ne – power of the many è un corso advanced level che studia la produzione di effetti complessi a partire dalla modellazione di comportamenti semplici su un insieme strutturato con un numero alto di elementi. Attraverso un approccio generico e scaleless sarà possibile affrontare la tematica generale su più fronti e in una molteplicità di declinazioni possibili. Il corso è rivolto a chi,indipendentemente dal proprio background (urbanistica, architettura, ingegneria, design, arte o altro) già possiede una esperienza di base con Rhinoceros e Grasshopper, e desidera sviluppare aspetti di gestione avanzata del flusso di articolato di informazioni attraverso una strategia guidata basata su esempi pratici e sull’implementazione di un progetto personale sul tema generale del “field behaviour”. Sarà trattato anche l’utilizzo di alcuni plug-ins quali gHowl e WeaverBird. Il numero dei partecipanti è fissato a un massimo di 20 per offrire un tutoraggio proficuo ed una effettiva esperienza di learning ad ogni iscritto.
[.] Temi:
teoria
. complessità, emergence, effetti di campo (field behaviour), sensibilità, efficienza multiperformance
tecnica
. dati:gestione e manipolazione avanzata del data tree, streaming e visualizzazione; transizione, blending e modulazione delle geometrie; generazione e controllo multiperformance di popolazioni di componenti; attrattori, drivers e tecniche di modulazione avanzate; uso delle mesh con WeaverBird; ottimizzazione con Galapagos
[.] Dettagli :
Tutors: Alessio Erioli + Andrea Graziano – Co-de-iT
Si richiede esperienza di base nella modellazione in Rhino (equivalente a Rhino training Level 1, il Level 2 è gradito – la documentazione per il training è disponibile gratuitamente all’indirizzo: http://download.rhino3d.com/download.asp?id=Rhino4Training&language=it) e nell’uso di Grasshopper (la suddivisione di una superficie NURBS in componenti tramite isotrim è data come base assodata)
. luogo:
IreCoop – via Vasco De Gama 27 _ Firenze
. durata:
25-27 febbraio 2010 – 3 giornate consecutive _ orario 9:00 – 18:00
. costo:
professionisti – 450.00 € studenti – 280.00 €
. note:
scadenza iscrizioni: 20 febbraio 2010 il corso sarà attivato con un numero minimo di 15 iscritti al termine sarà rilasciato un attestato di frequenza gli iscritti dovrano venire muniti dei propri laptop con software installato. una versione free per 30 giorni è disponibile sul sito www.rhino3d.com
. contatti:
iscrizioni + info alloggi: www.irecooptoscana.it (Cosa offriamo > formazione > altri corsi)
info sul corso: info@co-de-it.com…
noceros 3D, en caso de aprobar satisfactoriamente el examen, se les otorga un reconocimiento avalado por el CMJ y la Secretaría del Trabajo. Este workshop va dirigido principalmente a estudiantes de arquitectura; sin embargo, ya que la parametrización es una herramienta que abarca diferentes ámbitos del diseño, se pueden integrar estudiantes de diseño industrial, artistas o estudiantes que tengan relación con lo gráfico y lo formal. Al finalizar el curso, los asistentes serán capaces de manejar Rhinoceros y Grasshopper en un nivel medio, con el objetivo de que el alumno pueda continuar aprendiendo con alguno de nuestros workshops subsiguientes o de manera autodidacta.
Las personas inscritas deben tener conocimientos básicos de geometría y de preferencia utilizar algún programa de dibujo en 2D o modelación en 3d. Rhino.GetMe Rigid // Enfocado a construir un objeto de diseño parametrizado a cualquier escala, el workshop se divide en tres módulos: Módulo 1 // Rhinoceros 3D // Una sesión de cinco horas. Módulo 2 //Grasshopper // Una sesión de cinco horas. Módulo 3 // Ejercicios prácticos /Tres sesiones de diez horas c/u. Es necesario traer el equipo necesario para trabajar, se cuenta con equipos en caso de que algún alumno no cuente con laptop pero son limitados, por favor avísanos a la brevedad si lo requieres. Se les recomienda que traigan dispositivos de almacenamiento en caso de que necesitemos compartir información.
