Building the Front End
Scaffolding the user interface now that we have a functional smart contract.
Scaffolding the user interface now that we have a functional smart contract.
Essentially the heart of the NFT marketplace.
Time to start building.
The crucial process of getting the necessary tools in place and up-to-date before building.
As things stand, the first edition of this guide has been one of my most viewed Medium articles thus far.
Then it’s all official.


Redmi K30 live images leak, 120 Hz screen and 30W charger confirmed
by YordanXiaomi confirmed multiple times that we will see the Redmi K30 lineup in December, and the phone already started popping up on Chinese websites. A device with the model number M2001G7AE, said to be the regular Redmi K30, was certified by CCC with a 30W charger in the box.
It is also listed as "5G Digital Mobile Phone", confirming the support for next-gen cellular networks.
In the same time, live images of the phone, still wrapped in one of those pre-production cases, revealed spicy details about the specs. Apparently, the Redmi K30 will have Adreno 618 GPU, meaning it will come with the Snapdragon 730 chipset by Qualcomm. It will also have a 120Hz screen, one-upping OnePlus (among other manufacturers) and its 90Hz panels.
The device is spotted with a dual selfie camera in an oval punch-hole design, but the Redmi K30 and Redmi K30 Pro are likely to keep the trend from K20 and have an identical body, with just the insides being different. It should also have MIUI 11, but the screenshots do not reveal whether it will be based on Android 10.


{% extends "base.html" %} {% set active_page = "settings" %} {% block content %}
It looks like PostGIS Baselayers is not initialized in this database yet. A new schema called postgis_baselayers will be created where information about installed datasets is stored. After initializing the application you'll be able to load new datasets.
postgis_baselayers


package main
import (
"bufio"
"fmt"
"os"
"strconv"
"strings"
)
func main() {
reader := bufio.NewReader(os.Stdin)
fmt.Println("Enter the value of 'n' upto which you want the sum positive series:")
valueofn, _ := reader.ReadString('\n')
valueofn = strings.TrimSpace(valueofn)
intvalueofN, _ := strconv.Atoi(valueofn)
sum := 0
for count := 1; count <= intvalueofN; count++ {
sum = sum + count
}
fmt.Println("Sum of,intvalueofN,Positive series:", sum)
}
//Output:
Enter the value of 'n' upto which you want the sum of positive series:
10
Sum of 10 Positive series: 55
In this program, we calculate the sum of first natural number
"or" Positive series 1+2+3+.....n known as natural number
using (for loop). We take the value of 'n'from user as an input
upto which user want the sum positive series.
As an output we calculate the sum of positive series.
Accordingly to the user input value.


THE MAN WITHOUT A FACE (1993) A Film Review Copyright Dragan Antulov 1999
One of the riskiest and hardest moves in any actor's career is transition from the image of popular entertainer to the image of true artist. Mel Gibson saw that in early 1990s, when he tried to reach beyond his status of action superstar, shown in MAD MAX and LETHAL WEAPON movies. His first attempt, role in Zeffirelli's HAMLET, ended disastrously. Luckily, there was a second chance for him, and in 1993 he took that chance with THE MAN WITHOUT A FACE, coming-of-age drama based on the novel by Isabelle Holland. That film was also his directorial debut that laid the path that would lead to his BRAVEHEART triumph two years later.
Like his colleague Jodie Foster in LITTLE MAN TATE, Gibson decided to direct a movie with a young boy as protagonist. The plot takes place in small town in Maine 1968. Chuck Norstadt (played by Nick Stahl) is a 12-year old boy who lives together with his mother (played by Margaret Whitton) and two half-sisters. Being misunderstood and ignored by his family, he seeks rebellion in the idolatry of his late father, military pilot. His great ambition in life is to go to the military boarding school. That move, at the peak of anti-war movement, isn't just unpopular - it is very unlikely, because Chuck needs tutoring. Help comes in a form of Justin McLeod (played by Mel Gibson), former teacher with a terribly scarred face, who lives a hermit. McLeod begins teaching Norstadt and two of them become friends. Unfortunately, that only enflames the hostility of the town, and vicious rumours about teacher's dark past emerge, threatening the relationship between Chuck and McLeod.
At first glance, THE MAN WITHOUT A FACE looks surprisingly good for someone's directorial debut. But, those who are likely to nitpick Gibson's work would find that the directing seems somewhat too baroque for a simple drama that would be most suitable for TV films. The most attractive element in this film is acting. Gibson plays very good and thankful role of a misanthropic hermit who gradually regains love for humanity. That role was very carefully played, in order not to overshadow anyone else, including Nick Stahl, who was good in his part. The result is a well-acted, competently directed coming-of-age drama that doesn't drowns itself in cliches and cheap sentimentality.
Unfortunately, the screenplay by Malcolm McRury had touched the issues of homosexuality and paedophilia, and that was enough for this film to be criticised not for its own flaws, but for the shortcomings of its director. Before making this film, Gibson was branded as homophobic, because of an interview he had given. In the peak of Political Correctness, it was simply inconceivable arrogance for a notorious homophobe to direct a movie dealing with such issues. But the real reason why some left-leaning critics attacked the film wasn't in Gibson's treatment of homosexuality (which wasn't mentioned or implied on until the very last scenes in the film). It was the fact that Gibson gave a story about anti-establishment rebellion from a rather conservative point of view. The film is set in 1968, but the thing that bothers Chuck is not the old establishment; Chuck is disgusted with the new social freedoms that are enjoyed at the expense of newer generations (with Chuck's own family being the victim of endless divorces), and the character of Carl (played by Richard Masur), Chuck's potential stepfather, could be seen as the caricature of Baby Boomers and all their ideals. The subtlety with which the conservative ideas were introduced in this Hollywood film didn't hurt the film, but the very fact such ideas found their place on screen in that ultra-liberal era was enough to make this film better than its reputation.
RATING: 6/10 (++)
Review written on September 15th 1999
Dragan Antulov a.k.a. Drax Fido: 2:381/100 E-mail<EMAIL_ADDRESS>E-mail<EMAIL_ADDRESS>E-mail<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
to ASCII to HTML conversion.
Related links: index of all rec.arts.movies.reviews reviews


Need a gift for a gamer? We found 35 curved monitors that are on sale.
by Haley HenschelTL;DR: Curved monitors from Samsung, LG, Dell, Sceptre, and Acer are on sale at various retailers ahead of Black Friday.
You can look at retailers' pre-Black Friday sales in one of two ways: as marketing gimmicks designed to prolong the already-too-long Christmas shopping season, or as opportunities for you to get a head start on your holiday gift list while saving a bit of money.
Truth be told, there's probably a little bit of both at play here. But hey, you know what they say: If you can't beat commercialization, you might as well make it work to your wallet's advantage. (They say that, right?)
If you haven't yet begun your holiday shopping, don't panic: Lots of deals are only just going live.
Check 'em out below:
Samsung
- Samsung 24-inch Curved LED Gaming Monitor (LC24F390FHNXZA) — $149.99 (save $30)
- Samsung 27-inch C27F398 Curved LED Monitor (LC27F398FWNXZA) — $179.99 (save $40)
- Samsung 27-inch C27HG70 HDR QLED 144Hz 1ms Curved Gaming Monitor with FreeSync (C27HG70QQN) — $427.98 (save $172.01)
- Samsung 27-inch CRG5 240Hz Curved Gaming Monitor (LC27RG50FQNXZA) — $369.99 (save $30)
- Samsung 27-inch JG56 WQHD Curved Gaming Monitor (LC27JG56QQNXZA) — $279.99 (save $20)
- Samsung 32-inch C32HG70 HDR QLED 144Hz 1ms Curved Gaming Monitor with Freesync (LC32HG70QQN) — $499.99 (save $100)
- Samsung 32-inch JG56 WQHD Curved Gaming Monitor (LC32JG56QQNXZA) — $339.99 (save $40)
- Samsung 32-inch Curved FHD LCD Monitor (LC32F39MFUNXZA) — $179.99 (save $170.99)
- Samsung 32-inch Curved LED Monitor (LC32F391FWNXZA) — $226.99 (save $93)
- Samsung 34-inch CJ791 Ultrawide Curved Gaming Monitor (LC34J791WTNXZA) — $764.98 (save $135.01)
- Samsung 43-inch CJ89 Curved UltraWide 3840 X 1200 Resolution 120Hz Monitor (LC43J890DKNXZA) — $829.99 (save $70)
- Samsung 49-inch CHG90 144Hz Curved Gaming Monitor (LC49HG90DMNXZA) — $896.99 (save $203)
LG
- LG 34-inch 34GK950F-B 21:9 UltraGear WQHD Nano IPS Curved Gaming Monitor with Radeon FreeSync 2 — $827 (save $372.99)
- LG 34-inch 34WL85C-B UltraWide Curved WQHD IPS Monitor with HDR 10 — $599.99 (save $200)
- LG 34-inch 34GK950G-W 21:9 UltraGear QHD Curved Nano IPS Gaming Monitor with NVIDIA G-SYNC — $750.90 (save $649.09)
- LG 34-inch 34UC79G-B 21:9 UltraGear Full HD IPS Curved Gaming Monitor — $499.99 (save $100)
- LG 34-inch 34GL750-B 21:9 UltraGear Curved WFHD IPS 144Hz G-SYNC Compatible Gaming Monitor — $481.16 (save $68.83)
- LG 34-inch 21:9 34UC98-W Curved UltraWide QHD IPS Monitor with Thunderbolt — $599.99 (save $300)
- LG 38-inch 38UC99-W 21:9 Curved UltraWide QHD+ IPS Monitor with Bluetooth Speakers — $846.65 (save $42.35)
- LG 49-inch 49WL95C-W Curved 32: 9 Ultrawide DQHD IPS Monitor with HDR10 and USB Type-C — $1,276.99 (save $223)
Dell
- Dell 32-inch Curved Gaming Monitor (S3220DGF) — $419.99 (save $180)
- Dell 34-inch UltraSharp Curved LED-Lit Monitor (U3415W) — $579.99 (save $220)
- Dell 34-inch Ultrasharp WQHD Curved IPS USB-C Monitor (U3419W) — $745.99 (save $104)
- Dell 34-inch Alienware Curved Gaming Monitor (AW3418DW) — $749.99 (save $600)
- Dell 34-inch Alienware Curved Gaming Monitor (AW3420DW) — $999.99 (save $500)
- Dell 38-inch UltraSharp Curved Monitor (U3818DW) — $1,119.99 (save $280)
- Dell 49-inch UltraSharp Curved Monitor (U4919DW) — $1,349.99 (save $350)
Sceptre
- Sceptre 27-inch Curved 75Hz LED Monitor (C275W-1920RN) — $144.99 (save $14.98)
- Sceptre 27-inch Curved 144Hz Gaming LED Monitor (C275B-144RN) — $167.99 (save $20)
- Sceptre 30-inch 21:9 Curved Gaming Monitor (C305W-2560UN) — $199.97 (save $50)
- Sceptre 30-inch 21:9 Ultra Wide Curved Gaming Monitor (C305B-200UN) — $279.99 (save $20)
Acer
- Acer 23.6-inch ED242QR Curved Gaming Monitor — $149.99 (save $50)
- Acer 27-inch ED273 Curved Gaming Monitor — $199.99 (save $80)
- Acer 31.5-inch ED323QUR Abidpx WQHD Curved Gaming Monitor — $359.99 (save $40)
- Acer 31.5-inch ET322QR wmiix Curved Full HD VA Monitor — $179.99 (save $70)


Bulk carrier seized off Malaysia, 23 Russian and Ukrainian crew detained – media
All 23 crewmembers were detained after they failed to produce any proof of permission from the port authority to anchor.
A bulk carrier was seized and its 23 Russian and Ukrainian crew were detained off Johor's east coast by the Malaysian Maritime Enforcement Agency (MMEA).
Tanjung Sedili Zone MMEA director Mohd Zulfadli Nayan said in a press statement that the ship was seized some 3.5 nautical miles east of Tanjung Penyusop on Thursday (Nov 21), according to The Star.
"All 23 crewmembers were detained after they failed to produce any proof of permission from the port authority to anchor. The crew are Russians and Ukrainians between the age of 21 to 68," he said.
Mohd Zulfadli added that two of its crew were brought to the Tanjung Sedili Zone MMEA offices for further action.
The case is being investigated under Section 491B(1)(I) of the Merchant Shipping Ordinance 1952 for anchoring without permission.
Those found guilty face a fine of not more than RM100,000, maximum two-year jail sentence or both upon conviction.


