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Isar735.github.io
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Cognitive Development Activities
WRITING CLASSES writingclassesforkids.com.


A service for handling Firebase out-of-band actions
Project & README | Demo | Demo Source Code | Documentation
npm i @nowzoo/ngx-firebase-oob --save
Clone the main repo and npm install...
git clone https://github.com/nowzoo/ngx-libs.git
cd ngx-libs
npm i
The library files are in projects/ngx-firebase-oob
.
The demo code is in projects/ngx-firebase-oob-demo
.
Building the library...
ng build ngx-firebase-oob
Testing the library...
ng test ngx-firebase-oob
To test with Wallaby, use the wallaby.js
config at the root of the project directory.
Serving the demo...
# make sure you've built the library locally first with ng build ngx-firebase-oob
ng serve ngx-firebase-oob-demo
Please submit issues to the main repo here.


Devil's Isle Supporter:
This sword is an ancient relic of Devil's Isle. It was used to destroy those who fell under the curse.
Fearing its power, thay were finally able to weaken it by sealing away a few of its powers in a number of scrolls.
As you use it do defeat our enemies, thought, you'll acquire the ability to enhance the weapon to its former strenght.
You should know that there are several Dwarven adventurers also trapped on the island. Take the sword and Scroll of Enchant Weapon to one of them they'll make your weapon even more powerful!
Ask about the enemy.


Tags: music and stuff
Ulcerate - Stare Into Death And Be Still
Holy balls
Release date: 2020-04-24
[9.5/10]
Yaeji - What We Drew
Awesome bedroom electro-pop.
Release date: 2020-04-02
[8.7/10]
Farwarmth - Momentary Glow
FFO Ben Frost.
Release date:
[8.6/10]
Shabazz Palaces - The Don Of Diamond Dreams
Honestly while I do think they’re definitely one of the best in the experimental hip-hop game I couldn’t really finish any of their earlier albums. This one I can finish, and I dig it… The beats are playful and the instrumentation is lush, don’t really think there’s anything to pick on this album. Good stuff.
Release date: 2020-04-17
[8.6/10]
Laura Marling - Song For Our Daughter
Excellent folk record. Don’t think there’s anybody that would not like this album.
Release date: 2020-04-10
[8.5/10]
Evan Caminiti - Varispeed Hydra
Deep ambient dub.
Release date: 2020-04-03
[8.5/10]
Iceblink - Carpet Cocoon
Indietronica / folktronica / bedroom music. It’s got that intimacy in last year’s Ernest Hood record, but with more instrumentation and more jazz influence. I really dig it.
Release date: 2020-01-24
[8.4/10]
Midwife - Forever
Slowcore / indie pop.
Release date: 2021-05-31
[8.3/10]
DJ Trystero - High Speed Wind
Lo-fi dub techno.
Release date: 2020-03-13
[8.3/10]
Mamaleek - Come & See
FFO Botanist. Though I like the first two songs the most, every track on this album is very enjoyable experimental black metal song. I like how the guitars are drenched in reverb and instead of being ultra high gain they have a somewhat twang-ish quality.
Release date: 2019-12-06
[8.3/10]
Felicia Atkinson - Everything Evaporate
Droning, hypnagogic ambient. I think this is one of those albums that the listener would have to concentrate on listening in order to fully appreciate the intricacies of the entire thing.
Release date: 2020-04-03
[8.3/10]
Yves Tumor - Heaven To A Tortured Mind
I was under the impression that Yves Tumor produces music that are too hard to actually enjoy, although dude’s last album Safe In The Hands Of Love is actually pretty chill. This one carries over the atmospheric experimental R&B vibe from the said album, but the production is more minimalistic and stripped down, and the overall sound is more reminiscent of the old school R&B.
Release date: 2020-04-03
[8.3/10]
downy - 第七作品集『無題』
Basically what you’d expect from them. Awesome futuristic post-rock.
Release date: 2020-03-18
[8.2/10]
DJ Python - Mas Amable
Dub techno / ambient. Super hypnotic stuff.
Release date: 2020-04-10
[8.2/10]
Waclaw Zimpel - Massive Oscillations
Psyched out jazz + minimal electronica? Mesmerizing stuff.
Release date: 2020-01-31
[8.2/10]
Lyra Pramuk - Fountain
Experimental choir music? Everything on this record seems to be consisted of her voice only. The artist collaborated with Holly Herndon and Colin Self, so that kind of gives away what to expect on this album.
Release date: 2017-08-18
[8.2/10]
D.K. - The Goddess Is Dancing
Ambient house with elements from Vietnamese ritual music.
Release date: 2020-03-13
[8.1/10]
Rina Sawayama - Sawayama
In contrast to her debut mini album, which has a super prevalent vaporwave plus 90’s J-pop vibe, this one feels more grandiose, less nostalgic, and more in the context of contemporary pop music. The nu metal references are pretty evident, though personally I’m way into J-pop / R&B than nu metal I wouldn’t say the element’s appearance is out of place or bizarre. Take the track STFU! for example, when it came out as a single I was a bit taken aback but in the context of the entire album it feels way more natural and refreshing. Cue Poppy who actually came out with a djent-pop record earlier this year and totally butchered it…
Release date: 2020-04-17
Anyhow I think aesthetically I prefer Rina to this project but there are tracks that I enjoy quite a bit, like Bad Friend, Comme Des Garcons (Like The Boys) and Akasaka Sad.
[8.0/10]
Laurel Halo - Possessed
This one is another step from the older hypnagogic pop / techno stuff. I think overall while this album is indeed experimental and bold its predecessor Raw Silk Uncut Wood is much more approachable and sonially more appealing. Fav song on this album would be Hyphae, pretty unsettling track.
Release date: 2021-04-16
[7.9/10]
Electric Indigo - Ferrum
Pulsating ambient techno. I feel like there really isn’t a lot of higher pitches or tones in this album, and it’s full on percussion and wobbly beats.
Release date: 2021-01-15
[7.9/10]
Arca - @@@@@
On Spotify this album is a sinlge 62 minute track so it’s difficult to really pinpoint the songs or bits I like most. The one at around 40 minutes mark is pretty memorable and definitely the one that leaves the most impression to me but the album in its entirety is pretty enjoyable. Stylistically this one is a continuation from her previous album Arca, but less baroque (well at least that how I felt when listening to that album) and more approachable.
Release date: 2020-02-21
[7.8/10]
Nathan Fake - Blizzards
Vibrant IDM.
Release date: 2020-09-18
[7.8/10]
Thundercat - It Is What It Is
Didn’t really check out Drunk, maybe I should… this one doesn’t stray off from his comfort zone too much. The bass and all the other instruments are very stellar, the mix could be done a bit better though in my opinion.
Release date: 2020-04-03
[7.7/10]
Higher Intelligence Agency - Preform
Dub techno / IDM.
Release date: 2020-04-03
[7.6/10]
Daniel Avery, Alessandro Cortini - Illusion Of Time
I appreciate how this album showcases both artists’ artistic tendencies. Instead of sounding like Avery’s own rave-worthy dub techno this one features a fair share of Cortini’s almost post-rockish ambient textures. To be frank I prefer Song For Alpha more than this album, but this one isn’t a bad album by any means.
Release date: 2020-03-27
[7.6/10]
Old Man Gloom - Seminar IX: Darkness Of Being
Pretty gnarlly post-metal. The first track was really crushing but there are other songs that are borderline cheesy stoner metal like In Your Name, and I don’t really love those tracks.
Release date: 2020-03-23
[7.5/10]
Gil Scott-Heron, Makaya McCraven - We’re New Again: A Reimagining by Makaya McCraven
Nu jazz / blues.
Release date:
[7.4/10]
Witch Prophet - DNA Activation
Eastern Africa jazz + R&B. Pretty easy to follow along, but a bit too much on the safe side.
Release date: 2011-12-30
[7.3/10]
Menzi - Impazamo
So there’s this new music genre called Gqom in South Africa, and Menzi is one of the scene’s leading artists. This album can be best described as dark tribal experimental dance music, haven’t listened to any other stuff labeled as Gqom nor done any sort of looking up on more infos about the scene… I guess if you dig Tzusing then this might be your stuff?
Release date: 2020-03-27
[7.3/10]
Dean Blunt - Roaches 2012-2019
Left field experimental pop compilation. Has a bunch of radio indie rock samples but the vocals are purposely super off-key and weird…
Release date: 2020-03-25
[7.2/10]
Knxwledge - 1988
Basically a collection of cut up hip-hop / R&B samples. Some tracks are pretty decent but they don’t last long. Think Madvillainy vol. 3 but weaker and less fun.
Release date: 2020-03-27
[7.2/10]
Ohyung - Protector
Aggressive experimental trap. The more noise oriented tracks are my jam, but the track Shenme Gui, I’m like… 什麼鬼？
Release date: 2020-06-26
[6.8/10]
P22 - Human Snake
There’s a ton of Sonic Youth vibes in this EP. Not bad but not really what people would describe as highly original…
Release date: 2020-04-03
[6.7/10]
Nghtcrwlr - Let The Children Scream
Experimental goth trap / lo-fi noise pop. 有點中二…
Release date: 2020-02-21
[6.5/10]
The Strokes - The New Abnormal
I mean it’s not a bad album but I just don’t like post-punk revival as a whole, and the fact that the chords are pretty predictable does not help. I know this one’s been getting rave reviews but I’m like, meh…
Release date: 2020-04-10
Also there’s way too much unnecessary falsettos in this album. Not for me.
[6.3/10]
Fiona Apple - Fetch The Bolt Cutters
我真的是覺得還好……
Release date: 2020-04-17
[6.0/10]
Suhjan Stevens, Lowell Brams - Aporia
Ambient / new-age electronica. To me the album is overall pretty underdeveloped and feels like a soundtrack to some 80’s sci-fi movie. There are moments reminiscent of other big name ambient musicians, but the songs are just too short to leave any meaningful impression to me. If one wants to try Sufjan’s music it’s probably a good idea to start with another one…
Release date: 2020-03-24
[6.0/10]
Jon Hassell - Vernal Equinox
According to Spotify my go-to musical genre is Fourth World. Not sure why…
Release date: 1978
[8.7/10]
American Grandma - Superdog
Found this in The Flenser’s Facebook group. Slowcore.
Release date: 2014-09-29
[8.6/10]
Move D, Benjamin Brunn - Let’s Call It A Day
Deep house / ambient / minimal techno.
Release date: 2020-02-14
[8.4/10]
Cremation Lily - The Processes And Instruments Of Normal People
Lofi ambient techno.
Release date: 2017-09-07
[8.3/10]
Yazz Ahmed - Polyhymnia
Outstanding world jazz. No idea why Spotify put this in the recommended for section at Richard Dawson’s page though.
Release date: 2014
[8.2/10]
John Roberts - Can Thought Exist Without The Body
Classical influenced ambient music. Almost passed out with this on repeat while I was in the tub, damn…
Release date: 2019-10-18
[8.0/10]
100 Gecs - 1000 Gecs
I don’t get it…
Release date: 2019-05-31
[5.0/10]
Comments