El costo del Workshop es de $6500.00 para profesionales y $5000 pesos para estudiantes.
Pre-venta únicamente para estudiantes, hasta el día viernes 29 de junio, con un costo de $3500.00 pesos.
El cupo del evento es limitado puedes apartar tu lugar y terminar de liquidar antes del 29 de junio en pre-venta, antes del 6 de junio en admisión general.
Para hacer tu registro al workshop por favor envía un correo a workshop@transformalab.com incluyendo:
Nombre
Universidad u oficina de procedencia
Teléfono móvil
En el caso de estudiantes por favor incluyan una copia escaneada de su Constancia de Estudios para hacer válido su descuento.
Una vez recibida su información se les enviará un correo con la información necesaria para realizar su pago mediante depósito bancario, y posteriormente un mail de confirmación de su participación en el Workshop.
www.transformalab.com…
ust assume this is really what is being imported with the standard import line I see in all the examples:
# scriptcontext moduleimport RhinoPython.Host as __host'''The Active Rhino document (Rhino.RhinoDoc in RhinoCommon) while a scriptis executing. This variable is set by Rhino before the exection of every script.'''doc = None'''Identifies how the script is currently executing1 = running as standard python script2 = running inside grasshopper component3... potential other locations where script could be running'''id = 1'''A dictionary of values that can be reused between execution of scripts'''sticky = dict()def escape_test( throw_exception=True, reset=False ): "Tests to see if the user has pressed the escape key" rc = __host.EscapePressed(reset) if rc and throw_exception: raise Exception('escape key pressed') return rc def errorhandler(): ''' The default error handler called by functions in the rhinoscript package. If you want to have your own predefined function called instead of errorhandler, replace the scriptcontext.errorhandler value ''' return None…
Added by Nik Willmore at 7:47pm on October 10, 2015
ave pointed out, if the older version of Honeybee EPZone does not have the recirculatedAirPerArea proprety, then it must be the cause of the error as I am using the Honeybee_Export to OpenStudio component (VER 0.0.58 Nov_07_2015). Given the discrepancy between the version of the Honeybee components used to setup everything in the file all the way prior to the point feeding the zones' data into the Export to Open Studio component, I can see different options/questions to tackle this issue:
1- I have the OpenStudio 1.9.0 that works with EnergyPlusV8-3-0 installed on my computer and the reason that I had to use the newer version of the Honeybee_Export to OpenStudio component (VER 0.0.58 Nov_07_2015) is that I had initially received an error message using the component of the same version as consistent with the rest of the project (VER 0.0.57 Jul_15_2015) with the following content:
"Cannot find OpenStudio libraries. You can download the libraries from the link below. Unzip the file and copy it to C:\Users\Alireza\AppData\Roaming\Ladybug\OpenStudio and try again. Click on the link to copy the address.https://app.box.com/s/y2sx16k98g1lfd3r47zi"
The download link provided in the error message appears to be not active and thereby, I could not follow the instructions on the error message and make the Hoenybee_Export to OpenStudio component (VER 0.0.57 Jul_15_2015) work.
Therefore, if there is a way to make this version (VER 0.0.57 Jul_15_2015) of the Hoenybee_Export to OpenStudio component work by downloading the OpenStudio libraries or switching to a legacy version of the OpenStudio application prior to 1-9-0, then probably this would be one option to solve this issue.
