1.0;
glColor3f(0.2,0.2,0.2);
glBegin(GL_LINE_LOOP);
abr2xyz(x,y,z,a-dx,b-dy,r); glVertex3d(x,y,z);
abr2xyz(x,y,z,a-dx,b+dy,r); glVertex3d(x,y,z);
abr2xyz(x,y,z,a+dx,b+dy,r); glVertex3d(x,y,z);
abr2xyz(x,y,z,a+dx,b-dy,r); glVertex3d(x,y,z);
glEnd();
glColor3f(0.1,0.1,c );
glBegin(GL_QUADS);
abr2xyz(x,y,z,a-dx,b-dy,r); glVertex3d(x,y,z);
abr2xyz(x,y,z,a-dx,b+dy,r); glVertex3d(x,y,z);
abr2xyz(x,y,z,a+dx,b+dy,r); glVertex3d(x,y,z);
abr2xyz(x,y,z,a+dx,b-dy,r); glVertex3d(x,y,z);
glEnd();
}
i=0; j=0; ii=i+1; dy=mm*db[ii];
ij2ab(a,b,i,j); c=map[i][j]; c=0.1+(c*cm); if (c>1.0) c=1.0;
glColor3f(0.2,0.2,0.2);
glBegin(GL_LINE_LOOP);
for (j=0;j<nb[ii];j++) { ij2ab(a,b,ii,j); abr2xyz(x,y,z,a-dx,b-dy,r); glVertex3d(x,y,z); }
glEnd();
glColor3f(0.1,0.1,c );
glBegin(GL_TRIANGLE_FAN); abr2xyz(x,y,z,a ,b ,r); glVertex3d(x,y,z);
for (j=0;j<nb[ii];j++) { ij2ab(a,b,ii,j); abr2xyz(x,y,z,a-dx,b-dy,r); glVertex3d(x,y,z); }
glEnd();
i=na-1; j=0; ii=i-1; dy=mm*db[ii];
ij2ab(a,b,i,j); c=map[i][j]; c=0.1+(c*cm); if (c>1.0) c=1.0;
glColor3f(0.2,0.2,0.2);
glBegin(GL_LINE_LOOP);
for (j=0;j<nb[ii];j++) { ij2ab(a,b,ii,j); abr2xyz(x,y,z,a-dx,b+dy,r); glVertex3d(x,y,z); }
glEnd();
glColor3f(0.1,0.1,c );
glBegin(GL_TRIANGLE_FAN); abr2xyz(x,y,z,a ,b ,r); glVertex3d(x,y,z);
for (j=0;j<nb[ii];j++) { ij2ab(a,b,ii,j); abr2xyz(x,y,z,a-dx,b+dy,r); glVertex3d(x,y,z); }
glEnd();
the mm
is the grid cell size mm=0.5
is full cell size , less creates a space between cells
Partition the sphere into equal-area regions (bounded by parallels and meridians) as described in my answer there and count the points in each region.
The aspect ratio of the regions will not be uniform (the equatorial regions will be more "squarish" when N~M
, while the polar regions will be more elongated).
This is not a problem because the diameters of the regions go to 0 as N
and M
increase.
The computational simplicity of this method trumps the better uniformity of domains in the other excellent answers which contain beautiful pictures.
One simple modification would be to add two "polar cap" regions to the N*M
regions described in the linked answer to improve the numeric stability (when the point is very close to a pole, its longitude is not well defined). This way the aspect ratio of the regions is bounded.
If I understand correctly, you are trying to find the densepoint on sphere.
if points are denser at some point
Consider Cartesian coordinates and find the mean X,Y,Z of points
Find closest point to mean X,Y,Z that is on sphere (you may consider using spherical coordinates, just extend the radius to original radius).
Constraints
I am not master of mathematics but may be it can solve by analytical way as:
1.Short the coordinate
2.R=(Σ(n=0. n=max)(Σ(m=0. M=n)(1/A^diff_in_consecative))*angle)/Σangle
A=may any constant