Assume we have a 3D grid that spans some 3D space. This grid is made out of cubes, the cubes need not have integer length, they can have any possible floating point length.
Our goal is, given a point and a direction, to check linearly each cube in our path once and exactly once.
So if this was just a regular 3D array and the direction is say in the X direction, starting at position (1,2,0) the algorithm would be:
for(i in number of cubes)
{
grid[1+i][2][0]
}
But of course the origin and the direction are arbitrary and floating point numbers, so it's not as easy as iterating through only one dimension of a 3D array. And the fact the side lengths of the cubes are also arbitrary floats makes it slightly harder as well.
Assume that your cube side lengths are s = (sx, sy, sz), your ray direction is d = (dx, dy, dz), and your starting point is p = (px, py, pz). Then, the ray that you want to traverse is r(t) = p + t * d, where t is an arbitrary positive number.
Let's focus on a single dimension. If you are currently at the lower boundary of a cube, then the step length dt that you need to make on your ray in order to get to the upper boundary of the cube is: dt = s / d. And we can calculate this step length for each of the three dimensions, i.e. dt is also a 3D vector.
Now, the idea is as follows: Find the cell where the ray's starting point lies in and find the parameter values t where the first intersection with the grid occurs per dimension. Then, you can incrementally find the parameter values where you switch from one cube to the next for each dimension. Sort the changes by the respective t value and just iterate.
Some more details:
cell = floor(p - gridLowerBound) / s <-- the / is component-wise division
I will only cover the case where the direction is positive. There are some minor changes if you go in the negative direction but I am sure that you can do these.
Find the first intersections per dimension (nextIntersection is a 3D vector):
nextIntersection = ((cell + (1, 1, 1)) * s - p) / d
And calculate the step length:
dt = s / d
Now, just iterate:
if(nextIntersection.x < nextIntersection.y && nextIntersection.x < nextIntersection.z)
cell.x++
nextIntersection.x += dt.x
else if(nextIntersection.y < nextIntersection.z)
cell.y++
nextIntersection.y += dt.y
else
cell.z++
nextIntersection.z += dt.z
end if
if cell is outside of grid
terminate
I have omitted the case where two or three cells are changed at the same time. The above code will only change one at a time. If you need this, feel free to adapt the code accordingly.
Well if you are working with floats, you can make the equation for the line in direction specifiedd. Which is parameterized by t. Because in between any two floats there is a finite number of points, you can simply check each of these points which cube they are in easily cause you have point (x,y,z) whose components should be in, a respective interval defining a cube.
The issue gets a little bit harder if you consider intervals that are, dense.
The key here is even with floats this is a discrete problem of searching. The fact that the equation of a line between any two points is a discrete set of points means you merely need to check them all to the cube intervals. What's better is there is a symmetry (a line) allowing you to enumerate each point easily with arithmetic expression, one after another for checking.
Also perhaps consider integer case first as it is same but slightly simpler in determining the discrete points as it is a line in Z_2^8?
Related
Given a list of points forming a polygonal line, and both height and width of a rectangle, how can I find the number and positions of all rectangles needed to cover all the points?
The rectangles should be rotated and may overlap, but must follow the path of the polyline (A rectangle may contain multiple segments of the line, but each rectangle must contain a segment that is contiguous with the previous one.)
Do the intersections on the smallest side of the rectangle, when it is possible, would be much appreciated.
All the solutions I found so far were not clean, here is the result I get:
You should see that it gives a good render in near-flat cases, but overlaps too much in big curbs. One rectangle could clearly be removed if the previous were offset.
Actually, I put a rectangle centered at width/2 along the line and rotate it using convex hull and modified rotating calipers algorithms, and reiterate starting at the intersection point of the previous rectangle and the line.
You may observe that I took inspiration from the minimum oriented rectangle bounding box algorithm, for the orientation, but it doesn't include the cutting aspect, nor the fixed size.
Thanks for your help!
I modified k-means to solve this. It's not fast, it's not optimal, it's not guaranteed, but (IMHO) it's a good start.