2- When I realized I could not download the OpenStudio libraries as described in section 1 (see above) and make the Honeybee_Export to OpenStudio Component (VER 0.0.57 Jul_15_2015) work with the installed OpenStudio application (V1-9-0), I updated the entire installation of Ladybug + Honeybee User Object files to the new version (Ladybug_0_0_61 and Honeybee_0_0_58). This time the Honeybee_Export to OpenStudio component (VER 0.0.58 Nov_07_2015) seemed to be working with the installed OpenStudio application (V1-9-0) as I did not receive any error messages about missing OS libraries. However, I could not make things work since all other components in my project (eg. Creat HB Zones,Creat HB Surface) have been setup with the 0.0.57 version and obviously, the updated version of the Honeybee User Objects (V0.0.58) could not recognize my HB component of the previous version in the file.
If there is a way to make 'in-place' updates of HB components, for example updating the Honeybee_Create HB Zones in the file without having to re-wire everything from scratch, then it probably would work as the updated version will include the 'recirculatedAirPerArea' property. Otherwise, given the complexity of the scene, it appears to be impossible for me to start everything from scratch and setup the entire scene with the new version of HB components.
3- If none of the options in the last two sections (see above) would be possible, I was wondering if there is a way to open the zones' data as the outcome of the Honeybee_Solve Adjacency component (prior to feeding this data to the Honeybee_Open Studio Systems component and subsequently, to the the Hoenybee_Export to Open Studio) in a text-editor and manually add the missing recirculatedAirPerArea property to the zones' data; then probably I could do that and then eventually feed it to the Hoenybee_Export to Open Studio component.
These are the three options that I could think of in order to tackle this issue of mine. I apologize for the extended reply but I figured it would be better to give a more comprehensive description of my problem and previous attempts to solve it.
Any helps is most appreciated.
Please let me know if you need further information about the described issues in each section or the simulation scene setup in general.
Thank you,
Alireza
…
er). With the command "End Bulge" I noticed that G2 moves perpendicular to G1! But with an increase which is not equal... and is different, every time, depending on the angle between G0 and G1 and G2. How do I predict the position of G2 compared to G1 simulating the "End Bulge" command? Thank you for your professional answers.
^___^
Below you can see an example with a curve crimson ... If I move G1 of 1 unit G2 moves of 0.42 units (perpendicular) .. If I move of 2 units the next step is 0.46 unit... 3 units --> step 0,50 units... etc.
And each time changes depending on the initial conditions (G0/G1/G2 angle).
…
Added by Lucius Santo at 4:21pm on September 20, 2012
.com/forum/topics/use-pythoneditor-to-run?commentId=2985220%3AComment%3A138538
For now I am considering a simple test case in which a set of sliders are added together into a GH_number component called "output":
I am finding that from the Rhino Python Editor it is definitely possible to change the slider values and retrieve results in a loop. Below I copied the code that runs from the Rhino Python Editor, where I simply change the slider value of the slider with Nickname "Number Slider1" from 0 to 2. (note that grasshopper and the testfile are already open in this example)
This script prints out the following results as expected:
Slider value: 0.0Result value: 1.154Slider value: 1.0Result value: 2.154Slider value: 2.0Result value: 3.154
However using the exact same code in a GHPython component within Grasshopper the Grasshopper Python Script Editor's console reads:
Slider value: 2.0Result value: 3.154Slider value: 2.0Result value: 3.154Slider value: 2.0Result value: 3.154
It seems that the solver doesn't recompute during each iteration but just retrieves the final state of my script.
So basically I have been trying to trigger a 'runsolver' command inside my loop. I tried using the methods available trough the RhinoScript interface, as David describes here.
http://www.grasshopper3d.com/forum/topics/open-a-gh-automatically
I could create a loop looking like this:
But running this in the Grasshopper Component crashes Rhino. I have also tried this by Disabling the solver first using the DisableSolver() method. This does disable the solver but still Rhino crashes. Also I used the ExpireSolution(True) method on the slider object like:
However in this case I don't get any different results.
So I guess my question is simple:
Is there a way to recompute the solver after a slider change inside a GHPython script component during a loop?
