These are ** Rheotomic Surfaces** – from the Greek

* Rheo* – flow

and

** Tomos** – cut or section (as in tomography)

The horizontal sections of these surfaces correspond to the moving equipotential lines of a 2D Laplacian flow, with height mapped to time. Such surfaces are complete, embedded and *walkably connected*.

In this essay I present a type of mathematically generated surfaces with some unique geometric properties making them particularly well suited for architectural use.

I also present some interesting by-products from the development of these surfaces including a novel and simple way of making conformal grids from flows without the usual methods of vector field integration.

Finally, I suggest some possible directions for the future development of these ideas, both in architectural and purely geometric fields.

In their 1960s work on **‘The function of the oblique’** Claude Parent and Paul Virilio proposed a new architecture of ** habitable circulation** based not on the horizontal and vertical but on the slope. They sought to remove the distinction between floorspace and vertical circulation elements such as stairs.

*‘the last element to be revealed in architecture will be the floor’. That is the key. Architecture has always been about the wall, the column, the roof… The thing that is overlooked is the floor… Architecture in this sense becomes choreographic. Its value comes only from the fact that it engages the body in the same way that the great staircases of Palladio engage the body. Somehow that is architecture.*

*…it was necessary to discard the notion of vertical enclosure, whose*

**walls are made inaccessible by gravity**, and to**define habitable space by means of wholly accessible inclined planes**, thereby**increasing the usable surface areas**.*…In contrast to partitions or vertical walls, which provoke an opposition between*

By setting the structure on an incline, and making every part of the built surface (except for the underside) habitable and accessible,

**in front**and**behind**, a combination of oblique and horizontal planes would result only in**above**and**below**, surface and soffit.By setting the structure on an incline, and making every part of the built surface (except for the underside) habitable and accessible,

**the range of truly habitable spaces would be considerably increased.**The Function of the Oblique, Claude Parent and Paul Virilio

I was inspired by the potential these ideas had for the creation of a dynamic and highly 3-dimensional architecture, but saw several problems with their application as shown in the sketches. Namely: the awkward acute spaces under some of the slopes, the large steep areas, and the lack of structural rationale. All these issues are addressed by rheotomic surfaces.

There has been a surge of curved surface and ‘single-surface’ architectural schemes over the last couple of decades. This has been partly driven by the capabilities of modern 3D softwares, but is also often tied to the theories of Deleuze about *smooth* vs. *striated* space.

There has also been a growing appreciation of the structural potential of doubly curved surfaces, as exploited by Candela’s thin concrete shells for example.

Modern knowledge of these surfaces owes a great deal to the work of the mathematical giants Riemann and Gauss. Their ideas of manifolds and curvature have fundamentally changed some of our ways of thinking about space, and play an important part in Einstein’s theories of relativity. If an architecture is to express a worldview then it seems natural to seek an architecture which embodies some of these ideas.

One area of mathematics which has advanced dramatically since the advent of computers is the study of minimal surfaces (surfaces with zero mean curvature, as approximated by soap films) .

The newfound ability to visualize these surfaces has enabled the discovery of many beautiful new examples. Their appearance can provoke a fascinating sense of solid/void dichotomy.

Images of these surfaces have naturally caught the attention of architects, and attempts to use them in the design of buildings go at least as far back as the 1970s (see Pearce and Gabriel). Minimal surfaces which form repetitive 3-dimensional structures – the Triply Periodic Minimal Surfaces(TPMS) such as the Gyroid and its associate P and D surfaces have recieved particular attention. However, attempts at an architecture based on these concepts have so far been been held back by a number of factors:

One is the daunting nature of the mathematics involved. The growing popularity of parametric modeling has meant that architects are now often quite comfortable with surfaces that can be generated from a simple function giving *x y z* in terms of *u* and *v*, but rarely when faced with something more advanced like the Weierstrass elliptic functions used in minimal surface mathematics.

