splice - splice data to/from a pipe
#define _GNU_SOURCE /* See feature_test_macros(7) */
#include <fcntl.h>
ssize_t splice(int fd_in, loff_t *off_in, int fd_out,
loff_t *off_out, size_t len, unsigned int flags);
splice() moves data between two file descriptors without copying between
kernel address space and user address space. It transfers up to len
bytes of data from the file descriptor fd_in to the file descriptor
fd_out, where one of the file descriptors must refer to a pipe.
The following semantics apply for fd_in and
off_in:
- If fd_in refers to a pipe, then off_in must be NULL.
- If fd_in does not refer to a pipe and off_in is NULL, then
bytes are read from fd_in starting from the file offset, and the
file offset is adjusted appropriately.
- If fd_in does not refer to a pipe and off_in is not NULL,
then off_in must point to a buffer which specifies the starting
offset from which bytes will be read from fd_in; in this case, the
file offset of fd_in is not changed.
Analogous statements apply for fd_out and
off_out.
The flags argument is a bit mask that is composed by ORing
together zero or more of the following values:
- SPLICE_F_MOVE
- Attempt to move pages instead of copying. This is only a hint to the
kernel: pages may still be copied if the kernel cannot move the pages from
the pipe, or if the pipe buffers don't refer to full pages. The initial
implementation of this flag was buggy: therefore starting in Linux 2.6.21
it is a no-op (but is still permitted in a splice() call); in the
future, a correct implementation may be restored.
- SPLICE_F_NONBLOCK
- Do not block on I/O. This makes the splice pipe operations nonblocking,
but splice() may nevertheless block because the file descriptors
that are spliced to/from may block (unless they have the O_NONBLOCK
flag set).
- SPLICE_F_MORE
- More data will be coming in a subsequent splice. This is a helpful hint
when the fd_out refers to a socket (see also the description of
MSG_MORE in send(2), and the description of TCP_CORK
in tcp(7)).
- SPLICE_F_GIFT
- Unused for splice(); see vmsplice(2).
Upon successful completion, splice() returns the number of bytes spliced
to or from the pipe.
A return value of 0 means end of input. If fd_in refers to
a pipe, then this means that there was no data to transfer, and it would not
make sense to block because there are no writers connected to the write end
of the pipe.
On error, splice() returns -1 and errno is set to
indicate the error.
- EAGAIN
- SPLICE_F_NONBLOCK was specified in flags or one of the file
descriptors had been marked as nonblocking (O_NONBLOCK), and
the operation would block.
- EBADF
- One or both file descriptors are not valid, or do not have proper
read-write mode.
- EINVAL
- The target filesystem doesn't support splicing.
- EINVAL
- The target file is opened in append mode.
- EINVAL
- Neither of the file descriptors refers to a pipe.
- EINVAL
- An offset was given for nonseekable device (e.g., a pipe).
- EINVAL
- fd_in and fd_out refer to the same pipe.
- ENOMEM
- Out of memory.
- ESPIPE
- Either off_in or off_out was not NULL, but the corresponding
file descriptor refers to a pipe.
The splice() system call first appeared in Linux 2.6.17; library support
was added to glibc in version 2.5.
This system call is Linux-specific.
The three system calls splice(), vmsplice(2), and tee(2),
provide user-space programs with full control over an arbitrary kernel buffer,
implemented within the kernel using the same type of buffer that is used for a
pipe. In overview, these system calls perform the following tasks:
- splice()
- moves data from the buffer to an arbitrary file descriptor, or vice versa,
or from one buffer to another.
- tee(2)
- "copies" the data from one buffer to another.
- vmsplice(2)
- "copies" data from user space into the buffer.
Though we talk of copying, actual copies are generally avoided.
The kernel does this by implementing a pipe buffer as a set of
reference-counted pointers to pages of kernel memory. The kernel creates
"copies" of pages in a buffer by creating new pointers (for the
output buffer) referring to the pages, and increasing the reference counts
for the pages: only pointers are copied, not the pages of the buffer.
In Linux 2.6.30 and earlier, exactly one of fd_in and
fd_out was required to be a pipe. Since Linux 2.6.31, both arguments
may refer to pipes.
copy_file_range(2), sendfile(2), tee(2),
vmsplice(2), pipe(7)
This page is part of release 5.05 of the Linux man-pages project. A
description of the project, information about reporting bugs, and the latest
version of this page, can be found at https://www.kernel.org/doc/man-pages/.