There are two important modifications:
1- The distance measure
I used a Chebyshev-distance-inspired measure to see how far points are from each rectangle. To find distance from points to each rectangle, first I transformed all points to a new coordinate system, shifted to center of rectangle and rotated to its direction:
Then I used these transformed points to calculate distance:
d = max(2*abs(X)/w, 2*abs(Y)/h);
It will give equal values for all points that have same distance from each side of rectangle. The result will be less than 1.0 for points that lie inside rectangle. Now we can classify points to their closest rectangle.
2- Strategy for updating cluster centers
Each cluster center is a combination of C, center of rectangle, and a, its rotation angle. At each iteration, new set of points are assigned to a cluster. Here we have to find C and a so that rectangle covers maximum possible number of points. I don’t now if there is an analytical solution for that, but I used a statistical approach. I updated the C using weighted average of points, and used direction of first principal component of points to update a. I used results of proposed distance, powered by 500, as weight of each point in weighted average. It moves rectangle towards points that are located outside of it.
How to Find K
Initiate it with 1 and increase it till all distances from points to their corresponding rectangles become less than 1.0, meaning all points are inside a rectangle.
The results
Iterations 0, 10, 20, 30, 40, and 50 of updating cluster centers (rectangles):
Solution for test case 1:
Trying Ks: 2, 4, 6, 8, 10, and 12 for complete coverage:
Solution for test case 2:
P.M: I used parts of Chalous Road as data. It was fun downloading it from Google Maps. The I used technique described here to sample a set of equally spaced points.
It’s a little late and you’ve probably figured this out. But, I was free today and worked on the constraint reflected in your last edit (continuity of segments). As I said before in the comments, I suggest using a greedy algorithm. It’s composed of two parts:
A search algorithm that looks for furthermost point from an initial point (I used binary search algorithm), so that all points between them lie inside a rectangle of given w and h.
A repeated loop that finds best rectangle at each step and advances the initial point.
The pseudo code of them are like these respectively:
function getBestMBR( P, iFirst, w, h )
nP = length(P);
iStart = iFirst;
iEnd = nP;
while iStart <= iEnd
m = floor((iStart + iEnd) / 2);
MBR = getMBR(P[iFirst->m]);
if (MBR.w < w) & (MBR.h < h) {*}
iStart = m + 1;
iLast = m;
bestMBR = MBR;
else
iEnd = m - 1;
end
end
return bestMBR, iLast;
end
function getRectList( P, w, h )
nP = length(P);
rects = [];
iFirst = 1;
iLast = iFirst;
while iLast < nP
[bestMBR, iLast] = getBestMBR(P, iFirst, w, h);
rects.add(bestMBR.x, bestMBR.y, bestMBR.a];
iFirst = iLast;
end
return rects;
Solution for test case 1:
Solution for test case 2:
Just keep in mind that it’s not meant to find the optimal solution, but finds a sub-optimal one in a reasonable time. It’s greedy after all.
Another point is that you can improve this a little in order to decrease number of rectangles. As you can see in the line marked with (*), I kept resulting rectangle in direction of MBR (Minimum Bounding Rectangle), even though you can cover larger MBRs with rectangles of same w and h if you rotate the rectangle. (1) (2)
For example, in a 2D space, with x [0 ; 1] and y [0 ; 1]. For p = 4, intuitively, I will place each point at each corner of the square.
But what can be the general algorithm?
Edit: The algorithm needs modification if dimensions are not orthogonal to eachother
To uniformly place the points as described in your example you could do something like this:
var combinedSize = 0
for each dimension d in d0..dn {
combinedSize += d.length;
}
val listOfDistancesBetweenPointsAlongEachDimension = new List
for each d dimension d0..dn {
val percentageOfWholeDimensionSize = d.length/combinedSize
val pointsToPlaceAlongThisDimension = percentageOfWholeDimensionSize * numberOfPoints
listOfDistancesBetweenPointsAlongEachDimension[d.index] = d.length/(pointsToPlaceAlongThisDimension - 1)
}
Run on your example it gives:
combinedSize = 2
percentageOfWholeDimensionSize = 1 / 2
pointsToPlaceAlongThisDimension = 0.5 * 4
listOfDistancesBetweenPointsAlongEachDimension[0] = 1 / (2 - 1)
listOfDistancesBetweenPointsAlongEachDimension[1] = 1 / (2 - 1)
note: The minus 1 deals with the inclusive interval, allowing points at both endpoints of the dimension
2D case
In 2D (n=2) the solution is to place your p points evenly on some circle. If you want also to define the distance d between points then the circle should have radius around:
2*Pi*r = ~p*d
r = ~(p*d)/(2*Pi)
To be more precise you should use circumference of regular p-point polygon instead of circle circumference (I am too lazy to do that). Or you can compute the distance of produced points and scale up/down as needed instead.