Another problem is their symmetry. Most known minimal surfaces are either single inviolable entities or they are made up of endlessly repeating identical units. To be useful for architecture a geometric system needs a degree of flexibility, the ability to adapt to varied inputs.

One possible approach is to simply reject mathematical purity and take some of the techniques for working with curved surfaces and apply them in a free-form manner. But if the architect does not have real control of the tools he uses, the work is merely a collage or imitation, and without the integrity of the maths behind it, design quickly gets into difficult waters regarding structural performance and buildability.

As the great physicist Richard Feynman said:

*..”the Great Architect seems to be a mathematician”. To those who do not know mathematics it is difficult to get across a real feeling as to the beauty, the deepest beauty, of nature … Physicists cannot make a conversion to any other language. If you want to learn about nature, to appreciate nature, it is necessary to understand the language that she speaks in. She offers her information only in one form; we are not so unhumble as to demand that she change before we pay any attention.*

While it can be taxing, the benefits of using this language can be huge and often unexpected. In his famous essay on The Unreasonable Effectiveness of Mathematics in the Natural Sciences Eugene Wigner talks of the apparently miraculous way that maths sometimes seems to give more back out than we put in:

*the enormous usefulness of mathematics in the natural sciences is something bordering on the mysterious and there is no rational explanation for it. […] the mathematical formulation of the physicist’s often crude experience leads in an uncanny number of cases to an amazingly accurate description of a large class of phenomena. This shows that the mathematical language has more to commend it than being the only language which we can speak; it shows that it is, in a very real sense, the correct language.*

One area in which this unreasonable effectiveness, this magic manifests itself most strikingly is in the plane of complex numbers – created by combining the real number line with factors of * i*, the square root of minus one.

The introduction of these ‘imaginary’ quantities seems odd, even nonsensical at first, but for such a simple idea few inventions can rival it for the astonishing richness of worlds which have sprung from it and the vast range of applications it has found in mathematics, and also in descriptions of natural phenomena.

Indeed there is now hardly an area of modern physics which does not depend in some fundamental way upon the use of complex numbers.

One of the particularly elegant and beautiful places these magical numbers appear is within the world of Complex Analytic functions.

Harmonic functions are those which satisfy Laplace’s equation:

where is the Laplacian

Some elementary solutions are:

The point Source:

Velocity potential Stream function

and the Vortex:

Velocity potential Stream function

Because Laplace’s equation is linear, combinations or superpositions of these solutions are also solutions.

When I was exploring various geometric shapes during my architecture studies I started to use the technique of ** tomography** (imaging of 3D objects through sectioning, often used medically).

In particular, I found it useful to make ** tomographic animations** of objects – taking one of the 3 physical dimensions of space and mapping it to time to give a moving 2-dimensional picture which fully describes the form of the object.

This technique arose naturally when faced with the challenge of making architectural drawings of a building with no flat floors and no vertical walls. The plan is different for every small change in height so one has to show the continuous change.

Starting from a realisation that I could take helicoids and chop and mirror them to form a surface, I used these tomographic animations to develop a theory of ** walkable connectedness**.

One of the other problems with most other designs using smooth or minimal surfaces has been that although the surface is continuous, one often cannot get from one point to another on the surface without going upside-down somewhere in between.

This leads to absurdities such as these floating stairs in Toyo Ito’s Taichung Opera House…

…and holes needing rails to stop people falling down them, and generally makes the the curved surface begin to seem more like a problem than a solution.

The usefulness of the helicoid in the spiral stair is due to the fact that although it covers the same disc of horizontal space at many heights, they are connected in a ** walkable** way. This is precisely the quality which rheotomic surfaces exploit – by making an equivalence between the vortex in Laplace’s equation and the helicoid surface we can use the principle of superposition to build up any arrangement of clockwise and anti-clockwise helicoids, and join them smoothly into one continuous surface.

Simply put, two points are * walkably connected* if one can draw a curve on the surface between them along which top and bottom at never switch places.

