or a couple of thingies.
Pattern.gh
I defined parametrically a triangle which I then smoothed out to become more like a blob shape. After that I created a pretty simple pattern that I had in my mind (costed me a lot of time to make this in GH) and finally wanted to rotate each element as it goes higher . The dispatching part seems to be working pretty slow, so it might need an optimization, but I’m still happy with the result as it shows exactly what I wanted, so this is a minor issue in my case.
I then decided to try tessellating my extrusions. You’ll see the voronoi script which is a blob-group in the same Pattern.gh:
I had an idea of something and started the code from scratch, then decided to watch tutorials and implement the code shown there. I somehow coped to combine my code with this in the tutorials, but since my knowledge of Grasshopper is zero to basic my code seems to be very unoptimized and lagging.. When dragging the sliders, it takes a lot of time to compute the changes, although, I’m working on a 24gigs 6th gen i7 machine. It might also need optimization.
Here comes the first tricky part that I couldn’t sort out in an elegant way neither in Grasshopper nor in Rhino. I want a smooth transition between the wall and the ceiling, so that the voronoi tessellation doesn’t get interrupted. If I was to do it in Rhino I’d make a curve with a filleted edge which I’d then revolve/sweep along a rail.
Pattern.gh:
Second thing is – I’ve defined a shape which I want to rotate at a certain degree as it goes higher, however, I don’t have the knowledge to make this happen automatically and just copy the script over and over again. Is there a chance to somehow “loop” the code and parametrically define the degree of rotation and amount of units in the loop?
Next thing is I want to somehow be able to rotate each “6-storey-building” dependently on its surrounding buildings, so that their “terraces” never overlap. I’m using quotes, since they’re still some silly shapes that have nothing to do with buildings and terraces. The principle has to be something like gear wheels or the so-called rack wheels . There has to be some pace which I could set parametrically, but I’m still unsure how to do that in Grasshopper.
The pre-last thing is that I want to control the height of each “building” based on let’s say a topography. I presume this could be done somehow with height maps or some gradient mapper connected to curvature analysis. Not really sure how something like this would work, but I’ve seen such codes that control height depending on a variable.
The last one is more or less similar to the previous. I want to be able to “dissolve” the pattern that I initially created and make it irregular. I suppose this could be done with attractor curve, but again this is just a guess. Please note that this is a top view and the shapes on the upper-left corner have got more "wings" which means there is more floors in the according building. Let's say the buildings in the upper-left corner are 6-7 floors high, in the middle are 4-5 and to the right they're only 3 floors high.
Sorry for that many questions in a single thread. Please let me know if I have to split them in separate threads. All this information is needed for learning purposes. I’m now preparing myself for my bachelor thesis and try as much things as I could, so that I’ll be ready for the final stage of my bachelor’s degree.
Many thanks in advance! Cheers!…
ooking for an efficient way to perform glazing of complex shapes.
I've only followed the Energy modelling workshops so far so i may have missed some essential components or workflows to achieve my needs. But i've made an attached definition with all my current attempts to get a proper HBzone with the numerous windows faces i will always have to deal with in this project.
I first thought that i was not using the HBObjWGZ correctly, then after some readings it was maybe an upgrading issue, then effectively i had my Therm 7.5 that needed to be reinstaled, but then ... I must be missing an essential HB tricks or workflow i guess ...
So I divided my attempt in two series :
- The Serie 1 : is a simplier version of the project step i'm working on but i'd be glad to achieve it first !
- The Serie 2 : is the real final direction of the project, which consist in sorting/dispatch faces to windowon one side and to an other material on the other, according to the winter sun and a pourcentage param.
Despite it is more complicated than the Serie one, it seems seems to create the same diversity of issues.
Until now, with the 5 different combinations of Serie 1, and the 3 of Serie 2, with and without using the different Glazing/window components, here are the logs i got from both HBZone component or OpenStudio component:
From OpenStudio - "1. The simulation has not run correctly because of this severe error: ** Severe ** BuildingSurface:Detailed="00073E23257843B6A948", invalid Construction Name="ETFE" - has Window materials.">> Has to deal with the way i'm trying to assign too early a customized EPConstruction material ? Done it wrong ? I tried to reload it in the library but doesn't change anything...
From OpenStudio - "1. The simulation has not run correctly because of this severe error: ** Severe ** BuildingSurface:Detailed="000579CD749E46DFA5EA", invalid Construction Name="EXTERIOR WINDOW" - has Window materials.">> Is it an issue in the way i define my surfs both as "WINDOW" (5) for srfType and Outdoors on the same component ?