So each point p(i) can be defined as:
p(i).x = r*cos((i*2.0*Pi)/p)
p(i).y = r*sin((i*2.0*Pi)/p)
3D case
Just use sphere instead of circle.
ND case
Use ND hypersphere instead of circle.
So your question boils down to place p "equidistant" points to a n-D hypersphere (either surface or volume). As you can see 2D case is simple, but in 3D this starts to be a problem. See:
Make a sphere with equidistant vertices
sphere subdivision triangulation
As you can see there are quite a few approaches to do this (there are much more of them even using Fibonacci sequence generated spiral) which are more or less hard to grasp or implement.
However If you want to generalize this into ND space you need to chose general approach. I would try to do something like this:
Place p uniformly distributed place inside bounding hypersphere
each point should have position,velocity and acceleration vectors. You can also place the points randomly (just ensure none are at the same position)...
For each p compute acceleration
each p should retract any other point (opposite of gravity).
update position
just do a Newton D'Alembert physics simulation in ND. Do not forget to include some dampening of speed so the simulation will stop in time. Bound the position and speed to the sphere so points will not cross it's border nor they would reflect the speed inwards.
loop #2 until max speed of any p crosses some threshold
This will more or less accurately place p points on the circumference of ND hypersphere. So you got minimal distance d between them. If you got some special dependency between n and p then there might be better configurations then this but for arbitrary numbers I think this approach should be safe enough.
Now by modifying #2 rules you can achieve 2 different outcomes. One filling hypersphere surface (by placing massive negative mass into center of surface) and second filling its volume. For these two options also the radius will be different. For one you need to use surface and for the other volume...
Here example of similar simulation used to solve a geometry problem:
How to implement a constraint solver for 2-D geometry?
Here preview of 3D surface case:
The number on top is the max abs speed of particles used to determine the simulations stopped and the white-ish lines are speed vectors. You need to carefully select the acceleration and dampening coefficients so the simulation is fast ...
Given a bunch of arbitrary vectors (stored in a matrix A) and a radius r, I'd like to find all integer-valued linear combinations of those vectors which land inside a sphere of radius r. The necessary coordinates I would then store in a Matrix V. So, for instance, if the linear combination
K=[0; 1; 0]
lands inside my sphere, i.e. something like
if norm(A*K) <= r then
V(:,1)=K
end
etc.
The vectors in A are sure to be the simplest possible basis for the given lattice and the largest vector will have length 1. Not sure if that restricts the vectors in any useful way but I suspect it might. - They won't have as similar directions as a less ideal basis would have.
I tried a few approaches already but none of them seem particularly satisfying. I can't seem to find a nice pattern to traverse the lattice.
My current approach involves starting in the middle (i.e. with the linear combination of all 0s) and go through the necessary coordinates one by one. It involves storing a bunch of extra vectors to keep track of, so I can go through all the octants (in the 3D case) of the coordinates and find them one by one. This implementation seems awfully complex and not very flexible (in particular it doesn't seem to be easily generalizable to arbitrary numbers of dimension - although that isn't strictly necessary for the current purpose, it'd be a nice-to-have)
Is there a nice* way to find all the required points?
(*Ideally both efficient and elegant**. If REALLY necessary, it wouldn't matter THAT much to have a few extra points outside the sphere but preferably not that many more. I definitely do need all the vectors inside the sphere. - if it makes a large difference, I'm most interested in the 3D case.
**I'm pretty sure my current implementation is neither.)
Similar questions I found:
Find all points in sphere of radius r around arbitrary coordinate - this is actually a much more general case than what I'm looking for. I am only dealing with periodic lattices and my sphere is always centered at 0, coinciding with one point on the lattice.