Looked at in terms of tomographic animation, the problem of the overhangs in surfaces such as those made by joining planes with catenoids is equivalent to the movement of the contour stopping and reversing direction.

To keep the parts of the surface walkably connected, the movement of the contours must always continue to ** flow**.

*Tomographic animation of the surface shown in the flythrough at the top of the page*

Using Laplace’s equation makes it possible to generate a smooth continuous surface without ever having overhangs. At the singularites of the flow the surface turns vertical, but because this is a single point in plan, there is never an edge to fall off. The most direct route down is always on the surface.

This is also very useful ** structurally**, as it means loads can always be passed down into the surface. Indeed a rough test running these structures through an FEA structural analysis program indicated that the loads tend to get passed down towards the vertical axes of the helicoids.

Recalling the problems with the *oblique* architecture referred to at the start we can now see that they are all solved by rheotomic surfaces :

No acute spaces – The floor to ceiling height is everywhere constant.

Fewer steep areas – The average gradient becomes vanishingly small the larger the area of the surface considered (in fact the gradient at any point is inversely proportional to its horizontal distance from the axis)

Structural rationale – Development is still needed here, but initial indications are that their mathematical properties give them an intrinsically structural quality.

To summarise :

**Rheotomic surfaces combine useful and dynamic architectural form with structural performance.They do so through some of the most beautiful and profound ideas in modern mathematics.**

**They utilize advanced geometry not just as a fancy roof or a decorative pattern, but as the fundamental generator of an exciting new type of space, one which avoids many of the common pitfalls and provides a viable alternative to the flat parallel and orthogonal planes of architecture based on the Cartesian box.**

————————————–

By-products and future directions of development

**Conformal maps**

One of the advantages of pursuing a mathematical method of design is that you sometimes get to reap the benefits of its *unreasonable effectiveness*.

After realising that the streamlines and equipotentials of Harmonic flows where the answer I had been looking for in my development of these surfaces, there was a long period during which I tried to find ways of generating them.

I found various applets which could show a vector field as a grid of arrows, and some which would allow me to plot individual streamlines starting from any point. But none of the tools I found gave me the evenly spaced lines I wanted.

I developed a fascination with the strange beauty of conformal maps, with their curvilinear squares, but the only examples I could find of these were for highly regular arrangements.

So I set out to make my own tool for generating these. Using various tools and languages (such as Generative Components, Rhinoscript, Processing and Grasshopper) I looked in vain for a way to make these curves. Research suggested that I was going to have to learn about vector field integration techniques, which range from the simple but crude Euler method to the more accurate but worryingly difficult sounding 4th order Runge-Kutta method.

But then I realised that it was possible to generate the surfaces directly, which gave beautiful conformal maps ‘for free’ so to speak, from the sections of the surface.

These arrangements of mutually perpendicular curves are very interesting in their own right. Various engineers have looked at using these lines because of their ability to model the principal stresses in a structure.

In *On Growth and Form*, D’Arcy Wentworth Thompson refers to the example of Culmann’s crane, whose form was inspired by the curves in a section of trabecular bone. Also, Michell trusses – certain ‘ideal’ structures arising through a process of topological optimisation exhibit this characteristic arrangement of curved lines.

Perhaps most famously, Pier Luig Nervi used these ‘lines of force’ in the reinforcement pattern for the ceiling of his Gatti Wool Mill. Using my technique it should be possible to calculate such grids for an irregular arrangements of supports:

**Circle Packings**

I found that there also appear to be some interesting circle packings connected with these patterns.

I think some of the most interesting architectural geometry research of recent years has been in the areas of discrete minimal surfaces, PQ meshes, conical meshes, Laguerre geometry etc. Most of this work seems to be happening at TU Wien and the Geometry Group at TU Berlin.

Principal curvature lines and circle packings play an important role in some of this work and I have a hunch that my current work might relate to this in interesting ways, which I would like to explore further.