Are you missing a concert?
Select, add and share your memories 📸
You've attended all concerts in our list!
ID
Name
Location
Date
Venue
Festival
Attended


Package, dependency and environment management for any language: Python, R, Ruby, Lua, Scala, Java, Javascript, C/ C++, FORTRAN
Briefly specking, it's a combination of dependency/package management (pip) and environment management (virtualenv).
In my own point, it's simple but powerful just like python.
Anaconda is a tool set which contains :
So I think everyone starts to taste python should taste it first.
I suppose you use Ubuntu, it's also ok if you use other Linux publications.
After you install it, you got nothing special except an directory named anaconda3 in your home directory. I am not sure whether
it has already set the path for you, this command may help if it has not (change .zshrc
into .bashrc
if you use bash rather zsh):
echo 'export PATH="/you-home-directory-path/anaconda3/bin:$PATH"' >> ~/.zshrc
source ~/.zshrc
Then you can type echo $PATH
, you should get something like the following :
"/you-home-directory-path/anaconda3/bin:/usr/local/sbin:/usr/local/bin:..."
After that, you can use conda -V
to check you conda version and also verify you really have conda installed.
Since the order the path is printed is also the order the system search the command, so if you type python
then it will use the python in the anaconda3 rather than
the python you have previous installed. So do not need to worry if you already have python installed in your system.
If you have ever used any package manager like apt-get in Ubuntu, homebrew in Mac, you will feel at home while using conda.
conda create --name/-n environment-name [dependency list]
: create a new develop environment.
conda create --name/-n environment-name --clone source-environment-name
: make a copy of the source environmentsource activate environment-name
: change to specific environment
source deactivate
: exit from that specific environment.conda search package-name
: search if specific package is available for conda to install.conda install/remove [--name/-n] package-name
: install/uninstall specific package in specific environment, or current environment if environment is not specific.
conda remove --name/-n environment-name -all
: delete everything for a specific environment
conda list
: list all the packages you have installedconda info -e
: check all the environment you have.
conda update package-name
: update specific package
And you can also use pip in install packages when sometimes conda install could not manage it. The package is also isolated only inside current environment.
Since anaconda is nothing except the directory named anaconda3 and a line of code in the .zshrc
. Just remove those then it's uninstalled.


---
layout: casestudy
class: tictail
permalink: /work/tictail/
title: Tictail Case Study - 14islands
name: Tictail
headline: A better way for creatives to sell online.
description: A better way for creatives to sell online.
color: '#fcc100'
hoverColor: '#e3ae00'
logo: logo_tictail.min.svg
image: /images/work/tictail/tictail-illustration.jpg
priority: 4
private: false
og_image: /images/work/tictail/home-screenshot-16-9.jpg
---
{% include casestudy-header.html about="Tictail is a Stockholm and New York based startup that enables creative people to easily sell online. They wanted a modern website to attract more users and showcase what the product is all about." %}
{% include casestudy-video.html vimeoId="119937589" ratio="16_9" class="pjax-animate" %}
{% markdown %}
## Crafting it
The site experience is fully responsive for all devices and features nice interactions to make it pleasant to explore. The focus is on the content - making it easy for people to signup to Tictail.
We also put a lot of effort into performance to keep it as fast as possible. The site was built in Wordpress so all content is fully editable by the people at Tictail.
{% endmarkdown %}
{% include casestudy-responsive.html url="/images/work/tictail/tictail-iphone6-full-page-shortened.jpg" parallax=true parallaxOffset="-0.5" parallaxDirection="vertical" %}
{% markdown %}
## Design
The site was designed by our friends at [Studio Källbom](http://www.studiokallbom.se/){:target="_blank"}, a talented design studio with an artistic touch.
{% endmarkdown %}
{% include wide-content-image.html src="/images/work/tictail/home-screenshot-16-9.jpg" alt="Home page" margin="both" ratio="16_9" %}
{% markdown %}
The site features a magazine-like design; nice typography, bold colors and rich content to show features and tell Tictails story. We were totally inspired to make this our best work to date.
{% endmarkdown %}
{% markdown %}
## Making it happen
We worked in close collaboration with Tictail, often at their offices. Being able to test out ideas and get quick feedback made the process more enjoyable for all and it was a key element for its end result.
{% endmarkdown %}
{% include wide-content-image.html src="/images/work/tictail/friday-meeting-16-9.jpg" alt="The 14islands HQ" margin="both" ratio="16_9" %}
{% markdown %}
Picture from a Friday catch-up meeting where our very own Marco also gave an update about the site progress to the awesome people at Tictail.
{% endmarkdown %}
{% markdown %}
## Technologies
By using Responsive Web Design best practices we brought the best experience for modern mobile, tablet and desktop devices.
The site was built in WordPress using the following technologies.
{% endmarkdown %}
{% include casestudy-quote.html quote="Working with 14islands was awesome. They made sure to understand our needs and really delivered on them! Loved how we worked together as a team, compared to many other client/agency structures. This allowed us to challenge each other to create the best possible work and have a lot of fun while doing it. A+" author-image-src="/images/work/tictail/kaj-2-1.png" author-name="Kaj Drobin" author-job-title="CPO and Co-Founder at Tictail" %}
{% markdown %}
## A sense of pride
We are really happy with how this website turned out and we have gotten really great feedback from the community. A big thanks to everyone involved!
{% endmarkdown %}
{% include casestudy-button.html site-url="https://tictail.com/" %}


Coverage Report
Total
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Executed
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In Ghana, children are given their first name as a 'day name', after the day of the week they were born.These names are called the Akan Names.
This application is to help you know the day of the week you were born and your Akan Name corresponding to your day and your gender.
Fill the information about your date of birth and gender in the form to know your Akan Name:


I turn ideas into beautiful things, and I love what I do.
My main objective is to make sure that the clients' requirements are met at the best possible level, providing the highest quality, standards, compatibility and creative ideas. Do you need someone to transfer your ideas into masterpiece?


Spaying or neutering increases life expectancy: one study found neutered male cats live twice as long as intact males, while spayed female cats live 62% longer than intact females.:35 Having a cat neutered confers health benefits, because castrated males cannot develop testicular cancer, spayed females cannot develop uterine or ovarian cancer, and both have a reduced risk of mammary cancer.Despite widespread concern about the welfare of free-roaming cats, the lifespans of neutered feral cats in managed colonies compare favorably with those of pet cats.
About two hundred fifty heritable genetic disorders have been identified in cats, many similar to human inborn errors of metabolism. The high level of similarity among the metabolism of mammals allows many of these feline diseases to be diagnosed using genetic tests that were originally developed for use in humans, as well as the use of cats as animal models in the study of the human diseases.[173][174] Diseases affecting domestic cats include acute infections, parasitic infestations, injuries, and chronic diseases such as kidney disease, thyroid disease, and arthritis. Vaccinations are available for many infectious diseases, as are treatments to eliminate parasites such as worms and fleas


| Kelp Crab Dwelling among the branches of the kelp holdfastthe root system that holds the kelp to the bottomkelp crabs eat older, inner branches. This creates room among the roots for communities of small creatures. Kelp crabs are vegetarians in the spring, grazing on overgrown water plants and leaving stubby fields behind. In winter, they become carnivores, eating small shellfish and sea slugs. Occasionally, barnacle parasites latch onto the shells of kelp crabs, penetrating the crabs shell with an antenna. The parasite then sheds most of its own body parts and slides through the hollow antenna into the crabs body, where it feeds off its host and breeds offspring. |


{% extends "base.html" %} {% block title %} page not found {% endblock %} {% block content %}
The page you requested was lost.


{% extends "main.html" %} {% block err %}
- we are currently developping your next prefered free, open source, online crawler -


|
S2OPC OPCUA Toolkit
|
#include "sopc_array.h"
#include "sopc_mem_alloc.h"
#include <assert.h>
#include <stdint.h>
#include <stdlib.h>
#include <string.h>
Data Structures | |
| struct | _SOPC_Array |
Macros | |
| #define | ARRAY_ELT(a, idx) ((void*) (a->data + idx * a->element_size)) |
Functions | |
| SOPC_Array * | SOPC_Array_Create (size_t element_size, size_t initial_capacity, SOPC_Array_Free_Func free_func) |
| Creates a new array with a given capacity. More... | |
| SOPC_Array * | SOPC_Array_Copy (const SOPC_Array *array) |
| Makes a copy of an array. More... | |
| void | SOPC_Array_Delete (SOPC_Array *array) |
| Deletes an array. More... | |
| bool | SOPC_Array_Append_Values (SOPC_Array *array, const void *data, size_t n_elements) |
| Appends several values contiguous in memory to an array. More... | |
| void * | SOPC_Array_Get_Ptr (const SOPC_Array *array, size_t index) |
| Gets a pointer to a value in an array by its index. More... | |
| size_t | SOPC_Array_Size (const SOPC_Array *array) |
| Gets the number of elements in an array. More... | |
| void | SOPC_Array_Sort (SOPC_Array *array, SOPC_Array_Compare_Func compare_func) |
| Sorts the elements in an array. More... | |
| void * | SOPC_Array_Into_Raw (SOPC_Array *array) |
| Converts a SOPC_Array into a raw C array. More... | |
| SOPC_Array_Free_Func | SOPC_Array_Get_Free_Func (SOPC_Array *array) |
| Returns the function used to clear the elements of an array on deletion. More... | |
| void | SOPC_Array_Set_Free_Func (SOPC_Array *array, SOPC_Array_Free_Func func) |
| Sets the function used to clear the array elements when it is deleted. More... | |
| #define ARRAY_ELT | ( | a, | |
| idx | |||
| ) | ((void*) (a->data + idx * a->element_size)) |
| bool SOPC_Array_Append_Values | ( | SOPC_Array * | array, |
| const void * | data, | ||
| size_t | n_elements | ||
| ) |
Appends several values contiguous in memory to an array.
| array | The array. |
| data | The memory location of the first value. If NULL , the array grows by n_elements items, but does not initialize them. |
| n_elements | The number of values present in memory. |
TRUE
on success, FALSE
on memory allocation failure. | SOPC_Array* SOPC_Array_Copy | ( | const SOPC_Array * | array | ) |
Makes a copy of an array.
| array | The array. |
NULL
on memory allocation failure. | SOPC_Array* SOPC_Array_Create | ( | size_t | element_size, |
| size_t | initial_capacity, | ||
| SOPC_Array_Free_Func | free_func | ||
| ) |
Creates a new array with a given capacity.
| element_size | The size of one element of the array. |
| initial_capacity | The initial capacity to allocate (can be 0). |
| free_func | A function to call on each array element when the array is deleted. Can be NULL . |
NULL
on memory allocation failure.The actual allocated size might be greater than the requested capacity.
| void SOPC_Array_Delete | ( | SOPC_Array * | array | ) |
Deletes an array.
| array | The array. |
The free function passed in the constructor or via SOPC_Array_Set_Free_Func (if any) will be called for each element of the array before the array is freed.
| SOPC_Array_Free_Func SOPC_Array_Get_Free_Func | ( | SOPC_Array * | array | ) |
Returns the function used to clear the elements of an array on deletion.
| array | The array. |
NULL
if no such function is defined. | void* SOPC_Array_Get_Ptr | ( | const SOPC_Array * | array, |
| size_t | index | ||
| ) |
Gets a pointer to a value in an array by its index.
| array | The array. |
| index | The index of the value. |
| void* SOPC_Array_Into_Raw | ( | SOPC_Array * | array | ) |
Converts a SOPC_Array into a raw C array.
| array | The array. |
NULL
if the array was empty.This function releases the memory of the SOPC_Array itself, only keeping the data before returning it. The returned memory region holds the data exactly, without any padding before or after, and must be freed when no longer needed.
| void SOPC_Array_Set_Free_Func | ( | SOPC_Array * | array, |
| SOPC_Array_Free_Func | func | ||
| ) |
Sets the function used to clear the array elements when it is deleted.
| array | The array. |
| func | The function to use for clearing elements, or NULL if no such function should be called. |
| size_t SOPC_Array_Size | ( | const SOPC_Array * | array | ) |
Gets the number of elements in an array.
| array | The array. |
| void SOPC_Array_Sort | ( | SOPC_Array * | array, |
| SOPC_Array_Compare_Func | compare_func | ||
| ) |
Sorts the elements in an array.
| array | The array. |
| compare_func | The function to use to compare to elements. |
The sort is not guaranteed to be stable.