But I don't have a list of points but rather a matrix of vectors with which I can generate all the points.
How to efficiently enumerate all points of sphere in n-dimensional grid - the case for a completely regular hypercubic lattice and the Manhattan-distance. I'm looking for completely arbitary lattices and euclidean distance (or, for efficiency purposes, obviously the square of that).
Offhand, without proving any assertions, I think that 1) if the set of vectors is not of maximal rank then the number of solutions is infinite; 2) if the set is of maximal rank, then the image of the linear transformation generated by the vectors is a subspace (e.g., plane) of the target space, which intersects the sphere in a lower-dimensional sphere; 3) it follows that you can reduce the problem to a 1-1 linear transformation (kxk matrix on a k-dimensional space); 4) since the matrix is invertible, you can "pull back" the sphere to an ellipsoid in the space containing the lattice points, and as a bonus you get a nice geometric description of the ellipsoid (principal axis theorem); 5) your problem now becomes exactly one of determining the lattice points inside the ellipsoid.
The latter problem is related to an old problem (counting the lattice points inside an ellipse) which was considered by Gauss, who derived a good approximation. Determining the lattice points inside an ellipse(oid) is probably not such a tidy problem, but it probably can be reduced one dimension at a time (the cross-section of an ellipsoid and a plane is another ellipsoid).
I found a method that makes me a lot happier for now. There may still be possible improvements, so if you have a better method, or find an error in this code, definitely please share. Though here is what I have for now: (all written in SciLab)
Step 1: Figure out the maximal ranges as defined by a bounding n-parallelotope aligned with the axes of the lattice vectors. Thanks for ElKamina's vague suggestion as well as this reply to another of my questions over on math.se by chappers: https://math.stackexchange.com/a/1230160/49989
function I=findMaxComponents(A,r) //given a matrix A of lattice basis vectors
//and a sphere radius r,
//find the corners of the bounding parallelotope
//built from the lattice, and store it in I.
[dims,vecs]=size(A); //figure out how many vectors there are in A (and, unnecessarily, how long they are)
U=eye(vecs,vecs); //builds matching unit matrix
iATA=pinv(A'*A); //finds the (pseudo-)inverse of A^T A
iAT=pinv(A'); //finds the (pseudo-)inverse of A^T
I=[]; //initializes I as an empty vector
for i=1:vecs //for each lattice vector,
t=r*(iATA*U(:,i))/norm(iAT*U(:,i)) //find the maximum component such that
//it fits in the bounding n-parallelotope
//of a (n-1)-sphere of radius r
I=[I,t(i)]; //and append it to I
end
I=[-I;I]; //also append the minima (by symmetry, the negative maxima)
endfunction
In my question I only asked for a general basis, i.e, for n dimensions, a set of n arbitrary but linearly independent vectors. The above code, by virtue of using the pseudo-inverse, works for matrices of arbitrary shapes and, similarly, Scilab's "A'" returns the conjugate transpose rather than just the transpose of A so it equally should work for complex matrices.
In the last step I put the corresponding minimal components.
For one such A as an example, this gives me the following in Scilab's console:
A =
0.9701425 - 0.2425356 0.
0.2425356 0.4850713 0.7276069
0.2425356 0.7276069 - 0.2425356
r=3;
I=findMaxComponents(A,r)
I =
- 2.9494438 - 3.4186986 - 4.0826424
2.9494438 3.4186986 4.0826424
I=int(I)
I =
- 2. - 3. - 4.
2. 3. 4.
The values found by findMaxComponents are the largest possible coefficients of each lattice vector such that a linear combination with that coefficient exists which still land on the sphere. Since I'm looking for the largest such combinations with integer coefficients, I can safely drop the part after the decimal point to get the maximal plausible integer ranges. So for the given matrix A, I'll have to go from -2 to 2 in the first component, from -3 to 3 in the second and from -4 to 4 in the third and I'm sure to land on all the points inside the sphere (plus superfluous extra points, but importantly definitely every valid point inside) Next up:
Step 2: using the above information, generate all the candidate combinations.
function K=findAllCombinations(I) //takes a matrix of the form produced by
//findMaxComponents() and returns a matrix
//which lists all the integer linear combinations
//in the respective ranges.
