A tag is a keyword or label that categorizes your question with other, similar questions. Using the right tags makes it easier for others to find and answer your question.
| Type to find tags: |
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tomcat× 28789
Apache Tomcat (or simply
Tomcat, formerly also Jakarta Tomcat) is an open source Servlet
Container and is developed by the Apache Software Foundation (ASF).
|
haskell× 28080
an advanced functional
programming language, featuring strong static typing, lazy evaluation,
extensive parallelism and concurrency support, and unique abstraction
capabilities.
|
facebook-graph-api× 27940
a structured API for fetching objects and the connections between them from Facebook's social graph
|
url× 27870
a Uniform Resource
Identifier (URI) that specifies where an identified resource is
available and the mechanism for retrieving it.
|
|
silverlight× 27699
Microsoft's cross-browser, cross platform plug-in for media experiences and rich interactive applications.
|
firefox× 27653
a free, open source and cross-platform web browser created by Mozilla.
|
hadoop× 27618
an Apache open-source
project that provides software for reliable and scalable distributed
computing. The project itself includes a variety of other complementary
additions.
|
authentication× 27414
the process of determining whether someone or something is, in fact, who or what it is declared to be.
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|
winapi× 27385
The Windows API (formerly
called the Win32 API) is the core set of application programming
interfaces available for the Microsoft Windows operating systems. This
tag is for questions about developing …
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amazon-web-services× 27288
a collection of commercial
services centered around virtualized, commodity and clustered computing,
networking, database and storage, as well as supporting tools that are …
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pdf× 26968
an open standard for
electronic document exchange maintained by the International
Organization for Standardization (ISO). Questions can be about creating,
reading, ed…
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animation× 26440
the rapid display of a sequence of visuals in order to create an illusion of movement or change.
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generics× 26427
a form of parametric polymorphism found in a range of languages, including .NET languages, Java and in Swift.
|
android-fragments× 26377
Fragments represent reusable behaviors or portions of user interface in an Android app.
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cakephp× 26323
a rapid development
framework for PHP that provides an extensible architecture for
developing, maintaining, and deploying applications. It uses commonly
known design patterns like MVC and O…
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if-statement× 26166
a control structure in many programming languages that changes the execution flow depending on a condition.
|
|
jpa× 26127
a Java specification for
accessing, persisting, and managing data between Java objects/classes
and a relational database. It is part of the EJB 3.0 specification and …
|
events× 25960
a way for a class to provide notifications to listeners when a particular thing happens.
|
opengl× 25953
a graphics standard and API
which is platform independent and available for desktop, workstation
and mobile devices. It is designed to provide hardware-accelerated
rendering, and hence gives…
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redirect× 25871
A response by a webserver, that asks the user agent to not show the response body, but instead request a different resource.
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|
exception× 25774
a rarely occurring
(exceptional!) condition that requires deviation from the program's
normal flow. Normally, an exception should not result in total failure,
but instead be attended b…
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numpy× 25724
a scientific and numerical computing extension to the Python programming language.
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for-loop× 25655
a control structure used by
many programming languages to iterate over a range. It is a way of
repeating statements a number of times until the loop ends. Depending on
the language this …
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servlets× 25632
programs that run on a Web
or Application server and act as a middle layer between a request coming
from a Web browser or other HTTP client and databases or applications
on the HTTP serve…
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android-studio× 25463
Use for questions about
using Android Studio, an official IDE targeted at Android development.
Do NOT use for questions about programming for Android in general;
instead use [android].
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mod-rewrite× 25437
URL rewriting module for
the Apache web server. It is commonly used for so-called "pretty" URLs,
but also provides the power and flexibility to perform various request
handling tasks beyond simple sub…
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table× 25287
ambiguous. Use nothing for
SQL questions, for html use `html-table`, for css use `css-tables`. Read
the tag wiki for more alternate tag suggestions.
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grails× 25121
an Open Source, full stack,
web application framework that uses the Groovy programming language
(which is in turn based on the Java virtual machine (JVM) and Java. The
framework is oriented …
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|
dictionary× 24993
a data structure that maps
keys to values such that given a key its corresponding value can be
efficiently retrieved. For questions about Mapping Functions over col…
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ssl× 24807
a cryptographic protocol
that provides secure communications over the Internet. Often, SSL is
used as a blanket term and refers to both the SSL protocol and the
Transport…
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inheritance× 24767
the system in object
oriented programming that allows objects to support operations defined
by anterior types without having to provide their own definition. It is
the major vector for …
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java-ee× 24700
a specification defining a
collection of Java-based server and client technologies and how they
interoperate. The [java-ee] tag is rudimentary on focused questions…
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|
xslt× 24695
a transformation language
for XML designed to transform structured documents into other formats
(such as XML, HTML, and plain text). Questions should use one of the
xslt-1.0, xslt-2.0, or xslt…
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caching× 24625
a mechanism for temporarily
storing (caching) data locally in order to reduce access time to data
stored far away. For CPU/disk/web browsing please use relevant tags
(cpu-cache, diskcache,.…
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pandas× 24503
a Python library for Panel
Data manipulation and analysis, e.g. multidimensional time series and
cross-sectional data sets commonly found in statistics, experimental
science results, econome…
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dom× 24461
on questions regarding the
interaction of other languages with XML/HTML via the document object
model. Do not use it as shorthand for HTML, JavaScript, or SAX—use
additional tags to denot…
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A lightweight, easy to use, open-source (MIT license) clustering library for use with the Google Maps JavaScript API. It was inspired by the excellent MarkerClusterer library. Compared to MarkerClusterer, this library offers less flexibility, but has two distinct advantages:
If you like the library and have time, consider contributing to it!
View a live demo here!
This library uses many modern JavaScript features, and so requires a modern browser to run:
This library depends on the following 2 libraries to run:
underscore.js
. A lightweight and popular utility library used for a lot of the heavy computation. Get it here.Google Maps JavaScript API
. A pretty obvious requirement, although the heavy lifting is decoupled allowing for the future possibility of using it with other mapping libraries.Follow the steps below and start clustering away in minutes!
Get the source code. There are three JS files you’ll need: aj-clusterer-min.js
, aj-clusterer-async-min.js
, and aj-geometry-min.js
. They are all in the repository. They are minified to minimize download time. You are also welcome to exchange them for the non-minified versions. They are the same.
Load aj-clusterer.js and its dependencies in your page. Don’t load aj-clusterer-async-min.js
or aj-geometry-min.js
. These are used by background threads and are not used directly.
#######
####### var mapOptions = { center: { lat: 26.397, lng: –81.0}, zoom: 6, minZoom: 3 };
map = new google.maps.Map(document.getElementById('map-canvas'), mapOptions);
aj-clusterer-async-min.js
, aj-geometry-min.js
and underscore.js
. Background threads managed by the Clusterer will reference these URLs when they’re doing their work.####### var clusterer = new aj.geometry.Clusterer(map, delegate, “/path/to/aj-clusterer-async-min.js”, “/path/to/aj-geometry-min.js”, “/path/to/underscore-min.js”);
[lat, lon]
arrays). You can optionally add an object as the 3rd item of a coordinate to identify it when it is passed back to the delegate. If you do add an object, keep it small to maximize performance. (more info in the next steps).####### var coordinates = [ [26, –81, {name: ‘Miami’, country: ‘US’}], [27, –81, {name: ‘Ft. Lauderdale’, country: ‘US’}], [35, 139, {name: ‘Tokyo’, country: ‘JP’}], [2, 41, {name: ‘Barcelona’ country: ‘ES’}] ]
clusterer.addCoordinates(coordinates); //And they will magically appear on the map!
####### var infoWindow = new google.maps.InfoWindow({});
var delegate = {
didSelectCluster: function (clusterer, cluster, googleMarker) {
infoWindow.open(map, googleMarker); //See the reference for details on didSelectCluster.
}
};
//Rest of code goes here.
Clusterer
class, and how you can use it to dynamically change its behavior.


Quick Start
WordPress Information
To install this theme you must have a working version of WordPress already installed. If you need help installing WordPress, follow the instructions in WordPress Codex. Below are all the useful links for WordPress information.
- WordPress Codex – General info about WordPress and how to install on your server
- First Steps With WordPress – General info about multiple topics about WordPress.
- FAQ New To WordPress – The most popular FAQ’s regarding WordPress.
Hosting recommendation:
We recommending hosting with cPanel. List of popular providers:
http://lpwdev.com/lpw_wordpress/leadingprops.zip
Theme installation:
- Download LPW theme
- Log in to the WordPress Administration Panels.
- Select the Appearance panel, then Themes.
- Select Add New.
- Use the Upload link in the top links row to up load a zipped copy of a Theme that you have previously downloaded to your machine.
Theme setup:
- Activate theme Show image
- Install qtranslate Show image
- Setup qtranslate Show image
Supported locales:
- "ar" - "العربية"
- "en" - "English"
- "fr" - "Français"
- "de" - "Deutsch"
- "ru" - "Русский"
- "cs" - "Čeština"
- "zh" - "简体中文"
- "it" - "Italiano"
- "ja" - "日本語"
- "ko" - "한국어"
- "nb" - "Norwegian Bokmål"
- "th" - "ไทย"
More locales on demand<EMAIL_ADDRESS>- Select the Options -> General panel
Be sure that you follow instructions on all tabs.
- API - URL and Key
- Header - Logo/Phone/Email ...
- Footer - information in footer (like address)
- Social - Social links
- Google services - Google API key. For Google places service (autocomplete). GET A KEY
- Styles - Custom styles
- Scripts - Custom scripts as example analytics scripts (Google analytics)
- Default locations can be assigned to show on index page. Show image
Important:
LPW theme creating default pages (Pages panel). This pages created to assign scripts to list property objects from our API, and holding URL routing
Don't delete this pages. You can recreate or reassign this pages in Advanced options, but we aware you from this. Especially if you site is already in production.
Theme development
Be sure that you are using latest version of theme (check theme update in dashboard).
Our platform is on stage of active development and improvements. And our Wordpress theme updating too, to use all features of platform.
We don't recommending to change core files of our theme, because this changes will be rewrited on update.
Wordpress following this way too, and they have solution - Wordpress Child Themes.
Please follow documentation provided by Wordress for Child Theme development. Wordpress Child Themes.
We already create base child theme for easy start. You can download it here.
http://lpwdev.com/lpw_wordpress/lpw-wordpress-child-theme.zip
Support
Be sure that you are using latest version of theme (check theme update in dashboard).
For questions about theme installation please mail<EMAIL_ADDRESS>License
MIT License Copyright (c) 2016 The Leading Properties of the World Permission is hereby granted, free of charge, to any person obtaining a copy of this software and associated documentation files (the "Software"), to deal in the Software without restriction, including without limitation the rights to use, copy, modify, merge, publish, distribute, sublicense, and/or sell copies of the Software, and to permit persons to whom the Software is furnished to do so, subject to the following conditions: The above copyright notice and this permission notice shall be included in all copies or substantial portions of the Software.  IN NO EVENT SHALL THE AUTHORS OR COPYRIGHT HOLDERS BE LIABLE FOR ANY CLAIM, DAMAGES OR OTHER LIABILITY, WHETHER IN AN ACTION OF CONTRACT, TORT OR OTHERWISE, ARISING FROM, OUT OF OR IN CONNECTION WITH THE SOFTWARE OR THE USE OR OTHER DEALINGS IN THE SOFTWARE.


--- layout: post title: "Gutsy is HERE!" date: 2007-10-18 15:35:27 +0000 permalink: /2007/10/18/gutsy-is-here/ category: Linux redirect_from: - /blog/gutsy-is-here/ ---
Ubuntu Linux 7.10, the "Gutsy Gibbon", has arrived! The mirrors are being hammered, so please use the torrents if possible. Downloads are at: http://www.ubuntu.com/getubuntu/download. This version of Ubuntu Linux comes with several nice features in addition to the stability that Ubuntu is known for.