From Create HBZone -"1. Solution exception:'EPZone' object has no attribute 'shdCntrlZoneInstructs'"
>> Happens when i try to introduce my ETFE EpMaterial after creating my first HBZone, with a Set EP Zone Construction, so this material seems to be not working either before and after trying to create an HB Zone
From Create HBZone- "1. Solution exception: 73df51a3b2144b1e858b has been moved, scaled or rotated."If you need to move or rotate a Honeybee object you should use Honeybee move, rotate or mirror components. You can find them under 12|WIP tab.
>> >> wich seems to exist in some on other thread Here and was a coding bug supposed to be fixed.
And last but not least ...
From OpenStudio - "1. The simulation has not run correctly because of this severe error: ** Severe ** checkSubSurfAzTiltNorm: Outward facing angle of subsurface differs more than 90.0 degrees from base surface.2. The simulation has failed because of this fatal error: ** Fatal ** GetSurfaceData: Errors discovered, program terminates" .
I'm attaching the file with each attempt in this post. The definitions are disabled and the log already copied separatly so there is no need to compute each of them to see what's wrong.
If someone from the beginner to one of the Kings of HoneyBee has any relevant answer/solution to this attempt with complex geometry Issue it will be really nice for me so i could to move forward !!
Thanks in advance guys and have a great day !
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y from the Rhino model and having the absorption coefficients of the materials that are entered into Pachyderm, why is it not possible to generate a reverberation time diagram, without the need to start any analysis?
MAPPING METHOD: When for example the mapping of the Strenght Index (G) is generated through the "create map" option, succesively I can´t generate any other energy criterion map, but I have to redo the simulation.
Is it a limitation of the software or am I wrong something?
MAPPING METHOD: I kindly wanted to ask what is the difference between minimum and detailed convergence and why the number of reflections order it takes into account for the simulation is not specified. The mapping method take care only of the Raytracing Method or the Image Source too?
MAPPING METHOD: Why is the mapping value that can be exported to Rhino not generated for all the calculation raster points, but maximal only for 100 values?
MAPPING METHOD: This method hasn't been implemented in Grasshopper yet, has it?
RAYTRACING METHOD (Pach:RT): I did a raytracing through the components of GH, using only the Pach_RT, and I had these curious results in terms of time:
RaysCount: 15.000, IS_Order:1 = 5min
RaysCount: 15.000, IS_Order:2 = 12min
RaysCount: 15.000, IS_Order:3 = 3min
RaysCount: 15.000, IS_Order:4 = 8min
RaysCount: 15.000, IS_Order:5 = 3min
Why a raytracing with only 2 order, is more and more extensive than the 3/4 and 5 order?
ANALYSIS RESULT: Would there be a way to export all the results of a simulation, as is done via Odeon, to a .txt list?
I apologize in advance for asking so many questions, I hope you can find the time to answer,
Yours sincerely from Müller-BBM…
3. receiver gets data from sender via input (0) < the data here may be changed in the meantime, for instance if its a double then I would like to add 1 to it.
4. receiver sends data to sender's input(2)
5. go to 1.