val player: ClientPlayerApi
Provides access to the beta player api, including track playing and pausing endpoints.
Please consult the usage guide before calling any endpoint in this api.
These endpoints may break at any time.


Heatsim2 is a finite difference simulator for heat conduction. It is designed to let you define the grid and boundary conditions from Python, while implementing the calculations using optimized C code. It uses an alternating direction implicit (ADI) Crank- Nicholson solver. It can simulate anisotropic materials so long as the anisotropy is aligned to the simulation axes. It can also simulate thin (in z) specimens that have curvature along the x and/or y axes.
The first step is to define the grid over which heatsim2 will peform the finite difference calculations. This means defining the number of steps in the z, y, and x axes (if you want only a 2D or 1D calculation you can set the number of steps in one or more axis to 1). You also need to define the bounds of the region. Here the region will be bounded in z at 0 and 1.4 mm, bounded in y from -1.6mm to +1.6mm, and bounded in x at -1.5mm to +1.5mm. Then you can use the heatsim2.build_grid() function to define the grid point centers and grid point boundaries:
nz=5 ny=50 nx=55 (dz,dy,dx, z,y,x, zgrid,ygrid,xgrid, z_bnd,y_bnd,x_bnd, z_bnd_z,z_bnd_y,z_bnd_x, y_bnd_z,y_bnd_y,y_bnd_x, x_bnd_z,x_bnd_y,x_bnd_x, r3d,r2d) = heatsim2.build_grid(0,1.4e-3,nz, -1.6e-3,1.6e-3,ny, -1.5e-3,1.5e-3,nx)
The variables dz, dy, and dx represent the resulting axis step sizes. The variables z, y, and x are one-dimensional arrays of coordinates of the grid centers. The variables z_bnd, y_bnd, and x_bnd are one-dimensional arrays of coordinates of the grid boundaries. In this example, z_bnd is [ 0, .28e-3, .56e-3, .84e-3, 1.12e-3, 1.4e-3 ], representing the 6 boundaries of the 5 z grid elements. Likewise z is [ .14e-3, 42e-3, .7e-3, .98e-3, 1.26e-3 ] representing the midpoints of those grid elements. Note that if you want to guarantee an element centered at the origin, you should have symmetric spatial bounds and an odd number of elements in each axis.
The variables zgrid, ygrid, and xgrid represent the z, y, and x grid cell center coordinates, but shaped and broadcasted over a nz by ny by nx array. These are useful for evaluating distances and conditions. For example np.sqrt(xgrid**2 + ygrid**2 + zgrid**2) would calculate a three dimensional array of grid cell center distances from the origin. Similarly xgrid > 1e-3 is a three-dimensional array of truth values representing which cells have centers with x coordinates greater than 1 mm.
The variables z_bnd_z, z_bnd_y, and z_bnd_x are similar shaped and broadcasted arrays representing the coordinates of the centers of the cell boundaries along the z axis. They are nz+1 by ny by nx arrays and will be used in defining boundary conditions along the z axis. Likewise y_bnd_z, y_bnd_y, and y_bnd_x are (nz,ny+1,nx) arrays representing the coordinates of the centers of the y axis cell boundaries, and x_bnd_z, x_bnd_y, and x_bnd_x are (nz,ny,nx+1) arrays representing the coordinates of the centers of the x axis cell boundaries.
Finally r3d is a precalculated 3 dimensional array representing the distances of cell centers from the origin, and r2d is a precalculated 3 dimensional array representing the distance projected into the x-y plane of cell centers from the origin.
# define materials: #titanium_k=6.7 # W/m/deg K titanium_k=np.diag(np.array((6.7,6.7,6.7),dtype='d')) titanium_rho=4.43e3 # W/m/deg K titanium_c=526.3 # J/kg/deg K materials=( # material 0: titanium (heatsim2.TEMPERATURE_COMPUTE,titanium_k,titanium_rho,titanium_c), # material 1: Titanium, fixed temperature (Dirichlet boundary condition) (heatsim2.TEMPERATURE_FIXED,), )
Any number of materials can be defined. Every cell in your grid will need to have a material identified. They will be identified by their index into the materials tuple. Each material is defined by a nested tuple. The first element can be heatsim2.TEMPERATURE_FIXED which will inhibit any calculations causing temperature changes for the material, or heatsim2.TEMPERATURE_COMPUTE. If the latter then three more elements of the tuple should be given: The material thermal conductivity (k), density (rho), and specific heat (c). The thermal conductivity may be either a scalar (for an isotropic material) or a diagonal matrix (to represent anisotropy aligned with the coordinate axes). The commented titanium_k line above specifies would use the isotropic model, whereas the uncommented line would use the anisotropic model (with, admittedly, isotropic parameters).
boundaries=( # boundary 0: conducting #(heatsim2.boundary_conducting,), (heatsim2.boundary_conducting_anisotropic,), (heatsim2.boundary_insulating,), )
Similar to defining materials, a boundaries tuple must be specified. Every x, y, and z boundary between every grid element (including both internal and external boundaries) will need to be specified. Boundary classes will be identified by their index into the boundaries tuple. Each boundary class is specified by a python object or module that has qz(), qy(), and qx() callables. Additional elements in the boundary class tuple will be passed as additional parameters to the callables. The built-in boundary class modules are: heatsim2.boundary_insulating, heatsim2.boundary_conducting, heatsim2.boundary_conducting_anisotropic, and heatsim2.boundary_thininsulatinglayer. If you defined materials anisotropically, then you must use heatsim2.boundary_conducting_anisotropic in place of heatsim2.boundary_conducting for all of the internal boundaries.
volumetric=( # on material grid # 0: nothing (heatsim2.NO_SOURCE,), #1: impulse source @ t=0 (heatsim2.IMPULSE_SOURCE,0.0,10e3/dz), # t (sec), Energy J/m^2 )