Thanks!
This project couldn't happen with out you. We really can't say thanks enough! You are #1 in our book. As a small token of our gratitude, here's a video of a pale kid rapping fast:


|
|
CIFXOctreeCollection Class ReferenceInheritance diagram for CIFXOctreeCollection:
List of all members.
|
Public Member Functions |
| IFXRESULT | Initialize (IFXVector4 worldBound=IFXVector4(0, 0, 0, 1024.0), F32 k=1, U32 maxD=4) |
| COctreeNode * | GetRootNode () const |
| F32 | GetWorldSize () const |
| U32 | GetMaxDepth () const |
| F32 | GetLooseK () const |
| U32 | Insert (IFXSpatial *o, U32 Instance) |
| U32 | Insert (COctreeNode *q, IFXSpatial *pInSpatial, U32 Instance) |
| void | TraverseNodes (COctreeNode *on, void(*nf)(COctreeNode *on)) |
| void | TraverseNodes (COctreeNode *on, void(*nf)(COctreeNode *on, void *data)) |
| void | TraverseNodes (COctreeNode *on, void(*pre)(COctreeNode *on), void(*post)(COctreeNode *on)) |
| void | TraverseTree (void(*nf)(COctreeNode *on)) |
| U32 IFXAPI | AddRef () |
| U32 IFXAPI | Release () |
| IFXRESULT IFXAPI | QueryInterface (IFXREFIID interfaceId, void **ppv) |
| IFXRESULT IFXAPI | InitializeCollection (IFXSpatial **pInSpatials, U32 uInNumberOfSpatials, IFXSpatial::eType eIntype) |
| IFXRESULT IFXAPI | InitializeCollection (IFXCollection *pInCollection) |
| IFXRESULT IFXAPI | AddSpatials (IFXSpatial **pInSpatials, U32 uInNumberOfSpatials, IFXSpatial::eType eIntype) |
| IFXRESULT IFXAPI | RemoveSpatials (IFXSpatial **pInSpatials, U32 uInNumberOfSpatials, IFXSpatial::eType eIntype) |
| IFXRESULT IFXAPI | GetSpatials (IFXSpatial **&rpOutSpatials, U32 &ruOutNumberOfSpatials, IFXSpatial::eType eIntype) |
| const IFXGUID & | GetCID () |
Public Attributes |
| U32 * | DepthTotals |
Protected Member Functions |
| IFXRESULT | InCorporateSpatialBound (IFXSpatial **pInSpatials, U32 uInNumberOfSpatials, IFXVector4 &rSphere) |
| BOOL | FitsInBox (const IFXVector4 &inSpatialBound, F32 cx, F32 cy, F32 cz, F32 octHalfSize) const |
| BOOL | FitsInBox (IFXSpatial *o, U32 Instance, const IFXVector4 &c) const |
| BOOL | FitsInBox (const IFXVector4 &in, const IFXVector4 &c) const |
| U32 | InsertRecursivelyIntoBestFitOctreeNode (COctreeNode *q, IFXSpatial *spatial, U32 Instance) |
| void | ResursivelyAddSpatialsToList (COctreeNode *pCurrNode, IFXSpatial **&rpOutSpatials, U32 &ruOutNumberOfSpatials, U32 &ruListStart, IFXSpatial::eType eIntype) |
| | CIFXOctreeCollection () |
| virtual | ~CIFXOctreeCollection () |
| void | CleanUp () |
Protected Attributes |
| IFXVector4 | m_worldBound |
| U32 | m_minDepth |
| U32 | m_maxDepth |
| F32 | m_looseK |
| U32 | m_uRefCount |
| COctreeNode * | m_pRootNode |
| U32 | m_overflowCount |
Friends |
| IFXRESULT IFXAPI_CALLTYPE | CIFXOctreeCollection_Factory (IFXREFIID interfaceId, void **ppinterface) |
Constructor & Destructor Documentation
| CIFXOctreeCollection::CIFXOctreeCollection |
( |
|
) |
[inline, protected] |
|
| CIFXOctreeCollection::~CIFXOctreeCollection |
( |
|
) |
[protected, virtual] |
|
Member Function Documentation
| U32 CIFXOctreeCollection::AddRef |
( |
|
) |
[virtual] |
|
|
|
This method increments the reference count for an interface on a component.
- Note:
- It should be called for every new copy of a pointer to an interface on a given component.
- Returns:
- It returns a U32 that contains a value from 1 to 2^32 - 1 that defines the new reference count. The return value should only be used for debugging purposes.
Implements IFXUnknown. |
|
|
Adds the given spatials from the collection.
- Parameters:
-
| pInSpatials | The list of spatials to add to the collection. |
| uInNumberOfSpatials | The number of spatials in the list. |
| eInType | If this parameter is provided, the type of ALL of the provided spatials is assumed to be eInType. If not specified, each spatial is queryied for it's type separately. |
- Returns:
- One of the following IFXRESULT codes:
- IFX_OK
No error.
- IFX_E_OUT_OF_MEMORY
Not enough memory was available to initialize.
Implements IFXCollection. |
| void CIFXOctreeCollection::CleanUp |
( |
|
) |
[protected] |
|
| BOOL CIFXOctreeCollection::FitsInBox |
( |
const IFXVector4 & |
in, |
|
|
const IFXVector4 & |
c |
|
) |
const [protected] |
|
| BOOL CIFXOctreeCollection::FitsInBox |
( |
const IFXVector4 & |
inSpatialBound, |
|
|
F32 |
cx, |
|
|
F32 |
cy, |
|
|
F32 |
cz, |
|
|
F32 |
octHalfSize |
|
) |
const [protected] |
|
| const IFXGUID& CIFXOctreeCollection::GetCID |
( |
|
) |
[inline, virtual] |
|
| F32 CIFXOctreeCollection::GetLooseK |
( |
|
) |
const [inline] |
|
| U32 CIFXOctreeCollection::GetMaxDepth |
( |
|
) |
const [inline] |
|
| COctreeNode* CIFXOctreeCollection::GetRootNode |
( |
|
) |
const [inline] |
|
|
|
Returns a reference to the spatials, of the given type, within the collection.
- Parameters:
-
| eInType | The type of spatials to be returned from the collection. |
| rpOutSpatials | The address of the list of resultant spatials. |
| ruOutNumberOfSpatials | The number of resultant spatials. |
| eInType | If this parameter is provided, rpOutSpatials will contain only spatials of type specified. |
- Returns:
- One of the following IFXRESULT codes:
Implements IFXCollection. |
| F32 CIFXOctreeCollection::GetWorldSize |
( |
|
) |
const [inline] |
|
| IFXRESULT CIFXOctreeCollection::InCorporateSpatialBound |
( |
IFXSpatial ** |
pInSpatials, |
|
|
U32 |
uInNumberOfSpatials, |
|
|
IFXVector4 & |
rSphere |
|
) |
[protected] |
|
| IFXRESULT CIFXOctreeCollection::InitializeCollection |
( |
IFXCollection * |
pInCollection |
) |
[virtual] |
|
|
|
Initializes the Collection.
- Precondition:
- None; re-initialization is supported.
- Postcondition:
- If a spatial set is provided, the collection will contain these spatials, if not, it will be empty.
- Parameters:
-
| rpInSpatials | A reference to the address of the array of spatials to add to the collection. |
| uInNumberOfSpatials | The number of spatials in the rpInSpatial array. |
| eInType | If this parameter is provided, the type of ALL of the provided spatials is assumed to be eInType. If not specified, each spatial is queryied for it's type separately. |
- Returns:
- One of the following IFXRESULT codes:
- IFX_OK
No error.
- IFX_E_OUT_OF_MEMORY
Not enough memory was available to initialize.
Implements IFXCollection. |
| IFXRESULT CIFXOctreeCollection::QueryInterface |
( |
IFXREFIID |
interfaceId, |
|
|
void ** |
ppv |
|
) |
[virtual] |
|
|
|
This method provides access to the various interfaces supported by a component.
Upon success, it increments the component's reference count and hands back a pointer to the specified interface.
- Note:
- A number of rules must be adhered to by all implementations of IFXAPI QueryInterface . For a list of such rules, refer to the IFXCOM usage guidelines.
- Returns:
- Upon success, IFX_OK is returned. Otherwise, either IFX_E_INVALID_POINTER or IFX_E_UNSUPPORTED are returned.
Implements IFXUnknown. |
| U32 CIFXOctreeCollection::Release |
( |
|
) |
[virtual] |
|
|
|
This method decrements the reference count for the calling interface on a component.
- Note:
- If the reference count on a component falls to zero, the component is destroyed.
- Returns:
- It returns a U32 that contains a value from 1 to 2^32 - 1 that defines the new reference count. The return value should only be used for debugging purposes.
Implements IFXUnknown. |
| void CIFXOctreeCollection::TraverseTree |
( |
void(*)(COctreeNode *on) |
nf |
) |
[inline] |
|
Friends And Related Function Documentation
| IFXRESULT IFXAPI_CALLTYPE CIFXOctreeCollection_Factory |
( |
IFXREFIID |
interfaceId, |
|
|
void ** |
ppinterface |
|
) |
[friend] |
|
Member Data Documentation
© 1999 - 2006 Intel Corporation. All rights reserved.
* Other names and brands may be claimed as the property of others.
|
|


Welcome
A site where your goals and values can move you in the direction of a more essential and minimal lifestyle. Less is more.
Fun
On this site you will experience lots of fun and interactive actions to keep your life simple, yet fun to plan.
Simple
Setting up your account is simple and effective. want to start simplifying your life now? it's free to sign up!
Safe
This is a safe environment where there are no judging of any type. we are here to help you improve your life simply.


Page 1 of 1
My computer just died
Posted:
Sat Apr 18, 2009 11:50 am
by Karl G.
Hey all,
As the title suggests, my compy's fan bit the bucket. All of a sudden it got really loud, so I restarted and...bam, "fan error"
Getting a tech out here on Monday, but I won't be able to do any significant development till then. Or be online tonight like I was planning. :/
Karl
Re: My computer just died
Posted:
Sat Apr 18, 2009 12:39 pm
by Sex4Cash
go to the store and buy a new one, silly! Unless you have some strange-sized custom fan.
Re: My computer just died
Posted:
Sat Apr 18, 2009 1:22 pm
by Joe M.
Bad timing on the part of your computer. There are some wicked bugs right now.
Re: My computer just died
Posted:
Sat Apr 18, 2009 2:06 pm
by Karl G.
Sex4Cash wrote:go to the store and buy a new one, silly! Unless you have some strange-sized custom fan.
It's a laptop.
Joe M. wrote::( Bad timing on the part of your computer. There are some wicked bugs right now.
UGH I did so much testing to make sure the storage would work...it is so weird that this never happened to me. As soon as my computer gets up again, I'll get on it.
Re: My computer just died
Posted:
Sun Apr 19, 2009 4:05 am
by marzuku
Mm4 lost all his gear besides an aurelian plate.
Argent belt
Aurelian gloves
Devine aegis
Wand of Starlight
5 Bj's
all i can remember now
Re: My computer just died
Posted:
Sun Apr 19, 2009 4:22 am
by Sega Rally Pownz
Lost all my gear too -_-
Re: My computer just died
Posted:
Sun Apr 19, 2009 5:18 am
by Skippy
i also lost all my crappy gear
but it was my crappy gear </3
Re: My computer just died
Posted:
Sun Apr 19, 2009 6:23 am
by Joe M.
I'll be on in a few hours, sitting around sq, and on the Ventrilo server. Find me and I can restore your gear.
Re: My computer just died
Posted:
Sun Apr 19, 2009 10:38 am
by sourceofprovidence
yea i lost gear to this, joe restored all my gear pretty much. He's awesome. It was a storage bug, if you pull gear out and log it goes poof. The only item I am missing on my fig is a helm of spite eh joe! haha =D
Re: My computer just died
Posted:
Sun Apr 19, 2009 10:39 am
by sourceofprovidence
Get a Desktop, hehe or my laptop is a Aspireone acer which is pretty awesome.
Re: My computer just died
Posted:
Sun Apr 19, 2009 4:28 pm
by deathstalker
we need to find this gear disapearing gear bug
and server crashing bug. it is getting pretty bad.
every time the server goes down gear dissapears.
Re: My computer just died
Posted:
Sun Apr 19, 2009 10:55 pm
by Sega Rally Pownz
deathstalker wrote:we need to find this gear disapearing gear bug
and server crashing bug. it is getting pretty bad.
every time the server goes down gear dissapears.
Yeah, my gear disappears and I've done level 8-9 four times now in poo gear because it keeps disappear... I gave the game a chance now I'm outta here lol.
Re: My computer just died
Posted:
Sun Apr 19, 2009 11:02 pm
by Sex4Cash
Dude, this isn't normal. Hang in there. Apparently you weren't around for the rough days of xen. At least Karl and Joe are restoring gear. Can you see EJ EVER doing stuff like that? lol?
Re: My computer just died
Posted:
Mon Apr 20, 2009 5:54 am
by Rabit561
Sex4Cash wrote:Dude, this isn't normal. Hang in there. Apparently you weren't around for the rough days of xen. At least Karl and Joe are restoring gear. Can you see EJ EVER doing stuff like that? lol?
No.. He just does a wipe every chance he gets..
Re: My computer just died
Posted:
Mon Apr 20, 2009 7:31 am
by Sega Rally Pownz
Sex4Cash wrote:Dude, this isn't normal. Hang in there. Apparently you weren't around for the rough days of xen. At least Karl and Joe are restoring gear. Can you see EJ EVER doing stuff like that? lol?
I guess you're right. I'd be like level 12 now though.
Re: My computer just died
Posted:
Mon Apr 20, 2009 7:40 am
by Karl G.
I'm sorry to hear that you've had a rough time with the game. I'd normally never have allowed this critical of a bug to persist for more than a few hours, let alone days. Find me in-game sometime, or send me a PM when you'll be online later this week and I'll see what I can do. For now, I hope you can tolerate the problems (or maybe take a break today and come back once I fix this tonight!)
Re: My computer just died
Posted:
Mon Apr 20, 2009 10:22 am
by Sex4Cash
If you like, once they bugs are worked out, I'd be happy to take u around for a bit of shared exp.
Re: My computer just died
Posted:
Mon Apr 20, 2009 10:31 am
by Karl G.
Ugh. They just called and said they aren't coming until tomorrow.
This is crap, I'm going to figure out a way to work on a different machine.
Re: My computer just died
Posted:
Mon Apr 20, 2009 10:48 am
by Sex4Cash
Is your laptop under warranty? Or get an enclosure for a laptop hdd and pull the data to another pc. (assuming you can pop the drive out of the side)
Re: My computer just died
Posted:
Mon Apr 20, 2009 11:21 am
by Karl G.
Yeah it's under warranty, but their "next day on-site service" means Tuesday if you call on a weekend...including if you called Saturday morning. 4 days is not "next day" by a long shot. Grr.
Re: My computer just died
Posted:
Tue Apr 21, 2009 2:39 am
by Sex4Cash
looking forward to dell fixing your lappy! btw, if they give you any trouble, let me know. I know some ppl here at the dell main campus who could make it go a lot easier. ; )
Re: My computer just died
Posted:
Tue Apr 21, 2009 7:43 am
by Karl G.
haha thanks but I actually don't have a dell...it's a Thinkpad. For the most part, it's a super tank computer.


