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Las Ketchup The Ketchup Song Listen and discover ... - Last.fm
The Ketchup Song appears on the album 100 Zinderende Zomerhits. Las Ketchup is a 4-girl . Discover more music, concerts, videos, and pictures with the largest catalogue online at Last.fm. . Buy on Amazon MP3 Amazon MP3 Expand .
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The Ketchup Song (LAS KETCHUP) Official video HQ. - YouTube
May 14, 2010 . The Ketchup song, gr song, hope u enjoy n, Official video, HQ.
http://www.youtube.com/watch?v=JuMqmQnUonQ
Las Ketchup Album Mp3 Download
4.85 MB 192 kbps. LAS KETCHUP - The Ketchup Song (Asereje) (Album Version ) mp3. Play . Las Ketchup - Las Ketchup-Asereje (Final) mp3. Play. Download .
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Contents |
[hunters glen apartments pinehurst nc] History
Download the ketchup song asereje spanish version none for FREE
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Las Ketchup Free listening, concerts, stats, & pictures at Last.fm
Watch videos & listen free to Las Ketchup: Asereje, The Ketchup Song & more, plus 12 pictures. . Discover more music, concerts, videos, and pictures with the largest catalogue online at Last.fm. . Buy all tracks at Amazon MP3 See more .
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The Ketchup Song - Wikipedia, the free encyclopedia
For the song by Stompin' Tom Connors, see Ketchup Song (Stompin' Tom Connors song). . "The Ketchup Song" is the English title of the song "Aserejé," recorded by the Spanish . This page was last modified on 23 March 2013 at 16: 59.
http://en.wikipedia.org/wiki/The_Ketchup_Song
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Las Ketchup - Asereje: Free MP3 Download - Last 200 searches
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[roger lawson portuguese india] References
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Honest. was developed in order to track DSL outages within a single property, to be passed onto the user's ISP.
This is not intended to troubleshoot the entire scope of issue that may cause an outage, including (but not limited to) faulty routers, DNS Lookup issues, and exceeded data allowance.
If you are using this utility to record issues with the NBN network, you may also be interested in using MrMac's (Unofficial) NBN Speed Lookup to determine what kind of connection you have to your premises.
Download Links Coming Soon


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The index of the entity as it was found in the investment tables.
Mapped to IDestinyLoreDefinition in the manifest.
Mapped to IDestinyObjectiveDefinition in the manifest.
If this is true, then there is an entity with this identifier/type combination, but BNet is not yet allowed to show it. Sorry!
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When entities refer to each other in Destiny content, it is this hash that they are referring to.


| generate.MixSim {pmclust} | R Documentation |
This function utilizes MixSim to generate sets of data for testing algorithms.
generate.MixSim(N, p, K, MixSim.obj = NULL, MaxOmega = NULL, BarOmega = NULL, PiLow = 1.0, sph = FALSE, hom = FALSE)
N |
total sample size across all S processors, i.e.
sum over |
p |
|
K |
number of clusters. |
MixSim.obj |
an object returned from |
MaxOmega |
maximum overlap as in |
BarOmega |
averaged overlap as in |
PiLow |
lower bound of mixture proportion as in |
sph |
sph as in |
hom |
hom as in |
If MixSim.obj
is NULL, then BarOmega
and MaxOmega
will be used in MixSim
to obtain a new
MixSim.obj
.
A set of simulated data and information will be returned in a list variable including:
K | number of clusters, as the input |
p | dimension of data
X.spmd ,
as the input |
N | total sample size, as the input |
N.allspmds | a collection of sample sizes for all S processors, as the input |
N.spmd | total sample size of given processor, as the input |
X.spmd | generated data set with dimension with
dimension N.spmd * p |
CLASS.spmd
| true id of each data, a vector of
length N.spmd
and has values from 1 to K |
N.CLASS.spmd | true sample size of each clusters, a
vector of length K |
MixSim.obj | the true model where data
X.spmd generated from
|
Wei-Chen Chen<EMAIL_ADDRESS>and George Ostrouchov.
Melnykov, V., Chen, W.-C. and Maitra, R. (2012) “MixSim: Simulating Data to Study Performance of Clustering Algorithms”, Journal of Statistical Software, (accepted).
High Performance Statistical Computing (HPSC) Website: http://thirteen-01.stat.iastate.edu/snoweye/hpsc/
Programming with Big Data in R Website: http://r-pbd.org/
## Not run: # Save code in a file "demo.r" and run in 4 processors by # > mpiexec -np 4 Rscript demo.r ### Setup environment. library(pmclust, quiet = TRUE) ### Generate an example data.  PARAM.org <- set.global(K = K) # Set global storages. # PARAM.org <- initial.em(PARAM.org) # One initial. PARAM.org <- initial.RndEM(PARAM.org) # Ten initials by default. PARAM.new <- apecma.step(PARAM.org) # Run APECMa. em.update.class() # Get classification. ### Get results. N.CLASS <- get.N.CLASS(K) comm.cat("# of class:", N.CLASS, "\n") comm.cat("# of class (true):", data.spmd$N.CLASS.spmd, "\n") ### Quit. finalize() ## End(Not run)


Abhishek B
CSS means Cascading Style Sheets, it makes the html pages to appear more attractively and user friendly


TOTAL RECALL A film review by Mark R. Leeper Copyright 1990 Mark R. Leeper
Capsule review: Violence, chases, thoughtful plotting, special effects, gore, Arnold Schwarzenegger, a few intelligent ideas. They don't all seem as if they could be in one film. Nobody will be totally happy with TOTAL RECALL, but there is a surprising degree of good science fiction in what could be Arnold Schwarzenegger's most intelligent fantasy film to date. Rating: +2.
I have to say that I usually am not very impressed by action or violence in films. How much variation is there in chase scenes from one film to the next? To my mind there is almost none other than the background scenery changing. The same goes for violence. There are about as many ways to tear apart a human as there are to carve a turkey. It is a special effect that has been done so many times in film that it no longer is of any interest to me to see it. I am well aware that there are people who can enjoy chases and violence in film after film and enjoy them every time, just as there are people who listen to the "Top 40" radio stations and can enjoy hearing the same songs over and over. Chase scenes and violence to me seem like unimaginative filler. In addition and amazingly, I find I have this weird psychic ability to know at the beginning of a fight scene who is going to win the fight. If there are four armed thugs taking on an unarmed Arnold Schwarzenegger, psychic vibrations tell me at the beginning of the fight who is going to win. The vibrations work for chase scenes also and there, too, they remove much of the suspense.
There have been a number of films that have tried to marry action to a science fiction plot. They have been films such as THE TERMINATOR, PREDATOR, THEY LIVE, and ROBOCOP. I consistently like them less than the general public does and it is more than likely because the action and violence scenes have so little value for me. What I think I am really rating is the science fiction film that frames the action and violence-- often making for a much shorter film. Take the action and violence from the four films I mentioned and none is a particularly good science fiction film. Only THEY LIVE has a particularly engaging premise. That may be because THEY LIVE is an adaptation of a pre-existing, published science fiction story so to some extent the story has stood on its own. TOTAL RECALL is a new action film also based on an existing science fiction story and starring Arnold Schwarzenegger.
An Arnold Schwarzenegger action film based on a story by Philip K. Dick sounds almost like a contradiction in terms. Dick writes cerebral--not to say neurotic--science fiction about people who generally seem to live inside their heads. You could not fit Schwarzenegger into a Dick story with a crowbar. The main character of Dick's "We Can Remember It for You Wholesale" is a mousy, hen-pecked government clerk. Changes were inevitable if the story was to be made into an action vehicle and vast changes were indeed made. Yet the screenplay has retained much of the plot and most of the engaging ideas of the story before going off in its own direction. Even when it does diverge, some of the concepts it adds are thoughtful and intelligent. Of course, some unfortunately are not. I know of nobody who actually liked the last ten minutes or so of the film. Like many films, TOTAL RECALL was damaged by somebody's idea of a big finish.
This is a story with a lot of twists, particularly early on when it is still being faithful to the original story. This means that I cannot be very informative about the plot, but I can say that it starts out being about a sort of an average 21st century man with big muscles and an unusual problem. He keeps dreaming about Mars. There is nothing in life Doug Quaid wants more than to go to Mars. (In the story his name was Doug Quail, but it was changed, possibly because it sounded too much like Dan Quayle.) Unfortunately, only relatively few people can go to the mining colonies on Mars and Quaid is not one. Well, the next best thing to being there is having *been* there. The difference between having been there and not is having the memories. In this future world a company called REKALL can put artificial memories into your head more vivid and believable than real memories. So Quaid agrees to buy an artificial memory of Mars--just a minor adjustment to his reality. But any Philip K. Dick fan can tell you things go awry when you start adjusting reality. They certainly do for Quaid. The script is a remarkable piece of work that allows the viewer to look at the altering of reality to be a minor plot complication in an action film or it could be what the film is all about. My wife came up with reasonable internal evidence that the surface interpretation of what happens in the film is wrong and another interpretation of the reality is correct. Clearly the script is richer than one usually expects from a Schwarzenegger action chase film.
Visually there are some very unconvincing effects and some very nice ones. Some of the model work is below average for Industrial Light & Magic and Dream Quest, but there are some very impressive sights also. Audiences seem to enjoy the subway security station as an effect different from what ILM and DQ have done in the past. the special effects have been described as "eye-popping," a pun that will be appreciated in the first five minutes of the film but also an accurate one. That brings us to the gore. This film is directed by Dutchman Paul Verhoeven. He is generally good but uses a very great deal of gore and violence, particularly in his later films. This is a very violent film and viewers should go expecting that. Also go expecting to see a lot of familiar brand names that helped to finance the film. (Of course, Dick mentions a typewriter company by name in the original story, so there are precedents.)
In summary, TOTAL RECALL is a lot of different films. It should please pretty much anyone who likes science fiction films. It should have a broad range of appeal on many levels. I rate it a +2 on the -4 to +4 scale.
[The novelette "We Can Remember It for You Wholesale" can be found in the following magazines, collections, and anthologies: - MAGAZINE OF FANTASY & SCIENCE FICTION, April 1966 - MAGAZINE OF FANTASY & SCIENCE FICTION, 30th Anniversary Issue - THE PRESERVING MACHINE by Philip K. Dick - ALPHA 5 edited by Robert Silverberg - THE BEST FROM FANTASY & SCIENCE FICTION 16 edited by Edward L. Ferman - EARTH IN TRANSIT edited by Sheila Schwartz - NEBULA AWARD STORIES 2 edited by Brian W. Aldiss and Harry Harrison - THE ROAD TO SCIENCE FICTION, edited by James E. Gunn - TWENTY YEARS OF FANTASY & SCIENCE FICTION edited by Edward L. Ferman and Robert P. Mills - WORLD'S BEST SCIENCE FICTION: 1967 edited by Donald A. Wollheim and Terry Carr]
Mark R. Leeper att!mtgzx!leeper<EMAIL_ADDRESS>.
The review above was posted to the
rec.arts.movies.reviews newsgroup (de.rec.film.kritiken for German reviews).
The Internet Movie Database accepts no responsibility for the contents of the
review and has no editorial control. Unless stated otherwise, the copyright
belongs to the author.
Please direct comments/criticisms of the review to relevant newsgroups.
Broken URLs inthe reviews are the responsibility of the author.
The formatting of the review is likely to differ from the original due
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Related links: index of all rec.arts.movies.reviews reviews