You must also define any volumetric heat source classes you will need. This works similarly to the material and boundary classes. Possible identifiers are heatsim2.NO_SOURCE, heatsim2.IMPULSE_SOURCE (an impulse in time; parameters are the time for the impulse -- must exactly match a given timestep --, and the source energy in J/m^3), heatsim2.STEPPED_SOURCE (a stepped source; parameters are start time, end time, and intensity in Watts/m^3), heatsim2.IMPULSE_POINT_SOURCE_JOULES (an impulse in time, first parameter is the exact time, second parameter is energy specified in Joules into each element, which may be a scalar or a volumetric array), heatsim2.SPATIALLY_Z_DECAYING_TEMPORAL_IMPULSE (see comments/code in alternatingdirection_c_pyx.pyx for details),
# initialize all elements to zero (material_elements, boundary_z_elements, boundary_y_elements, boundary_x_elements, volumetric_elements)=heatsim2.zero_elements(nz,ny,nx) delam_depth=0.4e-3; delam_min_x=-1e-3 delam_max_x=1e-3 delam_min_y=-.6e-3 delam_max_y=.6e-3 boundary_z_elements[ (z_bnd_x > delam_min_x) & (z_bnd_x < delam_max_x) & (z_bnd_y > delam_min_y) & (z_bnd_y < delam_max_y) & (z_bnd_z==z_bnd[(np.abs(z_bnd-delam_depth)).argmin()])]=1 # set edges to insulating boundary_x_elements[:,:,0]=1 # insulating boundary_x_elements[:,:,-1]=1 # insulating boundary_y_elements[:,0,:]=1 # insulating boundary_y_elements[:,-1,:]=1 # insulating boundary_z_elements[0,:,:]=1 # insulating boundary_z_elements[-1,:,:]=1 # insulating volumetric_elements[0,:,:]=1 # impulse
Calling heatsim2.zero_elements(nz,ny,nx) returns empty grids initialized to zero for specifying the material, the z, y, and x boundaries, and the volumetric sources (the material and volumetric sources are shaped (nz,ny,nx) whereas boundary_z_elements is shaped (nz+1,ny,nx), boundary_y_elements is shaped (nz,ny+1,nx), etc.
In this case all of the material_elements are left at zero because there is only one material and all cells should be calculated. The outer boundaries of the simulation volume are all set to insulating (boundary index 1) rather than the pre-initialized index 0 because otherwise the simulation will attempt to reference cells outside the volume and fail.
This simulation represents a flash thermography test in the x-y plane of a specimen with a "delamination" (how titanium could ever delaminate is left as an exercise to the reader) at a depth of 0.4 mm with extent between +/- 1 mm in x and between +/- 0.6 mm in y. This delamination will be represented as rectangular region of internal z boundaries that are represented as insulating (index 1) rather than conducting (index 0). Thus the z boundary elements at the closest z boundary to 0.4 mm and within these specified x and y bounds are set to 1 (defined as boundary_insulating
The flash thermography excitation is represented by the top layer (z=0) of volumetric_elements being set to 1, selecting the #1 element of volumetric which specifies a 10 kJ/m^2 source. Note that we will need to be sure to provide a timestep at exactly t=0 in order for this source to operate correctly. Also note that the source is being represented as volumetric heating throughout the top layer, as opposed to the idealized behavior of a perfect impulse applied to the top boundary.
t0=0 dt=0.010 nt=200 tvec=t0+np.arange(nt,dtype='d')*dt
You need to define the times at which the the calculation should be performed, a range of times with consistent spacing dt. The timestep must be small enough to avoid convergence problems (because heatsim2 uses an implicit method you can use significantly larger timesteps than with explicit methods). These times must line up exactly with times specified for special boundary conditions such as heatsim2.IMPULSE_SOURCE. Note that these times are for the center time of the calculation. Each timestep (width dt) goes from tcenter-dt/2 to tcenter+dt/2. The initial values of temperature T that you provide to the simulation are assumed to correspond to values at t0-dt/2. Then the first update to that (from the first call to run_adi_steps is best interpreted as the temperatures at t=t0+dt/2. The output temperatures are defined not at the given timesteps but are shifted by dt/2!
(ADI_params,ADI_steps)=heatsim2.setup(z[0],y[0],x[0], dz,dy,dx, nz,ny,nx, dt, materials, boundaries, volumetric, material_elements, boundary_z_elements, boundary_y_elements, boundary_x_elements, volumetric_elements)
Call heatsim2.setup() as shown to initialize the solver. This step defines the equations that will be iterated to perform the finite difference calculations. There are two optional paramters, top_surface_y_curvatures and top_surface_x_curvatures which can additionally be supplied to represent the curvature of the surface corresponding to the smallest z index. They should be arrays over x and y (coordinates from (xygrid_y,xygrid_x) = np.meshgrid(y,x,indexing='ij')) representing curvatures along the y and x axes respectively, positive concave. The thickness should always be less than 1/maximum_curvature.
T=np.zeros((nt,nz,ny,nx),dtype='d') curtemp=np.zeros((nz,ny,nx),dtype='d'); for tcnt in range(nt): t=t0+dt*tcnt print("t=%f" % (t)) curtemp=heatsim2.run_adi_steps(ADI_params,ADI_steps,t,dt,curtemp,volumetric_elements,volumetric) T[tcnt,::]=curtemp pass
You need to define an arrays, T and curtemp in this example, to store the current temperature and/or time history. This example initializes the time history T and last timestep temperature field curtemp to 0. Call heatsim2.run_adi_steps() to evaluate the temperature at a new timestep from the temperature at the previous timestep. The parameters to run_adi_steps() should match the parameters and results from heatsim2.setup() except the value of t should be incremented by dt from the previous value.
pl.figure(1) pl.clf() pl.imshow(T[20,0,:,:],origin='lower',extent=(x_bnd[0]*1e3,x_bnd[-1]*1e3,y_bnd[0]*1e3,y_bnd[-1]*1e3)) pl.ylabel('Y position (mm)') pl.xlabel('X position (mm)') pl.title('Surface temperature increase (deg. C) at t=%f' % (tvec[20]+dt)) pl.colorbar() pl.figure(2) pl.clf() pl.loglog(tvec+dt/2.0,T[:,0,20,21]) pl.grid() pl.xlabel('Time (s)') pl.ylabel('Surface temp. increase (deg. C)') pl.title('Temperature vs. time at x=%f mm, y=%f mm' % (x[21]*1e3,y[20]*1e3)) pl.show()
Matplotlib can be used to plot the results. Please note that the times of the calculation output are offset by 1/2 timestep compared to the times of the calculation itself.