#include <lexer.h>
◆ dictionary_t
◆ function_t
◆ lexer()
◆ exec_regular()
operator matching function and execute if match return true otherwise return false
◆ is_quit()
| bool joy::lexer::is_quit |
( |
| ) |
|
◆ no_conversion()
| void joy::lexer::no_conversion |
( |
joy_stack & |
tokens | ) |
|
|
protectedvirtual |
display errors for any undefined tokens
Reimplemented in joy::parser.
◆ quit()
| void joy::lexer::quit |
( |
| ) |
|
◆ tokenize() [1/3]
split the line into recognised tokens bool_t, char_t, int_t, double_t, string_t mark any remainder as undef_t
◆ tokenize() [2/3]
◆ tokenize() [3/3]
convert user input line into joy_stack of a single undefined token {line, undef_t}
◆ root_stack
TODO: test performance if reserve large stack space at construction root stack
◆ root_type
The documentation for this class was generated from the following files:


new Event() Source: event.js, line 1 Author: tbking Creates an event object with received message Members data Source: event.js, line 8 Data received in the message Methods ack() Source: event.js, line 24 Method to acknowledge the message reject() Source: event.js, line 32 Method to reject the message


This build step is intended to support execution of automated tests from Micro Focus ALM Octane.
The builder searches for the "testsToRun" parameter which is sent from ALM Octane as part of the execution framework.
Once it is found, its value is converted to the format of the selected testing framework, and injected to the "testsToRunConverted" environment parameter.
Later, the new parameter can be used in the appropriate execution builder.
- To use in other parameter textboxes, use the following syntax: ${testsToRunConverted}
- To use in the scripts (shell, batch command), use the following syntax: (Windows) %testsToRunConverted%, and (Linux) $testsToRunConverted. For example
- (Surefire, Windows) mvn clean -Dtest=%testsToRunConverted% test
- (Failsafe, Linux) mvn clean -Dit.test=$testsToRunConverted verify
- To use in the pipeline script (workflow job), use the following syntax : ${params.testsToRunConverted}. For example: mvn clean -Dtest=${params.testsToRunConverted} test
* For UFT: In order to build a UFT MTBX file, this builder needs to know the test check-out directory. By default this is the job workspace directory.
If tests are checked out in another directory, define in the job a String parameter "testsToRunCheckoutDirectory" with the correct directory.
** For JUnit/TestNG: supported for JUnit 4.7+, Surefire Plugin 2.19+, Failsafe Plugin 2.12.1+


| 002:259 Khan | : |
Or like the one who passed by a town and it had tumbled over its roofs. He said: "Oh! How will Allah ever bring it to life after its death?"  He said: "How long did you remain (dead)?" He (the man) said: "(Perhaps) I remained (dead) a day or part of a day".  And thus We have made of you a sign for the people. Look at the bones, how We bring them together and clothe them with flesh". When this was clearly shown to him, he said, "I know (now) that Allah is Able to do all things." |
| 002:259 Maulana | : |
Or like him who passed by a town, and it had fallen in upon its roofs. He said: When will Allah give it life after its death? So Allah caused him to die for a hundred years, then raised him. He said: How long hast thou tarried? He said: I have tarried a day, or part of a day. He said: Nay, thou has tarried a hundred years; but look at thy food and drink , years have not passed over it!  And that We may make thee a sign to men. And look at the bones, how We set them together then clothe them with flesh. So when it became clear to him, he said: I know that Allah is Possessor of power over all things. |
| 002:259 Pickthal | : |
Or (bethink thee of) the like of him who, passing by a township which had fallen into utter ruin, exclaimed: How shall Allah give this township life after its death?  He said: How long hast thou tarried? (The man) said: I have tarried a day or part of a day. (He) said: Nay, but thou hast tarried for a hundred years. Just look at thy food and drink which have not rotted!  And, that We may make thee a token unto mankind, look at the bones, how We adjust them and then cover them with flesh! And when (the matter) became clear unto him, he said: I know now that Allah is Able to do all things. |
| 002:259 Rashad | : |
Consider the one who passed by a ghost town and wondered, "How can GOD revive this after it had died?" GOD then put him to death for a hundred years, then resurrected him. He said, "How long have you stayed here?" He said, "I have been here a day, or part of the day." He said, "No! You have been here a hundred years. Yet, look at your food and drink; they did not spoil.  Now, note how we construct the bones, then cover them with flesh." When he realized what had happened, he said, "Now I know that GOD is Omnipotent." |
| 002:259 Sarwar | : |
(Or have you heard) of the one who, on passing through an empty and ruined town, said, "When will God bring it to life?"  He replied, "One day or part of a day." The Lord said, "No, you have been here for one hundred years. Look at your food and drink. They have not yet decayed. But look at your donkey and its bones. To make your case evidence (of the Truth) for the people, see how we bring the bones together and cover them with flesh." When he learned the whole story, he said, "Now I know that God has power over all things." |
| 002:259 Shakir | : |
Or the like of him (Uzair) who passed by a town, and it had fallen down upon its roofs; he said: When will Allah give it life after its death?  He said: How long have you tarried? He said: I have tarried a day, or a part of a day. Said He: Nay! you have tarried a hundred years; then look at your food and drink, years have not passed over it; and look at your ass; and that We may make you a sign to men, and look at the bones, how We set them together, then clothed them with flesh; so when it became clear to him, he said: I know that Allah has power over all things. |
| 002:259 Sherali | : |
Or hast thou not heard of the like of him who passed by a town which had fallen down upon its roofs and exclaimed, 'When will ALLAH restore it to life after its destruction?' Then ALLAH caused him to die for a hundred years, then HE raised him and said, 'How long hast thou remained in this state?' He answered, 'I have remained a day or part of a day.' ALLAH said, 'It is so but thou hast also remained in this state for a hundred years.  And WE have done this that WE may make thee a Sign unto men. And look at the bones, how WE set them and then clothe them with flesh.' And when this became clear to him, he said, 'I know that ALLAH has the power to do all that HE wills.' |
| 002:259 Yusufali | : |
Or (take) the similitude of one who passed by a hamlet, all in ruins to its roofs. He said: "Oh! how shall Allah bring it (ever) to life, after (this) its death?" but Allah caused him to die for a hundred years, then raised him up (again). He said: "How long didst thou tarry (thus)?" He said: (Perhaps) a day or part of a day." He said: "Nay, thou hast tarried thus a hundred years; but look at thy food and thy drink; they show no signs of age; and look at thy donkey: And that We may make of thee a sign unto the people, Look further at the bones, how We bring them together and clothe them with flesh." When this was shown clearly to him, he said: "I know that Allah hath power over all things." |
Concepts/Themes Covered: أركان الإسلام > التوحيد > توحيد الله تعالي > صفات الله تعالى > القدير Pillars of Islam> Islamic> Oneness of Allah> His Glory's Characteristics> The Able to do All Things الإيمان > اليوم الآخر > البعث Faith> The Hereafter> The Resurrection العلوم والفنون > الحقائق العلمية و الإشاة إلى وقائع أيدتهاالإكتشافات العلمية > حول ما يدعى بالتطور Science and Art> The Scientific Facts and the Indication to Facts which have been supported by the Scientific Discoveries>About the so-called Development القصص والتاريخ > الذي أماته الله مئة عام The Stories and the History>The One who Allah has Made him Dead for One Hundred Years
This tool uses eight English parallel translations for the Holy Quran imported from Mr. Clay Smith. You can also visit Qurany Concepts for browsing the Quran themes or topics. If you want to search the Holy Quran for keywords, please visit Qurany Keywords.


Highlighted (Themed)
Under 50 Employees
$50 per month
Having 1 - 100 Employees
$100 per month
$1 per Employee
Having More Than 101 Employees
$150 per month
$0.5 per Employee


This is a heading
hello everyone, welcome to read my html learning code html5, thank you for coming here for fun>
HTML Text Formatting Elements
Tag Description
b Defines bold text
em Defines emphasized text
i Defines italic text
small Defines smaller text
strong Defines important text
sub Defines subscripted text
sup Defines superscripted text
ins Defines inserted text
del Defines deleted text
mark Defines marked/highlighted text


{% load staticfiles %}
There is always another side to the STORY
iOS Champion
Brogrammer to be
Javascript extraordinaire
The devil himself
Instagram API wiz kid
Munder's Twin
Works with models
Django models.
Head Of CS team
Superman
Head of Marketing
Professional Video Editor
Human Resources
Math geek
Content Moderator
JSON master
CFO
OK with finances
Head of Curriculum
Mrs. Nashef
Head of A lot of things
Good
ALL RIGHTS RESERVED. Groupic © 2015.


Hype machine is the mainstay of Ormsby Guitars. First released in 2008 as a Multiscale,
it was a hit from the start. Excellent fret access, compact body,
and an upper horn that extends out to the 12th fret provide a beautifully balance guitar.
Hype machine is the mainstay of Ormsby Guitars. First released in 2008 as a Multiscale,
it was a hit from the start. Excellent fret access, compact body,
and an upper horn that extends out to the 12th fret provide a beautifully balance guitar.
Hype machine is the mainstay of Ormsby Guitars. First released in 2008 as a Multiscale,
it was a hit from the start. Excellent fret access, compact body,
and an upper horn that extends out to the 12th fret provide a beautifully balance guitar.
Hype machine is the mainstay of Ormsby Guitars. First released in 2008 as a Multiscale,
it was a hit from the start. Excellent fret access, compact body,
and an upper horn that extends out to the 12th fret provide a beautifully balance guitar.


sim_info - Provides miscellaneous information about the current simulation.
sim_info [-h] <module> <option>
This command returns miscellaneous information about
current simulation of the specified module, depending on the option
supplied.
Command options:
- -h
- Prints usage.
- <option>
- option can be one of the following keyword:
- isStartOfRound
- Returns 1 if the simulation is at the start of a round, and 0
otherwise.
- isEndOfRound
- Returns 1 if the current round has just finished, and 0
otherwise. Usually if the simulation is at the end of a round, it is also at
the start of the round and vice versa. But there is a subtlety: at the start
of the initial round, isStartOfRound will return 1, but isEndOfRound will
return 0.
- atomOrdering
- Returns a linear order of the atoms. The sub-rounds of execution are
carried according to this order.
- variableOrdering
- Returns a linear order of the variables. Variables controlled by the
same atoms are grouped together.
- isUserTurn
- Returns 1 if it is the user's turn during the simulation, and 0
otherwise.
- isInitialRound
- Returns 1 if the current round is the initial round, and 0 otherwise.
- mode
- Returns the mode of the current simulation. The result is "random",
"manual" or "game".
- isSimulated
- Returns 1 if the module is being simulated, 0 otherwise.
Last updated on 1031104 18h39