VS 2013 studio project folder
SENDER
Public Class loopStart Inherits GH_Component
Dim cnt As Integer
Friend Property counter() As Integer Get Return cnt End Get Set(value As Integer) cnt = value End Set End Property
Dim iData As New GH_Structure(Of IGH_Goo)
Friend Property startData() As GH_Structure(Of IGH_Goo) Get Return iData End Get Set(value As GH_Structure(Of IGH_Goo)) iData = value End Set End Property
Public Sub New() MyBase.New("loopStart", "loopStart", "Start the loop with this one.", "Extra", "Extra") End Sub
Public Overrides ReadOnly Property ComponentGuid() As System.Guid Get Return New Guid("bdf1b60d-6757-422b-9d2d-08257996a88c") End Get End Property
Protected Overrides Sub RegisterInputParams(ByVal pManager As Grasshopper.Kernel.GH_Component.GH_InputParamManager) pManager.AddGenericParameter("Data", "dIn", "Data to loop", GH_ParamAccess.tree) pManager.AddIntegerParameter("Steps", "S", "Number of loops", GH_ParamAccess.item) pManager.AddGenericParameter("<X>", "<X>", "Please leave this one alone, don't input anything.", GH_ParamAccess.tree) pManager.Param(2).Optional = True End Sub
Protected Overrides Sub RegisterOutputParams(ByVal pManager As Grasshopper.Kernel.GH_Component.GH_OutputParamManager) pManager.AddGenericParameter("Data", "dOut", "Data to loop", GH_ParamAccess.tree) End Sub
Public Overrides Sub CreateAttributes() m_attributes = New loopStartAttributes(Me) End Sub
Protected Overrides Sub SolveInstance(ByVal DA As Grasshopper.Kernel.IGH_DataAccess)
Dim numLoop As Integer DA.GetData(1, numLoop)
Dim loopDt As New Grasshopper.Kernel.Data.GH_Structure(Of IGH_Goo)
If cnt = 0 Then Me.startData.Clear() DA.GetDataTree(0, Me.startData) loopDt = startData.Duplicate DA.SetDataTree(0, loopDt) End If
If cnt < numLoop - 1 And cnt > 0 Then DA.GetDataTree(2, loopDt) DA.SetDataTree(0, loopDt) Me.ExpireSolution(True) Else DA.GetDataTree(2, loopDt) DA.SetDataTree(0, loopDt) End If
cnt += 1
End Sub
End Class
RECEIVER
Public Class loopEnd Inherits GH_Component
Dim aData As New GH_Structure(Of IGH_Goo)
Friend Property anyData() As GH_Structure(Of IGH_Goo) Get Return aData End Get Set(value As GH_Structure(Of IGH_Goo)) aData = value End Set End Property
Public Sub New() MyBase.New("loopEnd", "loopEnd", "End the loop with this one.", "Extra", "Extra") End Sub
Public Overrides ReadOnly Property ComponentGuid() As System.Guid Get Return New Guid("3ffa3b66-8160-4ab3-87c9-356b2c17aadd") End Get End Property
Protected Overrides Sub RegisterInputParams(ByVal pManager As Grasshopper.Kernel.GH_Component.GH_InputParamManager) pManager.AddGenericParameter("Data", "dIn", "Data to loop", GH_ParamAccess.tree) End Sub
Protected Overrides Sub RegisterOutputParams(ByVal pManager As Grasshopper.Kernel.GH_Component.GH_OutputParamManager) pManager.AddGenericParameter("Data", "dOut", "Data after the loop", GH_ParamAccess.tree) End Sub
Protected Overrides Sub SolveInstance(ByVal DA As Grasshopper.Kernel.IGH_DataAccess) Me.aData.Clear() DA.GetDataTree(0, Me.aData) runner()
DA.SetDataTree(0, Me.aData) End Sub
Sub runner()
Dim doc As GH_document = Grasshopper.Instances.ActiveCanvas.Document Dim docl As list(Of iGH_DocumentObject) = (doc.Objects)
For i As Integer = 0 To docl.count - 1 Step 1 Dim comp As Object = docl(i) If comp.NickName = "loopStart" Then Dim compp As IGH_Param = comp.Params.input(2) compp.VolatileData.Clear() compp.AddVolatileDataTree(anyData) Exit For End If Next End Sub
End Class
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looked at autodesk simulation cfd 2015 and was optimistic because it had an export plugin from revit, which i use anyway for material takeoffs and etc, but found that it did not take solar radiation into account. This was a downer because I have heard that solar radiation could effect indoor airflow - convection - as much as 50 percent at a time.
Then I searched again and found that Hyperworks, a software by altair technology can be coupled with a radiation software. So I went through the trouble of obtaining an educational license of Hyperworks. However, though some email exchange I have found that the coupling is a one-way. The radiation analysis software was used, I think, for understanding the solar loading for a SOM project called church of light.
The support guy said : "Unfortunately our coupling with Hyperworks is really a one way coupling. We can accept H coefficients from their software in RadTherm, but they will not read in our wall temps. That said, it still can be a useful coupling in the sense that you can run the analysis in Hyperworks, send H coefficients to RadTherm, and run the analysis to better understand radiation and conduction. Most importantly, that analysis can be done for longer transient analysis, but will require much less compute time and resources."
Not only did I not understand what he means by the H coefficients, my wanting to get a CFD understanding coupled with solar radiation was again, unsatisfied. In the mean while I had to finish a presentation so I haven't had the time to try to get some result on the natural ventilation. I would probably need to look into how their solutions work before I can understand if their software would "do the job"
Thank you for letting me know about your work on this. I downloaded the Honeybee_Set EP Natural Ventilation component and made sure that it is allowed, but it does not show up in grasshopper.