I’m Building A Moat: Are You?
I’m Building A Moat. Are You?
In this weekly series, I opine on how words affect the way we understand the products and services around us. I do this for your entertainment and education (and, of course, to remind you that if you’re looking for a freelance copy, content, product, or technical writer… yada yada, hire me.
When I was young, my cousins and I oft played games of our own invention. These became staples of family holidays, and among the most memorable was “Leechers”.
The titular “Leechers” were an evil insectoid army that was perpetually trying to attack us in a bloodthirsty quest for our prized rations (white pizza and pizelle). As a team playing cooperatively, we’d scrounge up what we could in the house to build a base from within which we’d defend against the imagined assault.
Deciding how to build our fortifications strategically became the great joy of the game. We would dream up all sorts of creative uses for the couch cushions, coffee tables, and chairs around. We’d even build elaborate traps for these imaginary interlopers: blue-blanket moats abound.
You might then, as I do, find it fitting and ironic that even now I spend so much of my time still thinking about how to build a better moat.
Wait, What Are We Talking About?
Among the most important strategic considerations when trying to build a company or product is its “moat”.
Medieval castles were often enclosed by moats to defend against attackers. Crossing a moat would slow encroaching soldiers down enough for archers on the walls to pick them off more easily.
Warren Buffet is oft attributed as the most prominent drawer of said analogy to the world of business. In choosing investments, he looks for an “economic moat”, which is described as a business’ “competitive advantages [that can] protect its long-term profits and market share from competing firms”.
What Happens
There are many popular examples of strong economic moats in massive companies (such as McDonald’s food buying power, Apple’s immense supply chain and Amazon’s astronomical operational infrastructure). Of course, when you’re that massive, your size and scale is moat enough alone.
Yet, even for the tiniest of start-ups, I would argue that deliberately planning or building a moat from day one can be the deciding factor in whether you ever get that massive.
One pertinent present-day example of note is the rise of the machine learning start-ups who are beginning to take the business world by storm — each with its own exemplary moat in the making.
Generally speaking, machine learning systems become more effective over time. And even in the very SalesForce-clad CRM space, a new wave of disruption looms on the back of this new approach.
Fledgling players like Nudge.ai and Introhive have launched increasingly-popular tools that are built atop machine learning systems which, over time, will become harder to displace as the machines learn.
If these start-ups are successful building out a repeatable sales process while continuing to improve the underlying learning models, their learning data will become an incredibly effective moat.
The Result
Yet, moats need not be technical or product-related: they simply need to be hard to replicate and overcome.
FreshBooks’ customer support strategy, for example, is a great example of a well-conceived moat that has nothing to do with product.
Not only does the company have a large support staff to which affords great latitude in pleasing customers, but every single new employee spends the entire first month building empathy and helping customers by answering phone calls and emails. Plus, its’ support systems, SLAs, and office hours are specifically designed to ensure every customer call is answered by a human well before 4 rings.
From the outset, the company invested significantly in support, and as a result it has developed a powerful reputation — one that every single new competitor (and even established incumbents) needs to rival in order to attract or retain customers that FreshBooks could otherwise serve.
As a result, many choose FreshBooks for its support alone — even when there are countless competitive products across the price-to-potency spectrum.
I may be a touch biased, but the effect of its moat speaks for itself. Many of the 10 million people who’ve used FreshBooks since the company launched more than a decade ago have great things to say about the company, and its growth and success reflect that.
The Takeaway
So how do you build your own moat? There’s no simple answer, but I’m trying something specific with my own freelance business.
I’ve established a client policy that I’m deliberately enforcing during pre-sales as part of my moat. I never take on a client that won’t provide recurring business, even if that recurring business isn’t particularly lucrative.
How does that help my build a moat, you ask? You’re probably thinking that sounds more like a matter of cash flow and time management. And while those are indeed ancillary benefits, the main reason I’m taking this approach is so that I can develop a deep understanding of my client’s businesses.
As I work entirely with established businesses, I’ve learned over the last 10 years that businesses working with freelancers often have a difficult hurdle to overcome. By taking work outside, these businesses run the risk of hiring contractors who don’t know their product or their people or their prospects well enough to represent the company successfully — and who don’t necessarily care enough to develop that understanding and empathy.
Many businesses, then, use freelancers only as gap-fills until they can hire full-time staff or for lesser tasks which aren’t as strategic.
Thus, by having fewer clients but going deeper with those that I do have, I create a win-win situation for both parties:
- I become a more efficient freelancer by developing better context and a deeper understanding of their goals, their products, and their pains, which allows me to produce better, faster, and frequently
- They begin to get more ROI for their investment on freelancing and can keep less employee cost on their books without losing any of the dependability and deep contextual awareness.
This understanding — a direct result of the policy — is an effective moat. A new freelancer would have to get up to speed and build the same deep understanding and commitment to the business I have in order to win it.
It’s not a radically sophisticated strategy by any stretch, but by being aware of the need to build a moat, I force myself to be more deliberate and strategic in the way I run my business, which will increase long-term chance of success.
TL;DR
Building a moat that competitors can’t easily cross should be an important part of your business strategy.
If you’re building product, be aware that you need more than just a novel user experience and a whiz-bang UI to last. If you’re delivering a service, understand where to spend your time in order to keep that customer in the future.
What about you? Agree? Disagree? Respond away. And if you’d like to learn more about me or my business, visit http://www.frankcaron.com.