--- layout: post status: publish published: true title: "生老病死" author: Leask author_login: leask author_email<EMAIL_ADDRESS>author_url: https://leaskh.com wordpress_id: 517 wordpress_url: http://leaskh.wordpress.com/2006/06/24/%e7%94%9f%e8%80%81%e7%97%85%e6%ad%bb date: '2006-06-24 22:17:12 +0800' date_gmt: '2006-06-24 22:17:12 +0800' categories: - Life tags: [] comments: [] ---


HandleYouTubeLiveTransitionTesting
1. Broadcast element created: OK
2. Stream element created: OK
3. Stream and Broadcast binded: OK
4. Transitioning to Test: OK
HandleYouTubeLiveTransitionLive
1. Broadcast element created: OK
2. Stream element created: OK
3. Stream and Broadcast binded: OK
4. Transitioning to Test: OK
5. Transitioning to Live: OK
HandleYouTubeLiveOnAir
1. Broadcast element created: OK
2. Stream element created: OK
3. Stream and Broadcast binded: OK
4. Transitioning to Test: OK
5. Transitioning to Live: OK


This map, produced using census (ACS) data from 2016, displays commute times for each state. Check out different time ranges using the layer control in the bottom left corner!


|
SideCar
|
Go to the source code of this file.
Data Structures | |
| class | SideCar::IO::RecipientList |
| Maintain a shared list of the task IDs and their input channels which should receive a message. More... | |
Namespaces | |
| Logger | |
| Namespace for the Log logging device and support classes. | |
| SideCar | |
| Namespace for all entities specific to the 331 SideCar project. | |
| SideCar::IO | |
| Namespace for entities that handle SideCar data I/O. | |


- W3C Web Accessibility Perspectives: Understandable Content - video
- Print disabilities Wikipedia article
- Publications Office of the EU: How to write clearly - International resources for plain language
- Federal Plain Language Guidelines - US government official website
- Modal Dialog Example | WAI-ARIA Authoring Practices 1.2
- W3C Web Accessibility Tutorials: User Notifications
- BBC Mobile Accessibility Guidelines: Actionable Elements


About
About
I already introduced myself, and I stated my majors and minor at the University of Delaware. I am from Wilmington, De which is about 20 minutes from here. I have one brother and one sister.


Congrats! You have officially requested to book your trip. Please click on the trip and send a friendly message to your host explaining who you are and why you plan to visit.
| Status |
Dates |
{{recipient}} |
Location |
| {{result.status}} |
{{result.checkin | date : 'MMM, dd'}} - {{result.checkout | date}} |
{{result.name}} |
{{result.address}} |


What Day Would You Like To Eat? (DD/MM/YYYY): What Time Would you Like To Eat:
Number Of People In Your Party: 1 2 3 4 5 6 7 8 9


CROPR CODE FOR CROPPING POINT CLOUDS TO SPECIFIED REGION
The code is a very simple one designed to reduce the size of point-cloud files.
There are 3 options as described below: to crop a point cloud to a specified region,
to decimate a point cloud (take every nth point) or to thin a point cloud (take only the first point in each voxel).
As implemented, it only accepts point-cloud files in .las format.
When the files are selected, the total number of points in all the files and the
total extent of the data is shown in the menu.
Cropping
The user can modify the extent information in the menu as desired and the data will be cropped
to the resulting modified parameters.
Decimating
The menu contains a decimation ratio.
If the value is 1 (the default) then no decimation is done.
If it is =n larger than 1, then 1 out of every n points is transfered to the output.
The output is every nth point starting with point 0 for each block read.
Thinning
The bounding box of the data for each file is divided in all three dimensions into equal-sized voxels.
Only the first hit in any voxel is transfered to the output.
The size of the voxel is set from the menu.
Advantages over decimating: Ground-based lidar usually has very different sampling densities varying from very dense
on the ground close to the sensor and much less dense at longer ranges. So this technique compensates for this imbalance
whereas decimating does not.
Disadvantages: The resulting number of points cant be determined beforehand, so several passes may be necessary to get a reasonable number.
If multiple files are processed, then you may want different voxel resolutions for different files. You may want to sample more densely
at the focal point of a data collection than the surrounding areas.


Registration Number :
Flat Number :
Block Number :
Tax Number :
Meter Number :
Membership Fee Paid :
Name of Owner :
E-Mail Id :
Phone / Mobile :
Permanent Address Of Owner :
Current Address of Owner :
Name :
Phone / Mobile :
E-Mail Id :
Occupation :
JAN FEB MAR APR MAY JUN JUL AUG SEP OCT NOV DEC


{% extends "objectives/base.html" %} {% block main_content %}
Below is a summary of your {{ objectives|length }} objectives.


 By the way, we're now storing colors in your user account, and all the colors you previously added aren't in there. Just add some new ones for now :)
You are online.
Here's all the code for handling signin/signout, as well as storing, updating, loading and deleting colors. Plus, it'll all just continue to work when you're offline, and it syncs across all devices and browsers you're logged into!
Liking it so far? This is just the beginning!
Want to see something fun? Open this page in another browser, sign in with the same account, then add colors. Watch the magic happen…
Now turn of your internet connection. Add colors to both browsers. Turn on your internet connection again, and wait a moment.
Cool, huh?
What’s next?
Visit our official website: hood.ie. We are currently migrating to a new version, so some instructions on the website might be outdated. Best is to come say hi in the Hoodie Chat, we are happy to help! For the latest API docs see Hoodie Client README. If you are interested in the Hoodie Architecture, all repos are listed here
Thanks for taking the Hoodie Camp Tutorial, we hope you like it. Please let us know on Twitter and spread the word :)


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Hayley J. Bauman, Psy.D
Licensed Psychologist
"The right way to wholeness is full of detours and supposed wrong turns."
Serendipity and the Search for True Self
Serendipity and the Search for True Self reveals the ways in which we fruitlessly search for self in the outside world, and how we eventually come to the realization that there's nowhere left to search but within.
Believing that all paths lead to the same place, Dr. Bauman weaves seemingly distant topics like dreams, forgiveness, body-awareness, and critical inner voices into tools for connecting to your core. In her nonjudgmental way, Dr. Bauman teaches us to respect and value all parts of ourselves as she believes that "Every single energy inside of us is necessary, useful, and capable of complementing one another. The key is knowing when, where, and how to integrate our different parts so that we feel whole."
Serendipity and the Search for True Self takes you on a whimsical, yet practical journey to a land where spirituality is infused into even the most mundane of daily tasks. Full of inspirational anecdotes and down-to-earth humor, this work is a warm-hearted travel companion for anyone on the winding road of self discovery.


NETWORK & IT AUTOMATION SERVICES
Reduce human resource efforts in network deployment,
operation, and deployment timelines.
Lorem Ipsum is simply dummy text of the printing and typesetting industry. Lorem Ipsum has been the industry's standard dummy text ever since the 1500s, when an unknown printer took a galley of
View MoreLorem Ipsum is simply dummy text of the printing and typesetting industry. Lorem Ipsum has been the industry's standard dummy text ever since the 1500s, when an unknown printer took a galley of
View MoreLorem Ipsum is simply dummy text of the printing and typesetting industry. Lorem Ipsum has been the industry's standard dummy text ever since the 1500s, when an unknown printer took a galley of
View More


| File | Statements | Branches | Functions | Lines | |||||
|---|---|---|---|---|---|---|---|---|---|
| components/ | 84.62% | 11/13 | 66.67% | 4/6 | 100% | 2/2 | 91.67% | 11/12 | |
| components/button/ | 0% | 0/1 | 100% | 0/0 | 0% | 0/1 | 0% | 0/1 | |
| components/calendar/ | 1.32% | 1/76 | 0% | 0/37 | 0% | 0/8 | 1.32% | 1/76 | |
| components/carousel/ | 0% | 0/58 | 0% | 0/26 | 0% | 0/5 | 0% | 0/56 | |
| components/checkbox-group/ | 0% | 0/15 | 0% | 0/10 | 0% | 0/4 | 0% | 0/15 | |
| components/checkbox/ | 0% | 0/16 | 0% | 0/10 | 100% | 0/0 | 0% | 0/16 | |
| components/form-item/ | 1.64% | 1/61 | 0% | 0/51 | 0% | 0/2 | 1.69% | 1/59 | |
| components/form/ | 0% | 0/21 | 0% | 0/14 | 0% | 0/5 | 0% | 0/21 | |
| components/indicator/ | 21.43% | 3/14 | 0% | 0/2 | 0% | 0/4 | 21.43% | 3/14 | |
| components/input/ | 22.22% | 2/9 | 100% | 0/0 | 100% | 0/0 | 22.22% | 2/9 | |
| components/lazy/ | 2.68% | 3/112 | 0% | 0/50 | 0% | 0/30 | 2.86% | 3/105 | |
| components/message-box/ | 15.56% | 7/45 | 0% | 0/18 | 0% | 0/7 | 15.56% | 7/45 | |
| components/message/ | 20.83% | 5/24 | 0% | 0/6 | 20% | 1/5 | 20.83% | 5/24 | |
| components/mixins/ | 0% | 0/14 | 0% | 0/11 | 0% | 0/2 | 0% | 0/14 | |
| components/nav/ | 0% | 0/11 | 0% | 0/2 | 0% | 0/2 | 0% | 0/11 | |
| components/notify/ | 19.35% | 6/31 | 0% | 0/10 | 0% | 0/4 | 19.35% | 6/31 | |
| components/pagination/ | 0% | 0/67 | 0% | 0/50 | 0% | 0/1 | 0% | 0/67 | |
| components/progress/ | 0% | 0/6 | 0% | 0/2 | 0% | 0/1 | 0% | 0/6 | |
| components/radio/ | 0% | 0/3 | 100% | 0/0 | 100% | 0/0 | 0% | 0/3 | |
| components/rate/ | 0% | 0/6 | 0% | 0/6 | 100% | 0/0 | 0% | 0/6 | |
| components/select/ | 0% | 0/16 | 0% | 0/14 | 0% | 0/4 | 0% | 0/16 | |
| components/table-column/ | 6.9% | 2/29 | 0% | 0/14 | 0% | 0/5 | 7.14% | 2/28 | |
| components/table/ | 5.26% | 5/95 | 0% | 0/64 | 0% | 0/18 | 5.32% | 5/94 | |
| components/tabs/ | 0% | 0/29 | 0% | 0/10 | 0% | 0/2 | 0% | 0/28 | |
| components/theme-chalk/src/style/font/ | 55.36% | 31/56 | 30% | 6/20 | 63.64% | 7/11 | 100% | 1/1 | |
| components/transitions/ | 2.5% | 1/40 | 0% | 0/8 | 100% | 0/0 | 2.63% | 1/38 | |
| components/uploader/ | 6.14% | 17/277 | 0% | 0/163 | 0% | 0/35 | 6.39% | 17/266 | |
| directives/ | 22.73% | 5/22 | 0% | 0/22 | 0% | 0/7 | 25% | 5/20 | |
| loaders/ | 31.25% | 5/16 | 0% | 0/2 | 0% | 0/4 | 31.25% | 5/16 | |
| pages/ | 3.17% | 4/126 | 0% | 0/2 | 0% | 0/2 | 3.17% | 4/126 | |
| pages/components/ | 0% | 0/9 | 0% | 0/10 | 0% | 0/5 | 0% | 0/9 | |
| router/ | 100% | 1/1 | 100% | 0/0 | 100% | 0/0 | 100% | 1/1 | |
| utils/ | 12.64% | 35/277 | 2.01% | 4/199 | 10.71% | 6/56 | 13.21% | 35/265 |


Status
Neu...
Öffnen
Speichern
Speichern unter...
Undo
Redo
If you see this
something
went wrong!
Not implemented yet!.


