Category: Topology Geometry

Regular

THE 3,10 TORUS KNOT IN ROTATION

GROWTH & UNFURLMENT OF THE 3,10 KNOT

THE 3,10 KNOT Growing, Blossoming, Fading

THREE LOOPS IN ROTATION

THE ROUND DANCE

にょろにょろへびくん結び目 by  RURU – Knot Nabi.

にょろにょろへびくん結び目 by  RURU – Knot Nabi.

nerunodaisuki:

nerunodaisuki:

Abstract Cat

Topology in 2D and 3D

Grishin Lab

Branched Minimal Surfaces:  Much of my work    on minimal…

Branched Minimal Surfaces:

 Much of my work
   on minimal surfaces has involved  branched minimal surfaces, i.e., minimal surfaces with branch points.
This page is intended to provide pictures of branch points, without
going deeply into the mathematical formulas, although the most
elementary formulas will be mentioned here.

A branch point is a point where the surface is not
parametrized in a one-to-one fashion. At that point, it doesn’t meet the
classical definition of a geometric surface, which requires that the
surface look, in the vicinity of each point, like a curved disk.
However, one is forced to consider branch points because the keep on
arising in proofs as limits of surfaces without branch points. There are
nice formulas that describe the appearance of branch points, so one can
draw pictures of them and be assured that every branch point looks like
one of these pictures. The pictures are described by two integers: the order and the index. Branch points can be interior branch points or boundary branch points. We will start with pictures of boundary branch points:
[Note: in the Safari browser, if the pictures do not rotate after they
have finished loading, use the back button and then click the link
again. They should then start rotating immediately. Other browsers do
not seem to have this problem.]

image

Order 2, Index 1.(fig. 1)

image

Order 4, Index 2. (fig. 2)

One important thing that is not obvious from the pictures is
this: the unit normal extends continuously to the branch point. That
means that all the sheets of the surface flatten out near the center and
become horizontal. In my work I am mostly concerned with a very small
neighborhood of the branch point. Then the picture is much flatter. Here
is a picture that shows a smaller neighborhood of the order 2, index 1
branch point, in which you can see how the normal tends to vertical at
the origin:

image

Order 2, Index 1, r=0.2 (fig. 3)

These are called boundary branch points because they
could occur at the boundary of a surface. In these examples, you see
only a neighborhood of the boundary, and the boundary in question is a
straight line. The pictures show parts of the x, y, and z axes as well. The next picture shows an interior branch point. Essentially, the first picture above is half of this picture.

image

Interior branch point, order 2, index 1 (fig. 4)

 A branch point of order M and index k goes “around” M + 1 times while going
     “up and down”  M + k + 1 times.   When the branch point is on the boundary, only half of
 this surface is seen.   The order of a boundary branch point must be even if the surface is
 to touch the boundary monotonically–with odd order, it would double back on itself.   Thus order 2
 is the simplest case.   Index 0  would give a piece of a plane, so index 1 is the simplest three-dimensional
 case.  Thus order 2, index 1 goes around (as an interior branch point) 3 times while going up and down 4 times;
 and as a boundary branch point, it goes around one and a half times while going up and down twice.  An
 order 4, index 2 boundary branch point goes around two and a half times while going up and down three and
 a half times.  These are the cases illustrated at the links above.    

The surfaces illustrated have simple formulas using a complex variable z.  Namely, if
  the surface is given by three functions X(z), Y(z), and Z(z),
   then we have

X+iY = zM + 1/(M+1)  

Z = Re[ zM + k + 1/(M+ k1)]

Here Re means “the real part of”.  The first formula, which does not mention the real part explicitly,
  is just a way of saying that X and Y are the real and imaginary parts, respectively, of a constant
  times zm,  so they are (up to a constant) rM+1 cos((M+1)θ) and
  rM+1 sin((M+1) θ), where r and θ are the
  polar coordinates of z.   These formulas corroborate the English descriptions above using the
  phrase “goes around” so many times.   The pictures above show the part of the surface defined over the disk |z|
  ≤ 0.6.

  Here is a good problem for the beginner at this point:  How many lines of intersection of the surface with
       itself will there be,  in a branch point of order M and index k?  
 

 Any branch point must be given by formulas that start out like those above, but there may also be terms with
   higher powers of z.   If M+1 exactly divides M+k+1 then to the first approximation, the surface will trace over
     itself exactly. (You will have noticed that if you tried to solve the exercise above.)
  If there is to be any separation of the different “sheets” of the surface, that must
 arise from higher-order terms in the formula for the surface.   You can see that in the following
 picture, which shows a boundary branch point of order 2 and index 3, so M + 1 is 3 and
 M + k + 1 is 6. Notice that at first glance the surface appears to be like a
 distorted disk–but looking carefully, you can see from the coordinate markings on the surface
 that it actually does go around one and half times, with the last half time exactly overlapping
 the first half.

image

Order 2, Index 3 A false branch point.

If the overlap is exact, as in this picture, the branch point is called a  false branch point. But bear in mind that the picture could look almost
like this, with the sheets being separated by a very tiny amount (that
might not even be visible in a computer-graphic picture) due to a term
in a high power of z. A branch point that is not false is called, naturally, a true branch point.

Here’s one last, more complicated, picture:

image

Order 4, Index 2.

hyrodium:There exists locally isometric transformation between…

hyrodium:

There exists locally isometric transformation between helicoid and catenoid.
This is because these surfaces have same Gaussian curvature at each points.

Multi-resolution method for 3D multi-material topology…

Multi-resolution method for 3D multi-material topology optimization

3D topology (In mathematics, topology  is concerned with the properties of space that are preserved under continuous deformations, such as stretching and bending, but not tearing or gluing.) optimization problems are solved with multi-material consideration. Incorporating multi-resolution scheme, this new method generates higher resolution designs in an efficient manner. Multi-material consideration bring limited complexity but also opens up new opportunities for designers and engineers as it suggests potential design alternatives that are not intuitive. []

  • J. Park, A. Sutradhar, ‘A Multi-resolution Method for 3D Multi-material Topology Optimization’, Computer Methods in Applied Mechanics and Engineering, Volume 285, 2015, Pages 571–586. (Top 25 Hottest articles, Science direct) (Impact factor 2.959)
  • J. Park, A. Sutradhar, Design of 3D microstructures of isotropic materials for targeted elastic property using topology optimization, Advances in Mechanical Engineering, 2015 (in review).
  • J. Park, A. Sutradhar , Efficient heat dissipation structures using multi-material and multi-resolution topology optimization, International Journal of Solids and Structures, 2015 (in review)