Package-level declarations
An open source client library for Button merchants.
Types
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Asynchronous task used to report user activity to Button.
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class ButtonMerchant
Primary entry point for the Button merchant library.
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A concrete implementation of the ButtonProductCompatible interface.
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interface ButtonProductCompatible
An interface that defines the product properties that may be provided when reporting user activity.
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Represents an order placed by the user to be reported using reportOrder
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interface OrderListener
Callbacks for report order
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interface PostInstallIntentListener
Callbacks for post-install intent handler.
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interface UserActivityListener
Callbacks for tracking user activity.


Based on the data given below:
First username: {{name1}}
Second username: {{name2}}
Hypothetical tweet: {{hypo_tweet}}
The CLF algorithm has made the prediction below
The tweet likely originated from {{guess}}


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addAdminUser(Users)
- Method in class slender.services.core.users.impl.
UsersServiceImpl
addAdminUser(Users)
- Method in interface slender.services.core.users.
UsersService
addComment(Comment)
- Method in interface slender.services.core.comments.
CommentsService
addComment(Comment)
- Method in class slender.services.core.comments.impl.
CommentsServiceImpl
Add a comment, given a comment object.
addCompany(Company)
- Method in interface slender.services.core.company.
CompanyService
addCompany(Company)
- Method in class slender.services.core.company.impl.
CompanyServiceImpl
Add new Company
addProgress(Integer, Integer, int)
- Method in class slender.services.core.tasks.impl.
TasksProgressServiceImpl
Add progress to a task for a user using the hours spent on it
addProgress(Integer, Integer, int)
- Method in interface slender.services.core.tasks.
TasksProgressService
addProject(Project)
- Method in class slender.services.core.projects.impl.
ProjectsServiceImpl
Adds a new project to database
addProject(Project)
- Method in interface slender.services.core.projects.
ProjectsService
addTask(Task)
- Method in class slender.services.core.tasks.impl.
TasksServiceImpl
addTask(Task)
- Method in interface slender.services.core.tasks.
TasksService
addUser(Users)
- Method in class slender.services.core.users.impl.
UsersServiceImpl
addUser(Users)
- Method in interface slender.services.core.users.
UsersService
addUserToProject(Integer, Integer)
- Method in class slender.services.core.users.impl.
UsersServiceImpl
addUserToProject(Integer, Integer)
- Method in interface slender.services.core.users.
UsersService
addUserToTask(Integer, Integer)
- Method in class slender.services.core.users.impl.
UsersServiceImpl
addUserToTask(Integer, Integer)
- Method in interface slender.services.core.users.
UsersService
ATTACHMENTS_PATH
- Static variable in class slender.services.core.constants.
Constants
Folder for the attachments
authenticate(String, String)
- Method in class slender.services.core.accounts.impl.
UserAuthenticationServiceImpl
Allows an user to be authenticated.
authenticate(String, String)
- Method in interface slender.services.core.accounts.
UserAuthenticationService
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Index
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Find out more...
Elephant Carpaccio
Order
Pick a product
{{product.name}}
${{product.price}}
Enter a quantity
Shipping Address
Select a state
{{state.display}} ({{state.code}})
Pricing
Price before taxes
${{priceBeforeTaxes()}}
Price after taxes
No pricing engine found - we can't sell :(
Compute Total Price
{{$index+1}}. {{engine.name}}
${{data.cart.prices[engine.id].totalPrice}}
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| File Name | Subject | Date & Time Uploaded | Uploaded By | |
|---|---|---|---|---|
| English-Module-6 | English | 2015-12-04 11:59:30 | Jakey Fausto |
|
| English-Module-5 | English | 2015-12-04 11:45:06 | Jeo Marcos |
|
| Math-Module-5 | Math | 2015-12-01 21:22:23 | Pau Era |
|