You pointed out that "The component (and the corresponding equation) is mostly meant for cases where you have zones with windows that are NOT connected by an air wall (or a larger airflow network)." I wondered if you are suggesting it would be a code violation for zones to be connected by an air wall for fire safety reasons. It would be a violation I guess, like not putting an fiber insulation or some kind of smoke stop between Spandrel panels and the edge of a floor plate would be a code violation for a typical office building.
There is a project by kevin daly architects where you can see a section drawing with what seems like a cfd analysis (could be an illustration)
it was my initial visualization/simulation goals were for a facade design I am working on
1) an average air velocity across a zone at noon, for example, if a passive design strategy like this was used. for this I am guessing cfd is not entirely necessary. probably means that it could be used earlier in a design process, too. This would be more about user comfort.
2) at a later phase, like in detailing facade components, if airflow is indeed as expected for a zone that is connected to an air wall / chimney like feature (and to see if there is a proper mixing of air)
3) and a projection of energy savings, of course.
After seeing a video of simulation cfd I was optimistic, but like I said sim cfd does not take account of solar loading. I think I would probably go ahead start with one zone with sim cfd first, try three zones stacked on top of each other, then try hyperworks and try to factor in solar radiation.
For analyzing multiple zones on different levels, being able to add a chimney would be especially useful, I think. Having said that, I don't have a lot of experience of using honeybee except for the daylight component so it would take some time for me to understand the components.
I hope some of the information here is useful for you. after all, both sim cfd and hyperworks are commercial softwares and somewhat different than the e plus project you are working on, I guess but still trying to address a similar problem.
so.. in cased you missed it I was asking I downloaded the Honeybee_Set EP Natural Ventilation component and made sure that it is allowed and placed in the user object foler, but it does not show up in grasshopper. what could be the reason?
…
o express my gratitude. I've been experimenting with your definitions (and still am), but let me extend my question.
Actually what I'm trying to achieve, is to recreate another project by Andrew Kudless, the spore lamp (I mentioned the Chrysalis at the beginning just because of the animation, which wasn't included in the Spore Lamp presentation).
Basically the spore lamp seems to me to be something like a preliminary study to the Chrysalis III project (I think it's a similar approach).
Andrew stated on his site that he used kangaroo for this project, so the Spore Lamp consists in my opinion either of a relaxed voronoi 3d diagram (b-rep, b-rep intersection) on a sphere which then has been planarized, or more likely it is a sort of relaxed facet dome.
The trick is to:
1. obtain a nicely-balanced voronoish diagram (or facet dome cells)
2. keep each cell/polyline planar (or force them with kangaroo to be planar) in order to move scale and loft them later on.
Here is what I have by now. (files: matsys spore lamp attempt)
That's the closest appearance that I got so far (simple move scale and loft of facet dome cells with the amount of transformations being proportional to the power of the initial cell area: bigger cell = bigger opening etc.) - with no relaxation of the diagram. But it's obviously not the same thing as the matsys design.
Here are some of my attempts of facet dome relaxation, but well, it certainly still not the right approach, and most importantly I don't know how to keep or force the cells to be planar after the relaxation.
1. pulling vertices to a sphere - no anchor points. That obviously doesn't make sense at all, but the relaxation without anchor points gives at the beginning a pattern that is closer to what I am looking for. (files: relaxation 01)
2. pulling vertices to a sphere - two faces of the initial facet dome anchored (files: relaxation 02)
3. pulling vertices to the initial geometry (facet dome) no anchor points (files: relaxation 03)
The cell pattern of the lamp kinda looks like this:
you can find it here: http://www.grasshopper3d.com/forum/topics/kangaroo-0-095-released?g...
Done with Plankton (of course without the "gradient increase" appearance), but in fact not, I took a look at Daniel Parker's Plankton example files, and it's not quite the same thing. Also the cells aren't planar...
The last problem is that during the relaxation attempts that I did, the biggest initial cells became enormous, and it's not like that in the elegant project by Andrew Kudless, that I'd like to achieve.
So to sum up:
Goal no 1: Obtain an elegant voronoi /facet dome cell pattern on a sphere (or an ellipsoid surface, whatever).
Goal no 2: Keep the cells planar in order to be able to loft them later and obtain those pyramidal forms, and assemble easily
Any ideas? Or maybe there's a completely different approach to that?…
les automatically at the right angle to form the cap of an icosahedron.