NEUTROGENA TGEL THERAPEUTIC STUBBORN ITCH- coal tar shampoo
Neutrogena Corporation
Disclaimer: Most OTC drugs are not reviewed and approved by FDA, however they may be marketed if they comply with applicable regulations and policies. FDA has not evaluated whether this product complies.
For external use only
Ask a doctor or pharmacist before use if you are using this product with other forms of psoriasis therapy such as ultraviolet radiation or prescription drugs.
When using this product
For best results, use at least twice a week or as directed by a doctor.
Water
Sodium Laureth Sulfate
Cocamide MEA
Laureth-4
Fragrance
Polysorbate 20
Cocamidopropyl Betaine
Citric Acid
Sodium Chloride
Tetrasodium EDTA
DMDM Hydantoin.
Store away from direct sunlight. In rare instances, discoloration of gray, blonde, bleached, or tinted hair may occur.
NEUTROGENA®
T/Gel®
therapeutic
shampoo
Stubborn Itch
soothes intense
scalp itch with
cooling menthol
#1 DERMATOLOGIST
RECOMMENDED BRAND
Neutrogena®
2% NEUTAR®
(COAL TAR 0.5%)
4.4 FL OZ (130mL)
|
NEUTROGENA TGEL THERAPEUTIC STUBBORN ITCH
coal tar shampoo | ||||||||||||||||||||||||
| ||||||||||||||||||||||||
| ||||||||||||||||||||||||
| ||||||||||||||||||||||||
| ||||||||||||||||||||||||
|
| Labeler - Neutrogena Corporation (008254617) |


Welcome to my implementation of a sector generator for the Traveller role playing game!
This generator uses the default rules as provided in Mongoose Traveller 2nd edition. It creates a sector that is composed of 16 subsectors that are each 8 hexes wide and 10 hexes tall. These subsectors are arranged in a 4 by 4 grid to form the sector. The generator creates all of the planets in the sector and then constructs trade routes between them.
The results are first shown in a map of the sector, where the hex coordinates and planet name are inside each hex. In addition, trade routes shown as lines connecting hexes together. Hover over a hex and wait a moment to see the planet's name and UWP in a tooltip. A full table of all planets is also available below the map the shows each planet's location, UWP, bases, trade tags, and travel code.
To generate a sector, simple hit the generate button. If you wish to alter the density of planets in each subsector, you may modify the values in the "Subsector Densities" table. The default value is 0.5, meaning each hex in the corresponding subsector has a 50% to have a planet. A value of 1 will cause every hex in the subsector to have a planet, while a value of 0 will result in no planets existing in the subsector. The rulebook recommends using 0.5 as the default with 0.667 for densely populated subsectors, 0.333 for sparse subsectors, and 0.167 for rift subsectors.
Please note that generation may take a little while, so do not refresh the page or hit the generate button more then once. If the browser becomes unresponsive, just keep waiting and eventually the results will load.
| Subsector Densities | ||||
|---|---|---|---|---|
| Col 1 | Col 2 | Col 3 | Col 4 | |
| Row 1 | ||||
| Row 2 | ||||
| Row 3 | ||||
| Row 4 |
| Name | Coordinates | Code | Bases | Trade Codes | Travel Code |
|---|---|---|---|---|---|
| {{planet.name}} | {{planet.coordString}} | {{planet.profileString}} | {{planet.bases}} | {{planet.tradeCodes}} | {{planet.travelCode}} |
| Name | Coordinates | Code | Bases | Trade Codes | Travel Code |
|---|---|---|---|---|---|
| {{planet.name}} | {{planet.coordString}} | {{planet.profileString}} | {{planet.bases}} | {{planet.tradeCodes}} | {{planet.travelCode}} |


--- layout: page title: "Blog" description: "Blog about daily technical stuff" group: navigation --- {% include JB/setup %} Archive | Categories | TagsFeed: Atom | Rss


We apologize for the inconvenience.
We hope to be back up and rolling again soon!
Need assistance? Contact us at<EMAIL_ADDRESS>{% extends 'base_static.html' %} {% block extras %} {% endblock %} {% block content %}
We apologize for the inconvenience.
We hope to be back up and rolling again soon!
Need assistance? Contact us at lnl-w@wpi.edu.


data_helper.parse module¶
String parse wrapper functions to streamline common use cases
-
data_helper.parse.
list_filter
(pattern, iter, flags=0)[source]¶ Use regular expression patterns to filter a list of strings
Parameters: Returns: List of matching strings.
Return type:
-
data_helper.parse.
str_split_caps
(s, trim=True)[source]¶ Split a string on capital letters
Parameters: Returns: List of strings, each starting with a capital letter, in the same order as they appear in the string.
Return type:


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Ramaze is working correctly with this application, now you can start working.
To start you can modify:
view/index.xhtml
, this page.
view/page.xhtml
, the layout for this page.
controller/main.rb
, where you can change the header of this
page and the notemplate action
For more documentation, check out www.ramaze.net, which includes:
You can also read the rdocs or browse around the Ramaze source code.
For help with Ramaze, visit the #ramaze on irc.freenode.net (you can use this browser-based frontend), or post on the Ramaze Google Group.


(2015)
90% Rotten Tomatoes 7.4/10 IMDb 83% Metacritic Annihilation(2018)
88% Rotten Tomatoes 6.8/10 IMDb 79% Metacritic Thomas JeffersonChief Operating Officer James MadisonDeveloper James MonroeDeveloper Andrew JacksonDesigner John TylerDesigner James PolkProject Manager Zachary TaylorProject Manager


Bagatelle in the Osprey
by John DonohoeBagatelle Celebrate a phenomenal 40 Years of Original Music, Live at Osprey Hotel, Naas on Thursday, December 5th.
Bagatelle began their musical career back in 1978 and since then have remained ever popular on the Irish music circuit. Over the course of their forty years, they’ve had several No.1 hit singles with iconic songs such as ‘Summer In Dublin’, ‘Second Violin’ and ‘Trump Card’.
With platinum and gold status album sales and classic emigration songs like ‘Streets Of New York’, ‘Flight of Earls’ and ‘Boston Rose’, Bagatelle have remained a firm favourite with Irish audiences across the globe.
Over the course of their forty years, the band have shared stages with legends and international icons such as Bob Marley, John Denver, The Pogues, Duran Duran, The Pretenders, Van Morrison, U2, UB40, George Michael and Jose Feliciano, to name just a few.
The band were presented with an IMRO Award this year in recognition of their 40th anniversary and came out of their very short lived retirement of only 3 months and they have been playing a series of sold out gigs ever since.
Don’t miss out on what is going to be a very special night of music right on your doorstep!
Proudly sponsored by Smyth Auctioneers, Naas.
Tickets are €25 plus booking fee and are available from www.amientertainment.ie, Osprey reception desk, Jam Music Company and Smyth Auctioneers in Naas.