This specification defines APIs to get the driving information from an automotive device.
Summary of Methods
Interface
Method
MotorObject
Motor
MotorAPIError
ErrorCallback
void onerror(MotorAPIError error)
Introduction
The motor modules are :
info
status
hvac
drive
security
application
traffic
Access to the modules is provided through the interfaces :
motor.info
motor.status
motor.hvac
motor.drive
motor.security
motor.application
motor.traffic
Interfaces
MotorObject
Defines the motor interface as part of the window global object.
The motor interface will be always available within the Window object in the ECMAScript hierarchy.
readonly attribute Motor motor
Motor
Root interface.
This is the Automotive root interface that is part of the ECMAScript global object as a property as specified by the MotorObject interface.
MotorAPIError
Generic error interface.
This interface will be used by the APIs in order to throw errors synchronously or return them in the error callbacks of asynchronous methods.
The error codes defined in this interface the ones defined by the DOM Level 3 specification with some additions.
APIs may extend the list of error codes with module-specific ones through the use of the [Supplemental] WebIDL keyword. API specific error numbers start from 100 in order to avoid collision with future DOM Error codes
readonly attribute short code
readonly attribute DOMString message
const short UNKNOWN_ERR = 0
Generic error code
const short INDEX_SIZE_ERR = 1
const short DOMSTRING_SIZE_ERR = 2
const short HIERARCHY_REQUEST_ERR = 3
const short WRONG_DOCUMENT_ERR = 4
const short INVALID_CHARACTER_ERR = 5
const short NO_DATA_ALLOWED_ERR = 6
const short NO_MODIFICATION_ALLOWED_ERR = 7
const short NOT_FOUND_ERR = 8
const short NOT_SUPPORTED_ERR = 9
If the implementation does not support the requested object type or operation.
const short INUSE_ATTRIBUTE_ERR = 10
const short INVALID_STATE_ERR = 11
const short SYNTAX_ERR = 12
const short INVALID_MODIFICATION_ERR = 13
const short NAMESPACE_ERR = 14
const short INVALID_ACCESS_ERR = 15
const short VALIDATION_ERR = 16
const short TYPE_MISMATCH_ERR = 17
If the object type is incompatible with the expected type of the parameter associated to the object.
const short SECURITY_ERR = 18
If an attempt is made to perform an operation or access data in a way that presents a security risk or a violation of the user agent security policy.
const short NETWORK_ERR = 19
If a network error occurs in synchronous requests.
const short ABORT_ERR = 20
const short TIMEOUT_ERR = 21
If the operation timed out and was not completed.
const short INVALID_VALUES_ERR = 22
If the content of an object does not contain valid values.
ErrorCallback
Generic error callback interface.
This callback may be used by those functions that only require an error as input parameter in the error callback.
void onerror(MotorAPIError error)
Method that is invoked when the error occurs.
Features
When the feature
http://hyundai.com/api/motor
or any of the features hierarchically under that feature is successfully requested, the interface Motor is instantiated, and the resulting object appears in the global namespace as window.motor.
This is the list of URIs used to declare this API's features, for use in the widget config.xml. For each URL, the list of functions covered is provided.
http://hyundai.com/api/motor
Access to the automotive device APIí»s base module.


Pass Attractions
Home
(current)
Add customer
Passes
New Customer
My Passes
Vendor
Create Vendor
Company address
Email
Company name
Submit
Create Pass
Pass City
Pass length
Vendor id
Submit


Ashley is a senior at The Young Women's Leadership School of East Harlem located in upper Manhattan. She has an immense love for New York City, where she was born and raised.
Ashley plans on majoring in computer science in hopes of becoming a software engineer who can contribute to the effort being made to solving the problems of tomorrow. She also appreciates the power of language and wants to study languages and cultures more thoroughly in the future. Ashley is fluent in English and Spanish and is studying Korean and Spanish on her own!
I worked on an application called Storybook that would improve User Interface development for Software Engineers at American Express. With this app, you can see changes to your projects live, making it easier to integrate React componets and make changes to your IU without committing and pushing any of your work!
What's your favorite song? Submit its name, artist, MP3 and image URL to add it to my playlist! Press the X's to delete songs off of this playlist!
What will you choose? First to 10 wins. Can you beat the computer...? For this game, I learned how to use Comparison and Logical operators that helped determine the winner by comparing their choice to the object it wins or loses against
A GIF for every occasion! In this project, I explored and experimented with APIs. The gifs are derived from GIPHY's API
As an intern at the OSIRIS lab, I partnered with a PhD student of NYU Tandon School of Engineering whose project was an android application that proves the integrity of digital evidence
heTay igPay atinizerLay ashay ouryay ackbay! The PigLatinizer is a Minimum Viable Product (MVP) that comprises new methods I learned, such as split() and slice() that Pig Latinize the user's input
Never let important decisions go unanswered. This Magic 8 Ball was created during my first year of being introduced to coding. I implemented a new function called Math.random() that returns a pseudo-random number in the range 0–1 (inclusive of 0, but not 1) to generate a random response to the user's concern
One word. Six letters. One Life. This game of hangman was also created during the time I was being introduced to Computer Science. Here, I used an array to store the images which change when a letter is guessed
I was introduced to Computer Science as a freshman through Snap! Our first project was to create a videogame, so I built a Super Smash Bros parody. Press the green flag to start playing and press the space bar to jump over Meta Knight!