Having much enjoyed Phil Baker's biography of Austin Osman Spare, I have just started reading his earlier life of Dennis Wheatley, The Devil Is A Gentleman (2009). It is as informative, entertaining, and amusing as the Spare book. Here is Dennis, reminiscing about his visit to Germany in 1913 to learn about the family wine trade. He was much impressed by the officer class…
… a race apart, immune from arrest by the police, they could be tried only by their own courts of honour and, if found guilty of a disgraceful act, they were simply given a pistol with which to shoot themselves. The civilian population had been conditioned to regard them with abject veneration. Ladies, as well as men, when approaching one of them in a street, stepped off the pavement into the gutter to give them ample room to pass, which they accepted as their right and did not even acknowledge by the flicker of an eyelid. Awed, and admiring, I watched them greet one another with a graceful salute, a click of the heels and a sharp bow from the waist. It was years later before I realised that very few of them had any brains at all …


I am a responsive web developer who loves solving problems. Making a website pixel perfect, down to the little details, is a very rewarding experience for me, and making it work great on other devices just as well!
I was raised in Green Bay, WI, but moved to Columbus, WI just before high school started. I enjoy finding new ways to improve and grow, and learning new skills!
Besides for my love of computer technology and the web, my passions also include a little bit of videogames and binge watching House MD on the weekends!
Getting things to look and feel 'right' is what I love doing. Few things are as satisfying to me as getting a website to look and work just the way I want it to! Being detail oriented is one of my greatest strengths!


The world under heaven, after a long period of division, tends to unite; after a long period of union, tends to divide.
The empire, long divided, must unite; long united, must divide. Thus it has ever been.
Unity succeeds division and division follows unity. One is bound to be replaced by the other after a long span of time.


We have all heard that data is the new oil. While a novel metaphor, the value and importance of data to humankind should not surprise anyone. Centuries before the conception and development of the first written language, humans used styli to etch numerals into clay tablets as a record keeping and accounting mechanism. Over time, as language and technologies evolved, the need to record data kept pace. From humble beginnings as a means to track the sale or trade of goods, time keeping and eventually recording scientific discoveries, data evolved to drive the largest corporations in their quest for the top. However, one thing remains the same - humankind's insatiable need to record and preserve data.
We believe that in this history exist thousands of interesting data sets, ripe for visualizing using twenty first century tools. Thus the genesis for this new social experiment - Throwback Thursday. An initiative aimed at engaging the already active Tableau Community in discovering, socializing and visualizing historic data.
Every week, #ThrowbackDataThursday provides a data set for you to explore, along with details on the provenance of the data source. Then, you get your chance to visualize the data. After completing your viz, post it to Twitter with the hashtag #ThrowbackDataThursday and tagging @TThrowbackThurs. Towards the end of the week, the team will comb through the submissions finding the examples that we think best fit the data. These examples will be posted to http://throwback-thursday.com and our Twitter account, @TThrowbackThurs, for community feedback.
So, sit back and let us curate your historic data experience. We hope you enjoy!


Traditional
This dress style stays true to tradition with beautiful ornate embroidery found in old colonial times, or in recent popularity the Charro "Mariachi" style. These dresses are found within traditional solid colors, accents and fabrics.
A Quincenera dress is a very important part of a Quinceañera celebration. Picking a Quinceañera dress is almost as important as picking a wedding dress. The dress design shows the fact that the Quinceañera girl is no longer a young girl, but is now a senorita (miss). The dress should call attention to the fact that that the girl is leaving childhood and entering womanhood, as this is the purpose of the Quinceañera's party. This dress is the key to making the birthday girl feel like the princess she is on this big day.
This dress style stays true to tradition with beautiful ornate embroidery found in old colonial times, or in recent popularity the Charro "Mariachi" style. These dresses are found within traditional solid colors, accents and fabrics.
This dress style is very popular even within prom goers, and usually opted as the go to style since High School girls will also go to prom. This dress can come in many different styles however it is still popular to find it in a high gown with many ruffles and practically in any color.
This dress style is generally eye pop-ing it’s the kind of dress you wear once! and to make a statement. These dress are often found to take on a bold pattern or statement. As seen within the image the dress it taking the "traditional" and taking it one step further by adding beading and a sweetheart neck line.
This dress style of dress is usually found in one solid color with many ball gown "Disney Princess" like silhouettes.


American Made
Designed by AQL in California, Assembled in the USA
Environmentally Friendly
We want to leave the world better than we found it