Given a hamiltonian \( H \) and a trial wave function \( \Psi_T \), the variational principle states that the expectation value of \( \langle H \rangle \), defined through $$ E[H]= \langle H \rangle = \frac{\int d\boldsymbol{R}\Psi^{\ast}_T(\boldsymbol{R})H(\boldsymbol{R})\Psi_T(\boldsymbol{R})} {\int d\boldsymbol{R}\Psi^{\ast}_T(\boldsymbol{R})\Psi_T(\boldsymbol{R})}, $$ is an upper bound to the ground state energy \( E_0 \) of the hamiltonian \( H \), that is $$ E_0 \le \langle H \rangle . $$ In general, the integrals involved in the calculation of various expectation values are multi-dimensional ones. Traditional integration methods such as the Gauss-Legendre will not be adequate for say the computation of the energy of a many-body system.
The trial wave function can be expanded in the eigenstates of the hamiltonian since they form a complete set, viz., $$ \Psi_T(\boldsymbol{R})=\sum_i a_i\Psi_i(\boldsymbol{R}), $$ and assuming the set of eigenfunctions to be normalized one obtains $$ \frac{\sum_{nm}a^*_ma_n \int d\boldsymbol{R}\Psi^{\ast}_m(\boldsymbol{R})H(\boldsymbol{R})\Psi_n(\boldsymbol{R})} {\sum_{nm}a^*_ma_n \int d\boldsymbol{R}\Psi^{\ast}_m(\boldsymbol{R})\Psi_n(\boldsymbol{R})} =\frac{\sum_{n}a^2_n E_n} {\sum_{n}a^2_n} \ge E_0, $$ where we used that \( H(\boldsymbol{R})\Psi_n(\boldsymbol{R})=E_n\Psi_n(\boldsymbol{R}) \). In general, the integrals involved in the calculation of various expectation values are multi-dimensional ones. The variational principle yields the lowest state of a given symmetry.
In most cases, a wave function has only small values in large parts of configuration space, and a straightforward procedure which uses homogenously distributed random points in configuration space will most likely lead to poor results. This may suggest that some kind of importance sampling combined with e.g., the Metropolis algorithm may be a more efficient way of obtaining the ground state energy. The hope is then that those regions of configurations space where the wave function assumes appreciable values are sampled more efficiently.
The tedious part in a VMC calculation is the search for the variational minimum. A good knowledge of the system is required in order to carry out reasonable VMC calculations. This is not always the case, and often VMC calculations serve rather as the starting point for so-called diffusion Monte Carlo calculations (DMC). DMC is a way of solving exactly the many-body Schroedinger equation by means of a stochastic procedure. A good guess on the binding energy and its wave function is however necessary. A carefully performed VMC calculation can aid in this context.
Choose a trial wave function \( \psi_T(\boldsymbol{R}) \). $$ P(\boldsymbol{R})= \frac{\left|\psi_T(\boldsymbol{R})\right|^2}{\int \left|\psi_T(\boldsymbol{R})\right|^2d\boldsymbol{R}}. $$ This is our new probability distribution function (PDF). The approximation to the expectation value of the Hamiltonian is now $$ E[H(\boldsymbol{\alpha})] = \frac{\int d\boldsymbol{R}\Psi^{\ast}_T(\boldsymbol{R},\boldsymbol{\alpha})H(\boldsymbol{R})\Psi_T(\boldsymbol{R},\boldsymbol{\alpha})} {\int d\boldsymbol{R}\Psi^{\ast}_T(\boldsymbol{R},\boldsymbol{\alpha})\Psi_T(\boldsymbol{R},\boldsymbol{\alpha})}. $$
Define a new quantity $$ E_L(\boldsymbol{R},\boldsymbol{\alpha})=\frac{1}{\psi_T(\boldsymbol{R},\boldsymbol{\alpha})}H\psi_T(\boldsymbol{R},\boldsymbol{\alpha}), \label{eq:locale1} $$ called the local energy, which, together with our trial PDF yields $$ E[H(\boldsymbol{\alpha})]=\int P(\boldsymbol{R})E_L(\boldsymbol{R}) d\boldsymbol{R}\approx \frac{1}{N}\sum_{i=1}^NP(\boldsymbol{R_i},\boldsymbol{\alpha})E_L(\boldsymbol{R_i},\boldsymbol{\alpha}) \label{eq:vmc1} $$ with \( N \) being the number of Monte Carlo samples.
The Algorithm for performing a variational Monte Carlo calculations runs thus as this
The radial Schroedinger equation for the hydrogen atom can be written as $$ -\frac{\hbar^2}{2m}\frac{\partial^2 u(r)}{\partial r^2}- \left(\frac{ke^2}{r}-\frac{\hbar^2l(l+1)}{2mr^2}\right)u(r)=Eu(r), $$ or with dimensionless variables $$ -\frac{1}{2}\frac{\partial^2 u(\rho)}{\partial \rho^2}- \frac{u(\rho)}{\rho}+\frac{l(l+1)}{2\rho^2}u(\rho)-\lambda u(\rho)=0, \label{eq:hydrodimless1} $$ with the hamiltonian $$ H=-\frac{1}{2}\frac{\partial^2 }{\partial \rho^2}- \frac{1}{\rho}+\frac{l(l+1)}{2\rho^2}. $$ Use variational parameter \( \alpha \) in the trial wave function $$ u_T^{\alpha}(\rho)=\alpha\rho e^{-\alpha\rho}. \label{eq:trialhydrogen} $$
Inserting this wave function into the expression for the local energy \( E_L \) gives $$ E_L(\rho)=-\frac{1}{\rho}- \frac{\alpha}{2}\left(\alpha-\frac{2}{\rho}\right). $$ A simple variational Monte Carlo calculation results in
| \( \alpha \) | \( \langle H \rangle \) | \( \sigma^2 \) | \( \sigma/\sqrt{N} \) |
| 7.00000E-01 | -4.57759E-01 | 4.51201E-02 | 6.71715E-04 |
| 8.00000E-01 | -4.81461E-01 | 3.05736E-02 | 5.52934E-04 |
| 9.00000E-01 | -4.95899E-01 | 8.20497E-03 | 2.86443E-04 |
| 1.00000E-00 | -5.00000E-01 | 0.00000E+00 | 0.00000E+00 |
| 1.10000E+00 | -4.93738E-01 | 1.16989E-02 | 3.42036E-04 |
| 1.20000E+00 | -4.75563E-01 | 8.85899E-02 | 9.41222E-04 |
| 1.30000E+00 | -4.54341E-01 | 1.45171E-01 | 1.20487E-03 |
We note that at \( \alpha=1 \) we obtain the exact result, and the variance is zero, as it should. The reason is that we then have the exact wave function, and the action of the hamiltionan on the wave function $$ H\psi = \mathrm{constant}\times \psi, $$ yields just a constant. The integral which defines various expectation values involving moments of the hamiltonian becomes then $$ \langle H^n \rangle = \frac{\int d\boldsymbol{R}\Psi^{\ast}_T(\boldsymbol{R})H^n(\boldsymbol{R})\Psi_T(\boldsymbol{R})} {\int d\boldsymbol{R}\Psi^{\ast}_T(\boldsymbol{R})\Psi_T(\boldsymbol{R})}= \mathrm{constant}\times\frac{\int d\boldsymbol{R}\Psi^{\ast}_T(\boldsymbol{R})\Psi_T(\boldsymbol{R})} {\int d\boldsymbol{R}\Psi^{\ast}_T(\boldsymbol{R})\Psi_T(\boldsymbol{R})}=\mathrm{constant}. $$ This gives an important information: the exact wave function leads to zero variance! Variation is then performed by minimizing both the energy and the variance.
The helium atom consists of two electrons and a nucleus with charge \( Z=2 \). The contribution to the potential energy due to the attraction from the nucleus is $$ -\frac{2ke^2}{r_1}-\frac{2ke^2}{r_2}, $$ and if we add the repulsion arising from the two interacting electrons, we obtain the potential energy $$ V(r_1, r_2)=-\frac{2ke^2}{r_1}-\frac{2ke^2}{r_2}+ \frac{ke^2}{r_{12}}, $$ with the electrons separated at a distance \( r_{12}=|\boldsymbol{r}_1-\boldsymbol{r}_2| \).
The hamiltonian becomes then $$ \hat{H}=-\frac{\hbar^2\nabla_1^2}{2m}-\frac{\hbar^2\nabla_2^2}{2m} -\frac{2ke^2}{r_1}-\frac{2ke^2}{r_2}+ \frac{ke^2}{r_{12}}, $$ and Schroedingers equation reads $$ \hat{H}\psi=E\psi. $$ All observables are evaluated with respect to the probability distribution $$ P(\boldsymbol{R})= \frac{\left|\psi_T(\boldsymbol{R})\right|^2}{\int \left|\psi_T(\boldsymbol{R})\right|^2d\boldsymbol{R}}. $$ generated by the trial wave function. The trial wave function must approximate an exact eigenstate in order that accurate results are to be obtained.
Choice of trial wave function for Helium: Assume \( r_1 \rightarrow 0 \). $$ E_L(\boldsymbol{R})=\frac{1}{\psi_T(\boldsymbol{R})}H\psi_T(\boldsymbol{R})= \frac{1}{\psi_T(\boldsymbol{R})}\left(-\frac{1}{2}\nabla^2_1 -\frac{Z}{r_1}\right)\psi_T(\boldsymbol{R}) + \mathrm{finite \hspace{0.1cm}terms}. $$ $$ E_L(R)= \frac{1}{{\cal R}_T(r_1)}\left(-\frac{1}{2}\frac{d^2}{dr_1^2}- \frac{1}{r_1}\frac{d}{dr_1} -\frac{Z}{r_1}\right){\cal R}_T(r_1) + \mathrm{finite\hspace{0.1cm} terms} $$ For small values of \( r_1 \), the terms which dominate are $$ \lim_{r_1 \rightarrow 0}E_L(R)= \frac{1}{{\cal R}_T(r_1)}\left(- \frac{1}{r_1}\frac{d}{dr_1} -\frac{Z}{r_1}\right){\cal R}_T(r_1), $$ since the second derivative does not diverge due to the finiteness of \( \Psi \) at the origin.
This results in $$ \frac{1}{{\cal R}_T(r_1)}\frac{d {\cal R}_T(r_1)}{dr_1}=-Z, $$ and $$ {\cal R}_T(r_1)\propto e^{-Zr_1}. $$ A similar condition applies to electron 2 as well. For orbital momenta \( l > 0 \) we have $$ \frac{1}{{\cal R}_T(r)}\frac{d {\cal R}_T(r)}{dr}=-\frac{Z}{l+1}. $$ Similarly, studying the case \( r_{12}\rightarrow 0 \) we can write a possible trial wave function as $$ \psi_T(\boldsymbol{R})=e^{-\alpha(r_1+r_2)}e^{\beta r_{12}}. \label{eq:wavehelium2} $$ The last equation can be generalized to $$ \psi_T(\boldsymbol{R})=\phi(\boldsymbol{r}_1)\phi(\boldsymbol{r}_2)\dots\phi(\boldsymbol{r}_N) \prod_{i < j}f(r_{ij}), $$ for a system with \( N \) electrons or particles.
During the development of our code we need to make several checks. It is also very instructive to compute a closed form expression for the local energy. Since our wave function is rather simple it is straightforward to find an analytic expressions. Consider first the case of the simple helium function $$ \Psi_T(\boldsymbol{r}_1,\boldsymbol{r}_2) = e^{-\alpha(r_1+r_2)} $$ The local energy is for this case $$ E_{L1} = \left(\alpha-Z\right)\left(\frac{1}{r_1}+\frac{1}{r_2}\right)+\frac{1}{r_{12}}-\alpha^2 $$ which gives an expectation value for the local energy given by $$ \langle E_{L1} \rangle = \alpha^2-2\alpha\left(Z-\frac{5}{16}\right) $$
With closed form formulae we can speed up the computation of the correlation. In our case we write it as $$ \Psi_C= \exp{\left\{\sum_{i < j}\frac{ar_{ij}}{1+\beta r_{ij}}\right\}}, $$ which means that the gradient needed for the so-called quantum force and local energy can be calculated analytically. This will speed up your code since the computation of the correlation part and the Slater determinant are the most time consuming parts in your code.
We will refer to this correlation function as \( \Psi_C \) or the linear Pade-Jastrow.
We can test this by computing the local energy for our helium wave function $$ \psi_{T}(\boldsymbol{r}_1,\boldsymbol{r}_2) = \exp{\left(-\alpha(r_1+r_2)\right)} \exp{\left(\frac{r_{12}}{2(1+\beta r_{12})}\right)}, $$ with \( \alpha \) and \( \beta \) as variational parameters.
The local energy is for this case $$ E_{L2} = E_{L1}+\frac{1}{2(1+\beta r_{12})^2}\left\{\frac{\alpha(r_1+r_2)}{r_{12}}(1-\frac{\boldsymbol{r}_1\boldsymbol{r}_2}{r_1r_2})-\frac{1}{2(1+\beta r_{12})^2}-\frac{2}{r_{12}}+\frac{2\beta}{1+\beta r_{12}}\right\} $$ It is very useful to test your code against these expressions. It means also that you don't need to compute a derivative numerically as discussed in the code example below.
For the computation of various derivatives with different types of wave functions, you will find it useful to use python with symbolic python, that is sympy, see online manual. Using sympy allows you autogenerate both Latex code as well c++, python or Fortran codes. Here you will find some simple examples. We choose the \( 2s \) hydrogen-orbital (not normalized) as an example $$ \phi_{2s}(\boldsymbol{r}) = (Zr - 2)\exp{-(\frac{1}{2}Zr)}, $$ with $ r^2 = x^2 + y^2 + z^2$.
from sympy import symbols, diff, exp, sqrt
x, y, z, Z = symbols('x y z Z')
r = sqrt(x*x + y*y + z*z)
r
phi = (Z*r - 2)*exp(-Z*r/2)
phi
diff(phi, x)
This doesn't look very nice, but sympy provides several functions that allow for improving and simplifying the output.
We can improve our output by factorizing and substituting expressions
from sympy import symbols, diff, exp, sqrt, factor, Symbol, printing
x, y, z, Z = symbols('x y z Z')
r = sqrt(x*x + y*y + z*z)
phi = (Z*r - 2)*exp(-Z*r/2)
R = Symbol('r') #Creates a symbolic equivalent of r
#print latex and c++ code
print printing.latex(diff(phi, x).factor().subs(r, R))
print printing.ccode(diff(phi, x).factor().subs(r, R))
We can in turn look at second derivatives
from sympy import symbols, diff, exp, sqrt, factor, Symbol, printing
x, y, z, Z = symbols('x y z Z')
r = sqrt(x*x + y*y + z*z)
phi = (Z*r - 2)*exp(-Z*r/2)
R = Symbol('r') #Creates a symbolic equivalent of r
(diff(diff(phi, x), x) + diff(diff(phi, y), y) + diff(diff(phi, z), z)).factor().subs(r, R)
# Collect the Z values
(diff(diff(phi, x), x) + diff(diff(phi, y), y) +diff(diff(phi, z), z)).factor().collect(Z).subs(r, R)
# Factorize also the r**2 terms
(diff(diff(phi, x), x) + diff(diff(phi, y), y) + diff(diff(phi, z), z)).factor().collect(Z).subs(r, R).subs(r**2, R**2).factor()
print printing.ccode((diff(diff(phi, x), x) + diff(diff(phi, y), y) + diff(diff(phi, z), z)).factor().collect(Z).subs(r, R).subs(r**2, R**2).factor())
With some practice this allows one to be able to check one's own calculation and translate automatically into code lines.
#include "vmcsolver.h"
#include <iostream>
using namespace std;
int main()
{
VMCSolver *solver = new VMCSolver();
solver->runMonteCarloIntegration();
return 0;
}
#ifndef VMCSOLVER_H
#define VMCSOLVER_H
#include <armadillo>
using namespace arma;
class VMCSolver
{
public:
VMCSolver();
void runMonteCarloIntegration();
private:
double waveFunction(const mat &r);