The miniature electrostatic analyzer (MESA) obtained data on the neutral density of the
atmosphere in the altitude range of 120 to 400 km from the measurements of satellite deceleration due
to aerodynamic drag. The instrument consisted of three single-axis accelerometers, mounted mutually at
right angles, two in the spacecraft X-Y plane and the other along the Z-axis. The instrument determined
the applied acceleration from the electrostatic force required to recenter a proof mass. The output of
the device was a digital pulse rate proportional to the applied acceleration. The measurements allowed
determination of the density of the neutral atmosphere, monitored the thrust of the orbit-adjust
propulsion system (OAPS), determined the satellite minimum altitude, measured spacecraft roll, and
provided some attitude-sensing information. Spacecraft nutations of less than 0.01 deg were monitored.
The instrument had three sensitivity ranges: 8.E-3 earth's gravity (G) in OAPS monitor mode; 4.E-4 G
between 120 (plus or minus 2%) and 280 km (plus or minus 10%); and 2.E-5 G between 180 km (plus or minus 2%)
and 400 km (plus or minus 10%). Numbers in parentheses represent errors; in addition, there may be a
systematic error of up to plus or minus 5% due to drag coefficient uncertainty. The highest measurement
altitude was determined assuming the instrument could sense to 0.2% of full scale. More details can be
found in K. S. W. Champion et al., Radio Sci., v. 8, n. 4, p. 297, 1973. NSSDC has all the useful
data that exist from this investigation.
Version:2.0.0
The miniature electrostatic analyzer (MESA) obtained data on the neutral density of the
atmosphere in the altitude range of 120 to 400 km from the measurements of satellite deceleration due
to aerodynamic drag. The instrument consisted of three single-axis accelerometers, mounted mutually at
right angles, two in the spacecraft X-Y plane and the other along the Z-axis. The instrument determined
the applied acceleration from the electrostatic force required to recenter a proof mass. The output of
the device was a digital pulse rate proportional to the applied acceleration. The measurements allowed
determination of the density of the neutral atmosphere, monitored the thrust of the orbit-adjust
propulsion system (OAPS), determined the satellite minimum altitude, measured spacecraft roll, and
provided some attitude-sensing information. Spacecraft nutations of less than 0.01 deg were monitored.
The instrument had three sensitivity ranges: 8.E-3 earth's gravity (G) in OAPS monitor mode; 4.E-4 G
between 120 (plus or minus 2%) and 280 km (plus or minus 10%); and 2.E-5 G between 180 km (plus or minus 2%)
and 400 km (plus or minus 10%). Numbers in parentheses represent errors; in addition, there may be a
systematic error of up to plus or minus 5% due to drag coefficient uncertainty. The highest measurement
altitude was determined assuming the instrument could sense to 0.2% of full scale. More details can be
found in K. S. W. Champion et al., Radio Sci., v. 8, n. 4, p. 297, 1973. NSSDC has all the useful
data that exist from this investigation.
| Role | Person | |
|---|---|---|
| 1. | PrincipalInvestigator | spase://SMWG/Person/Kenneth.S.W.Champion |
Information about the Atmospheric Density Accelerometer (MESA) experiment on the AE-C mission.
Detailed information about the Atmospheric Density Accelerometer experiment on the AE-C mission.


WHIPPING THE HAKE.
IT is not improbable that the saying applied to the people of one of the Cornish fishing-towns, of" Who whipped the hake ?" may be explained by the following :--
"Lastly, they are persecuted by the hakes, who (not long silence) haunted the coast in great abundance; but now being deprived of their wonted bait, are much diminished, verifying the proverb, 'What we lose in hake we shall have in herring'." - Carew, Survey, p. 34.
Annoyed with the hakes, the seiners may, in their ignorance have actually served one of those fish as indicated.


If this wasn't on your Halloween playlist, then what were you even doing?

If this wasn't on your Halloween playlist, then what were you even doing?
Image via Pat Loika/Flickr


{% extends 'registration/registration_base.html' %} {% block subtitle %}Password Reset{% endblock %} {% block page_header %} Reset your password {% endblock %} {% block page_body %} {% if form.non_field_errors %}
Forgot your password? Enter the email address you registered with we will send you instructions for creating a new one.
{% endblock %}


{% load static %}
Comments
{% load static %}
Return
Main
My Groups
Logout
You are showing selected event comments
TimeStamp
Event
Time taken
Approval status
{% for item in event %}
{{ item }}
{% endfor %}
TimeStamp
By(username)
Comment
{% for TimeStamp,RelatedUser,CommentText in Comments %}
{{ TimeStamp }}
{{ RelatedUser }}
{{ CommentText }}
{% endfor %}
{% csrf_token %}
Comment
ADD


Accounts
{{person.accounts.length}}
Gross
£{{person.gross}}
Expenses
£{{person.totalExpenses}}
Net
£{{person.net}}
This person is not found!


--- permalink: /404.html layout: default title: 404 - Page Not Found ---
Sorry, the page you're looking for is missing or does not exist.


org.apache.axis.wsdl.fromJava
Class ParamRep
java.lang.Object
|
+--org.apache.axis.wsdl.fromJava.BaseRep
|
+--org.apache.axis.wsdl.fromJava.ParamRep
- public class ParamRep
- extends BaseRep
ParamRep is the representation of a class used inside the Java2WSDL
emitter. The information in the ParamRep can be changed by
user provided code to affect the emitted wsdl file. (See ClassRep)
- Author:
- Rich Scheuerle<EMAIL_ADDRESS>|
Field Summary |
static short |
IN
|
static short |
INOUT
|
static short |
OUT
|
|
Constructor Summary |
ParamRep(java.lang.String name,
java.lang.Class type,
short mode)
Constructor
Create a representation of ParamRep |
| Methods inherited from class java.lang.Object |
clone, equals, finalize, getClass, hashCode, notify, notifyAll, toString, wait, wait, wait |
IN
public static short IN
OUT
public static short OUT
INOUT
public static short INOUT
ParamRep
public ParamRep(java.lang.String name,
java.lang.Class type,
short mode)
- Constructor
Create a representation of ParamRep
- Parameters:
cls
- Class to use to create default ParamRep
getName
public java.lang.String getName()
- Getters/Setters
setName
public void setName(java.lang.String name)
getType
public java.lang.Class getType()
setType
public void setType(java.lang.Class cls)
getMode
public short getMode()
setMode
public void setMode(short mode)
Copyright © 2001 Apache XML Project. All Rights Reserved.


Invested TRX
Investors
Fixed ROI/Day
You need a Sponsor Address to join
Period: Until 200% of your Active Capital
Updates every single second
Your Wallet Balance: 0 TRX
Referral commission will be transfered to your Deposit Amount directly.
Each day you will have fixed 2.5% Recover Of Investment to make you increase your earnings.
Get +100% interest from your active capital. You will recover your active capital while earning interest.
10% comission will be shared in 5 levels of referrals. Referral comissions will increase your total active capital for more daily profit and to help system’s sustainability.
Fully Verified and Open Source Smart Contract. Extremely Huge Sustainable System.
1st level: 4%2nd level: 3%3rd level: 1%4th level: 1%5th level: 1%
Referral comissions will increase your total Active Capital for more daily profit and to help system’s sustainabilityTron Flow Plus - It is an open source ROI platform that is 100% transparent and fair to all users. This is a smart contract on the Tron Blockchain. All you have to do is deposit and reinvest or withdraw your profits. You will get profits every second until there is no money in the contract. Invest more TRX to earn more profits. You can refer people to this smart contract and earn referral commission up to 5 levels.