Class: Sprout::Executable::Param
- Inherits:
-
Object
- Object
- Sprout::Executable::Param
- Defined in:
- lib/sprout/executable/param.rb
Overview
The abstract base class for all Executable parameters.
This class provides a variety of template methods and general functionality to the different executable parameter types.
Many of these parameter attributes are exposed to Sprout::Executable concrete classes as the options hash like:
class Foo
include Sprout::Executable
add_param :name, String, :hidden_name => true
end
Constant Summary
- DEFAULT_DELIMITER =
Default value for the delimiter that will separate parameter names from their values.
'='
- DEFAULT_OPTION_PARSER_TYPE_NAME =
Defaut TYPE assumed for parameters when creating documentation for the OptionParser.
'STRING'
- DEFAULT_PREFIX =
Default value for the parameter prefix. Should usually be pulled from the belongs_to Sprout::Executable.
'--'
- DEFAULT_SHORT_PREFIX =
Default prefix for truncated parameters. Should usually be pulled from the belongs_to Sprout::Executable.
'-'
Instance Attribute Summary (collapse)
-
- (Object) belongs_to
The Sprout::Executable that this parameter instance belongs to.
-
- (Object) delimiter
Executable::Params join their name/value pair with an equals sign by default, this can be modified To a space or whatever you wish.
-
- (Object) description
The String description that will be used for RDoc documentation and user help.
- - (Object) file_expression
-
- (Object) hidden_name
Boolean value that hides the name parameter from the shell execution.
-
- (Object) hidden_value
Boolean value that hides the value parameter from the shell execution.
-
- (Object) name
The String (or Symbol) name of the parameter.
-
- (Object) prefix
Leading character for each parameter Can sometimes be an empty string, other times it’s a double dash ’--’ but usually it’s just a single dash ’-’.
-
- (Object) reader
A Symbol that refers to a method that will return the expected value when called.
-
- (Object) required
Boolean value that will cause a Sprout::Errors::UsageError if the executable is invoked without this parameter first being set.
- - (Object) shell_name
-
- (Object) short_name
The short name for this parameter.
-
- (Object) to_shell_proc
An optional Proc that should be called when this parameter is serialized to shell output.
-
- (Object) type
The data type of the parameter, used to generate more appropriate RDoc content for the concrete Sprout::Executable.
-
- (Object) value
The value that was assigned to this parameter when the concrete Sprout::Executable was instantiated and configured.
-
- (Object) writer
A Symbol that refers to a method (not accessor) that will be called when the value is set.
Instance Method Summary (collapse)
-
- (Object) clean_path(path)
protected
Clean the provided path using the current Sprout::System.
-
- (Object) default
Return the default value or nil if none was provided.
-
- (Object) default=(value)
Set the default value of the parameter.
- - (Object) default_option_parser_declaration
-
- (Boolean) file_is_output?(file)
protected
Return true if the Sprout::Executable that this parameter belongs_to has an output method (or parameter), and if the provided file matches the value of that parameter.
-
- (Boolean) hidden_name?
Should the param name be hidden from the shell? Used for params like ‘input’ on mxmlc.
-
- (Boolean) hidden_value?
Should the param value be hidden from the shell? Usually used for Boolean toggles like ’-debug’.
-
- (Param) initialize
constructor
Default constructor for Params, if you create a new concrete type, be sure to call super() in your own constructor.
-
- (Object) option_parser_declaration
How this parameter is provided to the Ruby OptionParser when being exposed as a Ruby Executable.
- - (Object) option_parser_name protected
-
- (Object) option_parser_short_name
The Ruby OptionParser short name with prefix.
- - (Object) option_parser_type_name protected
- - (Object) option_parser_type_output protected
-
- (Object) prepare
Prepare the parameter for execution or delegation, depending on what context we’re in.
- - (Object) prepare_prerequisites protected
-
- (Boolean) prepared?
Returns true if this parameter has already been prepared.
-
- (Boolean) required?
Returns Boolean value if this parameter is required.
-
- (Object) shell_value
The String representation of the value in a format that is appropriate for the terminal.
- - (Object) short_prefix
-
- (Object) to_rdoc
Create a string that can be turned into a file that rdoc can parse to describe the customized or generated task using param name, type and description.
-
- (Object) to_shell
Prepare and serialize this parameter to a string that is appropriate for shell execution on the current platform.
-
- (Object) validate
Ensure this parameter is in a valid state, raise a Sprout::Errors::MissingArgumentError if it is not.
-
- (Boolean) visible?
By default, Executable::Params only appear in the shell output when they are not nil.
Constructor Details
- (Param) initialize
Default constructor for Params, if you create a new concrete type, be sure to call super() in your own constructor.
234 235 236 237 238 239 240 |
# File 'lib/sprout/executable/param.rb', line 234 def initialize @description = 'Default Description' @hidden_value = false @hidden_name = false @delimiter = DEFAULT_DELIMITER @option_parser_type_name = DEFAULT_OPTION_PARSER_TYPE_NAME end |
Instance Attribute Details
- (Object) belongs_to
The Sprout::Executable that this parameter instance belongs to.
60 61 62 |
# File 'lib/sprout/executable/param.rb', line 60 def belongs_to @belongs_to end |
- (Object) delimiter
Executable::Params join their name/value pair with an equals sign by default, this can be modified To a space or whatever you wish.
66 67 68 |
# File 'lib/sprout/executable/param.rb', line 66 def delimiter @delimiter end |
- (Object) description
The String description that will be used for RDoc documentation and user help.
71 72 73 |
# File 'lib/sprout/executable/param.rb', line 71 def description @description end |
- (Object) file_expression
371 372 373 |
# File 'lib/sprout/executable/param.rb', line 371 def file_expression @file_expression ||= belongs_to.default_file_expression end |
Boolean value that hides the name parameter from the shell execution.
add_param :name, String, :hidden_name => true
Without this option, the above parameter would serialize to the process like:
foo --name=Value
But with this option, the above parameter would serialize to the process like:
foo Value
89 90 91 |
# File 'lib/sprout/executable/param.rb', line 89 def hidden_name @hidden_name end |
Boolean value that hides the value parameter from the shell execution.
add_param :visible, Boolean, :hidden_value => true
Without this option, the above parameter would serialize to the process like:
foo --visible=true
But with this option, the above parameter would serialize to the process like:
foo --visible
107 108 109 |
# File 'lib/sprout/executable/param.rb', line 107 def hidden_value @hidden_value end |
- (Object) name
The String (or Symbol) name of the parameter.
111 112 113 |
# File 'lib/sprout/executable/param.rb', line 111 def name @name end |
- (Object) prefix
Leading character for each parameter Can sometimes be an empty string, other times it’s a double dash ’--’ but usually it’s just a single dash ’-’
121 122 123 |
# File 'lib/sprout/executable/param.rb', line 121 def prefix @prefix ||= (belongs_to.nil?) ? DEFAULT_PREFIX : belongs_to.default_prefix end |
- (Object) reader
A Symbol that refers to a method that will return the expected value when called. This method can be private.
add_param :visible, Boolean, :reader => :get_visible
def get_visible
return @visible
end
133 134 135 |
# File 'lib/sprout/executable/param.rb', line 133 def reader @reader end |
- (Object) required
Boolean value that will cause a Sprout::Errors::UsageError if the executable is invoked without this parameter first being set.
add_param :visible, Boolean :required => true
Default false
144 145 146 |
# File 'lib/sprout/executable/param.rb', line 144 def required @required end |
- (Object) shell_name
375 376 377 |
# File 'lib/sprout/executable/param.rb', line 375 def shell_name @shell_name ||= prefix + name.to_s.split('_').join('-') end |
- (Object) short_name
The short name for this parameter. If it’s not explicitly, the first character of the parameter name will be used. When multiple parameters have the same first character, the first one encountered will win.
356 357 358 |
# File 'lib/sprout/executable/param.rb', line 356 def short_name @short_name ||= name.to_s.split('').shift end |
- (Object) to_shell_proc
An optional Proc that should be called when this parameter is serialized to shell output. The Proc should return a String value that makes sense to the underlying process.
add_param :visible, Boolean, :to_shell_proc => Proc.new {|p| "---result" }
153 154 155 |
# File 'lib/sprout/executable/param.rb', line 153 def to_shell_proc @to_shell_proc end |
- (Object) type
The data type of the parameter, used to generate more appropriate RDoc content for the concrete Sprout::Executable.
158 159 160 |
# File 'lib/sprout/executable/param.rb', line 158 def type @type end |
- (Object) value
The value that was assigned to this parameter when the concrete Sprout::Executable was instantiated and configured.
163 164 165 |
# File 'lib/sprout/executable/param.rb', line 163 def value @value end |
- (Object) writer
A Symbol that refers to a method (not accessor) that will be called when the value is set. This method is not responsible for actually storing the value, but should instead be thought of as a badly named callback that will be triggered with the new value whenever the value changes.
This method can be private.
add_param :visible, Boolean, :writer => :set_visible
private
def set_visible value
do_something_with value
value
end
184 185 186 |
# File 'lib/sprout/executable/param.rb', line 184 def writer @writer end |
Instance Method Details
- (Object) clean_path(path) (protected)
Clean the provided path using the current Sprout::System.
428 429 430 |
# File 'lib/sprout/executable/param.rb', line 428 def clean_path path Sprout::System.create.clean_path path end |
- (Object) default
Return the default value or nil if none was provided.
279 280 281 |
# File 'lib/sprout/executable/param.rb', line 279 def default @default end |
- (Object) default=(value)
Set the default value of the parameter. Using this option will ensure that required parameters are not nil, and default values can be overridden on instances.
add_param :name, String, :default => 'Bob'
272 273 274 275 |
# File 'lib/sprout/executable/param.rb', line 272 def default=(value) self.value = value @default = value end |
- (Object) default_option_parser_declaration
339 340 341 |
# File 'lib/sprout/executable/param.rb', line 339 def default_option_parser_declaration [ prefix, option_parser_name ] end |
- (Boolean) file_is_output?(file) (protected)
Return true if the Sprout::Executable that this parameter belongs_to has an output method (or parameter), and if the provided file matches the value of that parameter.
This method (convention) is used to avoid creating circular prerequisites in Rake. For most types of File parameters we want to make them into prerequisites, but not if the File is the one being created by the outer Sprout::Executable.
442 443 444 |
# File 'lib/sprout/executable/param.rb', line 442 def file_is_output? file belongs_to.respond_to?(:output) && belongs_to.output.to_s == file end |
Should the param name be hidden from the shell? Used for params like ‘input’ on mxmlc
300 301 302 |
# File 'lib/sprout/executable/param.rb', line 300 def hidden_name? @hidden_name end |
Should the param value be hidden from the shell? Usually used for Boolean toggles like ’-debug’
307 308 309 |
# File 'lib/sprout/executable/param.rb', line 307 def hidden_value? @hidden_value end |
- (Object) option_parser_declaration
How this parameter is provided to the Ruby OptionParser when being exposed as a Ruby Executable.
327 328 329 330 331 332 333 334 335 336 337 |
# File 'lib/sprout/executable/param.rb', line 327 def option_parser_declaration declaration = default_option_parser_declaration # TODO: Need to figure out how to support hidden name inputs... #if(hidden_name?) #declaration = [option_parser_type_output] # if(!hidden_value?) declaration << delimiter << option_parser_type_output end declaration.join('') end |
- (Object) option_parser_name (protected)
410 411 412 |
# File 'lib/sprout/executable/param.rb', line 410 def option_parser_name name.to_s.gsub('_', '-') end |
- (Object) option_parser_short_name
The Ruby OptionParser short name with prefix.
345 346 347 |
# File 'lib/sprout/executable/param.rb', line 345 def option_parser_short_name [ short_prefix, short_name ].join('') end |
- (Object) option_parser_type_name (protected)
414 415 416 |
# File 'lib/sprout/executable/param.rb', line 414 def option_parser_type_name @option_parser_type_name end |
- (Object) option_parser_type_output (protected)
418 419 420 421 |
# File 'lib/sprout/executable/param.rb', line 418 def option_parser_type_output type = hidden_value? ? '' : option_parser_type_name required? ? type : "[#{type}]" end |
- (Object) prepare
Prepare the parameter for execution or delegation, depending on what context we’re in.
286 287 288 289 |
# File 'lib/sprout/executable/param.rb', line 286 def prepare prepare_prerequisites @prepared = true end |
- (Object) prepare_prerequisites (protected)
423 424 |
# File 'lib/sprout/executable/param.rb', line 423 def prepare_prerequisites end |
- (Boolean) prepared?
Returns true if this parameter has already been prepared.
293 294 295 |
# File 'lib/sprout/executable/param.rb', line 293 def prepared? @prepared end |
- (Boolean) required?
Returns Boolean value if this parameter is required.
251 252 253 |
# File 'lib/sprout/executable/param.rb', line 251 def required? (required == true) end |
- (Object) shell_value
The String representation of the value in a format that is appropriate for the terminal.
For certain types of parameters, like File, spaces may be escaped on some platforms.
367 368 369 |
# File 'lib/sprout/executable/param.rb', line 367 def shell_value value.to_s end |
- (Object) short_prefix
320 321 322 |
# File 'lib/sprout/executable/param.rb', line 320 def short_prefix @short_prefix ||= (belongs_to.nil?) ? DEFAULT_SHORT_PREFIX : belongs_to.default_short_prefix end |
- (Object) to_rdoc
Create a string that can be turned into a file that rdoc can parse to describe the customized or generated task using param name, type and description
400 401 402 403 404 405 406 |
# File 'lib/sprout/executable/param.rb', line 400 def to_rdoc result = '' parts = description.split("\n") unless description.nil? result << "# #{parts.join("\n# ")}\n" unless description.nil? result << "def #{name}=(#{type})\n @#{name} = #{type}\nend\n\n" return result end |
- (Object) to_shell
Prepare and serialize this parameter to a string that is appropriate for shell execution on the current platform.
Calling to_shell will first trigger a call to the prepare template method unless prepared? returns true.
386 387 388 389 390 391 392 393 394 |
# File 'lib/sprout/executable/param.rb', line 386 def to_shell prepare if !prepared? validate return '' if !visible? return @to_shell_proc.call(self) unless @to_shell_proc.nil? return shell_value if hidden_name? return shell_name if hidden_value? return [shell_name, delimiter, shell_value].join end |
- (Object) validate
Ensure this parameter is in a valid state, raise a Sprout::Errors::MissingArgumentError if it is not.
258 259 260 261 262 |
# File 'lib/sprout/executable/param.rb', line 258 def validate if(required? && value.nil?) raise Sprout::Errors::MissingArgumentError.new("#{name} is required and must not be nil") end end |
- (Boolean) visible?
By default, Executable::Params only appear in the shell output when they are not nil
245 246 247 |
# File 'lib/sprout/executable/param.rb', line 245 def visible? !value.nil? end |


