3D mesh direction detection - algorithm

I have a 3D mesh consisting of triangle polygons. My mesh can be either oriented left or right:
I'm looking for a method to detect mesh direction: right vs left.
So far I tried to use mesh centroid:
Compare centroid to bounding-box (b-box) center
See if centroid is located left of b-box center
See if centroid is located right of b-box center
But the problem is that the centroid and b-box center don't have a reliable difference in most cases.
I wonder what is a quick algorithm to detect my mesh direction.
Update
An idea proposed by #collapsar is ordering Convex Hull points in clockwise order and investigating the longest edge:
UPDATE
Another approach as suggested by #YvesDaoust is to investigate two specific regions of the mesh:

Count the vertices in two predefined regions of the bounding box. This is a fairly simple O(N) procedure.
Unless your dataset is sorted in some way, you can't be faster than O(N). But if the point density allows it, you can subsample by taking, say, every tenth point while applying the procedure.
You can as well keep your idea of the centroid, but applying it also in a subpart.

The efficiency of an algorithm to solve your problem will depend on the data structures that represent your mesh. You might need to be more specific about them in order to obtain a sufficiently performant procedure.
The algorithms are presented in an informal way. For a more rigorous analysis, math.stackexchange might be a more suitable place to ask (or another contributor is more adept to answer ...).
The algorithms are heuristic by nature. Proposals 1 and 3 will work fine for meshes whose local boundary's curvature is mostly convex locally (skipping a rigorous mathematical definition here). Proposal 2 should be less dependent on the mesh shape (and can be easily tuned to cater for ill-behaved shapes).
Proposal 1 (Convex Hull, 2D)
Let M be the set of mesh points, projected onto a 'suitable' plane as suggested by the graphics you supplied.
Compute the convex hull CH(M) of M.
Order the n points of CH(M) in clockwise order relative to any point inside CH(M) to obtain a point sequence seq(P) = (p_0, ..., p_(n-1)), with p_0 being an arbitrary element of CH(M). Note that this is usually a by-product of the convex hull computation.
Find the longest edge of the convex polygon implied by CH(M).
Specifically, find k, such that the distance d(p_k, p_((k+1) mod n)) is maximal among all d(p_i, p_((i+1) mod n)); 0 <= i < n;
Consider the vector (p_k, p_((k+1) mod n)).
If the y coordinate of its head is greater than that of its tail (ie. its projection onto the line ((0,0), (0,1)) is oriented upwards) then your mesh opens to the left, otherwise to the right.
Step 3 exploits the condition that the mesh boundary be mostly locally convex. Thus the convex hull polygon sides are basically short, with the exception of the side that spans the opening of the mesh.
Proposal 2 (bisector sampling, 2D)
Order the mesh points by their x coordinates int a sequence seq(M).
split seq(M) into 2 halves, let seq_left(M), seq_right(M) denote the partition elements.
Repeat the following steps for both point sets.
3.1. Select randomly 2 points p_0, p_1 from the point set.
3.2. Find the bisector p_01 of the line segment (p_0, p_1).
3.3. Test whether p_01 lies within the mesh.
3.4. Keep a count on failed tests.
Statistically, the mesh point subset that 'contains' the opening will produce more failures for the same given number of tests run on each partition. Alternative test criteria will work as well, eg. recording the average distance d(p_0, p_1) or the average length of (p_0, p_1) portions outside the mesh (both higher on the mesh point subset with the opening). Cut off repetition of step 3 if the difference of test results between both halves is 'sufficiently pronounced'. For ill-behaved shapes, increase the number of repetitions.
Proposal 3 (Convex Hull, 3D)
For the sake of completeness only, as your problem description suggests that the analysis effectively takes place in 2D.
Similar to Proposal 1, the computations can be performed in 3D. The convex hull of the mesh points then implies a convex polyhedron whose faces should be ordered by area. Select the face with the maximum area and compute its outward-pointing normal which indicates the direction of the opening from the perspective of the b-box center.
The computation gets more complicated if there is much variation in the side lengths of minimal bounding box of the mesh points, ie. if there is a plane in which most of the variation of mesh point coordinates occurs. In the graphics you've supplied that would be the plane in which the mesh points are rendered assuming that their coordinates do not vary much along the axis perpendicular to the plane.
The solution is to identify such a plane and project the mesh points onto it, then resort to proposal 1.