@main("UMBooks") {
Most students spend around $1200 on textbooks per year. Don't be like most students. Save big on textbooks.
Use the form below to fill out the information for the book you'd like to sell


Juno <IP_ADDRESS> is a major update.
- New @RestChild annotation for identifying child resources.
-
New traversable and filterable attributes added to
RestMethod @RestMethod annotation.
Eliminates the need for PojoResource and FilteredRestResource classes.
- Simplified client API. Easier to use when making multiple connections to the same server.
- Support for pluggable authentication in the client API.
- Support for authenticating against Jazz Team Servers.
- Support for rendering package-level Javadocs in REST resources.
- Support for parsing of header values into specific object types.
- Changed default XML representation to not include JSON-type attributes. Produces cleaner XML.
-
New resourceUri attributed added to @Bean annotation to associate beans with resource URIs.
- Used for automatically creating hyperlinks in {@link oaj.html.HtmlSerializer}.
- Used for automatically creating uri attributes in {@link oaj.xml.XmlSerializer}.
- Used for automatically creating rdf:about attributes in RdfXmlSerializer.


Kogi Election: INEC Declares 30 Staff Missing (Full List)
by Philips SundayThe Independent National Electoral Commission (INEC), has declared 30 of its staff missing in the ongoing Kogi Election.
Naija News reports that the INEC ad-hoc staff took part in Saturday’s governorship election in Kogi state, north-central Nigeria.
This online news platform understands that the INEC staff were posted to Olamaboro Local Government Area (LGA) by the commission and were declared missing around 1 a.m. on Sunday during the final collation of results in the local government.
According to the commission, the missing INEC staff include Presiding Officers (POs) and Assistant Presiding Officers (APOs) of polling units in Imane ward 1 and 2 of Olamaboro LGA of Kogi State.
Many of the ad-hoc staff used by INEC are members of the National Youth Service Corps (NYSC).
Announcing the sad incident, the LGA Election Officer, in-charge of collating and announcing the local government’s results, Garba Mahmood, said the INEC ad-hoc staff were reported missing after the observation of some police officers who raised concern that they were last seen shortly after voting ended at 2 p.m. on Saturday.
Mahmood said repeated calls to their telephone numbers did not go through.
He therefore declared them missing and then released the names of the missing persons.
See the list of the missing staff as provided by INEC and the police at the Olamaboro collation centre.
Olamaboro III
Unit 002- (1) Oladipo Victor
(2) Achimi Samson P-08136653704
(3) Umar Faruk Sani-08032745663
(4) Adama Ibrahim
Unit 006- (1) Abayomi Roseline E.
(2) Onuche Abel E
(3) Onojah Emmanuel
(4) Umoru Mariam-
Unit 013- (1) Effiong Akwaowo-Ukpe
(2) Mattew Agada
(3) Samuel Ibrahim
(4) Sado Bello
Imane 1
Unit 006- (1) Nzeofia Kingsley- Presiding Officer (PO)
(2) Hassan Musa- Assistant Presiding Officer 1 (APO 1)
(3) Ekele Michael – Assistant Presiding Officer 2(APO 2)
(4) Ahmed Mattew – Assistant Presiding Officer 3(APO 3 )
Unit 012 -(1) Ovioawho Omonefe B.- Presiding Officer (PO)
(2) Baba Eric -Assistant Presiding Officer 1 (APO 1)
(3) Gabriel Samuel Assistant Presiding Officer 2 (APO 2)
Unit 015-(1) Nwafor Emmanuel- Presiding Officer (PO)
(2) Agada Ochegeugwa- Assistant Presiding Officer 1(APO 1)
(3) Ojih Martina- Assistant Presiding Officer 2(APO 2)
Unit 016 (1) Ezugwu Stanley- Presiding Officer (PO)
(2) Mohammed Abdullahi- Assistant Presiding Officer 1(APO 1)
(3) Mohammed Ibrahim- Assistant Presiding Officer 2(APO 2)
(4) Adejoh Joy- Assistant Presiding Officer 3(APO 3)
Unit 022 (1) Adebisi Comfort – Presiding Officer (PO)
(2) Yusuf Sofiat- Assistant Presiding Officer 1(APO 1)
(3) Onoja Alice- Assistant Presiding Officer 2(APO 2)
(4) Onuche Vincent- Assistant Presiding Officer 3(APO 3).


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Enter valid email
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These lists discuss frontier scientific, technological and philosophical concepts, futurist philosophy, promote ideas of liberty, economic freedom, various alternative intellectual activities and lifestyles, advanced educational methods, etc.
I recommend you to look into the
full ASCII version of this guide for more detailed descriptions of
publicly advertised interesting mailing lists as well as info on many lists
that are not publicly advertised.
[Some of the information in the ascii guide
may be no longer valid, as I haven't updated it in a while]
Here, you can directly access information on the following mailing lists:
For a comprehensive guide on mailing lists, I recommend you to look at E-mail Discussion Groups list from Interlinks.
A list of mailing lists that are run for free (with commercial ads at ther end of each message) can be found at www.onelist.com You can also use this service to start your own mailing list.
And finally, there are Two mailing lists where I share my own ideas with self-selected groups of subscribers.
If you need a private access to your mail from anywhere in the world, consider using Hushmail - a fully encrypted free email service.
If you already have a mailing list, you may consider using Critmail to make your archives available in linked hypertext form.
Please e-mail me at<EMAIL_ADDRESS>if you want me to add something to this list or have any comments.
I would also recommend you to visit the ListWebber which allows you to search through messages of many good mailing lists.


git-upload-archive - Send archive back to git-archive
git upload-archive <directory>
Invoked by git archive --remote and sends a generated archive to the other end over the Git protocol.
This command is usually not invoked directly by the end user. The UI for the protocol is on the git archive side, and the program pair is meant to be used to get an archive from a remote repository.
In order to protect the privacy of objects that have been removed from history but may not yet have been pruned, git-upload-archive avoids serving archives for commits and trees that are not reachable from the repository(cqs refs. However, because calculating object reachability is computationally expensive, git-upload-archive implements a stricter but easier-to-check set of rules:
h'-04' 1.h'+01'c
Clients may request a commit or tree that is pointed to directly by a ref. E.g., git archive --remote=origin v1.0.
h'-04' 2.h'+01'c
Clients may request a sub-tree within a commit or tree using the ref:path syntax. E.g., git archive --remote=origin v1.0:Documentation.
h'-04' 3.h'+01'c
Clients may not use other sha1 expressions, even if the end result is reachable. E.g., neither a relative commit like master^ nor a literal sha1 like abcd1234 is allowed, even if the result is reachable from the refs.
Note that rule 3 disallows many cases that do not have any privacy implications. These rules are subject to change in future versions of git, and the server accessed by git archive --remote may or may not follow these exact rules.
If the config option uploadArchive.allowUnreachable is true, these rules are ignored, and clients may use arbitrary sha1 expressions. This is useful if you do not care about the privacy of unreachable objects, or if your object database is already publicly available for access via non-smart-http.
<directory>
The repository to get a tar archive from.
Part of the git(1) suite