From: Mr. Ahmed Abdul Kadir E-mail: Reply<EMAIL_ADDRESS>Attention:The Managing Director Tell: +66 5108116. Private And Confidential To whom it may concern, It is my pleasure to write this mail to you and to say thank you for your effort in providing an opportunity to read my mail. I got your contact when I was making some searches on the internet. My name is Ahmed Abdul Kadir, a sudanese refugee; my Father was until recently, one of the personal aid to the former President of Iraq who was overthrown out of power during the War in Iraq which took many lives. I am contacting you to seek your co-operation in investing US$10.5 Million in your country or any other with good economic prospect. My late father was able to safe guard the fund with the contacts he had in the Diplomatic Corps and the funds are being held under the protection and custody of a Diplomat friend of his. I have decided to contact you because I am interested in investing these funds. Please kindly guide and assist me in making the right investment as I am really a novice when considering the technicalities and logistics involved in running a business. The details of the investment will be worked out to our respective satisfaction. In view of your participation, I am ready to give you a good negotiable percentage for your assistance, or better still commit it into a viable joint venture. Be assured that you stand no risk of any kind as the funds belong to me as the only surviving son and as soon as I get your consent, the necessary papers will be drawn up to facilitate the movement to the funds to your country for the investment. However, upon your acceptance to work as my partner, you can contact me by return e-mail for more details. I strongly believe that associating with you to embark on this and other business ventures will derive a huge success, please include you private contact telephone number and e-mail when replying. Yours Sincerely. Mr. Ahmed Abdul Kadir


--- layout: post date: 2008-03-26 time: "09:00:00" authors: ["Greg Wilson"] title: Nice Quote tags: ["Community", "Content"] ---
An article about computational science in a scientific publication is not the scholarship itself, it is merely advertising of the scholarship. The actual scholarship is the complete software development environment and the complete set of instructions which generated the figures.
—David L. Donoho, WaveLab and Reproducible Research, 1995, p. 5.
(via Andrew Lumsdaine)


| Home | Libraries | People | FAQ | More |
ReadablePropertyMap
A ReadablePropertyMap is used for mapping a position, as represented by a cursor, to a value.
elements
UnaryFunc
Must be a model of UnaryFunction.
cursor
Iter
Must be a model of ReadableIterator and IncrementableIterator.
key_type
ReadableIterator<Iter>::reference
The key type of the cursor
value_type
property_map::traits::value_type<UnaryFunc, Iter>::type
The value type of the elements property map
| Copyright © 2006 Eric Niebler |


Table of Contents
License Wizard Options
Using the Licensing Web Site
Entering a License
Connecting to an Existing License Server
Troubleshooting
|
|
Product Licensing Complete
This screen displays the location on your computer where your license file was saved. Your product will now run in licensed mode.
Click Exit to complete the licensing process.
Note
If, after completing the licensing process, your product does not run in licensed mode, consult the Installation and Licensing Guide in your product's online help system for additional licensing information. |
ITT Visual Information Solutions (February 17, 2009)
|


Ubers and Lyfts can be expensive, and finding a group that you’re
comfortable splitting the ride and cost with is not always easy
GroupRide offers a solution to this problem in the form of a mobile
social network application
We are a group of fun RPI students building this open source project to solve the infamous
rideshare problem our campus faces!
Fork us on Github!
Fork


Our Contributors
Check out our wonderful sponsors below, whose support made many things possible:
More About Select Sponsors
Stevens Capital Management LP is a quantitative hedge fund manager specializing in the rigorous development and disciplined implementation of empirically based trading strategies. Our flagship fund has been in business for more than 30 years. Our highly productive team works in a fast-paced collegial environment, utilizing extensive data sets, technology and the scientific method to devise and employ trading strategies throughout the world’s most liquid financial markets. SCM actively seeks candidates for career opportunities in quantitative financial research and C++ development. Alinea is an investing app for GenZs to invest in what matters to them like Clean Energy, Blockchain, or Women-Led companies. On Alinea, you can invest in stacks (bundles of stocks) which allow you to reduce your risk and diversify your investments from the start. Create your own stacks and share with friends! At Yugabyte, we are on a mission to build the default database for cloud-native applications in a multi-cloud world. We are well underway on this journey with YugabyteDB, the open-source, high-performance, distributed SQL database that runs on any cloud and enables developers to get instantly productive using well-known APIs. And the best is yet to come! We are looking for talented and driven people to join us on our ambitious mission and help us build a lasting and impactful company.
If you are interested in supporting all the things we do here at ACM, check out some of our opportunities for organizations to get involved. You can also view sponsorship details for the coming cycle here.


Huawei Mate 30 Pro officially makes its way to Europe, sortof
by MichailHuawei’s Mate 30 lineup was announced back in September but remained confined to China and a select group of Asian markets. Now, the Mate 30 Pro has officially arrived on European shores with Spain being the first country to get the latest Huawei flagship. There is still no word if the vanilla Mate 30 or Porsche Design variant will also make their way to Europe though.
The catch is that the Mate 30 Pro is available in limited quantities only at the Huawei Space Store in Madrid. The phone is going for €1,099 in its 8GB RAM and 256GB storage configuration and is only available in the Space Silver colorway.
There is also a hot launch promotion, which includes a €299 check that can be used towards other Huawei products. This offer is valid through December 9.
While this is a pretty sweet deal, the Mate 30 Pro is still lacking Google Mobile Services, which makes it a tough sell anywhere outside China. You can read our complete review to know how it works without them or check out the video version below.