v=I(1,:); //starting from the minimal vector
K=[];
next=1; //keeps track of what component to advance next
changed=%F; //keeps track of whether to add the vector to the output
while or(v~=I(2,:)) //as long as not all components of v match all components of the maximum vector
if v <= I(2,:) then //if each current component is smaller than each largest possible component
if ~changed then
K=[K;v]; //store the vector and
end
v(next)=v(next)+1; //advance the component by 1
next=1; //also reset next to 1
changed=%F;
else
v(1:next)=I(1,1:next); //reset all components smaller than or equal to the current one and
next=next+1; //advance the next larger component next time
changed=%T;
end
end
K=[K;I(2,:)]'; //while loop ends a single iteration early so add the maximal vector too
//also transpose K to fit better with the other functions
endfunction
So now that I have that, all that remains is to check whether a given combination actually does lie inside or outside the sphere. All I gotta do for that is:
Step 3: Filter the combinations to find the actually valid lattice points
function points=generatePoints(A,K,r)
possiblePoints=A*K; //explicitly generates all the possible points
points=[];
for i=possiblePoints
if i'*i<=r*r then //filter those that are too far from the origin
points=[points i];
end
end
endfunction
And I get all the combinations that actually do fit inside the sphere of radius r.
For the above example, the output is rather long: Of originally 315 possible points for a sphere of radius 3 I get 163 remaining points.
The first 4 are: (each column is one)
- 0.2425356 0.2425356 1.2126781 - 0.9701425
- 2.4253563 - 2.6678919 - 2.4253563 - 2.4253563
1.6977494 0. 0.2425356 0.4850713
so the remainder of the work is optimization. Presumably some of those loops could be made faster and especially as the number of dimensions goes up, I have to generate an awful lot of points which I have to discard, so maybe there is a better way than taking the bounding n-parallelotope of the n-1-sphere as a starting point.
Let us just represent K as X.
The problem can be represented as:
(a11x1 + a12x2..)^2 + (a21x1 + a22x2..)^2 ... < r^2
(x1,x2,...) will not form a sphere.
This can be done with recursion on dimension--pick a lattice hyperplane direction and index all such hyperplanes that intersect the r-radius ball. The ball intersection of each such hyperplane itself is a ball, in one lower dimension. Repeat. Here's the calling function code in Octave:
function lat_points(lat_bas_mx,rr)
% **globals for hyperplane lattice point recursive function**
clear global; % this seems necessary/important between runs of this function
global MLB;
global NN_hat;
global NN_len;
global INP; % matrix of interior points, each point(vector) a column vector
global ctr; % integer counter, for keeping track of lattice point vectors added
% in the pre-allocated INP matrix; will finish iteration with actual # of points found
ctr = 0; % counts number of ball-interior lattice points found
MLB = lat_bas_mx;
ndim = size(MLB)(1);
% **create hyperplane normal vectors for recursion step**
% given full-rank lattice basis matrix MLB (each vector in lattice basis a column),
% form set of normal vectors between successive, nested lattice hyperplanes;
% store them as columnar unit normal vectors in NN_hat matrix and their lengths in NN_len vector
NN_hat = [];
for jj=1:ndim-1
tmp_mx = MLB(:,jj+1:ndim);
tmp_mx = [NN_hat(:,1:jj-1),tmp_mx];
NN_hat(:,jj) = null(tmp_mx'); % null space of transpose = orthogonal to columns
tmp_len = norm(NN_hat(:,jj));
NN_hat(:,jj) = NN_hat(:,jj)/tmp_len;
NN_len(jj) = dot(MLB(:,jj),NN_hat(:,jj));
if (NN_len(jj)<0) % NN_hat(:,jj) and MLB(:,jj) must have positive dot product
% for cutting hyperplane indexing to work correctly
NN_hat(:,jj) = -NN_hat(:,jj);
NN_len(jj) = -NN_len(jj);
endif
endfor
NN_len(ndim) = norm(MLB(:,ndim));
