Metaballs


In computer graphics, metaballs are organic-looking n-dimensional isosurfaces, characterised by their ability to meld together when in close proximity to create single, contiguous objects. This "blobby" appearance makes them versatile tools, often used to model organic objects and also to create base meshes for sculpting. The technique for rendering metaballs was invented by Jim Blinn in the early 1980s to model atom interactions for Carl Sagan's 1980 TV series .

Definition

Each metaball is defined as a function in n dimensions. A thresholding value is also chosen, to define a solid volume. Then,
represents whether the volume enclosed by the surface defined by metaballs is filled at or not.

Implementation

A typical function chosen for metaballs is the inverse-square law, that is the contribution to the thresholding function falls off in a bell as the distance from the centre of the metaball increases.
For the three dimensional case, where
is the center of the metaball. However, due to the division, it is computationally expensive. For this reason, approximate polynomial functions are typically used.
When seeking a more efficient falloff function, several qualities are desired:
The simplest falloff curve that satisfies these criteria is, where r is the distance to the point. This formulation avoids expensive square root calls.
More complicated models use a Gaussian potential constrained to a finite radius or a mixture of polynomials to achieve smoothness. The Soft Object model by the Wyvill brothers provides higher degree of smoothness and still avoids square roots.
A simple generalization of metaballs is to apply the falloff curve to distance-from-lines or distance-from-surfaces.
There are a number of ways to render the metaballs to the screen. In the case of three dimensional metaballs, the two most common are brute force raycasting and the marching cubes algorithm.
2D metaballs were a very common demo effect in the 1990s. The effect is also available as an XScreensaver module.