Package org.jboss.stm.internal
Class RecoverableContainer<T>
- java.lang.Object
-
- org.jboss.stm.internal.RecoverableContainer<T>
-
- Direct Known Subclasses:
PersistentContainer
public class RecoverableContainer<T> extends java.lang.Object
Instances of this class represent the transactional memory within which non-persistent user objects can be placed and managed. Objects must implement an interface through which all transactional accesses occur. We don't mandate what the interface is, since that will depend upon the business logic. The interface, or the implementing class, must also use the @Transactional annotation.- Author:
- marklittle
-
-
Field Summary
Fields Modifier and Type Field Description protected int
_objectModel
protected java.util.WeakHashMap<T,T>
_transactionalProxies
protected int
_type
-
Constructor Summary
Constructors Modifier Constructor Description RecoverableContainer()
Create a container without a name.protected
RecoverableContainer(int objectModel)
RecoverableContainer(java.lang.String name)
Create a named container.protected
RecoverableContainer(java.lang.String name, int objectModel)
-
Method Summary
All Methods Instance Methods Concrete Methods Modifier and Type Method Description protected void
checkObjectType(java.lang.Object member)
protected T
createHandle(T member, int ot)
Return a handle through which the object should be used, rather than the one passed in.T
enlist(T member)
Given an object we create a new transactional instance of it and return that for future use.T
enlist(T member, Uid id)
Given an identified for an existing object, create another handle.T
getHandle(Uid reference)
Given a Uid, return the proxy for that instance.Uid
getUidForHandle(T proxy)
Given a real object, return the Uid if it exists in this container.Uid
getUidForOriginal(T member)
Given a real object, return the Uid if it exists in this container.boolean
isPessimistic(java.lang.Object member)
java.lang.String
name()
Get the name of the container.int
objectModel()
int
objectType()
java.lang.String
toString()
Gives the name of the container.
-
-
-
Constructor Detail
-
RecoverableContainer
public RecoverableContainer()
Create a container without a name. A name will be assigned automatically.
-
RecoverableContainer
public RecoverableContainer(java.lang.String name)
Create a named container.- Parameters:
name
- the name (should be unique, but this is not enforced).
-
RecoverableContainer
protected RecoverableContainer(int objectModel)
-
RecoverableContainer
protected RecoverableContainer(java.lang.String name, int objectModel)
-
-
Method Detail
-
name
public final java.lang.String name()
Get the name of the container.- Returns:
- the name.
-
enlist
public T enlist(T member)
Given an object we create a new transactional instance of it and return that for future use. All accesses on the returned object will be managed according to the rules defined in the various annotations. If the original object instance is used then no transactional manipulation will occur so you need to be careful! All handles are uniquely identified using Uid.- Parameters:
member
- the instance of type T that you want to be made transactional and persistent.- Returns:
- a handle into the transactional memory that the application should use to manipulate the object.
-
enlist
public T enlist(T member, Uid id)
Given an identified for an existing object, create another handle. This is particularly useful when using pessimistic concurrency control and we need one object instance per thread to ensure that state is safely managed.- Parameters:
member
- the instance of type T that you want to be made transactional and persistent.id
- the Uid of the object.- Returns:
- a handle into the transactional memory that the application should use to manipulate the object.
-
createHandle
protected T createHandle(T member, int ot)
Return a handle through which the object should be used, rather than the one passed in. Can specify the type of the object (recoverable, persistent, neither).
-
getHandle
public T getHandle(Uid reference)
Given a Uid, return the proxy for that instance.- Parameters:
reference
- the unique identifier for the handle.- Returns:
- the handle or null if not present.
-
getUidForOriginal
public Uid getUidForOriginal(T member)
Given a real object, return the Uid if it exists in this container.- Parameters:
member
- the real object.- Returns:
- the Uid for the object.
-
getUidForHandle
public Uid getUidForHandle(T proxy)
Given a real object, return the Uid if it exists in this container.- Parameters:
member
- the real object.- Returns:
- the Uid for the object if it exists in the container.
-
toString
public java.lang.String toString()
Gives the name of the container.- Overrides:
toString
in classjava.lang.Object
-
objectType
public final int objectType()
-
objectModel
public final int objectModel()
-
isPessimistic
public final boolean isPessimistic(java.lang.Object member)
-
checkObjectType
protected final void checkObjectType(java.lang.Object member)
-
-