Any suggestions, or references would be greatly appreciated!
(FYI: I am using Rhino5x64 and Grasshopper Version 0.9.0014, attached is the script I used both in the Rhino Python Editor and the GHPython component and the grasshopper file)…
y using the Honeybee_Update Honeybee component.
The video below (best viewed in full-screen mode) provides an idea of what these components are capable of being used for:
The video below shows how these components can be used in an existing Honeybee project (for additional links please open this video in youtube):
I have uploaded two examples as Hydra files that show how these components can be used for grid-point and image-based simulations:
Example1 : Grid Point Calculations
Example2: Image based simulation
Finally, a more esoteric application is demonstrated in this video:
These components are still in the beta-testing stage. Some of the limitations of the components are:
1. Only Type C photometry IES files are supported at present.
2. Rhino is likely to get sluggish if there are too many luminaires (i.e. light fixtures) present in a scene.
3. Due to the spectral limitations of the ray-tracing software (RADIANCE), simulations involving color mixing might not be physically realizable.
Additional details about photometric and spectral calculations are probably an overkill for this forum. However, I'd be glad to answer any related questions. Please report any bugs or request new features either on this forum or on Github.
Mostapha, Leland Curtis, Reinhardt Swart and Dr. Richard Mistrick provided valuable inputs during the development of these components.
Thanks,
Sarith
Update 16th January 2017:
An example with some new components and bug fixes since the initial release announcement can be found here
…
or GH with: 1. Animation Timeline 2. Rendering 3. API
Summary:
Animation Timeline: Smooth animation system that plays at the real-world speed; so you know the robot will run just right when you upload the code.
Rendering: Extensive options and outputs; so you can generate amazing videos.
API: Access our functions through Python and C# scripting; so you can manage parameters and actions for complex processes for each target.
More info:
Animation Timeline:
Build an animation from a list of Planes, it's that easy! Get these from points, curves or surfaces. Download the example files with the trial and test it yourself.
The unique Timeline component displays all the important robot warnings and the digital Input/Ouput:
RED – clash detection BLUE - singularities YELLOW – over rotation ORANGE – out of reach Digital Inut/Output: red=off, green=on
Rendering:
IO smoothly interpolates between all the Planes you set. This means you can generate keyframes for positions between Planes too e.g. you have two planes defining a tool path, IO can generate 2000 keyframes. Smooooth!
Rendered in full colour as standard, not GH red :-)
LiveBaking - let's you use Rhino render settings in real-time (can be a bit slow!)
Slider animation - use the native 'Animate' option to export hi-res images and create videos easily. Just set the number of frames you need (hint: divide total time in seconds by the frames-per-second rate)
Bake unlimited meshes as keyframes for export to render-pipelines in 3DS etc.
API
Accessing the IO functions through Python and C# let's you build more powerful definitions. You can assign data to every position the robot reaches, allowing you to control speed, acceleration, wait-times, actions and more. Examples comparing C# with Python are included in the examples files.
You can also use teh API build your own plugins that use the IO timeline to do all the hard work like IK and creating valid code, while you enjoy developing your new process...
Check out the website for more features and videos of the example definitions: www.robots.io
Download the PDF guide: 150314_IO_Primer_v1.pdf.
See www.robots.io for more info and pricing.
Developed by RoboFold Ltd. Used by leading academics, researchers and professionals.
…
Added by Gregory Epps at 10:15am on November 7, 2014
ndard length elements without any cutting, and using only simple connections, such as cable ties or scaffold swivel couplers.
To summarize the approach I present here:
Design an initial shape
Remesh this form so that the edges are all roughly the length of the tubes we will use to build the structure
Rotate and extend the edges of this mesh to create the crossings
Apply a relaxation to optimize the positions of the tubes for tangency
demo_reciprocal_structures.gh
Initial form
In this example I show how to apply this system to a simple sphere. You can replace this with any arbitrary shape. It can be open or closed, and have any topology.