Before Change
partial = r.consume("{"msgtype": "PATCH-DOC", "msgid": "10", "num_buffers":1}").result()
assert partial is None
partial = r.consume("{}").result()
assert partial is None
partial = r.consume("{"bar": 10}").result()
assert partial is None
After Change
partial = await r.consume("{"msgtype": "PATCH-DOC", "msgid": "10", "num_buffers":1}")
assert partial is None
partial = await r.consume("{}")
assert partial is None
partial = await r.consume("{"bar": 10}")


McConkey, Bill. “The Brain.” Europeana Collections, The European Union, www.europeana.eu/portal/en/record/9200579/uxntdnha.html?q=brain+AND+RIGHTS:*creative* AND NOT RIGHTS:*nc*+AND+NOT+RIGHTS:*nd*#dcId=1554156299157&p=4.
Dumlao, Nathan. “Silhouette of Man near Body of Water.” Unsplash.com, 21 Dec. 2017, unsplash.com/photos/kllOcwU1PeE.
Harmon, Jonny. “Silhouette of Four Men.” Unsplash.com, 18 Nov. 2018, unsplash.com/photos/vYX0NtD-TSA.
Heemer, Bill. “Person Using Professional Audio Mixer.” Unsplash.com, 27 Feb. 2019, unsplash.com/photos/OotB534-CBQ.
Kirchoff, Chad. “Silhouette of Crowd in Concert Grounds.” Unsplash.com/, 03 Oct. 2016, unsplash.com/photos/ivqGyYLtBI8.
Owens, Jakob. “Silhouette of Man Surrounded with Fog during Golden Hour.” Unsplash.com, 8 Aug. 2018, unsplash.com/photos/9Ke7dgNiAPU.
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Trivedi, Vivek. “Lost in Wilderness.” Unsplash.com, 27 July 2018, unsplash.com/photos/lpZcI7a_q10.
Battlefield High School Technology Student Association Chapter. "The Fool in the State of Arizona." 2019.
“Our School.” Battlefield High School, battlefieldhs.pwcs.edu/our_school.
Byun, Matthew, et al. TSA Digital Video Production 2018-2019, "The DPMC". 22 Feb. 2019, www.youtube.com/watch?v=UJNGr30SmkM.
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|
Standard Reference Data Program |
Data Gateway |
Chemistry WebBook |
|
NIST subscription sites provide data under the NIST Standard Reference Data Program, but require an annual fee to access. The purpose of the fee is to recover costs associated with the development of data collections included in such sites. Your institution may already be a subscriber. Follow the links above to find out more about the data in these sites and their terms of usage.
Go To: Top, Constants of diatomic molecules, References, Notes / Error Report
Data compilation copyright by the U.S. Secretary of Commerce on behalf of the U.S.A. All rights reserved.
Data evaluated as indicated in comments:
HL - E.P. Hunter and S.G. Lias
L - S.G. Lias
Data compiled as indicated in comments:
B - J.E. Bartmess
LBLHLM - S.G. Lias, J.E. Bartmess, J.F. Liebman, J.L. Holmes, R.D. Levin, and W.G. Mallard
LLK - S.G. Lias, R.D. Levin, and S.A. Kafafi
RDSH - H.M. Rosenstock, K. Draxl, B.W. Steiner, and J.T. Herron
View reactions leading to ClH+ (ion structure unspecified)
| Quantity | Value | Units | Method | Reference | Comment |
|---|---|---|---|---|---|
| IE (evaluated) | 12.744 ± 0.009 | eV | N/A | N/A | L |
| Quantity | Value | Units | Method | Reference | Comment |
| Proton affinity (review) | 556.9 | kJ/mol | N/A | Hunter and Lias, 1998 | HL |
| Quantity | Value | Units | Method | Reference | Comment |
| Gas basicity | 530.1 | kJ/mol | N/A | Hunter and Lias, 1998 | HL |
| IE (eV) | Method | Reference | Comment |
|---|---|---|---|
| 12.790 | PE | Wang, Dillon, et al., 1984 | LBLHLM |
| 12.752 ± 0.006 | PE | Pennetreau, Natalis, et al., 1983 | LBLHLM |
| 12.748 | PE | Von Niessen, Asbrink, et al., 1982 | LBLHLM |
| 12.747 ± 0.002 | PE | Natalis, Pennetreau, et al., 1982 | LBLHLM |
| 12.75 | PE | Kimura, Katsumata, et al., 1981 | LLK |
| 12.72 ± 0.03 | PI | Tiedemann, Anderson, et al., 1979 | LLK |
| 12.748 | EVAL | Huber and Herzberg, 1979 | LLK |
| 12.748 ± 0.005 | PE | Weiss, Lawrence, et al., 1970 | RDSH |
| 12.74 ± 0.01 | PE | Lempka, Passmore, et al., 1968 | RDSH |
| 12.742 ± 0.010 | PI | Nicholson, 1965 | RDSH |
| 12.74 ± 0.01 | PI | Watanabe, 1957 | RDSH |
| Ion | AE (eV) | Other Products | Method | Reference | Comment |
|---|---|---|---|---|---|
| Cl+ | 17.34 ± 0.01 | H | PI | Krauss, Walker, et al., 1968 | RDSH |
| H+ | 14.5 | Cl- | EI | Fox, 1957 | RDSH |
+ H+ =
| Quantity | Value | Units | Method | Reference | Comment |
|---|---|---|---|---|---|
| ΔrH° | 1395. | kJ/mol | N/A | Martin and Hepburn, 1998 | gas phase; Photodissociation of HCl to H+ and Cl-: ΔHacid(0K)=116288.7±0.6 cm-1, or ±2 cal/mol; B |
| ΔrH° | 1394.9 ± 0.42 | kJ/mol | D-EA | Trainham, Fletcher, et al., 1987 | gas phase; reported: 29138.3±0.5 cm-1; B |
| ΔrH° | 1396. ± 8.8 | kJ/mol | G+TS | Fujio, McIver, et al., 1981 | gas phase; value altered from reference due to change in acidity scale; B |
| Quantity | Value | Units | Method | Reference | Comment |
| ΔrG° | 1372.8 ± 0.42 | kJ/mol | H-TS | Martin and Hepburn, 1998 | gas phase; Photodissociation of HCl to H+ and Cl-: ΔHacid(0K)=116288.7±0.6 cm-1, or ±2 cal/mol; B |
| ΔrG° | 1372.8 ± 0.84 | kJ/mol | H-TS | Trainham, Fletcher, et al., 1987 | gas phase; reported: 29138.3±0.5 cm-1; B |
| ΔrG° | 1374. ± 8.4 | kJ/mol | IMRE | Fujio, McIver, et al., 1981 | gas phase; value altered from reference due to change in acidity scale; B |
Go To: Top, Gas phase ion energetics data, References, Notes / Error Report
Data compilation copyright by the U.S. Secretary of Commerce on behalf of the U.S.A. All rights reserved.
Data compiled by: K.P. Huber and G. Herzberg
| State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|
| Rydberg 1 | 200-210 eV | |||||||||||
| Hayes and Brown, 1972; Schwarz, 1975 | ||||||||||||
| Numerous absorption bands above 123000 cm-1, tentatively assigned to higher members of the Rydberg series starting with L and M and converging to A 2Σ+ of HCl+. | ||||||||||||
| Terwilliger and Smith, 1973 | ||||||||||||
| M (1Σ+) | (117811) | [1529] 2 | M ← X | 117093 | ||||||||
| missing citation | ||||||||||||
| L (1Σ+,1Π) | 111280 | 1531 | 52 3 | L ← X | 110555 | |||||||
| missing citation | ||||||||||||
| 4 | ||||||||||||
| Douglas and Greening, 1979 | ||||||||||||
| State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
| K 1Π | (89861) | [2604.6] Z | [9.230] 5 | [-12.6E-4] 5 | [1.3654] | K ← X R | 89680.5 Z | |||||
| Douglas and Greening, 1979 | ||||||||||||
| H 1Σ+ | (89120) | [2093.8] Z | [8.4410] | [8.93E-4] | [1.4278] | H ← X R | 88684.5 Z | |||||
| Douglas and Greening, 1979 | ||||||||||||
| E 1Σ+ | (84193) | [2138.6] Z | [6.6423] | [36.2] | [1.6096] | E ← X R | 83780.2 Z | |||||
| Douglas and Greening, 1979 | ||||||||||||
| g (3Σ-)1 | [84329.7] 6 | [10.36] 7 | [17E-4] 7 | [1.289] | g ← X | 82847.4 Z | ||||||
| missing citation | ||||||||||||
| State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
| f1 3Δ1 | [84006.1] 6 | [10.270] 8 | [-13E-4] 8 | [1.294] | f1 ← X | 82523.8 Z | ||||||
| missing citation | ||||||||||||
| D 1Π | [83972.0] 9 | [9.794] 10 | [20.5E-4] 10 | [1.326] | D ← X R | 82489.7 Z | ||||||
| missing citation | ||||||||||||
| d0 3Π0 | [83753.6] 9 | [9.404] 11 | [-2.2E-4] 11 | [1.353] | d0 ← X R | 82271.3 Z | ||||||
| missing citation | ||||||||||||
| f2 3Δ2 | [83497.7] 6 | [10.851] 12 | [29.5E-4] 12 | [1.259] | f2 ← X V | 82015.4 Z | ||||||
| missing citation | ||||||||||||
| State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
| f3 3Δ3 | [83308.2] 6 | [9.45] 8 | [-1.3E-4] 8 | [1.349] | f3 ← X R | 81825.9 Z | ||||||
| missing citation | ||||||||||||
| d1 3Π1 | [83255.6] 9 | [9.768] 13 | [8E-4] 13 | [1.327] | d1 ← X R | 81773.3 Z | ||||||
| missing citation | ||||||||||||
| d2 3Π2 | [83083] 9 | [8.632] 14 | [-14E-4] 14 | [1.412] | d2 ← X R | 81600.7 Z | ||||||
| missing citation | ||||||||||||
| C 1Π | 77575 15 | [2684.0] Z | 16 | [9.333] | 16 | [1.358] | C ← X 17 R | 77485.3 Z | ||||
| missing citation; Tilford, Ginter, et al., 1970 | ||||||||||||
| State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
| V 1Σ+ | 77293.0 18 | 877.16 Z | 16.04 19 | 2.727 | -0.026 | 1.02E-4 19 | 0.20E-4 | 2.512 | V ↔ X 20 R | 76245.3 Z | ||
| Jacques, 1959; Jacques and Barrow, 1959; missing citation | ||||||||||||
| V 1Σ+ 21 | V → A | |||||||||||
| Jacques and Barrow, 1959 | ||||||||||||
| b0 3Π0 | (75617) 15 | [2712] | [10.36] 22 | [1.289] | b0 ← X 23 | 75490.4 Z | ||||||
| Price, 1938; missing citation | ||||||||||||
| b1 3Π1 | (75195) 15 | (2900) | (79) | [9.87] 22 | [1.320] | b1 ← X R | 75142.6 Z | |||||
| Price, 1938; missing citation | ||||||||||||
| State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
| b2 3Π2 | [76322.2] 15 | [9.18] 22 | [1.369] | b2 ← X 23 R | 74839.9 Z | |||||||
| Price, 1938; missing citation | ||||||||||||
| A (1Π) 24 25 | A ← X | |||||||||||
| Datta and Banerjee, 1941; Romand, 1949 | ||||||||||||
| X 1Σ+ | 0 | 2990.9463 26 | 52.8186 27 | 0.22437 | 10.593416 26 28 | 0.307181 29 | 5.3194E-4 28 30 | 1.274552 31 32 | ||||
| Rank, Eastman, et al., 1962; Rank, Rao, et al., 1965 | ||||||||||||
| Rotation spectrum 33 34 | ||||||||||||
| Hansler and Oetjen, 1953; Jones and Gordy, 1964; Rosenberg, Lightman, et al., 1972 | ||||||||||||
| Raman cross sections | ||||||||||||
| Kaiser, 1970; de Leeuw and Dymanus, 1973 | ||||||||||||
| Mol. beam electric reson. 35 | ||||||||||||
| Kaiser, 1970; de Leeuw and Dymanus, 1973 | ||||||||||||
| Mol. beam magnetic reson. 36 | ||||||||||||
| Code, Khosla, et al., 1968 |
| 1 | Rydberg series corresponding to excitation of a 2p electron. |
| 2 | v=0...5 observed. Assigned as 3pσ3pπ4 5sσ. 39 |
| 3 | Assigned as 3pσ3pπ4 4pσ/π. 39 |
| 4 | Many other absorption bands in the region 83000 - 93000 cm-1 corresponding to Rydberg states strongly perturbed by the V 1Σ+ state which itself gives rise to many perturbed bands. |
| 5 | Average B, D values; B(R,P)-B(Q) = +0.385. |
| 6 | Configuration ...σ2π3 4pπ. |
| 7 | Average B, D values; B(1+)-B(1-) = - 0.060. |
| 8 | Refers to Δ+; Q branch not resolved. |
| 9 | Configuration ...σ2π3 4pσ. |
| 10 | Average B, D values; B(Π+)-B(Π-) = +0.063. |
| 11 | Average B, D values; B(Π+)-B(Π-) = -0.040. |
| 12 | Average B, D values; B(Δ+)-B(Δ-) = -0.030. |
| 13 | Average B, D values; B(Π+)-B(Π-) = -0.160. |
| 14 | Average B, D values; B(Π+)-B(Π-) = -0.667. |
| 15 | Configuration σ2π3 4sσ. |
| 16 | v=1,2,3 are increasingly diffuse; B1 = 9.296. Tilford, Ginter, et al., 1970 give ωe = 2817.5, ωexe = 66.0, Be = 9.44, αe = 0.15. |