double localEnergy(const mat &r);
int nDimensions;
int charge;
double stepLength;
int nParticles;
double h;
double h2;
long idum;
double alpha;
int nCycles;
mat rOld;
mat rNew;
};
#endif // VMCSOLVER_H
#include "vmcsolver.h"
#include "lib.h"
#include <armadillo>
#include <iostream>
using namespace arma;
using namespace std;
VMCSolver::VMCSolver() :
nDimensions(3),
charge(2),
stepLength(1.0),
nParticles(2),
h(0.001),
h2(1000000),
idum(-1),
alpha(0.5*charge),
nCycles(1000000)
{
}
void VMCSolver::runMonteCarloIntegration()
{
rOld = zeros<mat>(nParticles, nDimensions);
rNew = zeros<mat>(nParticles, nDimensions);
double waveFunctionOld = 0;
double waveFunctionNew = 0;
double energySum = 0;
double energySquaredSum = 0;
double deltaE;
// initial trial positions
for(int i = 0; i < nParticles; i++) {
for(int j = 0; j < nDimensions; j++) {
rOld(i,j) = stepLength * (ran2(&idum) - 0.5);
}
}
rNew = rOld;
// loop over Monte Carlo cycles
for(int cycle = 0; cycle < nCycles; cycle++) {
// Store the current value of the wave function
waveFunctionOld = waveFunction(rOld);
// New position to test
for(int i = 0; i < nParticles; i++) {
for(int j = 0; j < nDimensions; j++) {
rNew(i,j) = rOld(i,j) + stepLength*(ran2(&idum) - 0.5);
}
// Recalculate the value of the wave function
waveFunctionNew = waveFunction(rNew);
// Check for step acceptance (if yes, update position, if no, reset position)
if(ran2(&idum) <= (waveFunctionNew*waveFunctionNew) / (waveFunctionOld*waveFunctionOld)) {
for(int j = 0; j < nDimensions; j++) {
rOld(i,j) = rNew(i,j);
waveFunctionOld = waveFunctionNew;
}
} else {
for(int j = 0; j < nDimensions; j++) {
rNew(i,j) = rOld(i,j);
}
}
// update energies
deltaE = localEnergy(rNew);
energySum += deltaE;
energySquaredSum += deltaE*deltaE;
}
}
double energy = energySum/(nCycles * nParticles);
double energySquared = energySquaredSum/(nCycles * nParticles);
cout << "Energy: " << energy << " Energy (squared sum): " << energySquared << endl;
}
double VMCSolver::localEnergy(const mat &r)
{
mat rPlus = zeros<mat>(nParticles, nDimensions);
mat rMinus = zeros<mat>(nParticles, nDimensions);
rPlus = rMinus = r;
double waveFunctionMinus = 0;
double waveFunctionPlus = 0;
double waveFunctionCurrent = waveFunction(r);
// Kinetic energy, brute force derivations
double kineticEnergy = 0;
for(int i = 0; i < nParticles; i++) {
for(int j = 0; j < nDimensions; j++) {
rPlus(i,j) += h;
rMinus(i,j) -= h;
waveFunctionMinus = waveFunction(rMinus);
waveFunctionPlus = waveFunction(rPlus);
kineticEnergy -= (waveFunctionMinus + waveFunctionPlus - 2 * waveFunctionCurrent);
rPlus(i,j) = r(i,j);
rMinus(i,j) = r(i,j);
}
}
kineticEnergy = 0.5 * h2 * kineticEnergy / waveFunctionCurrent;
// Potential energy
double potentialEnergy = 0;
double rSingleParticle = 0;
for(int i = 0; i < nParticles; i++) {
rSingleParticle = 0;
for(int j = 0; j < nDimensions; j++) {
rSingleParticle += r(i,j)*r(i,j);
}
potentialEnergy -= charge / sqrt(rSingleParticle);
}
// Contribution from electron-electron potential
double r12 = 0;
for(int i = 0; i < nParticles; i++) {
for(int j = i + 1; j < nParticles; j++) {
r12 = 0;
for(int k = 0; k < nDimensions; k++) {
r12 += (r(i,k) - r(j,k)) * (r(i,k) - r(j,k));
}
potentialEnergy += 1 / sqrt(r12);
}
}
return kineticEnergy + potentialEnergy;
}
double VMCSolver::waveFunction(const mat &r)
{
double argument = 0;
for(int i = 0; i < nParticles; i++) {
double rSingleParticle = 0;
for(int j = 0; j < nDimensions; j++) {
rSingleParticle += r(i,j) * r(i,j);
}
argument += sqrt(rSingleParticle);
}
return exp(-argument * alpha);
}
#include <armadillo>
#include <iostream>
using namespace arma;
using namespace std;
double ran2(long *);
class VMCSolver
{
public:
VMCSolver();
void runMonteCarloIntegration();
private:
double waveFunction(const mat &r);
double localEnergy(const mat &r);
int nDimensions;
int charge;
double stepLength;
int nParticles;
double h;
double h2;
long idum;
double alpha;
int nCycles;
mat rOld;
mat rNew;
};
VMCSolver::VMCSolver() :
nDimensions(3),
charge(2),
stepLength(1.0),
nParticles(2),
h(0.001),
h2(1000000),
idum(-1),
alpha(0.5*charge),
nCycles(1000000)
{
}
void VMCSolver::runMonteCarloIntegration()
{
rOld = zeros<mat>(nParticles, nDimensions);
rNew = zeros<mat>(nParticles, nDimensions);
double waveFunctionOld = 0;
double waveFunctionNew = 0;
double energySum = 0;
double energySquaredSum = 0;
double deltaE;
// initial trial positions
for(int i = 0; i < nParticles; i++) {
for(int j = 0; j < nDimensions; j++) {
rOld(i,j) = stepLength * (ran2(&idum) - 0.5);
}
}
rNew = rOld;
// loop over Monte Carlo cycles
for(int cycle = 0; cycle < nCycles; cycle++) {
// Store the current value of the wave function
waveFunctionOld = waveFunction(rOld);
// New position to test
for(int i = 0; i < nParticles; i++) {
for(int j = 0; j < nDimensions; j++) {
rNew(i,j) = rOld(i,j) + stepLength*(ran2(&idum) - 0.5);
}
// Recalculate the value of the wave function
waveFunctionNew = waveFunction(rNew);
// Check for step acceptance (if yes, update position, if no, reset position)
if(ran2(&idum) <= (waveFunctionNew*waveFunctionNew) / (waveFunctionOld*waveFunctionOld)) {
for(int j = 0; j < nDimensions; j++) {
rOld(i,j) = rNew(i,j);
waveFunctionOld = waveFunctionNew;
}
} else {
for(int j = 0; j < nDimensions; j++) {
rNew(i,j) = rOld(i,j);
}
}
// update energies
deltaE = localEnergy(rNew);
energySum += deltaE;
energySquaredSum += deltaE*deltaE;
}
}
double energy = energySum/(nCycles * nParticles);
double energySquared = energySquaredSum/(nCycles * nParticles);
cout << "Energy: " << energy << " Energy (squared sum): " << energySquared << endl;
}
double VMCSolver::localEnergy(const mat &r)
{
mat rPlus = zeros<mat>(nParticles, nDimensions);
mat rMinus = zeros<mat>(nParticles, nDimensions);
rPlus = rMinus = r;
double waveFunctionMinus = 0;
double waveFunctionPlus = 0;
double waveFunctionCurrent = waveFunction(r);
// Kinetic energy, brute force derivations
double kineticEnergy = 0;
for(int i = 0; i < nParticles; i++) {
for(int j = 0; j < nDimensions; j++) {
rPlus(i,j) += h;
rMinus(i,j) -= h;
waveFunctionMinus = waveFunction(rMinus);
waveFunctionPlus = waveFunction(rPlus);
kineticEnergy -= (waveFunctionMinus + waveFunctionPlus - 2 * waveFunctionCurrent);
rPlus(i,j) = r(i,j);
rMinus(i,j) = r(i,j);
}
}
kineticEnergy = 0.5 * h2 * kineticEnergy / waveFunctionCurrent;
// Potential energy
double potentialEnergy = 0;
double rSingleParticle = 0;
for(int i = 0; i < nParticles; i++) {
rSingleParticle = 0;
for(int j = 0; j < nDimensions; j++) {
rSingleParticle += r(i,j)*r(i,j);
}
potentialEnergy -= charge / sqrt(rSingleParticle);
}
// Contribution from electron-electron potential
double r12 = 0;
for(int i = 0; i < nParticles; i++) {
for(int j = i + 1; j < nParticles; j++) {
r12 = 0;
for(int k = 0; k < nDimensions; k++) {
r12 += (r(i,k) - r(j,k)) * (r(i,k) - r(j,k));
}
potentialEnergy += 1 / sqrt(r12);
}
}
return kineticEnergy + potentialEnergy;
}
double VMCSolver::waveFunction(const mat &r)
{
double argument = 0;
for(int i = 0; i < nParticles; i++) {
double rSingleParticle = 0;
for(int j = 0; j < nDimensions; j++) {
rSingleParticle += r(i,j) * r(i,j);
}
argument += sqrt(rSingleParticle);
}
return exp(-argument * alpha);
}
/*
** The function
** ran2()
** is a long periode (> 2 x 10^18) random number generator of
** L'Ecuyer and Bays-Durham shuffle and added safeguards.
** Call with idum a negative integer to initialize; thereafter,
** do not alter idum between sucessive deviates in a
** sequence. RNMX should approximate the largest floating point value
** that is less than 1.
** The function returns a uniform deviate between 0.0 and 1.0
** (exclusive of end-point values).
*/
#define IM1<PHONE_NUMBER>
#define IM2<PHONE_NUMBER>
#define AM (1.0/IM1)
#define IMM1 (IM1-1)
#define IA1 40014
#define IA2 40692
#define IQ1 53668
#define IQ2 52774
#define IR1 12211
#define IR2 3791
#define NTAB 32
#define NDIV (1+IMM1/NTAB)
#define EPS 1.2e-7
#define RNMX (1.0-EPS)
double ran2(long *idum)
{
int j;
long k;
static long idum2 = 123456789;
static long iy=0;
static long iv[NTAB];
double temp;
if(*idum <= 0) {
if(-(*idum) < 1) *idum = 1;
else *idum = -(*idum);
idum2 = (*idum);
for(j = NTAB + 7; j >= 0; j--) {
k = (*idum)/IQ1;
*idum = IA1*(*idum - k*IQ1) - k*IR1;
if(*idum < 0) *idum += IM1;
if(j < NTAB) iv[j] = *idum;
}
iy=iv[0];
}
k = (*idum)/IQ1;
*idum = IA1*(*idum - k*IQ1) - k*IR1;
if(*idum < 0) *idum += IM1;
k = idum2/IQ2;
idum2 = IA2*(idum2 - k*IQ2) - k*IR2;
if(idum2 < 0) idum2 += IM2;
j = iy/NDIV;
iy = iv[j] - idum2;
iv[j] = *idum;
if(iy < 1) iy += IMM1;
if((temp = AM*iy) > RNMX) return RNMX;
else return temp;
}
#undef IM1
#undef IM2
#undef AM
#undef IMM1
#undef IA1
#undef IA2
#undef IQ1
#undef IQ2
#undef IR1
#undef IR2
#undef NTAB
#undef NDIV
#undef EPS
#undef RNMX
// End: function ran2()
#include <iostream>
using namespace std;
int main()
{
VMCSolver *solver = new VMCSolver();
solver->runMonteCarloIntegration();
return 0;
}
The Metropolis algorithm , see the original article (see also the FYS3150 lectures) was invented by Metropolis et. al and is often simply called the Metropolis algorithm. It is a method to sample a normalized probability distribution by a stochastic process. We define \( {\cal P}_i^{(n)} \) to be the probability for finding the system in the state \( i \) at step \( n \). The algorithm is then
We wish to derive the required properties of \( T \) and \( A \) such that \( {\cal P}_i^{(n\rightarrow \infty)} \rightarrow p_i \) so that starting from any distribution, the method converges to the correct distribution. Note that the description here is for a discrete probability distribution. Replacing probabilities \( p_i \) with expressions like \( p(x_i)dx_i \) will take all of these over to the corresponding continuum expressions.
The dynamical equation for \( {\cal P}_i^{(n)} \) can be written directly from the description above. The probability of being in the state \( i \) at step \( n \) is given by the probability of being in any state \( j \) at the previous step, and making an accepted transition to \( i \) added to the probability of being in the state \( i \), making a transition to any state \( j \) and rejecting the move: $$ {\cal P}^{(n)}_i = \sum_j \left [ {\cal P}^{(n-1)}_jT_{j\rightarrow i} A_{j\rightarrow i} +{\cal P}^{(n-1)}_iT_{i\rightarrow j}\left ( 1- A_{i\rightarrow j} \right) \right ] \,. $$ Since the probability of making some transition must be 1, \( \sum_j T_{i\rightarrow j} = 1 \), and the above equation becomes $$ {\cal P}^{(n)}_i = {\cal P}^{(n-1)}_i + \sum_j \left [ {\cal P}^{(n-1)}_jT_{j\rightarrow i} A_{j\rightarrow i} -{\cal P}^{(n-1)}_iT_{i\rightarrow j}A_{i\rightarrow j} \right ] \,. $$
For large \( n \) we require that \( {\cal P}^{(n\rightarrow \infty)}_i = p_i \), the desired probability distribution. Taking this limit, gives the balance requirement $$ \sum_j \left [ p_jT_{j\rightarrow i} A_{j\rightarrow i} -p_iT_{i\rightarrow j}A_{i\rightarrow j} \right ] = 0 \,. $$ The balance requirement is very weak. Typically the much stronger detailed balance requirement is enforced, that is rather than the sum being set to zero, we set each term separately to zero and use this to determine the acceptance probabilities. Rearranging, the result is $$ \frac{ A_{j\rightarrow i}}{A_{i\rightarrow j}} = \frac{p_iT_{i\rightarrow j}}{ p_jT_{j\rightarrow i}} \,. $$
The Metropolis choice is to maximize the \( A \) values, that is $$ A_{j \rightarrow i} = \min \left ( 1, \frac{p_iT_{i\rightarrow j}}{ p_jT_{j\rightarrow i}}\right ). $$ Other choices are possible, but they all correspond to multilplying \( A_{i\rightarrow j} \) and \( A_{j\rightarrow i} \) by the same constant smaller than unity.\footnote{The penalty function method uses just such a factor to compensate for \( p_i \) that are evaluated stochastically and are therefore noisy.}
Having chosen the acceptance probabilities, we have guaranteed that if the \( {\cal P}_i^{(n)} \) has equilibrated, that is if it is equal to \( p_i \), it will remain equilibrated. Next we need to find the circumstances for convergence to equilibrium.
The dynamical equation can be written as $$ {\cal P}^{(n)}_i = \sum_j M_{ij}{\cal P}^{(n-1)}_j $$ with the matrix \( M \) given by $$ M_{ij} = \delta_{ij}\left [ 1 -\sum_k T_{i\rightarrow k} A_{i \rightarrow k} \right ] + T_{j\rightarrow i} A_{j\rightarrow i} \,. $$ Summing over \( i \) shows that \( \sum_i M_{ij} = 1 \), and since \( \sum_k T_{i\rightarrow k} = 1 \), and \( A_{i \rightarrow k} \leq 1 \), the elements of the matrix satisfy \( M_{ij} \geq 0 \). The matrix \( M \) is therefore a stochastic matrix.
The Metropolis method is simply the power method for computing the right eigenvector of \( M \) with the largest magnitude eigenvalue. By construction, the correct probability distribution is a right eigenvector with eigenvalue 1. Therefore, for the Metropolis method to converge to this result, we must show that \( M \) has only one eigenvalue with this magnitude, and all other eigenvalues are smaller.