Related

How to compute the set of polygons from a set of overlapping circles?

This question is an extension on some computation details of this question.
Suppose one has a set of (potentially overlapping) circles, and one wishes to compute the area this set of circles covers. (For simplicity, one can assume some precomputation steps have been made, such as getting rid of circles included entirely in other circles, as well as that the circles induce one connected component.)
One way to do this is mentioned in Ants Aasma's and Timothy's Shields' answers, being that the area of overlapping circles is just a collection of circle slices and polygons, both of which the area is easy to compute.
The trouble I'm encountering however is the computation of these polygons. The nodes of the polygons (consisting of circle centers and "outer" intersection points) are easy enough to compute:
And at first I thought a simple algorithm of picking a random node and visiting neighbors in clockwise order would be sufficient, but this can result in the following "outer" polygon to be constructed, which is not part of the correct polygons.
So I thought of different approaches. A Breadth First Search to compute minimal cycles, but I think the previous counterexample can easily be modified so that this approach results in the "inner" polygon containing the hole (and which is thus not a correct polygon).
I was thinking of maybe running a Las Vegas style algorithm, taking random points and if said point is in an intersection of circles, try to compute the corresponding polygon. If such a polygon exists, remove circle centers and intersection points composing said polygon. Repeat until no circle centers or intersection points remain.
This would avoid ending up computing the "outer" polygon or the "inner" polygon, but would introduce new problems (outside of the potentially high running time) e.g. more than 2 circles intersecting in a single intersection point could remove said intersection point when computing one polygon, but would be necessary still for the next.
Ultimately, my question is: How to compute such polygons?
PS: As a bonus question for after having computed the polygons, how to know which angle to consider when computing the area of some circle slice, between theta and 2PI - theta?
Once we have the points of the polygons in the right order, computing the area is a not too difficult.
The way to achieve that is by exploiting planar duality. See the Wikipedia article on the doubly connected edge list representation for diagrams, but the gist is, given an oriented edge whose right face is inside a polygon, the next oriented edge in that polygon is the reverse direction of the previous oriented edge with the same head in clockwise order.
Hence we've reduced the problem to finding the oriented edges of the polygonal union and determining the correct order with respect to each head. We actually solve the latter problem first. Each intersection of disks gives rise to a quadrilateral. Let's call the centers C and D and the intersections A and B. Assume without loss of generality that the disk centered at C is not smaller than the disk centered at D. The interior angle formed by A→C←B is less than 180 degrees, so the signed area of that triangle is negative if and only if A→C precedes B→C in clockwise order around C, in turn if and only if B→D precedes A→D in clockwise order around D.
Now we determine which edges are actually polygon boundaries. For a particular disk, we have a bunch of angle intervals around its center from before (each sweeping out the clockwise sector from the first endpoint to the second). What we need amounts to a more complicated version of the common interview question of computing the union of segments. The usual sweep line algorithm that increases the cover count whenever it scans an opening endpoint and decreases the cover count whenever it scans a closing endpoint can be made to work here, with the adjustment that we need to initialize the count not to 0 but to the proper cover count of the starting angle.
There's a way to do all of this with no trigonometry, just subtraction and determinants and comparisons.

Snapping vector to a point from a grid on a sphere (icosahedron)