Updates from 2018 - “Spectral Relativity”
PolymathicPerfraction: Spectral Relativity and the #ManyBodyProblem
Simulated particles systems have three challenges:
1) Continuity problems: requires the Hamiltonian & Conservation of Energy
- high magnitude force calculations (force splatting)
- infinitessimal-to-zero values resulting in discontinuities in the gradient calculation
- non-smooth values used for force calculation
- performance trade-offs
- infinitessimal-to-zero values resulting in discontinuities in the gradient calculation
2) Boundary Problems:
- the specific solution you choose impacts the conservation of energy for hamiltonian
- “fixing” this violation of the hamiltonian is the primary challenge with boundary problems
3) Distribution of mass/charge
- particle systems aren’t point-like
- addressing electrical configurations of ionic/covalent bonding is difficult
- this results in local relativistic effects for some elements (mercury)
4) Special Relativity
- Brute force approaches to relativity
- challenges with discrete computations of a continuous system,
- where relativistic effects occur over a large scale of distance
- challenges with discrete computations of a continuous system,
- Interesting to explore: do the relativistic effects found in mercury electrons impact interactions b/w some electrons in large, highly regular crystals?
general means of disaggregating/deconstructing behavior of physical systems:
1) Hamiltonian:
- particle position/momentum
- energy equilibrium
2) Subgroupings of components (of the hamiltonian)
3) Application of Spectral analysis to hamiltonian components
- FFT(dp/dt)
- FFT(dq/dt)
- FFT(d(.)) == d(FFT(.))
4) inference of the structure of interdepenency of variance from expected outcome
- hamiltonian components as distributions (with max/min, moments, variance)
- more useful with momentum
- spatial distribution of entropy and kinematics of entropy changes over time
5) Stochastic Calculus
- analyzing possible short-term trajectories of particles (and phase space
- short-term trajectories a la “instantaneous impact” from Lie Algebra
6) Kinematics
7) Special-relativistic inferences
- examine impact of relativistic parameters on deformation of phase space
- again, “instantaneous impact” from Lie Algebra
- when crossing relativistic inferences with the spectral decomposition of hamiltonian, more information should be produced
8) mechanics of continuity
- all of the above must be connected, yet all preserve energy equilibrium
then the system must have ideal paths in phase space (at least in classical mechanics)
- measures of phase space path deviation (in aggregate) must be connected
- for analyzed observations or simulated systems
- this has to be reconciled with the classical Hamiltonian…
- measures of phase space path deviation (in aggregate) must be connected
9) Concept of Linear Hull (& Hamel Basis?)
- (this is incorrect, i’m talking about something else)
- as applied to the Solution Space of Phase Space
- examine the phase space curves and connections between curves
for all configurations of the system
- how and why do these phase space curves follow along common paths,
while being “chaotic”?
- i.e. any point along a curve represents a potential starting configuration of the system for which the phase space curve will be a subset
- then, for all points in phase space, which points are connected as curves?
- are all these phase space curves disjoint?
- if they are disjoint, how do rational & algebraic numbers transform into values along the curves?
- the systems are differential & thus the rationality/algebraicity of values along paths in phase space feed in and out of each other (this definitely connects to Lie Algebra and E8)
- how and why do these phase space curves follow along common paths,
while being “chaotic”?
- and other number theory concepts as applied
- differential operator and linear hull…
- quotient spaces & number theory (does this lead to E8)
- examine the phase space curves and connections between curves
for all configurations of the system
In which, I convolute ideas with those I’ve recently acquired from #ExteriorAlgebra with:
-
Hamiltonian, conservation of energy and phase space
-
spectral components of position/momentum in #DoublePendulums
- conserve/reconstruct continuity
- gradient descent applied towards observed #Divergence from expected paths through phase space
-
Why spatial invariance of physical laws and composition of aggregate quantities like #Entropy necessitates interesting extrapolations
-
Detection of local/global #Convexity & #Concavity on combinatorial multivariate surfaces in high-dimensional cost functions and how this applies to efficient feature prioritization in #MachineLearning algorithms
-
DifferentialForms, as applied to the anticipation & detection of expected/actual dissonance
from true conservation of energy.
- The #FreeAlgebra, as applied to the differential operator, to create a direct summation of tensor products, where #Algebraicity, connected quotient spaces, and #Continuity are preserved. This constructs something similar to a #Manifold, mapping low dimensional spaces to higher dimensional surfaces of the differential operator or 1-forms, 2-forms, etc.
Other new ideas.
Content from 2016
Ars Technica recently posted an article on an exciting new development in dark matter and this piqued my interest on the subject. Another article I just saw on Gizmodo teases a Nobel-worthy revelation on gravity waves. I’ve had a lot of questions about dark matter and gravity that my current understanding of physics can’t answer. Again, yet another subject where my understanding of math limits me.
Nobel Worthy Gravity Waves
The Gizmodo article mentions a possible Nobel-worthy discovery of gravity waves. Apparently a binary blackhole merger has been discovered, which is one of the few events that would produce gravity waves detectable by current means.
TL;DR; Gravity is Wierd
As far as I can see, understanding gravity necessitates a shift in how we model space. I’ve used a few thought experiments to help simplify the important pieces. Here’s a few of the more profound questions escaping me at the moment. I wish I knew more of the math and physics to understand this more completely.
Update: I started looking further into some of the questions that I asked and found that these are indeed very relevant issues to be discussed. Frustratingly, I have again found that my intuition is particularly accurate here - frighteningly so, considering I dropped out of university physics.  For most of the questions that I’ve asked, the answers have not yet been conclusively determined.
I may update some of the questions in the future, to map my exploration to existing concepts. I used the word ‘frighteningly’ above for a reason. In particular, de Sitter Invariant Special Relativity represents an approach to answering many issues that confounded me in this article. Doubly Special Relativity was another interesting topic because some of the approaches used model spacetime with ‘momentum space’ instead of position space. I didn’t mention this in the article, but I got the feeling certain issues with relativity can only conclusively be resolved using momentum, yet I couldn’t really elaborate on why that was. Like I said, it was a feeling. Quantum Geometry is being developed to resolve how interactions are processed at lengths relevant to the Planck Length, though it’s implemented differently for each theory of Quantum Gravity.
My point is, someone with my education shouldn’t be able to understand much of this, beyond the typical summarization of high level information from A Brief History of Time. Yet, dipping into the math and specific theories, I’m able to pick some of this up without anyone guiding me along.
And I now understand why Quantum Gravity is so difficult. The approaches are so diverse, varied and intricate. The experimental evidence for Quantum Gravity isn’t there, nor will it be anytime soon, so all we have to go on is theory, hoping that we’ll get indirect clues from further experiments. The biggest missing element is the quantum structure of space. If we understand that, we’ll understand the mechanism of gravity. The biggest mathematical challenge is that, for analogy, whereas General Relativity is an Initial Value Problem (IVP), formulating Quantum Field Theory in curved spacetime is like a meta-IVP. It’s like an IVP wrapping another IVP, where the mathematic structures to use to resolve the problem are undeterminable. That’s my intuition speaking. Resolving the math is so challenging because the same spacetime curvature can ‘look’ different from each point.
Is there a distinction between gravity and the space it curves?
Or is gravity literally the ripple in space? That would imply space is simpler than it seems. That’s a bummer.
Does gravity cause the path of gravitation itself to curve?
This makes sense. If gravitons exist, they should follow similar rules as photons, right? It’d be weird if most bosons, like photons, followed the curvature of spacetime, but others didn’t at all. It’d make sense if each boson interacted in it’s own way with the curved nature of spacetime, yet still adhered to the same features of local space.
And it’d just be weird to have a set of bosons, that interacts via a completely different kind of space. Your model would have to account for multiple models of space: one relativistic and another, who knows. It’s a lot simpler if all the bosons are in the same space.
In other words, what I’m trying to ask is –
If gravitons follow curved spacetime, how does this affect other bosons?
And this is the question I got stuck on tonight: If a gravity wave is moving in the exact same direction as several parallel beams of photons, how are they affected? The photons that are moving just outside of parallel to the gravity wave would certainly be affected and the more their trajectory is altered, I can say confidently that the influence of gravity on them would only increase.
However, this would seem to break some kind of directional or spatial invariance of gravity, relativity or spacetime. Why is it that the photon whose trajectory exactly matches a gravity wave not be affected, while all adjacent photons with the same origin would be greatly affected? They would all assume and adhere to a change in distribution, causing a doppler effect. Except for this one beam of photons that wouldn’t be affected at all. This would be a violation of continuity in this function.
Here’s Some Gravitational Lensing
Notice how the objects seem to move away from the black hole as it first approaches. That is happening because rays that would otherwise not be directed towards you are following the curved spacetime. Here’s an image describing how light bends around massive objects.
Gravitational Lens Geometry
In the presence of one mass, light will follow a path that only curves in one direction. After passing the object, the light will gradually return to traveling in a straight line, but it only curves towards the gravitational source. It doesn’t curve back the other way as it returns to a straight path.
Thought experiment: traveling with a gravity wave
If you imagine a uniformly distributed narrow beam of protons, all traveling perfectly parallel to each other and traveling in sync with a gravity wave, you’ll get an idea of how the resulting distorted distribution of photons would look a bit odd. Imagine the photons beginning from various adjacent sources and they are all parallel, but that the gravity wave was emitted from a single source, so there are slightly varied angles of incidence to each photon. Some photons lie in the crest of the gravity wave and some in the trough.
For the most part, the photons that lie in the crest of the wave get their trajectory bent slightly inward. And those that lie on the trough of the trajectory get bent slightly outward (i think). So you can imagine that the resulting distrbution of photons, in this idealized scenario, would look parabolized. That is, except for the beam of photons that is exactly in line with the gravity wave, which may be technically impossible under real conditions. This beam, informed by my current understanding of general relativity and curved spacetime, could not be slowed down because it’s traveling at the speed of light and that is constant. It is taking a straight path through spacetime that has been curved, but such that the curved spacetime does not affect it’s apparent trajectory. And thus, this beam of light would not be distorted in any way by the gravity, but would stick out like a sore thumb in the parabolized distribution of photons.
It’s a violation of continuity because of a problem with invariance. Unless my understanding of this is incorrect, which is likely, then this center beam of photons must also be slowed down to some degree, but I can’t resolve how. And thus, the photons traveling in crest of the wave would slow down a bit, apparently. The photons traveling in the trough of the wave would speed up a bit, so that all the photons would be uniformly distorted.
However, this thought experiment has been set up with idealized conditions, similar to those for general relativity. In this problem, the originating mass for the gravity wave is point-like and can apparently alter its mass with no change in position, producing a perfectly circular gravity wave, which is impossible in nature. Also, in nature, it would be impossible to produce a stream of photons that are exactly in line with the origin of the gravity wave, unless you could ensure that it was lined up down to the plank length, but I’m not sure I really understand that.
If gravitons alter the spacetime that other bosons operate on …
Then how do you even resolve that dependency graph? One would need to take precedence over another … or something. In other words, if none of the bosons alter spacetime, then one can assume that spacetime is fairly consistent, except for the exception of matter that moves, but that’s really not that hard to resolve.
All the particles operate on the same space. If the space changes, all particles, for the most part, react accordingly and at the same time. There are some exceptions maybe with the propagation of gravity. Here you can’t really have quantum gravity.
However, if gravitons alter the spacetime that these other bosons are using, how does one deal with that dependency graph that arises? If you view bosons as units in streams of information that modify states of other particles, then what stream of information do gravitons make up? Do they comprise a stream to the surrounding space? How so? Would that mean space itself is composed of particles too? Would it stream information all those spatial particles simultaneously? That gets complicated. How do you deal with deformed space if the plank length is constant? Does that mean that space is voxelized?
How do scalar bosons, like the Higgs, differ from Gauge bosons?
I don’t really know enough to elaborate on this, but there should be some fundamental differences in how scalar bosons work.
If energy is mass, does gravitational energy interact with space or mass in transit?
If gravity travels at the speed of light and force is mass, and if all matter exhibits gravitational force on all other matter, then what happens to the gravitational energy between two massive objects moving away from each other, whose gravitational energy takes significant time to reach the other object?
Would space curve for the objects in between, because of the gravitational energy in transit? If this gravitation energy does cause space to curve while it’s in transit, does the source of the gravity affect how space curves? Or is the force expressed on space simply an aggregate of all the forces being transferred through that space?
Another Thought Experiment
Even with the limits of relativity, one can imagine situations where the gravitational force expressed on two objects could never reach the other side, AFAIK. E.G. if large two objects, both traveling toward each other at half the speed of light, relative to a nearby observer, then miss each other and continue to travel at nearly half the speed of light in opposite directions, it could take nearly an eternity for the force of gravity to exert influence on the other object.
How do we preserve conservation of energy with quantum gravity?
So, it’s clear that quantum gravity has some complex issues to resolve. Otherwise, there are loopholes under which the conservation of energy would be violated. This may be an indication that gravity operates via a non-local mechanism. Or, in other words, we need more dimensions to explain it mathematically. We can be fairly sure that the force that gravity exhibits travels at the speed of light over space, but does that mean all of the mechanisms of gravity operate over our 3-space?
What is the nature of these other dimensions?
So if gravity operates via mechanisms in other dimensions, how does the speed of light apply there? Is there some similar limit? What is the structure and nature of these dimensions and why do they not seem to affect existing observations? Have we not noticed them before because the other 3 forces do not interact with these dimensions? Is this a kind of compartmentalization that’s required to prevent quantum gravity from creating dependency issues? By this, I mean it may be mathematically simpler if gravity operates on a different space than the space it manipulates.
The universe is composed of streams of information
I found it interesting to think about photons, bosons, etc as streams of information. That is, we’re not looking at a star, but we’re looking at a stream of photons and imagining the star that’s producing them. And when we look at the night sky, were receiving long, unbroken streams of photons for each star in the sky. These streams aren’t just directly to us, but are more like a radial stream of photons from the star.
It’s useful to think of other quantum phenomena in the same way i think. Yet it’s really hard to imagine gravity as we know it in this way. If objects in motion require spacetime to determine their trajectory, what stream of information could provide the spacetime with the information needed to distort? We know that gravity is not the result of the interaction of two masses, but instead the interaction of two masses through curved spacetime.
Einstein Rings
When the observer is directly in line with a black hole and a large galaxy further behind it, you can see Einstein Rings. In this generated image, as it zooms further in, you can even see that light from the observer’s region of space is being redirected back towards the viewer in alternating rings. For more information, check out the wikipedia entry.
Is the speed of light truly constant for all conditions?
The main issue I have with all this is that gravity, which theoritically also travels at c, the speed of light, also effects the medium through which it flows. And as I’ve shown above, light is always slowed down by gravity. This is because the only value for which light will not curve is a value that is exactly in line with gravity’s influence and this is impossible. Therefore, light will always be affected in some way and slowed down by gravity. Technically, the light doesn’t slow down, but it’s flowing through more “space,” as it’s affected by gravity. And if light is “slowed down” by a gravity wave, then it would always be slowed down in some way by the net influence of gravity on space.
Is gravity really the sum of effects on curved spacetime?
Which begs the question: are two areas of space functionally equivalent if they have the same net distortion of space from any number of gravitational sources? That is, if you can ensure that two areas of space have the exact same net component for gravity, even though that gravity is caused by different sources, is the effect on masses in that area of space exactly the same.
I’m fairly confident that it’s not. If there is some structure to spacetime, than you could not produce two regions with identically composed spacetime without providing the exact input from masses. That is, just because you have created a net equivalent of gravitational forces doesn’t mean that your spacetime is functionally equivalent in all respects.
Example: you’ve got two planets. One is huge and the other is small. You’re in a spaceship in the middle. Measure the net force of gravity on your spaceship. Now, increase the mass of the planets, but move them further away, so that the net force of gravity is the same. Is the state of spacetime that your ship occupies identical to it’s previous state? No, for a dozen reasons. And I think getting this to work to control the state of spacetime would be pretty difficult.
Does gravity lose energy to dispersion?
If gravity is also similarly “slowed down” in the same way that light would be, does that mean that a gravity wave loses energy as it propagates through space?
If the apparent speed of light varies from place to place…
– and I’m pretty sure this section is shit, but I left it in anyways –
How does this affect how we make observations. Then the speed of light itself becomes a kind of initial value problem, where you can’t pin it down because it’s impossible to measure the net forces distorting local spacetime.
But then, what is c, really? If the measurement of this constant can’t be understood as accurate because it would require measuring the net distortion of local spacetime, then how does this affect the other laws of physics?
Like I said, I almost threw this out, but it’s interesting to think about the dependencies between various laws of physics. Which are dependent on c? Would the be dependent on local or universal c? And how does this affect the conclusions we’ve reached using statistic modeling of the cosmos? And it’s an interesting thought experiment to examine the dependencies of theories in physics.
Does spacetime have memory?
If spacetime is distorted by mass, and particularly, if spacetime is composed of some quantum structure, is this structure permanently changed by the presence of mass? Is local space directly connected to the mass that occupies it?
How to extend the notion of singularity to two or three points?
So if a singularity for a black hole is a point so massive it creates an event horizon from which light cannot escape, are there extensions for systems with two or three such points?  Would there be a singularity that “streched” across space, forming a line? This seems impossible, but what would the space between these singularities be like?
And if there was a trinary black hole system that was collapsing, it seems like an extremely interesting situation could emerge, where a “triangular” region of space is formed, surrounded by event horizons linking each singularity. Learning more about what happens here might tell us more about the nature of space when a singularity forms, since prior to that the massive object has volume and will be decomposed into a singularity in a chain reaction.
Dark Matter’s Incoherent Doppler Shift
The Ars Technica article discusses unexpected low-energy gamma rays, whose sources can’t be determined. It is suspected that extremely rare interactions with dark matter are triggering these gamma ray bursts.
The article mentions an interesting inverse correlation in the doppler shift in dark matter suspected gamma ray bursts (GRB) in relation to the observed doppler shift from other sources of matter. Perhaps not an inverse correlation per se, but a lack of coherence with the doppler shift normally exhibited by normal matter we observe. Most matter in our galaxy is spiraling inwards towards the center and moving, on average, at specific speeds in relation to us. Because of the difference in speed, we observe the doppler shift and because the motion of all matter in our galaxy is more or less synchronously spiraling inwards, we observe a predictable, smooth doppler pattern for normal matter.
Yet, dark matter doesn’t interact with matter, except through gravity. The only reason we suspect it exists is because our observations don’t match our cosmological models. They mostly match; that is, on a micro scale, our models for gravity seem to work. But on the cosmic scale, there seems to be an enormous amount of missing mass out there than we can’t account for. Personally, I’m not so convinced this exists at all, instead feeling that there’s something subtly wrong with our models.
This research looked into the doppler shift of the GRB’s, which is around 3.5 KeV, whereas normal light signal is between 1.5eV and 3.5eV. Because of the speed difference between the sun and dark matter, measuring the doppler shift requires sensing very low energy differences. But new satellites will be launched with gear that should be capable of doing this.
This research is significant because we may have observed direct evidence of dark matter that lines up with our expectations. Hopefully, the frequency of the GRB’s we see are spatially coherent with the distortion that our models predict for dark matter’s effect on mass in each area of our galaxy.
Basically, dark matter’s average motion is distinct from the average motion of the galaxy and this is what allows us to distinguish the doppler shift data. GRB’s shift towards blue when we would expect normal matter to shift red, which means it’s moving away from the majority of matter (that we’re moving.
My Thoughts on Dark Matter
My own uneducated thoughts: I get the feeling that there’s something subtly off with our model of the universe. We see that there’s some general variance that’s spatially distributed with the observations that accompany our data. That is, our observations work in smaller systems, but on a larger scale, there’s this huge disparity in the motion we see in galaxies and clusters. We suspect that dark matter causes galaxies to cluster and even to form in the first place, but simply because we can’t explain it otherwise.
But the stars in nearby galaxies? They seem to cohere to our model’s predictions, at their interactions with local stars do. IMO, there’s something missing from our model of gravity or our understanding of the structure of space.