| 17 | A1so observed in inert matrices Boursey, 1975. |
| 18 | Typica1 "V" state with configuration ... σπ4 σ*. |
| 19 | missing note |
| 20 | Very extended progression in absorption, not yet analyzed in detail. The higher vibrational levels are strongly perturbed by Rydberg states Tilford and Ginter, 1971, Douglas and Greening, 1979. The vibrational and rotational constants given were obtained from the emission spectrum with v≤3 Jacques, 1959, Jacques and Barrow, 1959 but because of the perturbations have only very limited meaning. |
| 21 | Continuous absorption starting at 44000 cm-1, maximum 40 at 65500 cm-1. |
| 22 | Diffuse rotational structure; 1-0 and 2-0 are increasingly diffuse. |
| 23 | The b2←X and b0←X components have only 1/50 of the intensity of b1←X. |
| 24 | Configuration ...σ2π3 σ*. |
| 25 | Continuous aabsorption starting at 44000 cm-1, maximum at 65500 cm-1. |
| 26 | Applying the Dunham corrections Rank, Rao, et al., 1965 obtain ωe = 2991.0904 and Be = 10.593553. Additional corrections (adiabatic, non- adiabatic) discussed by Bunker, 1972. Vibrational levels up to v=5 have been observed in infrared absorption Rank, Birtley, et al., 1960, Rank, Eastman, et al., 1962, Rank, Rao, et al., 1965 and emission Mould, Price, et al., 1960, higher levels in the V→X bands Jacques, 1959, Jacques and Barrow, 1959. Dunham potential coefficients Ogilvie and Koo, 1976. Most recent ab initio values of the ground state molecular constants Meyer and Rosmus, 1975; charge distribution Cade, Bader, et al., 1969. |
| 27 | ωeze = -0.01218 Rank, Rao, et al., 1965. |
| 28 | Slightly different constants in Plyler and Tidwell, 1960, Levy, Rossi, et al., 1965, Levy, Rossi, et al., 1966. These papers and Webb and Rao, 1968 give also constants for H37Cl. |
| 29 | +0.0017724(v+1/2)2 - 0.0001201(v+1/2)3. |
| 30 | -7.510E-6(v+1/2) + 4.00E-7(v+1/2)2; higher order terms in Rank, Rao, et al., 1965. See also Herman and Asgharian, 1966. |
| 31 | Uncorrected value from the Be(=Y01) given in the table. The internuclear distance at the minimum of the Born-Oppenheimer curve is re = 1.2746149 Bunker, 1972, Watson, 1973. |
| 32 | Rot.-vibr. Bands 41 34 |
| 33 | Absolute intensity measurements Chamberlain and Gebbie, 1965, Sanderson, 1967. |
| 34 | Pressure-induced shifts (by foreign gases) of rotation-vibration and rotation lines Rank, Eastman, et al., 1960, Ben-Reuven, Kimel, et al., 1961, Gebbie and Stone, 1963, Jaffe, Friedmann, et al., 1963, Jaffe, Hirshfeld, et al., 1964. For discussions of pressure-induced bands and pure rotation lines (ΔJ=2) see Atwood, Vu, et al., 1967, Weiss and Cole, 1967. Self and foreign-gas line broadening Benedict, Herman, et al., 1956, Babrov, Ameer, et al., 1959, Goldring and Benesch, 1962, Jaffe, Kimel, et al., 1962, Plyler and Thibault, 1962, Alamichel and Legay, 1966, Levy, Mariel-Piollet, et al., 1970, Toth, Hunt, et al., 1970, Rich and Welsh, 1971, Rosenberg, Lightman, et al., 1972. Infrared absorption in liquid and solid phases Katz and Ron, 1970, Khatibi and Vu, 1972. |
| 35 | μel(v=0,1,2)= 1.1085, 1.1390, 1.1685 D, respectively Kaiser, 1970. Dipole moment function Kaiser, 1970, Smith, 1973; see also Bunker, 1973, Kaiser, 1974. gJ = 0.4594, also quadrupole and other hyperfine coupling constants Kaiser, 1970, de Leeuw and Dymanus, 1973; see also Tokuhiro, 1967, Bunker, 1973. |
| 36 | Proton spin - rotation interaction constant Leavitt, Baker, et al., 1961, Code, Khosla, et al., 1968. |
| 37 | From D00(H2), D00(Cl2), and ΔHof0(HCl) |
| 38 | From the photoelectron spectrum Frost, McDowell, et al., 1967, Lempka, Passmore, et al., 1968, Weiss, Lawrence, et al., 1970; photoionization measurements give similar results Watanabe, Nakayama, et al., 1962, Nicholson, 1965. A somewhat smaller I.P.(12.730 eV) may be derived from the second band system in the photoelectron spectrum at 16.254 eV corresponding to A 2Σ+ of HCl+. Higher ionization potentials at 207.1 and 208.7 eV correspond to the removal of a 2p electron Hayes and Brown, 1972. |
| 39 | Strongly broadened by preionization (lifetime τ= 1.1E-14 s) Terwilliger and Smith, 1973. |
| 40 | Absorption coefficient k=40. |
| 41 | Absolute intensities (cm-2atm-1) of the 1-0 band: 130 Benedict, Herman, et al., 1956 2-0 band: 2.9 Benedict, Herman, et al., 1956 3.70 Jaffe, Kimel, et al., 1962, Toth, Hunt, et al., 1970 3-0 band: 0.023 Benedict, Herman, et al., 1956 |
Go To: Top, Gas phase ion energetics data, Constants of diatomic molecules, Notes / Error Report
Data compilation copyright by the U.S. Secretary of Commerce on behalf of the U.S.A. All rights reserved.
Hunter and Lias, 1998
Hunter, E.P.; Lias, S.G.,
Evaluated Gas Phase Basicities and Proton Affinities of Molecules: An Update,
J. Phys. Chem. Ref. Data, 1998, 27, 3, 413-656. [doi:10.1063/1.556018]
[all data]
Wang, Dillon, et al., 1984
Wang, R.-G.; Dillon, M.A.; Spence, D.,
Electron spectroscopy of hydrogen chloride from 5 to 19 eV,
J. Chem. Phys., 1984, 80, 63. [all data]
Pennetreau, Natalis, et al., 1983
Pennetreau, P.; Natalis, P.; Longton, L.; Collin, J.E.,
Ionization energies for the vibronic transitions from DCl X1Σ+(v" = 0) to DCl+ X2Π(v' = 0-18) and A2Σ+ (v' = 0-17) determined by photoelectron spectroscopy,
J. Electron Spectrosc. Relat. Phenom., 1983, 28, 295. [all data]
Von Niessen, Asbrink, et al., 1982
Von Niessen, W.; Asbrink, L.; Bieri, G.,
30.4 nm He(II) Photoelectron spectra of organic molecules. Part VI. Halogeno-compounds (C,H,X: X = Cl, Br, I),
J. Electron Spectrosc. Relat. Phenom., 1982, 26, 173. [all data]
Natalis, Pennetreau, et al., 1982
Natalis, P.; Pennetreau, P.; Longton, L.; Collin, J.E.,
Ionisation energy values for the vibronic transitions from HCl X1Σ+ (v" = 0) to HCl+ ionic states X2Π (v' = 0-13) and A2Σ+ (v' = 0-12), determined by photoelectron spectroscopy,
J. Electron Spectrosc. Relat. Phenom., 1982, 27, 267. [all data]
Kimura, Katsumata, et al., 1981
Kimura, K.; Katsumata, S.; Achiba, Y.; Yamazaki, T.; Iwata, S.,
Ionization energies, Ab initio assignments, and valence electronic structure for 200 molecules
in Handbook of HeI Photoelectron Spectra of Fundamental Organic Compounds, Japan Scientific Soc. Press, Tokyo, 1981. [all data]
Tiedemann, Anderson, et al., 1979
Tiedemann, P.W.; Anderson, S.L.; Ceyer, S.T.; Hirooka, T.; Ng, C.Y.; Mahan, B.H.; Lee, Y.T.,
Proton affinities of hydrogen halides determined by the molecular beam photoionization method,
J. Chem. Phys., 1979, 71, 605. [all data]
Huber and Herzberg, 1979
Huber, K.P.; Herzberg, G.,
Molecular Spectra and Molecular Structure. IV. Constants of Diatomic Molecules,, Van Nostrand Reinhold Co., 1979, ,1. [all data]
Weiss, Lawrence, et al., 1970
Weiss, M.J.; Lawrence, G.M.; Young, R.A.,
Photoelectron spectroscopy of HCI and DCI using molecular beams,
J. Chem. Phys., 1970, 52, 2867. [all data]
Lempka, Passmore, et al., 1968
Lempka, H.J.; Passmore, T.R.; Price, W.C.,
The photoelectron spectra and ionized states of the halogen acids,
Proc. Roy. Soc. (London), 1968, A304, 53. [all data]
Nicholson, 1965
Nicholson, A.J.C.,
Photoionization-efficiency curves. II. False and genuine structure,
J. Chem. Phys., 1965, 43, 1171. [all data]
Watanabe, 1957
Watanabe, K.,
Ionization potentials of some molecules,
J. Chem. Phys., 1957, 26, 542. [all data]
Krauss, Walker, et al., 1968
Krauss, M.; Walker, J.A.; Dibeler, V.H.,
Mass spectrometric study of photoionization. X. Hydrogen chloride and methyl halides,
J. Res. NBS, 1968, 72A, 281. [all data]
Fox, 1957
Fox, R.E.,
Negative ion formation in hydrogen chloride by electron impact,
J. Chem. Phys., 1957, 26, 1281. [all data]
Martin and Hepburn, 1998
Martin, J.D.D.; Hepburn, J.W.,
Determination of bond dissociation energies by threshold ion-pair production spectroscopy: An improved D-0(HCl),
J. Chem. Phys., 1998, 109, 8139-8142. [all data]
Trainham, Fletcher, et al., 1987
Trainham, R.; Fletcher, G.D.; Larson, D.J.,
One- and Two-Photon Detachment of the Negative Chlorine Ion,
J. Phys. B, 1987, 20, L777. [all data]
Fujio, McIver, et al., 1981
Fujio, M.; McIver, R.T., Jr.; Taft, R.W.,
Effects on the acidities of phenols from specific substituent-solvent interactions. Inherent substituent parameters from gas phase acidities,
J. Am. Chem. Soc., 1981, 103, 4017. [all data]
Hayes and Brown, 1972
Hayes, W.; Brown, F.C.,
Absorption by some molecular gases in the extreme ultraviolet,
Phys. Rev. A: Gen. Phys., 1972, 6, 21. [all data]
Schwarz, 1975
Schwarz, W.H.E.,
Interpretation of the core electron excitation spectra of hydride molecules and the properties of hydride radicals,
Chem. Phys., 1975, 11, 217. [all data]
Terwilliger and Smith, 1973
Terwilliger, D.T.; Smith, A.L.,
Analysis of autoionizing Rydberg states in the vacuum ultraviolet absorption spectrum of HCl and DCl,
J. Mol. Spectrosc., 1973, 45, 366. [all data]
Douglas and Greening, 1979
Douglas; Greening,
Unpublished cited in Huber and Herzberg, 1979, 2, 1979, 287. [all data]
Tilford, Ginter, et al., 1970
Tilford, S.G.; Ginter, M.L.; Vanderslice, J.T.,
Electronic spectra and structure of the hydrogen halides. The b3Πi and C1Π states of HCl and DCl,
J. Mol. Spectrosc., 1970, 33, 505. [all data]
Jacques, 1959
Jacques,
D. Phil. Thesis, Oxford, 1959, 1. [all data]
Jacques and Barrow, 1959
Jacques, J.K.; Barrow, R.F.,
The transition v1Σ+-x1Σ+ in hydrogen chloride,
Proc. Phys. Soc. London, 1959, 73, 538. [all data]
Price, 1938
Price, W.C.,
The absorption spectra of the halogen acids in the vacuum ultra-violet,
Proc. Roy. Soc. (London), 1938, A167, 216. [all data]
Datta and Banerjee, 1941
Datta, S.; Banerjee, S.,
The continuous absorption spectra of the hydrogen-halides. Part II. HCl,
Proc. Natl. Inst. Sci. India, 1941, 7, 305. [all data]
Romand, 1949
Romand, J.,
Absorption ultraviolette dans la region de Schumann etude de: ClH, BrH et lH gazeux,
Ann. Phys. (Paris), 1949, 4, 527. [all data]
Rank, Eastman, et al., 1962
Rank, D.H.; Eastman, D.P.; Rao, B.S.; Wiggins, T.A.,
Rotational and vibrational constants of the HCl35 and DCl35 molecules,
J. Opt. Soc. Am., 1962, 52, 1. [all data]
Rank, Rao, et al., 1965
Rank, D.H.; Rao, B.S.; Wiggins, T.A.,
Molecular constants of HCl35,
J. Mol. Spectrosc., 1965, 17, 122. [all data]
Hansler and Oetjen, 1953
Hansler, R.L.; Oetjen, R.A.,
The infrared spectra of HCl, DCl, HBr, and NH3 in the region from 40 to 140 microns,