Controller
interface.XMLReader
object.Thread
that analyzes the request sent by Slack.SlashCommandGlobalConfiguration
object and stores the data
sent by Slack.SlackWebhookEndpoint
and delegates the execution of
commands to the classes to which they are associated.


Climate March Draws Thousands of Protesters Alarmed by Trump's Environmental Agenda
On the president's 100th day in office, demonstrators descended on Washington in an attempt to drown out the administration's climate change deniers.
Read MoreOn the president's 100th day in office, demonstrators descended on Washington in an attempt to drown out the administration's climate change deniers.
Read MoreHow about a reasonable converstation on what to do about our warming planet?
Read MoreAn appeals court said it would delay a decision on the legality of the rule, which aims to tackle global warming by cutting emissions from coal-fired plants.
Read MoreA group known for attacking climate science has set its sights on America's public schools.
Read MorePort Arthur, the famous prison that housed the British Empire's toughest convicts in the 19th century, is facing an onslaught from the sea.
Read MoreNearly half of the nation's largest corporations have set emissions reductions targets, even as the Trump administration walks away from goals set by President Obama.
Read More


Four Indian soldiers, two civilians killed in Siachen avalanche
SRINAGAR (Reuters) - Four Indian army officers and two porters were killed on Monday in an avalanche on the Siachen Glacier, a defense spokesman said on Monday.
The incident, in which eight other people were trapped, occurred at an altitude of 19,000 feet on the glacier.
“The cause of death is extreme hypothermia,” the spokesman said, adding that two of the eight people had been rescued.
The Siachen Glacier in the Karakorum range is known as the highest militarized zone in the world.
Thousands of Indian and Pakistani troops contest an area at altitudes above 20,000 feet where they must deal with altitude sickness, high winds, frostbite and temperatures as low as minus 60 degrees Celsius.


Please note that the numbers to the left of each feature here correspond to the feature numbers in the OpenCar Runtime Support Requirements spreadsheet, for example, "Embedding custom non-visible data" here corresponds to the "dataset & data-* attributes" feature in the spreadsheet. As in the spreadsheet, the individual items in green here are required, and those in blue are preferred. This series of tests checks if a browser recognizes a particular feature, it does not ascertain if the browser has implemented that feature correctly.


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Version: @version@ - Date: @date@
A specification by definition contains a set of feasible implementations. In the code, each implementation is also a Specification class. It is possible to obtain a single feasible implementation for a given specification:
@file(net/sf/opendse/tutorial/Part3.java)The corresponding XML representation of the specification looks as follows:
@file(Specification3.xml)The corresponding XML representation of the obtained implementation looks as follows:
@file(Implementation3.xml)
The resulting implementation looks as follows in the viewer:


{% extends 'layout-af.html' %} {% block pageTitle %} Healthcare for armed forces serving Personnel {% endblock %} {% block beforeContent %} {% endblock %} {% block content %}
Find information and support about healthcare for serving personnel, mobilised reservists and family members.
The Ministry of Defence (MoD) is responsible for providing both basic and specialist healthcare needed for all serving personnel and mobilised reservists.
If you are a reservist who is not currently actively serving, you receive your healthcare in the same way as a veteran.
Basic check-ups and treatments for serving personnel and mobilised reservists both overseas and in the UK are provided by the Defence Medical Services (DMS).
The DMS is made up of the Royal Navy Medical Services, the Army Medical Services, the Royal Air Force Medical Services and Headquarters DMS Group.
Basic care you receive through the DMS includes:
All basic care services are staffed by regular uniformed and reserve medical personnel from the British Army, the Royal Navy and the Royal Air Force.
If you need to return to the UK for specialist or emergency treatment, you will receive hospital care through the NHS.
You will be treated in an NHS hospital with specialist wards and staff dedicated to treating serving personnel.
The main treatment centre for seriously injured serving personnel is the Royal Centre for Defence Medicine (RCDM). This is a specialist centre provided by the DMS and the NHS.
The RCDM is based at the Queen Elizabeth Hospital in Birmingham (QECB). Most injured serving personnel returning to the UK will be taken to QECB.
You will be placed in either the specialist military ward or go straight to intensive care depending on your injuries.
The military ward contains staff from both military and civilian backgrounds, and has many features for serving personnel such as a physiotherapy suite, communal spaces and a quiet room for family members and visitors.
The Defence Medical Welfare Service (DMWS) will visit you regularly. They will help you with your day to day needs, and maintain a link with your unit.
The DMS provides many rehabilitation services across the UK. These are known as Primary Care Rehabilitation Facilities (PCRFs) and Regional Rehabilitation Units (RRUs).
Most serving personnel will receive physiotherapy and exercise rehabilitation through PCRFs. If you have more serious injuries, you will be referred to an RRU.
The DMS also works with the Defence and National Rehabilitation Centre (DNRC). This is a specialist centre committed to supporting serving personnel in their rehabilitation.
www.thednrc.org.uk
If you are based in England and need non-urgent or routine hospital treatment, you will be referred through the NHS.
You may be placed on waiting lists or have limited choices for your treatment depending on your situation.
Find more information about how NHS care works for the armed forces community
It is important to know what options you have and actions you can take if you or your partner are either pregnant or looking to get pregnant while in the armed forces.
Find information and advice about pregnancy and fertility when in the armed forces on our support for armed forces families page.
The DMS provides mental health support for serving personnel and mobilised reservists, including crisis support and specialist care.
There are also charity helplines that are available for you to talk to.
Find out more information about mental health support for serving personnel and their families.
If you have been sexually assaulted while in the armed forces or as a veteran, it is important to not be afraid of getting help.
Find help after rape and sexual assault
Forward Assist’s Salute Her UK: advice and support for women who are veterans or currently serving
www.forwardassist.com
There is a range of support and advice available for families of armed forces serving personnel and mobilised reservists.
This includes services and charities dedicated to helping you with any healthcare and welfare concerns, such as supporting your family when moving to a new posting.
Find more information about support for armed forces families
{% endblock %}


Mort’s small traces
Mort Yao“Tiger got to hunt, bird got to fly;
Man got to sit and wonder ‘why, why, why?’
Tiger got to sleep, bird got to land;
Man got to tell himself he understand.”
— Kurt Vonnegut
Contents
- Mathematics
- Naive set theory
- Mathematical logic
- General topology
- Calculus
- Linear algebra
- Abstract algebra
- Category theory and homological algebra
- Analysis
- Measure theory
- Applied mathematics
- Probability theory and statistics
- Algorithms
- Computational geometry
- Cryptography
- Computational complexity theory
- Programming language theory
- Formal semantics
- Type theory and Curry-Howard correspondence
- Program analysis and transformation
- Machine learning
- Artificial neural networks
- Computer vision and image processing
- Natural language processing
- Software technology
- Computer systems and assembly
- Unix and system programming
- TCP/IP and socket programming
- Web and databases
- Compilers
- Information security
- Proof-carrying code


In this blog post, I will talk a little bit about my experience in building my personal website. I would have to say, at first, I was very intimidated at the idea of creating my own personal website because I did not really have much experience in designing websites before. I also was having a difficult time with CSS which made creating a website even more intimidating. But after having made a website, although it is still very basic, I feel more confident in my ability to plan and build a website from scratch.
I have really liked the fact that there are numerous tools that we can use to make a website that is both personal and professional. As the onsite portion begins, I am very eager to build on the CSS knowledge I have and make more changes to my website as I become more comfortable writing CSS. The most challenging aspect of this exercise in making a website was picking up CSS. I had a difficult time getting used to CSS and I am not entirely sure the reason for this. It may be because of that fact that there are so many options to choose from that I sometimes get mixed up with the functions of each different property. The most rewarding aspect of making a website was going to my URL and knowing that I had made this website completely from scratch which is a very amazing feeling. Overall, I would say that I enjoyed making my own website and hope to build on my existing knowledge to make it more dynamic and unique in the next few weeks.


--- layout: archive title: Zulip Chat Archive permalink: /stream/113488-general/topic/This.20will.20brick.20your.20computer!.html ---
import data.int.basic set_option trace.class_instances true #check λ n : ℤ, (n : ℕ)
This is well known. Lean will time out trying to coerce an int into a nat rather than give up
remove the first line and it's fine!
Hopefully fixed in Lean 4
import data.polynomial universe u variables {α : Type u} [comm_semiring α] [decidable_eq α] def derivative (p : polynomial α) : polynomial α := finsupp.sum p $ λ n c, n * polynomial.C c * polynomial.X^(n-1) @[simp] lemma derivative_C_mul_X (x : α) (n : ℕ) : derivative (polynomial.C x * polynomial.X^n) = n * polynomial.C x * polynomial.X^(n-1) := begin unfold derivative, rw [← polynomial.single_eq_C_mul_X, finsupp.sum_single_index], all_goals { rw [polynomial.C_0, mul_zero, zero_mul] } end --timeout @[simp] lemma derivative_C (x : α) : derivative (polynomial.C x) = 0 := derivative_C_mul_X x 0
there are some nontrivial defeq simplifications there
at least try by simpa using derivative_C_mul_X x 0
first
it's intentionally incorrect
then what's the surprise?
well Lean should tell me instead of time out
you just asked it to reduce some big expression to 0
it's got to unfold a bunch of definitions and run the power function, etc
it's not obviously not defeq
I don't actually know if it's defeq
neither does lean...
oh wow it's already done
i'm lucky i realized so soon
{% endraw %}Last updated: Apr 24 2020 at 19:02 UTC


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What’s open, closed on Veterans Day
by Miyoko WolfMany businesses and public services will be closed or operating on a different schedule Monday for Veterans Day.
Here’s what’s closed:
• Most government offices, as well as public libraries and community centers
• Most banks and credit unions
• Financial markets
• Post offices; mail will not be delivered.
Also worth noting:
• In Seattle, on-street parking is free on the holiday.
• Seattle garbage, food and yard waste and recycling collections will run on a normal schedule for Veterans Day.
• For public-transportation users, some King County Metro Transit and Sound Transit routes will run on a reduced weekday schedule. To plan a trip, check websites for King County Metro Transit, the Washington State Department of Transportation and Sound Transit for information.
• Water taxis: West Seattle and Vashon routes will not be in service on Veterans Day.
Miyoko Wolf: miwolf@seattletimes.com;


#include <b2WeldJoint.h>
Public Member Functions | |
| b2Vec2 | GetAnchorA () const |
| Get the anchor point on bodyA in world coordinates. | |
| b2Vec2 | GetAnchorB () const |
| Get the anchor point on bodyB in world coordinates. | |
| b2Vec2 | GetReactionForce (float32 inv_dt) const |
| Get the reaction force on body2 at the joint anchor in Newtons. | |
| float32 | GetReactionTorque (float32 inv_dt) const |
| Get the reaction torque on body2 in N*m. | |
Protected Member Functions | |
| b2WeldJoint (const b2WeldJointDef *def) | |
| void | InitVelocityConstraints (const b2TimeStep &step) |
| void | SolveVelocityConstraints (const b2TimeStep &step) |
| bool | SolvePositionConstraints (float32 baumgarte) |
Protected Attributes | |
| b2Vec2 | m_localAnchorA |
| b2Vec2 | m_localAnchorB |
| float32 | m_referenceAngle |
| b2Vec3 | m_impulse |
| b2Mat33 | m_mass |
Friends | |
| class | b2Joint |
A weld joint essentially glues two bodies together. A weld joint may distort somewhat because the island constraint solver is approximate.
| b2WeldJoint::b2WeldJoint | ( | const b2WeldJointDef * | def | ) | [protected] |
| b2Vec2 b2WeldJoint::GetAnchorA | ( | ) | const [virtual] |
Get the anchor point on bodyA in world coordinates.
Implements b2Joint.
| b2Vec2 b2WeldJoint::GetAnchorB | ( | ) | const [virtual] |
Get the anchor point on bodyB in world coordinates.
Implements b2Joint.
Get the reaction force on body2 at the joint anchor in Newtons.
Implements b2Joint.
Get the reaction torque on body2 in N*m.
Implements b2Joint.
| void b2WeldJoint::InitVelocityConstraints | ( | const b2TimeStep & | step | ) | [protected, virtual] |
Implements b2Joint.
| bool b2WeldJoint::SolvePositionConstraints | ( | float32 | baumgarte | ) | [protected, virtual] |
Implements b2Joint.
| void b2WeldJoint::SolveVelocityConstraints | ( | const b2TimeStep & | step | ) | [protected, virtual] |
Implements b2Joint.
friend class b2Joint [friend] |
b2Vec3 b2WeldJoint::m_impulse [protected] |
b2Vec2 b2WeldJoint::m_localAnchorA [protected] |
b2Vec2 b2WeldJoint::m_localAnchorB [protected] |
b2Mat33 b2WeldJoint::m_mass [protected] |
float32 b2WeldJoint::m_referenceAngle [protected] |


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“The world is one big data problem.” – by Andrew McAfee, co-director of the MIT Initiative
© Copyright 2021 myClass


Simple ARIA Toolbar Widget
A generic pattern for "toolbars" which offer buttons for manipulating content in some way. In this case, it's sorting a list.
Sorting crab names
- Fiddler crab
- Hermit crab
- Red crab
- Robber crab
- Sponge crab
- Yeti crab
Source: heydonworks.com


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