(I think there might also be a generalisation of Doyle spirals here)

**Structural performance**

Rheotomic surfaces certainly appear to have some very useful structural qualities, but it is obvious that in their pure form as described here they do not deal with loads in an ideal way, as they become asymptotically planar far from the vortices. Perhaps they could be optimised in a catenary fashion, or maybe combining sources with each vortex would help give the necessary curvature.

**Non-orientability**

One issue not addressed so far here is the way space is divided by the surface into 2 separate volumes, and the surface into 2 walkably connected areas. This is an outcome of the mathematical fact that any surface without edges or self intersections must be oriented. One simple way to deal with this might be to join the surface in parts with helicoids at half the vertical scale, thus making it non-orientable and fully walkably connected. I will provide illustrations of this shortly.

**Moving vortices**

Rheotomic surfaces are not in general minimal surfaces, as they contain vertical lines at each vortex, and any minimal surface with straight lines must be symmetric with respect to 180 degree rotation about that line. Certain arrangements are very closely related with minimal surfaces, and Matthias Weber and Martin Traizet have explored some of these in this paper

So far I have considered the vortices to be stationary, but it might be interesting to consider how they are themselves moved by the flow.

(as described here)

For example a pair of counter rotating vortices will propagate in a straight line, (which would give a surface more like Riemann’s minimal surface) and a pair of similar vortices would circle around each other (twisting the surface to become more like the helicoid with handles).

**Vortices in higher dimensions**

Instead of looking at flows caused by arrangements of singularities in 2 dimensions, I thought it would be interesting to look for equivalent 3-dimensional vortices. Instead of points, one then has lines and circles about which the space revolves. I began to explore this a bit in my post here, using stereographic projection in 4D. Things rapidly become rather confusing, with the non-commutativity of rotations, one gets into spinors and double covers. Instead of complex numbers, quaternions seem to be the natural language for such explorations.

**Harmonic Duals**

It is interesting to see how by varying one parameter we can continuously change a source into a clockwise vortex, into a sink, into an anti-clockwise vortex and back again.

Here I must refer to the beautiful book Visual Complex Analysis by Tristan Needham. This book has inspired my explorations more than any other.

Finally, I end with an observation of the visual connection with John Whitney’s *incremental drift* as shown in the Whitney Music Box

Except where otherwise noted, content on this site is licensed under an Attribution-Noncommercial-Share Alike 3.0 Creative Commons License

February 21, 2009 at 7:59 pm

[…] Boxes rotated by a Laplacian field (as I wrote more about earlier): […]

February 24, 2009 at 11:50 pm

[…] long been fascinated by this area of math/physics. For more on this, take a look at rheotomic surfaces (its a bit of a long read, but skip down to see all the pictures and […]

February 27, 2009 at 12:43 pm

Thanks for this essay. Exactly the right mix of theory and pretty pictures that makes for an interesting read. I’ll guess I’ll have to be playing with this inside Rhino sometime soon.

February 28, 2009 at 7:07 pm

this is amazing stuff – have you been able to produce Rheotomic surfaces in Grasshopper? are they available to check out?

March 14, 2009 at 5:39 pm

Hello, we are students in architecture in EPFL in Switzerland doing our master.

Your work is very interesting and we are looking for generate a kind of magnetic field like you show on the top of your post.

If you could tell us a bit more, that could be amazing.

Best regards,

RGVL_Team / EPFL

March 17, 2009 at 1:16 am

Thanks guys. These surfaces and images were produced in Grasshopper. I want to fix a couple of things before posting the definition, but will do soon

March 24, 2009 at 2:00 am

responded to a post at my site but wanted to say here also; Lines of Force have always seemed more compelling to me than the simple ‘magnetic’ disturbed grid, but the Rheotomic surface moves another step further. It is exciting to see on your blog the possibilities suggested by research rather than just exploring the geometric modeling as an end.

The connection to (extension of!) Parent’s and Virilio’s oblique is great as well.