J. Chem. Phys., 1953, 21, 1340. [all data]
Jones and Gordy, 1964
Jones, G.; Gordy, W.,
Extension of submillimeter wave spectroscopy below a half-millimeter wavelength,
Phys. Rev., 1964, 135, 295. [all data]
Rosenberg, Lightman, et al., 1972
Rosenberg, A.; Lightman, A.; Ben-Reuven, A.,
Interferometric measurements of the pure rotational spectra of HCl and DCl,
J. Quant. Spectrosc. Radiat. Transfer, 1972, 12, 219. [all data]
Kaiser, 1970
Kaiser, E.W.,
Dipole moment and hyperfine parameters of H35Cl and D35Cl,
J. Chem. Phys., 1970, 53, 1686. [all data]
de Leeuw and Dymanus, 1973
de Leeuw, F.H.; Dymanus, A.,
Magnetic properties and molecular quadrupole moment of HF and HCl by molecular-beam electric-resonance spectroscopy,
J. Mol. Spectrosc., 1973, 48, 427. [all data]
Code, Khosla, et al., 1968
Code, R.F.; Khosla, A.; Ozier, I.; Ramsey, N.F.; Yi, P.N.,
Nuclear magnetic hyperfine spectra of H35Cl and H37Cl,
J. Chem. Phys., 1968, 49, 1895. [all data]
Boursey, 1975
Boursey, E.,
Electronic excitation of HCl trapped in inert matrices,
J. Chem. Phys., 1975, 62, 3353. [all data]
Tilford and Ginter, 1971
Tilford, S.G.; Ginter, M.L.,
Electronic spectra and structure of the hydrogen halides: states associated with the (σ2π3) cπ and (σ2π3) cσ configurations of HCl and DCl,
J. Mol. Spectrosc., 1971, 40, 568. [all data]
Bunker, 1972
Bunker, P.R.,
On the breakdown of the Born-Oppenheimer approximation for a diatomic molecule,
J. Mol. Spectrosc., 1972, 5, 478. [all data]
Rank, Birtley, et al., 1960
Rank, D.H.; Birtley, W.B.; Eastman, D.P.; Rao, B.S.; Wiggins, T.A.,
Precise measurements of some infrared bands of hydrogen chloride,
J. Opt. Soc. Am., 1960, 50, 1275. [all data]
Mould, Price, et al., 1960
Mould, H.M.; Price, W.C.; Wilkinson, G.R.,
Infra-red emission from gases excited by a radio-frequency discharge,
Spectrochim. Acta, 1960, 16, 479. [all data]
Ogilvie and Koo, 1976
Ogilvie, J.F.; Koo, D.,
Dunham potential energy coefficients of the hydrogen halides and carbon monoxide,
J. Mol. Spectrosc., 1976, 61, 332-336. [all data]
Meyer and Rosmus, 1975
Meyer, W.; Rosmus, P.,
PNO-Cl and CEPA studies of electron correlation effects. III. Spectroscopic constants and dipole moment functions for the ground states of the first-row and second-row diatomic hydrides,
J. Chem. Phys., 1975, 63, 2356. [all data]
Cade, Bader, et al., 1969
Cade, P.E.; Bader, R.F.W.; Henneker, W.H.; Keaveny, I.,
Molecular charge distributions and chemical binding. IV. The second-row diatomic hydrides AH,
J. Chem. Phys., 1969, 50, 5313. [all data]
Plyler and Tidwell, 1960
Plyler, E.K.; Tidwell, E.D.,
The rotational constants of hydrogen chloride,
Z. Elektrochem., 1960, 64, 717. [all data]
Levy, Rossi, et al., 1965
Levy, A.; Rossi, I.; Joffrin, C.; Van Thanh, N.,
Spectre de vibration-rotation de l'acide chlorhydrique gazeux. Etude de la bande v0→2 a 1,7 micron,
J. Chim. Phys. Phys.-Chim. Biol., 1965, 62, 600. [all data]
Levy, Rossi, et al., 1966
Levy, A.; Rossi, I.; Haeusler, C.,
Constantes de vibration-rotation de l'acide chlorhydrique gazeux etude des bandes vo→2 et vo→3,
J. Phys. (Paris), 1966, 27, 526. [all data]
Webb and Rao, 1968
Webb, D.U.; Rao, K.N.,
Vibration rotation bands of heated hydrogen halides,
J. Mol. Spectrosc., 1968, 28, 121. [all data]
Herman and Asgharian, 1966
Herman, R.M.; Asgharian, A.,
Finite nuclear mass effects on the centrifugal stretching constant in H35Cl,
J. Chem. Phys., 1966, 45, 2433. [all data]
Watson, 1973
Watson, J.K.G.,
The isotope dependence of the equilibrium rotational constants in 1Σ states of diatomic molecules,
J. Mol. Spectrosc., 1973, 45, 99. [all data]
Chamberlain and Gebbie, 1965
Chamberlain, J.E.; Gebbie, H.A.,
Sub-millimetre dispersion and rotational line strengths of the hydrogen halides,
Nature (London), 1965, 208, 480. [all data]
Sanderson, 1967
Sanderson, R.B.,
Measurement of rotational line strengths in HCl by asymmetric Fourier transform techniques,
Appl. Opt., 1967, 6, 1527. [all data]
Rank, Eastman, et al., 1960
Rank, D.H.; Eastman, D.P.; Birtley, W.B.; Wiggins, T.A.,
Perturbation of molecular rotation-vibration energy levels by rare gases,
J. Chem. Phys., 1960, 33, 323. [all data]
Ben-Reuven, Kimel, et al., 1961
Ben-Reuven, A.; Kimel, S.; Hirshfeld, M.A.; Jaffe, J.H.,
Theory and measurement of pressure-induced shifts of HCl lines due to noble gases,
J. Chem. Phys., 1961, 35, 955. [all data]
Gebbie and Stone, 1963
Gebbie, H.A.; Stone, N.W.B.,
Measurement of widths and shifts of pure rotation lines of hydrogen chloride perturbed by rare gases,
Proc. Phys. Soc. London, 1963, 82, 309. [all data]
Jaffe, Friedmann, et al., 1963
Jaffe, J.H.; Friedmann, H.; Hirshfeld, M.A.; Ben-Reuven, A.,
Pressure-induced shifts of molecular lines in emission and in absorption,
J. Chem. Phys., 1963, 39, 1447. [all data]
Jaffe, Hirshfeld, et al., 1964
Jaffe, J.H.; Hirshfeld, M.A.; Ben-Reuven, A.,
Pressure-induced shifts of DCl lines due to HCl: shift oscillation,
J. Chem. Phys., 1964, 40, 1705. [all data]
Atwood, Vu, et al., 1967
Atwood, M.R.; Vu, H.; Vodar, B.,
Forme et structures fines de la bande induite par la pression dans la bande fondamentale de vibration-rotation des molecules HF, HCl et HBr,
Spectrochim. Acta, 1967, 23, 553. [all data]
Weiss and Cole, 1967
Weiss, S.; Cole, R.H.,
Pressure-induced rotational quadrupole spectra of HCl and HBr,
J. Chem. Phys., 1967, 46, 644. [all data]
Benedict, Herman, et al., 1956
Benedict, W.S.; Herman, R.; Moore, G.E.; Silverman, S.,
The strengths, widths, and shapes of infrared lines. II. The HCl fundamental,
Can. J. Phys., 1956, 34, 850. [all data]
Babrov, Ameer, et al., 1959
Babrov, H.; Ameer, G.; Benesch, W.,
Line strengths and widths in the HCl fundamental band,
J. Mol. Spectrosc., 1959, 3, 185. [all data]
Goldring and Benesch, 1962
Goldring, H.; Benesch, W.,
Widths of HCl overtone lines at various temperatures,
Can. J. Phys., 1962, 40, 1801. [all data]
Jaffe, Kimel, et al., 1962
Jaffe, J.H.; Kimel, S.; Hirshfeld, M.A.,
Refraction spectrum of gases in the infrared intensities and widths of lines in the 2-0 band of HCl,
Can. J. Phys., 1962, 40, 113. [all data]
Plyler and Thibault, 1962
Plyler, E.K.; Thibault, R.J.,
Foreign gas broadening of the lines of hydrogen chloride and carbon monoxide,
J. Res. Nat. Bur. Stand. Sect. A, 1962, 66, 435. [all data]
Alamichel and Legay, 1966
Alamichel, C.; Legay, F.,
Etude de la dispersion dans le doublet isotopique R2 de la premiere bande harmonique de vibration-rotation de HCl,
J. Phys. (Paris), 1966, 27, 233. [all data]
Levy, Mariel-Piollet, et al., 1970
Levy, A.; Mariel-Piollet, E.; Bouanich, J.-P.; Haeusler, C.,
Spectre de vibration-rotation du gaz chlorhydrique comprime. Intensites et largeurs de raies dans la bande v0-2,
J. Quant. Spectrosc. Radiat. Transfer, 1970, 10, 203. [all data]
Toth, Hunt, et al., 1970
Toth, R.A.; Hunt, R.H.; Plyler, E.K.,
Line strengths, line widths, and dipole moment function for HCl,
J. Mol. Spectrosc., 1970, 35, 110. [all data]
Rich and Welsh, 1971
Rich, N.H.; Welsh, H.L.,
Measurement of the pressure broadening of the rotational Raman lines of HCl,
Chem. Phys. Lett., 1971, 11, 292. [all data]
Katz and Ron, 1970
Katz, B.; Ron, A.,
Far infrared spectra of HCl and DCl in a nitrogen matrix,
Chem. Phys. Lett., 1970, 7, 357. [all data]
Khatibi and Vu, 1972
Khatibi, P.; Vu, H.,
Spectres d'absorption infrarouge de HCl et de HBr en phases denses. I. Spectres dans le fondamental de vibration-rotation,
J. Chim. Phys. Phys.-Chim. Biol., 1972, 69, 654. [all data]
Smith, 1973
Smith, F.G.,
Dipole moment function and vibration-rotation matrix elements of HCl35 and DCl35,
J. Quant. Spectrosc. Radiat. Transfer, 1973, 13, 717. [all data]
Bunker, 1973
Bunker, P.R.,
The breakdown of the Born-Oppenheimer approximation for a diatomic molecule: the dipole moment and nuclear quadrupole coupling constants,
J. Mol. Spectrosc., 1973, 45, 151. [all data]
Kaiser, 1974
Kaiser, E.W.,
Note: Comment to "Dipole moment function and vibration-rotation matrix elements of HCl35 and DCl35",
J. Quant. Spectrosc. Radiat. Transfer, 1974, 14, 317. [all data]
Tokuhiro, 1967
Tokuhiro, T.,
Vibrational and rotational effects on the nuclear quadrupole coupling constants in hydrogen, deuterium, and tritium halides,
J. Chem. Phys., 1967, 47, 109. [all data]
Leavitt, Baker, et al., 1961
Leavitt, J.A.; Baker, M.R.; Nelson, H.M.; Ramsey, N.F.,
Proton radio-frequency spectrum of HCl35,
Phys. Rev., 1961, 124, 1482. [all data]
Frost, McDowell, et al., 1967
Frost, D.C.; McDowell, C.A.; Vroom, D.A.,
Photoelectron spectra of the halogens and the hydrogen halides,
J. Chem. Phys., 1967, 46, 4255. [all data]
Watanabe, Nakayama, et al., 1962
Watanabe, K.; Nakayama, T.; Mottl, J.,
Ionization potentials of some molecules,
J. Quant. Spectry. Radiative Transfer, 1962, 2, 369. [all data]
Huber and Herzberg, 1979, 2
Huber, K.P.; Herzberg, G.,
Molecular Spectra and Molecular Structure. IV. Constants of Diatomic Molecules, Van Nostrand Reinhold Company, New York, 1979, 716. [all data]
Go To: Top, Gas phase ion energetics data, Constants of diatomic molecules, References
| AE | Appearance energy |
| IE (evaluated) | Recommended ionization energy |
| ΔrG° | Free energy of reaction at standard conditions |
| ΔrH° | Enthalpy of reaction at standard conditions |
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Abdominal Washout
Bilateral tubal ligation
Biopsy
Caesarean section
Cauterization of vulva or perineal warts
Ceclage
Colposcopy
Conservative management
Coterization
Cystectomy
Cystoscopy
Decapitation
Diagnostic laparascopy
Dilation and curettage
Drainage of abscess
Dressing
Dressing with vaseline gause
Evacuation/Manual Vacuum Aspiration
Exam under anaesthesia
Excision
Exploratory laparatomy +/- adnexectomy
Fistula repair
Foreign body aspiration
Gaped episiotomy repair
Hysterectomy
Hysterescopy
Incision and drainage
Lung maturation
Macdonald suture
Marsupilisation
Musculisation
Myomectomy
Ofrectomy
Polypectomy
Reopening
Repair of uterus
Salpingectomy
Slinging
Subtotal abdominal hysterectomy +/- adnexectomy
Suturing and dressing
Suturing of cervical or vaginal injury under anaesthesia
Suturing of perineum
Total abdominal hysterectomy +/- adnexectomy
Tubal ligation
Uterine evacuation
Vaginal Reconstruction
Vaginal hysterectomy
Vulvectomy