NN_hat(:,ndim) = MLB(:,ndim)/NN_len(ndim); % the lowest recursion level normal
% is just the last lattice basis vector
% **estimate number of interior lattice points, and pre-allocate memory for INP**
vol_ppl = prod(NN_len); % the volume of the ndim dimensional lattice paralellepiped
% is just the product of the NN_len's (they amount to the nested altitudes
% of hyperplane "paralellepipeds")
vol_bll = exp( (ndim/2)*log(pi) + ndim*log(rr) - gammaln(ndim/2+1) ); % volume of ndim ball, radius rr
est_num_pts = ceil(vol_bll/vol_ppl); % estimated number of lattice points in the ball
err_fac = 1.1; % error factor for memory pre-allocation--assume max of err_fac*est_num_pts columns required in INP
INP = zeros(ndim,ceil(err_fac*est_num_pts));
% **call the (recursive) function**
% for output, global variable INP (matrix of interior points)
% stores each valid lattice point (as a column vector)
clp = zeros(ndim,1); % confirmed lattice point (start at origin)
bpt = zeros(ndim,1); % point at center of ball (initially, at origin)
rd = 1; % initial recursion depth must always be 1
hyp_fun(clp,bpt,rr,ndim,rd);
printf("%i lattice points found\n",ctr);
INP = INP(:,1:ctr); % trim excess zeros from pre-allocation (if any)
endfunction
Regarding the NN_len(jj)*NN_hat(:,jj) vectors--they can be viewed as successive (nested) altitudes in the ndim-dimensional "parallelepiped" formed by the vectors in the lattice basis, MLB. The volume of the lattice basis parallelepiped is just prod(NN_len)--for a quick estimate of the number of interior lattice points, divide the volume of the ndim-ball of radius rr by prod(NN_len). Here's the recursive function code:
function hyp_fun(clp,bpt,rr,ndim,rd)
%{
clp = the lattice point we're entering this lattice hyperplane with
bpt = location of center of ball in this hyperplane
rr = radius of ball
rd = recrusion depth--from 1 to ndim
%}
global MLB;
global NN_hat;
global NN_len;
global INP;
global ctr;
% hyperplane intersection detection step
nml_hat = NN_hat(:,rd);
nh_comp = dot(clp-bpt,nml_hat);
ix_hi = floor((rr-nh_comp)/NN_len(rd));
ix_lo = ceil((-rr-nh_comp)/NN_len(rd));
if (ix_hi<ix_lo)
return % no hyperplane intersections detected w/ ball;
% get out of this recursion level
endif
hp_ix = [ix_lo:ix_hi]; % indices are created wrt the received reference point
hp_ln = length(hp_ix);
% loop through detected hyperplanes (updated)
if (rd<ndim)
bpt_new_mx = bpt*ones(1,hp_ln) + NN_len(rd)*nml_hat*hp_ix; % an ndim by length(hp_ix) matrix
clp_new_mx = clp*ones(1,hp_ln) + MLB(:,rd)*hp_ix; % an ndim by length(hp_ix) matrix
dd_vec = nh_comp + NN_len(rd)*hp_ix; % a length(hp_ix) row vector
rr_new_vec = sqrt(rr^2-dd_vec.^2);
for jj=1:hp_ln
hyp_fun(clp_new_mx(:,jj),bpt_new_mx(:,jj),rr_new_vec(jj),ndim,rd+1);
endfor
else % rd=ndim--so at deepest level of recursion; record the points on the given 1-dim
% "lattice line" that are inside the ball
INP(:,ctr+1:ctr+hp_ln) = clp + MLB(:,rd)*hp_ix;
ctr += hp_ln;
return
endif
endfunction
This has some Octave-y/Matlab-y things in it, but most should be easily understandable; M(:,jj) references column jj of matrix M; the tic ' means take transpose; [A B] concatenates matrices A and B; A=[] declares an empty matrix.
Updated / better optimized from original answer:
"vectorized" the code in the recursive function, to avoid most "for" loops (those slowed it down a factor of ~10; the code now is a bit more difficult to understand though)
pre-allocated memory for the INP matrix-of-interior points (this speeded it up by another order of magnitude; before that, Octave was having to resize the INP matrix for every call to the innermost recursion level--for large matrices/arrays that can really slow things down)
Because this routine was part of a project, I also coded it in Python. From informal testing, the Python version is another 2-3 times faster than this (Octave) version.