{% extends parent_template|default:"core/base.html" %} {% load staticfiles %} {% block body %}
Diversify Portfolio allows investors to analyze their stock portfolios and look for opportunities using several interactive tools.
A few key features include:
Data to Site turns spreadsheet data into great looking cards on your website.
A few key features include:
This is a Kanban board implemented as a SPA using React and Redux on the front end with Django Rest Framework on the back end.
A few key features include:
Who Knows is a question and answer site similar to Stack Overflow or Quora.
It includes all the core functionality you would expect from a Q&A site such as:


ÁVision Build Log
Tool Versions:
IDE-Version: ÁVision V5.16a Copyright (C) 2015 ARM Ltd and ARM Germany GmbH. All rights reserved. License Information: D C, C, LIC=---- Tool Versions: Toolchain: MDK-Lite Version: 5.16a Toolchain Path: C:\Keil_v5\ARM\ARMCC\Bin C Compiler: Armcc.exe V5.06 (build 20) Assembler: Armasm.exe V5.06 (build 20) Linker/Locator: ArmLink.exe V5.06 (build 20) Library Manager: ArmAr.exe V5.06 (build 20) Hex Converter: FromElf.exe V5.06 (build 20) CPU DLL: SARMCM3.DLL V5.16a Dialog DLL: DCM.DLL V<IP_ADDRESS> Target DLL: STLink\ST-LINKIII-KEIL_SWO.dll V<IP_ADDRESS> Dialog DLL: TCM.DLL V<IP_ADDRESS>Project:
D:\MyWORK\STM32_DENKOV\CUBE\STM32Cube_FW_F7_V1.3.0\Projects\STM32746G-Discovery\Applications\LibJPEG\LibJPEG_Decoding\MDK-ARM\Project.uvprojx Project File Date: 04/18/2016Output:
*** Using Compiler 'V5.06 (build 20)', folder: 'C:\Keil_v5\ARM\ARMCC\Bin' Rebuild target 'STM32746G-DISCOVERY' compiling stm32f7xx_hal_dma_ex.c... compiling stm32f7xx_hal_cortex.c... compiling stm32f7xx_hal_gpio.c... compiling stm32f7xx_hal_flash.c... compiling stm32f7xx_ll_fmc.c... compiling stm32f7xx_hal_dma2d.c... compiling stm32f7xx_hal_rcc.c... compiling stm32f7xx_hal_dma.c... compiling stm32f7xx_hal.c... compiling stm32f7xx_hal_pwr_ex.c... compiling stm32f7xx_hal_sdram.c... compiling stm32f7xx_ll_sdmmc.c... compiling stm32f7xx_hal_uart.c... compiling stm32f7xx_hal_rcc_ex.c... compiling stm32f7xx_hal_sai.c... compiling stm32f7xx_hal_i2c_ex.c... compiling stm32f7xx_hal_pwr.c... compiling stm32f7xx_hal_flash_ex.c... compiling stm32f7xx_hal_ltdc.c... compiling stm32f7xx_hal_sd.c... compiling stm32f7xx_hal_i2c.c... compiling stm32f7xx_hal_sai_ex.c... compiling sd_diskio.c... compiling decode.c... ..\Inc\MPEG.h(148): warning: #1-D: last line of file ends without a newline #endif /* __MPEG_H */ ..\Src\decode.c: 1 warning, 0 errors compiling stm32f7xx_it.c... ..\Inc\MPEG.h(148): warning: #1-D: last line of file ends without a newline #endif /* __MPEG_H */ ..\Src\stm32f7xx_it.c: 1 warning, 0 errors compiling main.c... ..\Inc\MPEG.h(148): warning: #1-D: last line of file ends without a newline #endif /* __MPEG_H */ ..\Src\my_waveplayer.c(182): warning: #1-D: last line of file ends without a newline ..\Src\my_waveplayer.c: 2 warnings, 0 errors assembling startup_stm32f746xx.s... compiling MPEG.c... ..\Inc\MPEG.h(148): warning: #1-D: last line of file ends without a newline #endif /* __MPEG_H */ ..\Src\MPEG.c(462): warning: #68-D: integer conversion resulted in a change of sign return -99; ..\Src\MPEG.c(803): warning: #111-D: statement is unreachable if(dac_intr.sound_reads >= (prevSamplesSound * soundSampleBlocks)) ..\Src\MPEG.c(549): warning: #546-D: transfer of control bypasses initialization of: variable "soundSampleByte" (declared at line 573) variable "soundSampleBlocks" (declared at line 574) variable "timeScaleCoeff" (declared at line 576) variable "outflag" (declared at line 721) variable "count" (declared at line 721) variable "pause" (declared at line 721) goto EXIT_PROCESS; ^ ..\Src\MPEG.c(423): warning: #550-D: variable "fps" was set but never used uint32_t fps, frames, prevFrames, sample_time_limit; ..\Src\MPEG.c(423): warning: #550-D: variable "prevFrames" was set but never used uint32_t fps, frames, prevFrames, sample_time_limit; ..\Src\MPEG.c(423): warning: #177-D: variable "sample_time_limit" was declared but never referenced uint32_t fps, frames, prevFrames, sample_time_limit; ..\Src\MPEG.c(424): warning: #550-D: variable "numEntry" was set but never used uint32_t samples, frameDuration, numEntry; ..\Src\MPEG.c(431): warning: #177-D: variable "fpsCnt" was declared but never referenced uint8_t fpsCnt = 0; ..\Src\MPEG.c(432): warning: #177-D: variable "fps1Hz" was declared but never referenced const char fps1Hz[] = "|/-\\"; ..\Src\MPEG.c(442): warning: #550-D: variable "soundEndFlag" was set but never used int soundEndFlag = 0; ..\Src\MPEG.c(664): warning: #550-D: variable "limitter" was set but never used float limitter; ..\Src\MPEG.c(721): warning: #550-D: variable "outflag" was set but never used int outflag = 0, count = 0, pause = 0; ..\Src\MPEG.c(721): warning: #550-D: variable "count" was set but never used int outflag = 0, count = 0, pause = 0; ..\Src\MPEG.c(721): warning: #177-D: variable "pause" was declared but never referenced int outflag = 0, count = 0, pause = 0; ..\Src\MPEG.c(883): warning: #177-D: label "EXIT_LOOP" was declared but never referenced EXIT_LOOP: ..\Src\MPEG.c: 16 warnings, 0 errors compiling stm32746g_discovery_sdram.c... compiling system_stm32f7xx.c... compiling ff_gen_drv.c... compiling diskio.c... compiling stm32746g_discovery.c... compiling stm32746g_discovery_sd.c... compiling wm8994.c... compiling ff.c... compiling jdinput.c... compiling jccolor.c... compiling jutils.c... compiling stm32746g_discovery_audio.c... compiling jctrans.c... compiling jidctint.c... compiling stm32746g_discovery_lcd.c... compiling jdtrans.c... compiling jccoefct.c... compiling jcdctmgr.c... compiling jddctmgr.c... compiling jdsample.c... compiling jquant2.c... compiling jdcolor.c... compiling jdmaster.c... compiling jaricom.c... compiling jdcoefct.c... compiling jcmarker.c... compiling jidctfst.c... compiling jcapistd.c... compiling jcsample.c... compiling jdapimin.c... compiling jfdctfst.c... compiling jcmaster.c... compiling jfdctflt.c... compiling jmemmgr.c... compiling jcmainct.c... compiling jdarith.c... compiling jdmainct.c... compiling jerror.c... compiling jcparam.c... compiling jcinit.c... compiling jdatasrc.c... compiling jdmarker.c... compiling jchuff.c... compiling jdapistd.c... compiling jdmerge.c... compiling jidctflt.c... compiling jcapimin.c... compiling jcprepct.c... compiling jquant1.c... compiling jdhuff.c... compiling jdpostct.c... compiling jdatadst.c... compiling jcomapi.c... compiling jfdctint.c... compiling jmemnobs.c... compiling jcarith.c... linking... STM32746G-DISCOVERY\STM32746G-DISCOVERY.axf: error: L6050U: The code size of this image (66870 bytes) exceeds the maximum allowed for this version of the linker. Finished: 0 information, 0 warning, 0 error and 1 fatal error messages. "STM32746G-DISCOVERY\STM32746G-DISCOVERY.axf" - 1 Error(s), 23 Warning(s).Software Packages used:
Package Vendor: ARM http://www.keil.com/pack/ARM.CMSIS.4.3.0.pack ARM::CMSIS:CORE:4.1.0 CMSIS (Cortex Microcontroller Software Interface Standard) * Component: CORE Version: 4.1.0Collection of Component include folders:
D:\MyWORK\STM32_DENKOV\CUBE\STM32Cube_FW_F7_V1.3.0\Projects\STM32746G-Discovery\Applications\LibJPEG\LibJPEG_Decoding\MDK-ARM\RTE C:\Keil_v5\ARM\PACK\ARM\CMSIS\4.3.0\CMSIS\Include C:\Keil_v5\ARM\PACK\Keil\STM32F7xx_DFP\2.5.0-dev5\Drivers\CMSIS\Device\ST\STM32F7xx\IncludeCollection of Component Files used:
* Component: ARM::CMSIS:CORE:4.1.0 Target not created. Build Time Elapsed: 00:00:44