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Ocean [au50], ocean, in The Inner Sea ------------------------------------------------------------------------ Routes leaving Ocean: North, to Ocean [at50], 6 days East, to Ocean [au51], 6 days South, to Ocean [av50], 6 days West, to Ocean [au49], 6 days


You and your partner will both use one computer to complete this activity (so that we know which trials are paired).
Decide who is Player 1 and who is Player 2.
Choose the experiment below according to where you are seated.
Section A: Between subjects
Section B: Within subjects not counterbalanced
Section C: Within subjects, with randomization
Click 'Ready' when you are ready
Ready
Enter the word correctly as fast as you can. Hit enter to continue.
You won't be able to submit a word that is typed incorrectly.
Thanks, you're done.


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Indicates if keyboard hot keys should be used.
Boolean, default = true
If .keyboard property is true, the grid will add an event listener to listen for
keyboard events. There are several hot keys that are mapped to the grid actions:
- Arrow up - previous record
- Arrow down - next record
- Delete - trigger delete action
- Ctl + a (Cmd + a on mac) - select all records
This property can be defined during object creation:
Or any time after the grid has been created:
If there more then one grid on the screen and all of them have .keyboard set to true, then the last grid
where user selects a record will active keyboard listener.


Download and install the Java Runtime Environment. JRE 7 or newer is required:
Oracle Java SE downloads
C:\ProgramData\Mireka
.
Mails are stored in subdirectories in the installation directory,
so the protected Program Files
directory is not ideal,
unless you replace the affected subdirectories with links to C:\ProgramData\Mireka
subdirectories.
Setup permissions if your use case requires it. The recommended permissions are the same as on Linux. See the comments in the Setup file ownerships section of the Installing binary tarball on Ubuntu page.
Download the Apache Commons Daemon Windows binary archive from here: www.apache.org/dist/commons/daemon/binaries/windows/
You can find more information about Commons Daemon here: commons.apache.org/proper/commons-daemon/binaries.html
The archive contains binaries for both 32 and 64 bit systems.
Copy prunmgr.exe
and the prunsrv.exe
corresponding to your processor architecture into the bin
directory of Mireka.
Start a command shell running it as administrator in the Mireka home directory.
Rename the two exe files to be more specific:
rename bin\prunsrv.exe mireka.exe rename bin\prunmgr.exe mirekaw.exe
Install the service:
bin\mireka install mireka --DisplayName="Mireka Mail Server" --Description="Mireka Mail Server and SMTP Proxy" --StartMode=jvm --StopMode=jvm --StartPath="%CD%" --StopPath="%CD%" --Classpath=classes;lib/*;conf ++JvmOptions=-Dlogback.configurationFile=conf/logback.xml ++JvmOptions=-Dmireka.home="%CD%" ++JvmOptions=-Djava.net.preferIPv4Stack=true --Startup=auto --StartClass=mireka.startup.Start --StopClass=mireka.startup.Stop --LogPath=log
You can start the Mireka service in the Services Management Console GUI, or by issuing the command:
net start mireka
Check the logs, including the daemon utility log in the log
subdirectory.
To remove the service:
bin\mireka delete
GUI to view/change service parameters:
bin\mirekaw
Detailed status information about the service:
sc query mireka
Mireka home directory is the directory where you extracted the Mireka zip file.
You will find the log files in the log
, the configuration files in the conf
subdirectories.