here is a problem that will turn your brain inside out, I'm trying to deal with it for a quite some time already.
Suppose you have sphere located in the origin of a 3d space. The sphere is segmented into a grid of equidistant points. The procedure that forms grid isn't that important but what seems simple to me is to use regular 3d computer graphics sphere generation procedure (The algorithm that forms the sphere described in the picture below)
Now, after I have such sphere (i.e. icosahedron of some degree) I need a computationally trivial procedure that will be capable to snap (an angle) of a random unit vector to it's closest icosahedron edge points. Also it is acceptable if the vector will be snapped to a center point of triangle that the vector is intersecting.
I would like to emphasise that it is important that the procedure should be computationally trivial. This means that procedures that actually create a sphere in memory and then involve a search among every triangle in sphere is not a good idea because such search will require access to global heap and ram which is slow because I need to perform this procedure millions of times on a low end mobile hardware.
The procedure should yield it's result through a set of mathematical equations based only on two values, the vector and degree of icosahedron (i.e. sphere)
Any thoughts? Thank you in advance!
============
Edit
One afterthought that just came to my mind, it seems that within diagram below step 3 (i.e. Project each new vertex to the unit sphere) is not important at all, because after bisection, projection of every vertex to a sphere would preserve all angular characteristics of a bisected shape that we are trying to snap to. So the task simplifies to identifying a bisected sub triangle coordinates that are penetrated by vector.
Make a table with 20 entries of top-level icosahedron faces coordinates - for example, build them from wiki coordinate set)
The vertices of an icosahedron centered at the origin with an
edge-length of 2 and a circumscribed sphere radius of 2 sin (2π/5) are
described by circular permutations of:
V[] = (0, ±1, ±ϕ)
where ϕ = (1 + √5)/2
is the golden ratio (also written τ).
and calculate corresponding central vectors C[] (sum of three vectors for vertices of every face).
Find the closest central vector using maximum of dot product (DP) of your vector P and all C[]. Perhaps, it is possible to reduce number of checks accounting for P components (for example if dot product of P and some V[i] is negative, there is no sense to consider faces being neighbors of V[i]). Don't sure that this elimination takes less time than direct full comparison of DP's with centers.
When big triangle face is determined, project P onto the plane of that face and get coordinates of P' in u-v (decompose AP' by AB and AC, where A,B,C are face vertices).
Multiply u,v by 2^N (degree of subdivision).
u' = u * 2^N
v' = v * 2^N
iu = Floor(u')
iv = Floor(v')
fu = Frac(u')
fv = Frac(v')
Integer part of u' is "row" of small triangle, integer part of v' is "column". Fractional parts are trilinear coordinates inside small triangle face, so we can choose the smallest value of fu, fv, 1-fu-fv to get the closest vertice. Calculate this closest vertex and normalize vector if needed.
It's not equidistant, you can see if you study this version:
It's a problem of geodesic dome frequency and some people have spent time researching all known methods to do that geometry: http://geo-dome.co.uk/article.asp?uname=domefreq, see that guy is a self labelled geodesizer :)
One page told me that the progression goes like this: 2 + 10·4N (12,42,162...)
You can simplify it down to a simple flat fractal triangle, where every triangle devides into 4 smaller triangles, and every time the subdivision is rotated 12 times around a sphere.
Logically, it is only one triangle rotated 12 times, and if you solve the code on that side, then you have the lowest computation version of the geodesic spheres.
If you don't want to keep the 12 sides as a series of arrays, and you want a lower memory version, then you can read about midpoint subdivision code, there's a lot of versions of midpoint subdivision.
I may have completely missed something. just that there isn't a true equidistant geodesic dome, because a triangle doesn't map to a sphere, only for icos.

How to fill polygon with points regularly?

It is simple to fill rectangle: simply make some grid. But if polygon is unconditioned the task becomes not so trivial.
Probably "regularly" can be formulated as distance between each other point would be: R ± alpha. But I'm not sure about this.
Maybe there is some known algorithm to achieve this.
Added:
I need to generate net, where no large holes, and no big gathering of the points.
Have you though about using a force-directed layout of the points?
Scatter a number of points randomly over the bounding box of your polygon, then repeatedly apply two simple rules to adjust their location:
If a point is outside of the polygon, move it the minimum possible distance so that it lies within, i.e.: to the closest point on the polygon edge.
Points repel each other with a force inversely proportional to the distance between them, i.e.: for every point, consider every other point and compute a repulsion vector that will move the two points directly apart. The vector should be large for proximate points and small for distant points. Sum the vectors and add to the point's position.
After a number of iterations the points should settle into a steady state with an even distribution over the polygon area. How quickly this state is achieved depends on the geometry of the polygon and how you've scaled the repulsive forces between the points.
You can compute a Constrained Delaunay triangulation of the polygon and use a Delaunay refinement algorithm (search with this keyword).
I have recently implemented refinement
in the Fade2D library, http://www.geom.at/fade2d/html/. It takes an
arbitrary polygon without selfintersections as well as an upper bound on the radius of the circumcircle of each resulting triangle. This feature is not contained in the current release 1.02 yet, but I can compile the current development version for Linux or Win64 if you want to try that.