For reference, here is the old, much slower code in the original posting of this answer:
% (OLD slower code, using for loops, and constantly resizing
% the INP matrix) loop through detected hyperplanes
if (rd<ndim)
for jj=1:length(hp_ix)
bpt_new = bpt + hp_ix(jj)*NN_len(rd)*nml_hat;
clp_new = clp + hp_ix(jj)*MLB(:,rd);
dd = nh_comp + hp_ix(jj)*NN_len(rd);
rr_new = sqrt(rr^2-dd^2);
hyp_fun(clp_new,bpt_new,rr_new,ndim,rd+1);
endfor
else % rd=ndim--so at deepest level of recursion; record the points on the given 1-dim
% "lattice line" that are inside the ball
for jj=1:length(hp_ix)
clp_new = clp + hp_ix(jj)*MLB(:,rd);
INP = [INP clp_new];
endfor
return
endif
I have a list of points moving in two dimensions (x- and y-axis) represented as rows in an array. I might have N points - i.e., N rows:
1 t1 x1 y1
2 t2 x2 y2
.
.
.
N tN xN yN
where ti, xi, and yi, is the time-index, x-coordinate, and the y-coordinate for point i. The time index-index ti is an integer from 1 to T. The number of points at each such possible time index can vary from 0 to N (still with only N points in total).
My goal is the filter out all the points that do not move in a certain way; or to keep only those that do. A point must move in a parabolic trajectory - with decreasing x- and y-coordinate (i.e., moving to the left and downwards only). Points with other dynamic behaviour must be removed.
Can I use a simple sorting mechanism on this array - and then analyse the order of the time-index? I have also considered the fact each point having the same time-index ti are physically distinct points, and so should be paired up with other points. The complexity of the problem grew - and now I turn to you.
NOTE: You can assume that the points are confined to a sub-region of the (x,y)-plane between two parabolic curves. These curves intersect only at only at one point: A point close to the origin of motion for any point.
More Information:
I have made some datafiles available:
MATLAB datafile (1.17 kB)
same data as CSV with semicolon as column separator (2.77 kB)
Necessary context:
The datafile hold one uint32 array with 176 rows and 5 columns. The columns are:
pixel x-coordinate in 175-by-175 lattice
pixel y-coordinate in 175-by-175 lattice
discrete theta angle-index
time index (from 1 to T = 10)
row index for this original sorting
The points "live" in a 175-by-175 pixel-lattice - and again inside the upper quadrant of a circle with radius 175. The points travel on the circle circumference in a counterclockwise rotation to a certain angle theta with horizontal, where they are thrown off into something close to a parabolic orbit. Column 3 holds a discrete index into a list with indices 1 to 45 from 0 to 90 degress (one index thus spans 2 degrees). The theta-angle was originally deduces solely from the points by setting up the trivial equations of motions and solving for the angle. This gives rise to a quasi-symmetric quartic which can be solved in close-form. The actual metric radius of the circle is 0.2 m and the pixel coordinate were converted from pixel-coordinate to metric using simple linear interpolation (but what we see here are the points in original pixel-space).
My problem is that some points are not behaving properly and since I need to statistics on the theta angle, I need to remove the points that certainly do NOT move in a parabolic trajoctory. These error are expected and fully natural, but still need to be filtered out.
MATLAB plot code:
% load data and setup variables:
load mat_points.mat;
num_r = 175;
num_T = 10;
num_gridN = 20;
% begin plotting:
figure(1000);
clf;
plot( ...
num_r * cos(0:0.1:pi/2), ...
num_r * sin(0:0.1:pi/2), ...
'Color', 'k', ...
'LineWidth', 2 ...