At Krystal Crunch, we specialize in making the best of the best pizzas.
We believe in quality as well as quantity. With our skilled chefs and craftsmen, we mould dough
into a fine masterpiece. You will definitely like it here!!
We are looking forward to your next visit. Feel free to reccomend us to your friends.


You can find the latest release on GitHub.
Make sure you have jQuery loaded, or load it from a public CDN:
<script src="https://ajax.googleapis.com/ajax/libs/jquery/2.1.4/jquery.min.js"></script>
Grab the following files from the repo and put them in your page <head>:
<script src="poker.js"></script>
<link href="poker.css" rel="stylesheet" type="text/css" />
Poker.poke(message, options = {});
Poker.poke('This is a test of a default poke');
Poker.poke('This is a test of a quick poke', { timeout: 1000 });
These are all the options you can override in the options parameter:
{
close_button: true,
container: {
css: {
maxWidth: '400px',
padding: '0 12px',
position: 'fixed',
zIndex: '9999'
}
},
timeout: 5000,
x: 'right',
y: 'top'
}


{% extends "layout/crm_layout.html" %} {% block content %}
| Name | Phone | Location | Director Details | Category | Sector | Nature of Business | Date of Issues | Actions |
|---|---|---|---|---|---|---|---|---|
| {{ client.company_name }} | {{ client.company_phone }} | {{ client.physical_location }} | {{ client.director_info }} | {{ client.category }} | {{ client.sector }} | {{ client.nature_of_business }} | {{ client.date_of_issue }} | zoom_in edit delete |


--- title: Israel shot 090 date: 2004-03-31T00:00:00.000Z filepathOriginal: photos/IMG0051.jpg filepathThumbnail: photos/IMG0051.thumbnail.jpg filepathPreview: photos/IMG0051.preview.jpg ---
Raf, Asher, Gabes, Michal, Shtern, Ofer, and of course Toto, about to start a day's hike through the desert


---
title: "BOTANY FOR GARDENERS"
date: "2000-01-01 20:02:06 -06:00"
categories:
- adult
subtitle: ""
layout: "events"
event-image: "botany-for-gardeners.jpg"
event-dates: "THURSDAYS, FEB 6-20"
event-location: "Red Butte Garden Classroom"
button-type: "register"
tickets-link: "https://continue.utah.edu/lifelong/class/llhg_488_botany_for_gardeners"
registration-info: "Contact Info:<PHONE_NUMBER>
Lifelong Learning: LLHG 488"
instructor-info: "Michelle Cook"
member-cost: "$74"
public-cost: "$80"
event-notes: ""
tickets-button: ""
published: false
---
TUESDAYS, FEBRUARY 6 - 20, 6:30 - 8:30PM
REGISTRATION REQUIRED
Don't go dormant this winter! Join us as we learn basic plant morphology and terminology--knowledge that will help you better understand plant growth and take some of the guesswork out of gardening. In this hands-on class, you'll learn why some shrubs are pruned immediately after flowering while others are pruned in late winter/early spring; how to tell a pine from a spruce and why it matters; the reasons behind the differing watering practices for turf and trees, and other common gardening questions. Co-sponsored with Lifelong Learning. Members py $69 +sp fee; register for section 002.


A dynamic Bubble chart interated with a range input
Year (2008-2022)
This goes in the documents header:

Put this where you want the chart to show up:

<canvas id="cvs" width="900" height="350">[No canvas support]</canvas>

<input type="range" min="2008" max="2022" value="2022" id="myRange" style="width: 900px" />

Year (2008-2022)

This is the code that generates the chart - it should be placed AFTER the canvas tag(s):


Match Play. Red leads 5-0 to 13. How should Red play 53?
pips Red=163 White=134
(CorrectAnswer= 0/0, ErrorScore= 0)
Irrespective of his match lead Red must still follow basic backgammon principles.
With White having a single rear checker Red should follow the standard game plan of attacking it with 5/2*. After that the five should be used to bring another checker into the attack zone. Red should unstack his 16-pt by playing 16/11.
Any non-hitting play is a blunder. Even 10/2* is a blunder because it insufficiently develops Red’s position. The over the board play of 16/13, 10/5 was a really weak effort.
With White having a single rear checker Red should follow the standard game plan of attacking it with 5/2*. After that the five should be used to bring another checker into the attack zone. Red should unstack his 16-pt by playing 16/11.
Any non-hitting play is a blunder. Even 10/2* is a blunder because it insufficiently develops Red’s position. The over the board play of 16/13, 10/5 was a really weak effort.
1. Cubeful 2-ply 16/11 5/2* Eq.: -0.089 0.459 0.118 0.003 - 0.541 0.159 0.007 2. Cubeful 2-ply 10/2* Eq.: -0.154 (-0.065) 0.429 0.107 0.003 - 0.571 0.154 0.006 3. Cubeful 2-ply 13/8 5/2* Eq.: -0.159 (-0.070) 0.445 0.113 0.003 - 0.555 0.190 0.009 4. Cubeful 2-ply 16/13 10/5 Eq.: -0.173 (-0.085) 0.406 0.094 0.003 - 0.594 0.120 0.004 5. Cubeful 2-ply 16/11 10/7 Eq.: -0.175 (-0.086) 0.421 0.097 0.003 - 0.579 0.150 0.005