Remeshing
The new ReMesher component takes an input mesh, and a target edge length, and iteratively flips/splits/collapses edges in order to achieve a triangulated mesh of roughly equal edge lengths.
Press the Reset button to initialize, then hold down the F5 key on your keyboard to run several iterations until it has stabilized. (F5 just recomputes the solution, and this can be a quick alternative to using a timer)
Once the remeshing is complete, bake the result into Rhino and reference it into the next part of the definition (I recommend doing this rather than connecting it directly, so that you don't accidentally alter the mesh and recompute everything downstream later).
Alternatively you can create your mesh manually, or using other techniques.
Rotate and Extend
We generate the crossings using an approach similar to that described by Tomohiro Tachi for tensegrity structures here:
http://www.tsg.ne.jp/TT/cg/FreeformTensegrityTachiAAG2012.pdf
Using the 'Reciprocal' component found in the Kangaroo mesh tab, each edge is rotated about an axis through its midpoint and normal to the surface, then extended slightly so that they cross over.
By changing the angle you can change whether the fans are triangular or hexagonal, and clockwise or counter-clockwise.
Choose values for the angle and scaling so that the lines extend beyond where they cross, but not so far that they clash with the other edges.
Note that each rod has 4 crossings with its surrounding rods.
There are multiple possibilities for the over/under pattern at each 'fan', and which one is used affects the curvature:
A nice effect of creating the pre-optimization geometry by rotating and extending mesh edges in this way is that the correct over/under pattern for each fan gets generated automatically.
Optimization for tangency
We now have an approximate reciprocal structure, where the lines are the centrelines of our rods, but the distances between them where they cross vary, so we would not actually be able to easily connect the rods in this configuration.
To attach the rods to form a structure, we want them to be tangent to one another. A pair of cylinders is tangent if the shortest line between their centrelines is equal to the sum of their radii:
Achieving tangency between all crossed rods in the structure is a tricky problem - if we move any one pair of rods to be tangent, we usually break the tangency between other pairs, and because there are many closed loops, we cannot simply start with one and solve them in order.
Therefore we use a dynamic relaxation approach, where forces are used to solve all the tangency constraints simultaneously, and over a number of iterations it converges to a solution where they are all met. The latest Kangaroo includes a line-line force, which can be used to pull and push pairs of lines so that they are a certain distance apart. Each rod is treated as a rigid body, so forces applied along its length will cause it to move and rotate.
The reciprocal component uses Plankton to find the indices of which lines in the list cross, which are then fed into the force for Kangaroo. We also use springs to keep each line the same length.
If the input is good, when we run the relaxation (by double clicking Kangaroo and pressing play), the rods should move only a little. We can see whether tangency has been achieved by looking at the shortest distance between the centerlines of the crossing rods. When this is twice the rod radius, they are tangent. Wait for it to solve to the desired degree of accuracy (there's no need to wait for 1000ths of a millimeter), and then press pause on the Kangaroo controller and bake the result.
The radius you choose for the pipes, curvature of the form and length of the edges all affect the result, and at this stage you may need to tweak these input values to get a final result you are happy with. If you find the rods are not reaching a stable solution but are sliding completely off each other, you might want to try adding weak AnchorSprings to the endpoints of the lines, to keep them from drifting too far from their original positions.
For previewing the geometry during relaxation I have used the handy Mesh Pipe component from Mateusz Zwierzycki, as it is much faster than using actual surface pipes.
To actually build this, you then need to extract the distances along each rod at which the crossings occur, and whether it crosses over or under, mark the rods accordingly, and assemble (If there is interest I will also clean up and post the definition for extracting this information). While this technique doesn't require much equipment, it does need good coordination and numbering!
There is also a ReciprocalStructure user object component that can be found in the Kangaroo utilities tab, which attempts to apply steps 3 and 4 automatically. However, by using the full definition you have more control and possibility to troubleshoot if any part isn't working.