{% if comments %} {% for comment in comments %}
Comment #{{ comment.id }} by {{ comment.username || safe }} at {{ comment.time || safe }} - reply
{{ comment.body || safe }}
{{ error }}
error: {{ error }}
Comment #{{ comment.id }} by {{ comment.username || safe }} at {{ comment.time || safe }} - reply
{{ comment.body || safe }}


--- layout: default title: Paragraphs number: 7 ---
Markdown has several ways of formatting paragraphs.
Let's take a few lines of poetry as an example. Suppose you want to write text that looks like this:
Do I contradict myself?
Very well then I contradict myself,
(I am large, I contain multitudes.)
Now, you might think that simply typing each verse onto its own line would be enough to solve the problem:
Do I contradict myself? Very well then I contradict myself, (I am large, I contain multitudes.)
Unfortunately, you'd be wrong! This Markdown would render simply as a single straight line: Do I contradict myself? Very well then I contradict myself, (I am large, I contain multitudes.).
If you forcefully insert a new line, you end up breaking the togetherness:
Do I contradict myself? Very well then I contradict myself, (I am large, I contain multitudes.)
This is what's known as a hard break; what our poetry asks for is a soft break. You can accomplish this by inserting two spaces after each new line. This is not possible to see, since spaces are invisible, but it'd look something like this:
Do I contradict myself?·· Very well then I contradict myself,·· (I am large, I contain multitudes.)
Each dot ( ·
) represents a space on the keyboard.
Let's try this technique out. In the box below, insert the necessary number of spaces to make the poem render correctly:
Fantastic work!
Aside from formatting poetry, one of the common uses for these soft breaks is in formatting paragraphs in lists. Recall in the previous lesson that we inserted a new line for multiple paragraphs within a list.
In the box below, instead of using hard breaks, tighten the sub-paragraphs with soft breaks:


[USER INFO]
____________________
[FULLNAME]
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[USERNAME]
[USERNAME]
[EMAIL]
[EMAIL]
[ROLES]
[ROLES]
[SOCIAL]
|
[SOCIAL]
[ANONYMOUS]


{% extends "mailbody/_mailbase.html" %}
{% block content %}
Hello {{ name }}, thanks for signing up to {{ project_name}}!
PlatformU is a tool designed specifically for area managers. This platform is
a work in progress, we will be learning and adapting the functionality of the
platform based on your needs. Check out the help section of the site to learn
how to use the basic features. If you have any questions don’t hesitate to
throw your comments into the forum. If you have any suggestions to improve the
functionality of the site, add a new work item to the list.
The platform has been developed and is hosted by the Metabolism of Cities team.
Our goal is to make cities more resource efficient places to live and work by
improving data and knowledge of how cities work. For more information the
non-for-profit organisation, head to metabolismofcities.org.
We wish you good luck!
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{% endblock %}


This notebook explores a data set about abalones, which are essentially sea snails. Specifically, the data set describes several physical characteristics of abalones, and then gives a number of rings found in the shell. Counting rings is time-consuming and difficult, providing a motive to build a machine-learning algorithm capable of predicting the number of rings from other physical characteristics.
In this notebook, we'll explore the abalone shell data, examine distributions, and figure out first steps toward modeling the data and making predictions.
Start by importing libraries:
%matplotlib inline
# ml
from sklearn import linear_model, svm
# numbers
import numpy as np
import pandas as pd
# stats
import statsmodels.api as sm
import scipy.stats as stats
# plots
import matplotlib.pyplot as plt
import seaborn as sns
# utils
import os, re
Now grab the data from the abalone/
directory:
# List data files
os.listdir('abalone/')
# x data labels
xnlabs = ['Sex']
xqlabs = ['Length','Diameter','Height','Whole weight','Shucked weight','Viscera weight','Shell weight']
xlabs = xnlabs + xqlabs
# y data labels
ylabs = ['Rings']
# data
df = pd.read_csv('abalone/Dataset.data', header=None, sep=' ', names=xlabs+ylabs)
train_df = df[:3000]
test_df = df[3000:]
# Czech it out
df.info()
Start exploring the data by plotting some histograms of different quantities. Once we do that, we'll get a better idea of how they are distributed amongst the population of abalones sampled for this data set.
fig = plt.figure(figsize=(14,4))
ax1 = fig.add_subplot(131)
ax2 = fig.add_subplot(132)
ax3 = fig.add_subplot(133)
# Plot weight information
sns.distplot(df['Whole weight'], label='Whole', ax=ax1)
sns.distplot(df['Shucked weight'], label='Shucked', ax=ax1)
sns.distplot(df['Viscera weight'], label='Viscera', ax=ax1)
sns.distplot(df['Shell weight'], label='Shell', ax=ax1)
ax1.legend()
# Plot growth information
sns.distplot(df['Length'], label='Length', ax=ax2)
sns.distplot(df['Diameter'], label='Diameter', ax=ax2)
sns.distplot(df['Height'], label='Height', ax=ax2)
ax2.legend()
# Plot system response
sns.distplot(df['Rings'], bins=18, ax=ax3)
It is worth noting that we also have a "Sex" column that indicates whether the abalone is a male, a female, or an infant. We would expect infants to be significantly different from adults, so we'll split the data into the infant and adult groups, and look at histograms for each.
inf_df = df[df['Sex']=='I']
ni_df = df[df['Sex']<>'I']
fig = plt.figure(figsize=(14,10))
ax1 = fig.add_subplot(231)
ax2 = fig.add_subplot(232)
ax3 = fig.add_subplot(233)
ax4 = fig.add_subplot(234)
ax5 = fig.add_subplot(235)
ax6 = fig.add_subplot(236)
# Non infant weight info
sns.distplot(ni_df['Whole weight'], label='Whole', ax=ax1)
sns.distplot(ni_df['Shucked weight'], label='Shucked', ax=ax1)
sns.distplot(ni_df['Viscera weight'], label='Viscera', ax=ax1)
sns.distplot(ni_df['Shell weight'], label='Shell', ax=ax1)
ax1.legend()
ax1.set_title('Non-Infant Weights')
# Infant weight info
sns.distplot(inf_df['Whole weight'], label='Whole', ax=ax4)
sns.distplot(inf_df['Shucked weight'], label='Shucked', ax=ax4)
sns.distplot(inf_df['Viscera weight'], label='Viscera', ax=ax4)
sns.distplot(inf_df['Shell weight'], label='Shell', ax=ax4)
ax4.set_title('Infant Weights')
# Non-infant growth
sns.distplot(ni_df['Length'], label='Length', ax=ax2)
sns.distplot(ni_df['Diameter'], label='Diameter', ax=ax2)
sns.distplot(ni_df['Height'], label='Height', ax=ax2)
ax2.set_title('Non-Infant Growth')
ax2.legend()
# Infant growth
sns.distplot(inf_df['Length'], label='Length', ax=ax5)
sns.distplot(inf_df['Diameter'], label='Diameter', ax=ax5)
sns.distplot(inf_df['Height'], label='Height', ax=ax5)
ax5.set_title('Infant Growth')
# Plot system response
sns.distplot(ni_df['Rings'], bins=18, ax=ax3)
ax3.set_title('Non-Infant Rings')
sns.distplot(inf_df['Rings'], bins=18, ax=ax6)
ax6.set_title('Infant Rings')
ax1.set_xlabel('')
ax2.set_xlabel('')
ax3.set_xlabel('Rings')
ax4.set_xlabel('')
ax5.set_xlabel('')
ax6.set_xlabel('Rings')
Here are a few pieces of information we can glean from these distributions.
Weight distributions:
Length, height, and diameter distribution:
Infant vs. adult:
We can also explore variable transforms to see if there is a more appropriate way to look at the input parameters. Here, we try taking the log or the exponential of a quantity:
fig = plt.figure(figsize=(14,4))
ax1 = fig.add_subplot(131)
ax2 = fig.add_subplot(132)
ax3 = fig.add_subplot(133)
sns.distplot(ni_df['Length'].apply(lambda x : np.log10(x)), label='Length', ax=ax1)
sns.distplot(ni_df['Diameter'].apply(lambda x : np.log10(x)), label='Diameter', ax=ax1)
ax1.set_title('Log Length and Log Diam')
sns.distplot(ni_df['Length'], label='Length', ax=ax2)
sns.distplot(ni_df['Diameter'], label='Diameter', ax=ax2)
ax2.set_title('Length and Diam')
sns.distplot(ni_df['Length'].apply(lambda x : np.exp(x)), label='Length', ax=ax3)
sns.distplot(ni_df['Diameter'].apply(lambda x : np.exp(x)), label='Diameter', ax=ax3)
ax3.set_title('Exp Length and Exp Diam')
ax1.legend(loc='best')
plt.show()
None of these distributions indicate that any particular transform would work better than the original quantity, so we'll leave height and diameter alone for now.
If we look at how different variables correlate with one another, it may be possible to find a useful combination of variables.
For example, suppose we want to correlate the measured dimensions (height, length, and diameter) to the weight of the organism. Because height, length, and diameter all have units of length, the product of all three of these would give a quantity with units of length cubed, or volume. This approximate volume of the orgnaism should correlate with the weight of the organism - the slope of volume (x) vs. weight (y) would have a slope equal to the density.
Therefore, for an abalone, the volume is proportional to the length times diameter times height,
$$ V \sim L \times D \times H $$Looking at abalone shells, they are shaped like an oval bowl, with the height indicating the depth of the bowl. The shell's circular area can be computed from the area of an ellipse, which is $\pi a b$, where $a$ and $b$ are the major and minor axes. In the case of an abalone the major axis is proportional to the length, while the minor axis is proportional to the diameter.
ni_df = ni_df[ni_df['Height']>0]
inf_df = inf_df[inf_df['Height']>0]
ni_df.loc[:,'Volume'] = ni_df['Length'].values*ni_df['Diameter'].values*ni_df['Height'].values
inf_df.loc[:,'Volume'] = inf_df['Length'].values*inf_df['Diameter'].values*inf_df['Height'].values
fig = plt.figure(figsize=(14,4))
ax1 = fig.add_subplot(131)
ax2 = fig.add_subplot(132)
ax3 = fig.add_subplot(133)
ax1.plot(ni_df['Volume'], ni_df['Viscera weight'],'b*', color=sns.xkcd_rgb['dusty red'])
ax2.plot(ni_df['Volume'], ni_df['Shell weight'],'g*', color=sns.xkcd_rgb['cornflower'])
ax3.plot(ni_df['Volume'], ni_df['Shucked weight'],'*', color=sns.xkcd_rgb['dusty purple'])
ax1.set_xlabel('Volume')
ax2.set_xlabel('Volume')
ax3.set_xlabel('Volume')
ax1.set_ylabel('Viscera weight')
ax2.set_ylabel('Shell weight')
ax3.set_ylabel('Shucked weight')
ax2.set_title('Adult Abalones')
fig = plt.figure(figsize=(14,4))
ax1 = fig.add_subplot(131)
ax2 = fig.add_subplot(132)
ax3 = fig.add_subplot(133)
ax1.plot(inf_df['Volume'], inf_df['Viscera weight'],'b*', color=sns.xkcd_rgb['denim blue'])
ax2.plot(inf_df['Volume'], inf_df['Shell weight'],'g*', color=sns.xkcd_rgb['dusty green'])
ax3.plot(inf_df['Volume'], inf_df['Shucked weight'],'*', color=sns.xkcd_rgb['mauve'])
ax1.set_xlabel('Volume')
ax2.set_xlabel('Volume')
ax3.set_xlabel('Volume')
ax1.set_ylabel('Viscera weight')
ax2.set_ylabel('Shell weight')
ax3.set_ylabel('Shucked weight')
ax2.set_title('Infant Abalones')
From the plots above, it looks like adult abalones have a strong correlation between the "volume" and the viscera weight. Infant abalones, on the other hand, have a strong correlation between the volume and the shell weight.
The plots above can help to identify outliers - abalones whose volume is abnormally high for their viscera or shell weights, or vice-versa. (It appears some abalones have extremely small volumes.)
If we regress the volume versus viscera weight, we'll get a line. If we then compute the residuals from this linear model, we can identify the major outliers, and use those to prune problematic points.
plt.plot(ni_df['Volume'], ni_df['Shell weight'],'b*', color=sns.xkcd_rgb['dusty red'])
plt.xlabel('Volume')
plt.ylabel('Shell weight')
plt.title('Adult Abalones')
plt.show()
X = ni_df['Volume']
Y = ni_df['Shell weight']
lin = sm.OLS(Y,X).fit()
lin.summary()
Yhat = lin.predict(ni_df['Volume'])
ni_df.loc[:,'Predicted shell weight'] = Yhat
ni_df.loc[:,'Residual'] = Y - Yhat
ni_df.loc[:,'MSE'] = (Y - Yhat)**2
plt.plot(ni_df['Volume'], ni_df['Shell weight'],'*', color=sns.xkcd_rgb['dusty red'])
plt.plot(ni_df['Volume'], Yhat,'-', color=sns.xkcd_rgb['carmine'])
plt.show()
MSE = ni_df['MSE']
fig = plt.figure(figsize=(4,4))
ax = fig.add_subplot(111)
stats.probplot(MSE, dist='norm', plot=ax)
plt.show()
ni_df.sort_values('MSE',ascending=False).head()
thresh = 0.5
new_ni_df = ni_df[ni_df['MSE'] < thresh]
records_removed = len(ni_df) - len(new_ni_df)
print "Number of data points removed: %d"%(records_removed)
print "%0.1f%% of data was removed"%((float(records_removed)/len(df))*100)
We can also do the same thing with data about infant abalones - removing outliers.
plt.plot(inf_df['Volume'], inf_df['Shell weight'],'b*', color=sns.xkcd_rgb['dusty blue'])
plt.xlabel('Volume')
plt.ylabel('Shell weight')
plt.title('Infant Abalones')
plt.show()
X = inf_df['Volume']
Y = inf_df['Shell weight']
lin2 = sm.OLS(Y,X).fit()
lin2.summary()
Yhat = lin2.predict(inf_df['Volume'])
inf_df.loc[:,'Predicted shell weight'] = Yhat
inf_df.loc[:,'Residual'] = Y - Yhat
inf_df.loc[:,'MSE'] = (Y - Yhat)**2
plt.plot(inf_df['Volume'], inf_df['Shell weight'],'*', color=sns.xkcd_rgb['dusty blue'])
plt.plot(inf_df['Volume'], Yhat,'-', color=sns.xkcd_rgb['light blue'])
plt.show()
MSE = inf_df['MSE']
fig = plt.figure(figsize=(4,4))
ax = fig.add_subplot(111)
stats.probplot(MSE, dist='norm', plot=ax)
plt.show()
inf_df.sort_values('MSE',ascending=False).head()
thresh = 0.05
new_inf_df = inf_df[inf_df['MSE'] < thresh]
records_removed = len(inf_df) - len(new_inf_df)
print "Number of data points removed: %d"%(records_removed)
print "%0.2f%% of data was removed"%((float(records_removed)/len(df))*100)
It is interesting to note that the linear regression of "volume" versus predicted shell weight has nearly the same slope between the infants and adults - 6.87 for infants, 6.69 for adults.
While the quantile plot shows that the trendline is not really linear, the fact that both infant and adult abalones had similar slopes is an indication that the general upward trend holds true across abalones of different ages, and the rate of growth does not slow down once the abalones reach adulthood.
We can wrap all of this functionality (loading the data, fitting volume versus weight, and removing outliers) in a function that can be used in other notebooks.
def abalone_load(data_file, infant=False):
# x data labels
xnlabs = ['Sex']
xqlabs = ['Length','Diameter','Height','Whole weight','Shucked weight','Viscera weight','Shell weight']
xlabs = xnlabs + xqlabs
# y data labels
ylabs = ['Rings']
# data
df = pd.read_csv(data_file, header=None, sep=' ', names=xlabs+ylabs)
if(infant):
new_df = df[ df['Sex']=='I' ]
else:
new_df = df[ df['Sex']<>'I' ]
return new_df
def infant_abalone_load(data_file):
return abalone_load(data_file,True)
def adult_abalone_load(data_file):
return abalone_load(data_file,False)
def abalone_removeoutliers(df,mse_tol,verbose=False):
df.loc[:,'Volume'] = df['Length'].values*df['Diameter'].values*df['Height'].values
X = df['Volume']
Y = df['Shell weight']
lin = sm.OLS(Y,X).fit()
Yhat = lin.predict(df['Volume'])
df.loc[:,'Predicted shell weight'] = Yhat
df.loc[:,'Residual'] = Y - Yhat
df.loc[:,'MSE'] = (Y - Yhat)**2
MSE = df['MSE']
thresh = 0.5
new_df = df[df['MSE'] < thresh]
records_removed = len(df) - len(new_df)
if(verbose):
print "Number of data points removed: %d"%(records_removed)
print "%0.2f%% of data was removed"%((float(records_removed)/len(df))*100)
del df['Predicted shell weight']
del df['Residual']
del df['MSE']
return df
def infant_abalone_removeoutliers(df):
return abalone_removeoutliers(df,0.5)
def adult_abalone_removeoutliers(df):
return abalone_removeoutliers(df,1.0)
my_inf_df = infant_abalone_removeoutliers(infant_abalone_load('abalone/Dataset.data'))