April 1, 2009 at 12:59 pm

Hello, I got your file about MagneticField, his really good. I start to try to create line who follow the vectors, but I didn’t find a good solution. If you could help me a bit that will be great, and don’t worry this completely academic work and I will of course put your name Daniel.

Best regards,

Renaud Ganiere / EPFL

here the file I start to scratch:

http://grasshopper3d.googlegroups.com/web/Magnetic.ghx?hl=en&gda=IpbBUT4AAAC19Ve3i4OoV9kZmG4Q4msc946sW3s-ACBdfbRuMDJk1NmUVOxdYStKdo7rupEwIHzjsKXVs-X7bdXZc5buSfmx&gsc=3HsBxAsAAACUXNyyfFT295Bl3GxGpCj9

April 29, 2009 at 12:12 am

[…] Rheotomic Surfaces « Space Symmetry Structure (tags: architecture geometry math design) […]

October 18, 2009 at 1:32 pm

Hello Daniel,

Being student at the EPFL (as well as the students above), studying rheotomic surfaces and encoutering your blog, I am very interested in your joined helicoid surface. Is there a chance of getting some more specifications or maybe a model file ? Trying to understand the surface and space I would like to try make a 3D print..

Kind regards,

Sjoerd.

November 9, 2009 at 9:37 pm

is there any grasshopper file to try out ?

November 11, 2009 at 7:57 pm

Not yet, but soon

January 29, 2010 at 1:17 am

Hi Daniel,

This was a great read, it would be great to explore more – I was wondering whether you had any luck with that grasshopper definition? Would be great to play around :)

Best,

Adel

February 15, 2010 at 1:28 pm

[…] One possible approach is to simply reject mathematical purity and take some of the techniques for working with curved surfaces and apply them in a free-form manner. But if the architect does not have real control of the tools he uses, the work is merely a collage or imitation, and without the integrity of the maths behind it, design quickly gets into difficult waters regarding structural performance and buildability.” Daniel’s work is definitely inspiring to me, more of his work and research can be found on his blog. […]

June 14, 2010 at 8:51 am

What do you get if the helicoids have different periods? e.g. Im(log(z-z0)±2*log(z-z1)). Guess I’ll have to try it in Povray sometime.

November 1, 2010 at 1:31 pm

Do you have the source file in Rhino and grasshopper to study for the first images?

Thanks.

February 14, 2011 at 11:22 am

Hi,daniel,really great work, iam just wondering if you can release the GH file,right now i am studying in architecture in SCIARC, working with the scripts,really appreciate if you can send me the GH

File…thanks again …. usherhsx@gmail.com

April 7, 2011 at 8:52 am

[…] and mirroring a helicoidal surface results in a rheotomic surface, that is a walkably continuous surface connecting two levels without any discontinuity caused by […]

September 30, 2011 at 11:37 am

apple ipad future…Keep working ,great job!…

October 8, 2011 at 11:19 pm

Hi,

Daniel,really interesting work! I’ve been spending long time to try to figure the script for that too, but…

Wondering if you can release the grasshopper file to study!

Thank you!

jie

October 17, 2011 at 1:47 pm

Hi Daniel,

Thanks again for your work. It’s definitely a much more dynamic way to teach complex mathematics and has deepened my understanding of it.

I was wondering how you generate the flowlines in the first video? Is the definition available? Thanks!

January 25, 2012 at 2:16 pm

[…] I also present some interesting by-products from the development of these surfaces including a novel and simple way of making conformal grids from flows without the usual methods of vector field integration. Finally, I suggest some possible directions for the future development of these ideas, both in architectural and purely geometric fields. Rheotomic Surfaces « Space Symmetry Structure […]

June 18, 2012 at 12:37 am

I am really interested in the rheotomic surfaces, however I cannot get a grasp on the construction of Laplacian geometry – can anybody help?

I would like to give the geometry programmatic functions.

thanks in advance