The approach described here was first tested and refined at the 2013 Salerno Structural Geometry workshop, lead by Gennaro Senatore and myself, where we built a small pavilion using this technique with PVC tubes and cable ties. Big thanks to all the participants!
Finally - this is all very experimental work, and there are still many unanswered questions, and a lot of scope for further development of such structures. I think in particular - which of the relative degrees of freedom between pairs of rods are constrained by the connection (sliding along their length, bending, and twisting) and how this affects the structural behaviour would be interesting to examine further.
Steps 3 and 4 of the approach presented above would also work with quad meshes, which would have different stability characteristics.
There is also the issue of deformation of the rods - as the procedure described here solves only the geometric question of how to make perfectly rigid straight cylinders tangent. The approach could potentially be extended to adjust for, or make use of the flexibility of the rods.
I hope this is useful to somebody. Please let me know if you do have a go at building something using this.
Any further discussion on these topics is welcome!
Further reading on reciprocal structures:
http://vbn.aau.dk/files/65339229/Three_dimensional_Reciprocal_Structures_Morphology_Concepts_Generative_Rules.pdf
http://www3.ntu.edu.sg/home/cwfu/papers/recipframe/
http://albertopugnale.wordpress.com/2013/04/05/form-finding-of-reciprocal-structures-with-grasshopper-and-galapagos/
…
option, after downloading check if .ghuser files are blocked (right click -> "Properties" and select "Unblock"). Then paste them in File->Special Folders->User Object Folder. You can download the example files from here. They act in similar way, Ladybug Photovoltaics components do: we pick a surface, and get an answer to a question: "How much thermal energy, for a certain number of persons can my roof, building facade... generate if I would populate them with Solar Water Heating collectors"? This information can then be used to cover domestic hot water, space heating or space cooling loads:
Components enable setting specific details of the system, or using simplified ones. They cover analysis of domestic hot water load, final performance of the SWH system, its embodied energy, energy value, consumption, emissions... And finding optimal system and storage size. By Dr. Chengchu Yan and Djordje Spasic, with invaluable support of Dr. Willian Beckman, Dr. Jason M. Keith, Jeff Maguire, Nicolas DiOrio, Niraj Palsule, Sargon George Ishaya and Craig Christensen. Hope you will enjoy using the components! References: 1) Calculation of delivered energy: Solar Engineering of Thermal Processes, John Wiley and Sons, J. Duffie, W. Beckman, 4th ed., 2013. Technical Manual for the SAM Solar Water Heating Model, NREL, N. DiOrio, C. Christensen, J. Burch, A. Dobos, 2014. A simplified method for optimal design of solar water heating systems based on life-cycle energy analysis, Renewable Energy journal, Yan, Wang, Ma, Shi, Vol 74, Feb 2015
2) Domestic hot water load: Modeling patterns of hot water use in households, Ernest Orlando Lawrence Berkeley National Laboratory; Lutz, Liu, McMahon, Dunham, Shown, McGrue; Nov 1996. ASHRAE 2003 Applications Handbook (SI), Chapter 49, Service water heating
3) Mains water temperature Residential alternative calculation method reference manual, California energy commission, June 2013. Development of an Energy Savings Benchmark for All Residential End-Uses, NREL, August 2004. Solar water heating project analysis chapter, Minister of Natural Resources Canada, 2004.
4) Pipe diameters and pump power: Planning & Installing Solar Thermal Systems, Earthscan, 2nd edition
5) Sun postion and POA irradiance, the same as for Ladybug Photovoltaics (Michalsky (1988), diffuse irradiance by Perez (1990), ground reflected irradiance by Liu, Jordan (1963))
6) Optimal system and storage tank size: A simplified method for optimal design of solar water heating systems based on life-cycle energy analysis, Renewable Energy journal, Yan, Wang, Ma, Shi, Vol 74, Feb 2015.…