);
axis equal;
xlim([0 num_r]);
ylim([0 num_r]);
hold all;
% setup grid (yea... went crazy with one):
vec_tickValues = linspace(0, num_r, num_gridN);
cell_tickLabels = repmat({''}, size(vec_tickValues));
cell_tickLabels{1} = sprintf('%u', vec_tickValues(1));
cell_tickLabels{end} = sprintf('%u', vec_tickValues(end));
set(gca, 'XTick', vec_tickValues);
set(gca, 'XTickLabel', cell_tickLabels);
set(gca, 'YTick', vec_tickValues);
set(gca, 'YTickLabel', cell_tickLabels);
set(gca, 'GridLineStyle', '-');
grid on;
% plot points per timeindex (with increasing brightness):
vec_grayIndex = linspace(0,0.9,num_T);
for num_kt = 1:num_T
vec_xCoords = mat_points((mat_points(:,4) == num_kt), 1);
vec_yCoords = mat_points((mat_points(:,4) == num_kt), 2);
plot(vec_xCoords, vec_yCoords, 'o', ...
'MarkerEdgeColor', 'k', ...
'MarkerFaceColor', vec_grayIndex(num_kt) * ones(1,3) ...
);
end
Thanks :)
Why, it looks almost as if you're simulating a radar tracking debris from the collision of two missiles...
Anyway, let's coin a new term: object. Objects are moving along parabolae and at certain times they may emit flashes that appear as points. There are also other points which we are trying to filter out.
We will need some more information:
Can we assume that the objects obey the physics of things falling under gravity?
Must every object emit a point at every timestep during its lifetime?
Speaking of lifetime, do all objects begin at the same time? Can some expire before others?
How precise is the data? Is it exact? Is there a measure of error? To put it another way, do we understand how poorly the points from an object might fit a perfect parabola?
Sort the data with (index,time) as keys and for all locations of a point i see if they follow parabolic trajectory?
Which part are you facing problem? Sorting should be very easy. IMHO, it is the second part (testing if a set of points follow parabolic trajectory) that is difficult.
Generally we traverse the array by row or column but here I want to traverse it in an angle.
I will try and explain what I mean,
So lets say if the angle is 45 degree then rather than row by col it would search as (0,0) then (0,1) (1,0) then (0,2) , (1,1) ,(2,0) and so on.. .(sorry could not upload an image as I am new user and not allowed to do so, may be try and imagine/draw an array that would help get what I am trying to say)
But what will happen if the user inputs an angle like 20 degree how can we determine how to search the array.
i just wanted to know if there is any algorithm which does something similar to this? Programming language is not an issue i guess the issue is more of algoritham sort.
Any ideas would be welcome.
Please feel free to ask if I am not able to explain clearly what I am looking for.
Thanks guys.
Easy. Take an angle (let's say 45). This corresponds to a vector v=(1, 1) in your case. (This can be normalized to a unitary vector (sqrt(2)/2, sqrt(2)/2), but this is not necessary)
For every single point in your array, you have their coordinates (x, y). Simply do the scalar product of these coordinates with the vector. Let's call f(x, y) = scalarProduct((x, y), v)
Sort the values of f(x, y) and you've got the "traversing" you're looking for!
A real example.
Your matrix is 3x3
The scalar products are :
(0,0).(1,1) = 0
(0,1).(1,1) = 1
(0,2).(1,1) = 2
(1,0).(1,1) = 1
(1,1).(1,1) = 2
(1,2).(1,1) = 3
(2,0).(1,1) = 2
(2,1).(1,1) = 3
(2,2).(1,1) = 4
If you order these scalar products by ascending order, you obtain the ordering (0,0), (1,0), (1,0), (2,0), (1,1), (0,2), (2,1)...
And if you want to do it with the angle 20, replace all occurences of v=(1, 1) with v=(cos(20), sin(20))
Here's an illustration of a geometrical interpretation. The scalar products correspond to the intersections of the vector v (in red) with the blue lines.
For every starting point (the leftmost point of every row), use trigonometry to determine an ending point for the given angle. The tan(angle) is defined as (height difference / width of the array), so your height differece is tan(angle)*(witdh of the array). You only have to calculate the height difference once. If y+height difference is greater than the height of the array, just subtract the height (or use the modulo operator).
Now that you have a starting point and an ending point you could use Bresenham's Algorithm to determine the points in between: http://en.wikipedia.org/wiki/Bresenham%27s_line_algorithm
You want to look for a space-filling-curve for example a morton curve or z-curve. If you want to subdivide the array in 4 tiles you may want to look for a hilbert curve or a moore curve.