Subdivided icosahedron - how to find the nearest vertex to an arbitrary point

I have an application that creates an approximation to sphere by subdividing an icosahedron. The Cartesian vertex coordinates are converted to spherical coordinates so that all vertices sit on the surface of a unit sphere.
What I need to do next is find the nearest vertex to an arbitrary point on the surface of the sphere. I have come up with two simple algorithms...
Brute force search - will be OK for a small number of vertices, but will be excessive for finer subdivisions.
Sorted / Indexed search - sort the vertices into some form of order by azimuth and inclination and then create a rough index to speed up a brute force search by limiting its scope.
I was wondering if there was a more subtle, and hopefully higher performing algorithm that I can use instead of one of the two above.
Update 1: I have just recalled that for another part of the application the vertices store information about their neighbours. My new algorithm is
Pick an arbitrary start vertex. Find which of its neighbours has a smaller distance to the point to locate. Use this neighbour as the new start vertex. Repeat until none of the vertex's neighbours has a smaller distance to the point. This vertex is the closest to the point.
Scanning through the responses, I think I may be off base, but what you're after is simple. I think.
Since you're dealing with just points that sit on the sphere, you can just drop a line from the vertex to the center of the sphere, drop another line from the arbitrary point to the center and solve for the angle created between them. Smaller is better. The easiest and cheapest way I think would be the dot product. The angle basically falls out of it. Here's a link about it: http://www.kynd.info/library/mathandphysics/dotProduct_01/
For testing them, I would suggest picking a vertex, testing it, then testing its neighbors. It SHOULD always be in the direction of the smallest neighbor (angle should always decrease as you get closer to the vertex you're after)
Anyhow, I hope that's what you're after.
Oh, and I came across this page while looking for your subdivision algorithm. Hard to find; if you could post a link to it I think it would help out a lot more than just myself.
One of possible solutions is to build BSP tree for vertices: http://en.wikipedia.org/wiki/Binary_space_partitioning
If the icosahedron has one vertex at the north pole and the opposite vertex at the south pole then there are 2 groups each of 5 vertices which are in planes parallel to the equator. With a little geometry I figure that these planes are at N/S 57.3056° (decimals, not dd.mmss). This divides your icosahedron into 4 latitude zones;
anything north (south) of 28.6528° is closest to the vertex at the nearer pole;
anything between the equator and north (south) 28.6528° is closer to one of the 5 vertices in that zone.
I'm working this as a navigator would, arcs measured in degrees and denoted north and south; if you prefer a more mathematical convention you can translate this all to your version of spherical coordinates quite easily.
I suspect, though I haven't coded it, that checking the distance to 5 vertices and selecting the nearest will be quicker than more sophisticated approaches based on partitioning the surface of the sphere into the projections of the faces of the icosahedron, or projecting the points on the sphere back onto the icosahedron and working the problem in that coordinate system.
For example, the approach you suggest in your update 1 will require the computation of the distance to 6 vertices (the first, arbitrarily chosen one and its 5 neighbours) at least.
It doesn't matter (if you only want to know which vertex is nearest) whether you calculate distances in Cartesian or spherical coordinates. However, calculation in Cartesian coordinates avoids a lot of calls to trigonometric functions.
If, on the other hand, you haven't arranged your icosahedron with vertices at the poles of your sphere, well, you should have !