To complete the full icosahedron, we consider just the six points we already know, the five pentagon vertices and the raised pyramid tip and reorient one of the vertices using three-point transformation so it obtains the exact same relationship between vertices only one more stage beyond our little cap pyramid, and we do a five-fold polar array:
I used a password-protected cluster I ran into one the forum somewhere to reproduce Rhino's 3-point orient command:
A final 3-point orientation transforms in space the original pyramid tip down to the bottom:
Now we can create a convex hull which gives an icosahedron mesh:
So that's how you build an icosahedron in Rhino from scratch, only using rather long winded Grasshopper.
Now we use the Weaverbird plug-in to subdivide the faces and then project the vertices out onto a sphere via finding the closest points to a sphere and then recreating a convex hull to make a geodesic dome mesh:
Subdividing two times works fine but 3 times blows up convex hull, so I'll just have due with the the subdivision step and leave out projecting back to a sphere, since the algorithm already gives a nice spherical result that you can see inside this disaster:
Now you know what a standard geodescic dome is, just an icosahedron with faces divided into smaller triangles, projected out to a sphere.
Actually, the mere subdivision is just a bit blobby instead of a sphere, damn it, so I'll have to topologically recreate the mesh after projecting the points indeed back onto our sphere.
Using a subdivision plug-in may be slightly throwing the perfect result off, so manually creating subdivision points on each mesh face may be in order, doing them flat against each icosahedron face:
You can also start with the two other triangulated Platonic solids but those give less regular triangles:
…
ree..
First-End List Component cannot manage branches inside every dimensions..
"Smart T8" Component is developed for managing the multi dimensional data tree with first-end algorithm.
It works with path index location..
"-1" or negative numbers mean the location of item..
"0" means the location of the last path index..
positive numbers mean the location from the back..
----
Now look at this example.. a simple 3-dimensional boxes..
In the data tree.. of {0;0;i;j} (k)
"k" is the item index.. Y direction..
"j" is the last path.. X direction..
and "i" is the level.. Z direction..
----
When index < 0 (i.e. "-1" or negative)
"Smart T8" performs like the First-End Item Component..
It selects first items in each list and puts them out to "F"..
and in this example.. they are boxes with same Y coordinate(=0)..
In the below image..
F(Red) M(Transparent Green) E(Blue) are classified by Y coordinates..
----
When index = 0
"Smart T8" focuses on the last path index..
It selects first list of every {0; 0; i; *} set of lists.. (i.e. every levels)
In this example.. they are boxes with same X coordinate(=0)..
because the last path means X grid..
In the below image..
F(Red) M(Transparent Green) E(Blue) are classified by X coordinates..
----
When index = 1
"Smart T8" focuses on the third path index.. (i.e. 1 step from the back)
It selects first list of every {0; 0; *; j} set of lists..
Actually in this case.. they are first levels of every YZ planes..
In this example.. they are boxes with same Z coordinate(=0)..
because "Smart T8" manages levels now (index=1)..
In the below image..
F(Red) M(Transparent Green) E(Blue) are classified by levels..
----
When index > 1.. (if it is meaningless index or out of range..)
It performs First-End List Component..
It selects only the first and end list of all lists..
----
The "Smart T8" component works with 3 or more dimensional data tree well..
Please control the focusing index and enjoy it.. :)
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a problem with SSL. Any Ideas? I am using the following code:
import json,httplib connection = httplib.HTTPSConnection('api.parse.com', 443) connection.connect() connection.request('GET', '/1/classes/MY-CLASS', '', { "X-Parse-Application-Id": "MY-APP-ID", "X-Parse-REST-API-Key": "MY-REST-API-KEY" }) result = json.loads(connection.getresponse().read()) print result
I Get the Following Messages:
Runtime error (IOException): Authentication failed because the remote party has closed the transport stream. Traceback: line 280, in do_handshake, "C:\Program Files\Rhinoceros 5.0 (64-bit)\Plug-ins\IronPython\Lib\ssl.py" line 120, in __init__, "C:\Program Files\Rhinoceros 5.0 (64-bit)\Plug-ins\IronPython\Lib\ssl.py" line 336, in wrap_socket, "C:\Program Files\Rhinoceros 5.0 (64-bit)\Plug-ins\IronPython\Lib\ssl.py" line 1156, in connect, "C:\Program Files\Rhinoceros 5.0 (64-bit)\Plug-ins\IronPython\Lib\httplib.py" line 3, in script Any help would be greatly appreciated! Thanks in advance! -Zach…
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.…