Trim extreme values from an atomic vector, and replace with a specific value (typically NA_*
).
trim_numeric(x, bounds=c(-Inf, Inf), replacement=NA_real_) trim_integer(x, bounds=c(-2147483647L,<PHONE_NUMBER>L), replacement=NA_integer_) trim_date( x, bounds = as.Date(c("1940-01-01", "2029-12-31")), replacement = as.Date(NA_character_) )
| x | The input vector to be trimmed. Required |
|---|---|
| bounds | A two-element vector that establishes the lower and upper inclusive bounds of |
| replacement | A scalar that will replace all instances of |
An atomic vector with the same number of elements as x
.
The data type of x
, bounds
, and replacement
must match the atomic data type of the function.
In other words, trim_numeric()
accepts only parameters of type 'numeric' (otherwise known as
'double-precision floating point'). Likewise, trim_date()
accepts only parameters of type Date
.
The lower bound must be less than or equal the upper bound.
The default bounds for numerics and integers are at the extremes of the data type. The default bounds for dates are arbitrary, because the origin is slippery.
#> [1] 4.073051 NA NA 4.847309 4.430007 7.572395 NA 6.847370 #> [9] NA NA#> [1] NA NA NA NA 4 5 6 7 8 NA NAtrim_date( x = as.Date(c("1902-02-02", "1999-09-09", "2020-02-22", "1930-01-01", "1930-01-02")), bounds = as.Date(c("1990-01-01", "2030-01-01")) )#> [1] NA "1999-09-09" "2020-02-22" NA NAtrim_datetime( x = as.POSIXct(c("1902-02-02", "1999-09-09", "2020-02-22", "1930-01-01", "1930-01-02")), bounds = as.POSIXct(c("1990-01-01", "2030-01-01")) )#> [1] NA "1999-09-09 CDT" "2020-02-22 CST" NA #> [5] NA


Welcome to Type Racer
Type this text as quick as possible. Then press enter to finish typing.
Your time
Play Again


m.redraw
Redraws the view for the currently active module. Use m.module()
to activate a module.
This method is called internally by Mithril's auto-redrawing system. Usually you don't need to call it manually unless you are doing recurring asynchronous operations (i.e. using setInterval
) or if you want to decouple slow running background requests from the rendering context (see the background
option in m.request
.
By default, if you're using either m.route
or m.module
, m.redraw()
is called automatically by Mithril's auto-redrawing system once the controller finishes executing.
m.redraw
is also called automatically on event handlers defined in virtual elements.
Note that calling this method will not do anything if a module was not activated via either m.module()
or m.route()
. This means that m.redraw
doesn't do anything when instantiating controllers and rendering views via m.render
manually.
If there are pending m.request
calls in either a controller constructor or event handler, the auto-redrawing system waits for all the AJAX requests to complete before calling m.redraw
.
This method may also be called manually from within a controller if more granular updates to the view are needed, however doing so is generally not recommended, as it may degrade performance. Model classes should never call this method.
If you are developing an asynchronous model-level service and finding that Mithril is not redrawing the view after your code runs, you should use m.startComputation
and m.endComputation
to integrate with Mithril's auto-redrawing system instead.
Changing redraw strategy
If you need to change how Mithril performs redraws, you can change the value of the m.redraw.strategy
getter-setter to either "all"
, "diff"
or "none"
. By default, this value is set to "all"
when running controller constructors, and it's set to "diff"
for all subsequent redraws.
var module1 = {}
module1.controller = function() {
//this module will attempt to diff its template when routing, as opposed to re-creating the view from scratch.
//this allows config contexts to live across route changes, if its element does not need to be recreated by the diff
m.redraw.strategy("diff")
}
module1.view = function() {
return m("h1", {config: module1.config}, "test")
}
module1.config = function(el, isInit, ctx) {
if (!isInit) ctx.data = "foo"
}
Preventing redraws on events
Similarly, it's possible to skip redrawing altogether by calling m.redraw.strategy("none")
m("input", {onkeydown: function(e) {
if (e.keyCode == 13) ctrl.save() //do things and re-render only if the `enter` key was pressed
else m.redraw.strategy("none") //otherwise, ignore
}})
Signature
void redraw() { GetterSetter strategy }
where:
GetterSetter :: String getterSetter([String value])
-
m.redraw.strategy
GetterSetter strategy
The
m.redraw.strategy
getter-setter indicates how the next module redraw will occur. It can be one of three values:"all"
- recreates the DOM tree from scratch"diff"
- updates only DOM elements if needed"none"
- leaves the DOM tree intact
This value can be programmatically changed in controllers and event handlers to modify the next redrawing strategy. It is modified internally by Mithril to the value
"all"
before running controller constructors, and to the value"diff"
after all redraws.Calling this function without arguments returns the currently assigned redraw strategy.


Blacksmith Silvera:
Sorry! You are not yet qualified to be an Artisan. I warn you: it is not an easy path. To even take the test, you must first meet certain minimum qualifications. Gain more experience. Then return to me after you have reached at least level 18.


xx
{{message}}
Title
Paragraph 1
Paragraph 2
Title111
Paragraph 111
Paragraph 222
Username
Email
Username
Email
{{index}} - {{item.message}}
aaaaa
bbbbb
ccccc
123


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Field Documentation
etByte
et_info::base
etByte
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etByte
et_info::flags
char
et_info::fmttype
etByte
et_info::prefix
etByte
et_info::type
The documentation for this struct was generated from the following files:
deps/sqlite/
sqlite3.c
deps/sqlite-3.7.3/
sqlite3.c
Generated on Wed Jul 20 01:03:41 2011 for upkeeper by
1.4.7


The quality of protection determines the level of security that is used when sending and receiving messages. Microsoft Digest selects a level based on the requirements of the client and server.
When using Digest as a SASL mechanism, applications can specify that messages be kept confidential using encryption. The server specifies the ciphers it supports for encrypted messages, and the client selects a cipher from this list.
The following topics discuss these security mechanisms in detail:
Quality of Protection
Ciphers


Patterns
A pattern represents an ordered series of Expressions that evaluate into notes or chords when used inside a Clip. The basic idea is that when describing patterns of notes in Warp, you just type in simple text expressions. Warp then evaluates these and they become notes.
Expressions can be very simple lists of notes or chords, or they can also include more complex modifiers. When starting out, just learn to type in notes and chords -- once you get those working, you can try Modifier Expressions and then Transforms, which are basically a kind of MIDI effect.
In addition to the text (notes) in the pattern:
- A pattern may also define a tempo multiplier rate such as 0.5 (half speed) or 2 (double speed).
- A pattern may optionally define a Scale to override the scale of the Scene or Song, which is used if not overridden by the Clip.
A Quick Example
Patterns will make more sense if we show some examples. The simplest possible pattern is a scale:1
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I
IV
V
i
iv
v
1
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1
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C4
D4
F6
Eb5
F#7
F0
A3