Finding a stable placement of an irregular (non-convex) shape

Given an image of a 2-dimensional irregular (non-convex) shape, how would I able to compute all the ways in which it could lie stable on a flat surface? For example, if the shape is a perfect square rectangle, then it will surely have 4 ways in which it is stable. A circle on the other hand either has no stable orientation or every point is a stable orientation.
EDIT: There's this nice little game called Splitter (Beware, addictive game ahead) that seems close to what I want. Noticed that you cut a piece of the wood out it would fall to the ground and lay in a stable manner.
EDIT: In the end, the approach I took is to compute center of mass (of the shape) and compute the convex hull (using OpenCV), and then loop through every pair of vertices. If the center of mass falls on top of the line formed by the 2 vertices, it is deemed stable, else, no.
First find its center of mass (CM). A stable position is one in which the CM will be higher if you make a slight rotation. Now look at the hull, the smallest convex region that encloses the shape:
(source: walkytalky.net)
If the hull is a polygon, then a stable position is one in which the shape is resting on one of the sides, and the CM is directly over that side (not necessarily over the midpoint of the side, just somewhere over it.
If the hull has curves (that is, if the shape has curves which touch the hull), they must be give special treatment. The shape will be stable when resting on a curved edge iff the CM is directly above the lowest point of the curve, and the radius of the curve at that point is greater than the height of the CM.
Examples:
A rectangle. The hull is simply the rectangle, and the CM is at the center. The shape is stable on each of the four sides.
A rectangle with the sides hollowed, but the corners still intact. The hull is still the original rectangle, and the CM is close to where it used to be. All four sides of the hull are still stable (that is, you can still rest the shape on any two corners).
A circle. The CM is in the center, the hull is the circle. There are no stable positions, since the radius of the curve is always equal to the height of the CM. Give it a slight touch, and it will roll.
An ellipse. The CM is at the center, the hull is the shape. Now there are two stable positions.
A semicircle. The CM is somewhere on the axis of symmetry, the hull is the shape. Two stable positions.
A narrow semicircular crescent. The hull is a semicircle, the CM is outside the shape (but inside the hull). Two stable positions.
(source: walkytalky.net)
(The ellipse position marked with an X is unstable, because the curvature is smaller than the distance to the centre of mass.)
note: this answer assumes your shape is a proper polygon.
For our purposes, we'll define an equilibrium position as one where the Center of Mass is directly above a point that is between the leftmost and rightmost ground-contact points of the object (assuming the ground is a flat surface perpendicular to the force of gravity). This will work in all cases, for all shapes.
Note that, this is actually the physical definition of rotational equilibrium, as a consequence of Newtonian Rotational Kinematics.
For a proper polygon, if we eliminate cases where they stand on a sole vertex, this definition is equivalent to a stable position.
So, if you have a straight downward gravity, first find the left-most and right-most parts of it that are touching the ground.
Then, calculate your Center of Mass. For a polygon with known vertices and uniform density, this problem is reduced to finding the Centroid (relevant section).
Afterwards, drop a line from your CoM; if the intersection of the CoM and the ground is between those two x values, it's at equilibrium.
If your leftmost point and rightmost point match (ie, in a round object), this will still hold; just remember to be careful with your floating point comparisms.
Note that this can also be used to measure "how stable" an object is -- this measure is the maximum y-distance the Center of Mass can move before it is no longer within the range of the two contact points.
EDIT: nifty diagram made hastily
So, how can you use this to find all the ways it can sit on a table? See:
EDIT
The programmable approach
Instead of the computationally expensive task of rotating the shape, try this instead.
Your shape's representation in your program should probably have a list of all vertices.
Find the vertices of your shape's convex hull (basically, your shape, but with all concave vertices -- vertices that are "pushed in" -- eliminated).
Then Iterate through each of pair of adjacent vertices on your convex hull (ie, if I had vertices A, B, C, D, I'd iterate through AB, BC, CD, DA)
Do this test:
Draw a line A through the two vertices being tested
Draw a line perpendicular to A, going through CoM C.
Find the intersection of the two lines (simple algebra)
If the intersection's y value is in between the y value of the two vertices, it stable. If the y values are all equal, compare the x values.
That should do the trick.
Here is an example of the test being running on one pair of vertices:
If your shape is not represented by its vertices in your data structure, then you should try to convert them. If it's something like a circle or an ellipse, you may use heuristics to guess the answer (a circle has infinite equilibrium positions; an ellipse 4, albeit only two "stable" points). If it's a curved wobbly irregular shape, you're going to have to supply your data structure for me be able to help in a program-related way, instead of just providing case-by-case heuristics.
I'm sure this is not the most efficient algorithm, but it's an idea.
If you can order the verticles of the polygon (assuming it has a finite number of vertices), then just iterate over adjacent pairs of vertices and record the angle it rests at through some form of simulation. There will be duplicate orientations for it to sit on in the case of weird shapes, like stars, but you can accomodate for that by keeping track of the resting rotation.

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