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John Garo, Role = Guest Speaker


ENTRAPMENT
Reviewed by Harvey Karten, Ph.D. 20th Century Fox Director: Jon Amiel Writer: Ron Bass and William Broyles; Ron Bass and Michael Hertzberg (story) Cast: Sean Connery, Catherine Zeta-Jones, Will Patton, Maury Chaykin, Ving Rhames, Kevin McNally, Terr O'Neill, Madhav Sharma, David Yip, Tim Potter, Eric Meyers, Aaron Swartz, William Marsh, Tony Xu, Rolf Saxon
One way that critics' opinions of movies often differ from those of fans is that regular folks are often content with excitement and romance while reviewers are obsessed with originality and believability. "Entrapment" has been getting mixed notices, with many critics complaining that little is credible, while vast crowds of moviegoers credit the film for its style. Surprisingly, Roger Ebert goes along with the latter group, saying in his review that though "Entrapment" has a "preposterous plot [there is] so much chemistry between attractive actors that we don't care....I didn't believe a second of it, and I didn't care that I didn't." The Great Man is on the money this time: "Entrapment," which recalls stylish vehicles like "Topkapi" and "To Catch a Thief," is neither original nor plausible, but then, is anything done by the successful James Bond series feasible? Logical action is not the point with such a genre. Technique is everything, and this movie is adept in various spheres. Note Phil Meheux's startling photography (especially the night scenes and the vista that contrasts a dirt-poor Malaysian neighborhood with the high- rise palaces of Kuala Lumpur's business sector). Let the special chemistry between its two principal performers register: director John Amiel will have you wondering whether the 69-year-old Sean Connery's attention to the 29-year-old Catherine Zeta-Jones is sexual or paternal.
Sean Connery (who could still play Bond, for my money) takes on the role of Mac, a wealthy thief who now steals not for the money but for the excitement. With a particular expertise in making off with the works of the masters in art museums, he turns his skills to stealing a Chinese mask. When Gin (Catherine Zeta-Jones), an insurance investigator, seeks to entrap him by tempting him to take on a daring assignment, Mac at first does not trust her but agrees to make her a partner in the theft of a $40 million Chinese mask on exhibit in Scotland. With his partner Thibadeaux (Ving Rhames), he is later to move on to the attempt the biggest haul in history: the lifting of eight billion dollars in corporate deposits, while Gin's boss, Hector Cruz (Will Patton) ventures to capture him.
If you're wondering why Ms. Zeta-Jones is depicted in an acrobatic pose in the posters, the posture is not simply an attention getter to entrap prospective viewers. While entering a museum, cat-like to avoid invisible laser beams seen only by Mac with a special instrument, Gin must bend and twist her curvaceous body lest a misstep of an inch set off alarms and foil the theft.
"Entrapment" engulfs the viewer in both its focus on the two attractive actors and in its photography of a series of capers including one in which Mac dangles from a 70-story building while opening a security system. While younger fans (the movie is rated PG-13 because of its relative absence of violence) will be absorbed in the impressive stunt work, those of a romantic bent will be fascinated particularly by Catherine Zeta-Jones, who is not simply a knockout in the looks department but has smarts and spark to match.
Though "Entrapment" recycles some of the classics--its many clever twists conforming to the usual Hollywood playing-by-the-numbers--its exotic locales, clever repartee between actors of different generations, and breathtaking stunts give "Entrapment" a handsome look, a mischievous bearing, and a good time for its patrons.
Rated PG-13. Running Time: 113 minutes. (C) 1999 Harvey Karten
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Teaching Experience
Fall 2022
TA for DSC 291 - Interpretability and Explainability in Machine Learning
May 2011 – August 2013
Differential Calculus Tutor


Birthday Cake
问题描述 :
Ting-a-ling, the chef was called on by Remmarguts. “You must prepare an immense birthday cake for lovely Princess Uyuw in a single day,” said Remmarguts. Though Remmarguts’ order is outrageous, the chef eventually rushed to buy flour, sugar, fat, and some other ingredients.
There had been chaos caused by war for quite a long time. The price of everything has been highly raised. Being the head accountant of country UDF – United Delta of Freedom, you must weight the cake carefully to make sure the chef did not perform a cheat on the ingredients.
The cake is made up of N levels. There is a ‘cube’ in each level, while the length of cube on k-th level (count from the topmost) is exactly k! For Remmarguts lives in an M-Dimension world unlike our, you should notice that the ‘cube’ here means M-Dimension cube, and the volume of a cube with length k is k ^ M.
You are to calculate the total volume of such an immense cake.
输入:
输出:
样例输入:
2 3 3 6 5
样例输出:
36 12201
解题代码:
import java.io.*; import java.util.*; import java.math.*; /** * * @author gongshaoqing */ public class Main { private static int NULL=0; public static void main(String[] args) { Scanner cin = new Scanner(System.in); int i, j, t; int m; BigInteger N, b[][], c,ans,temp; b = new BigInteger[102][102]; b[1][1]=BigInteger.ONE; b[2][1]=BigInteger.ONE; b[2][2]=BigInteger.valueOf(2); for (i = 3; i <= 100; i++) { b[i][1]=BigInteger.ONE; for (j = 2; j <= i; j++) { if((i-1)< j)b[i-1][j]=BigInteger.ZERO; b[i][j]=b[i-1][j-1].add(b[i-1][j]); b[i][j]=b[i][j].multiply(BigInteger.valueOf(j)); } } /*for(i=1;i<=100;i++) { for(j=1;j<=i;j++) System.out.print(b[i][j]+" "); System.out.println(); }*/ t=cin.nextInt(); while(cin.hasNext()) { if(t==0)break; t--; N=cin.nextBigInteger(); m=cin.nextInt(); temp=N.add(BigInteger.ONE); ans=BigInteger.ZERO; for(i=1;i<=m;i++) { c=temp.multiply(N); temp=c.divide(BigInteger.valueOf(i+1)); c=temp.multiply(b[m][i]); ans=ans.add(c); N=N.subtract(BigInteger.ONE); if(N.compareTo(BigInteger.ZERO)==0) break; } System.out.println(ans); } // TODO code application logic here } }
确实有点难度，搞了好久。int溢出要注意
不错，再多来的CF上面的题
给力，赞一个
嗯，尽量吧。题目太多了，很多解题报告是用程序自动发布的，所以就只有代码了
说的就是无向图啊，有向图的算法也是类似的
Java真是解决大数的利器
这张页面太松散拉，重新编辑一下，弄紧凑一点。
mark, 备用
很有意思，可惜我很菜啊
哎，path[0]应该是从零开始吧，为什么是赋值1呢？
“可以发现,树将是满二叉树,”这句话不对吧，构造的树应该是“完全二叉树”，而非“满二叉树”。
全是智力分析的题
I like your publish. It is great to see you verbalize from the coronary heart and clarity on this essential subject matter can be easily noticed.