Survey
About Yo
u
Name(required)
Link to Photo Image (Required)
Question 1
Q1
Question 2
Q2
Question 3
Q3
Question 4
Q4
Question 5
Q5
Question 6
You find it easy to stay relaxed and focused even when there is some pressure.
Question 7
Get this payload moving already!
Question 8
It's acurate to say that you're not a salty player.

Question 10
Competitive is where you go all out.


There are kids today in this country who go without student lunches. Our
mission is to bring that number down to zero. We provide an efficient method for schools to broadcast the needs of
their students by declaring a monetary goal that they need to reach in order to provide lunches for any students that
may not have the necessary means to obtain one.
Values
We believe every child has the right to a nutritious lunch. Food is not only vital
to a child's learning capacity but lunchtime plays a vast role on a child's social interaction with other
students. Research demonstrates that school meal programs play an important role in supporting obesity prevention,
overall student health and academic achievement by improving children’s diets and combatting hunger.
Make a Difference
Displaying our need for donations is admitting that we have a problem with our
current meal programs in school. We are constantly rallying for an increased funding for these programs but
until then we need your help. Make a difference in a child's health and future by providing them with
necessities that need to succeed.
According to USDA, the new regulations added 10 cents to the cost of preparing every school lunch and 27 cents
for every breakfast. To help schools meet the rules, Congress provided school meal programs
only 6 additional cents for each lunch and no additional funds for breakfast.
A study found that, on average, the full cost to produce a reimbursable school lunch was $2.91, exceeding the free lunch subsidy, which
at the time of the study was conducted, was $2.51. To boost operational revenue, many school meal programs rely on a la carte sales,
provide catering services or contract with community programs
Children from families with incomes at or below 130% of the poverty level are eligible for free school meals.
Those with incomes between 130% and 185% of the poverty level are eligible for reduced price meals
(student pays 30 cents for breakfast and 40 cents for lunch). For the 2018-19 school year, 130% of the poverty level
is $32,630 for a family of four and 185% is $46,435.


Our Product Quality is Top of the class. we provide world class after sale services. Performance wise we make sure you get the expected results on time. We get educated and experienced Engineers for you.
We accept payment by so many methods like pay by cheque, Bank Transfer, Credit Cards, Debit Cards, Payumoney, Bank Wire, Cash Deposit on bank account, Online Bank Transfer (NEFT), Western Union,
We are available to help you whole day in different time zones of the world. So don't check world clock, just ring us or come on our live chat. And mind you, our chat really works and gets answered.
A.V. Kitchens India Is one of the leading commercial food service equipment Importer and supplier in India. A team of professionals who has vast experience and in-depth knowledge of the Hospitality Industry & who can better understand about the customers needs and their priorities.
AV KITCHEN INDIAN is one of the largest Supplier, Exporter and Importer of Commercial Kitchen, Refrigeration, Bakery
Equipment’s in India. AVKI specializes in providing total solutions - including consultancy, designing, layout plans with
complete technical details of F & B Equipment’s for Commercial Kitchens, Canteens, Bakeries & Messes etc. on turnkey
project as well as individual product basis. Our services also extend to designing, layouts and installation of Exhaust and
Fresh Air systems as well as L.P.G pipeline for safety and economy of the project. AVKI has been associated with
Kitchen Equipment industry for well over two decades, and successfully providing our expertise to Hospitality Industry,
Hotels, Restaurants, Banquet Halls, Residential Schools, Learning Institutes, Hospitals, Messes of Armed Forces,
Industrial Canteens, Clubs, Cafeterias etc in India as well as in other countries.
AVKI corporate policy is to provide best Quality Products, Prompt Service and Timely Execution of projects / delivery of products to our customers at all times. These are watchwords in AVKI and no deviation of any kind is tolerated in this regard. Management and workforce of AVKI is constantly engaged in upgrading new generation technological changes as per the requirement of the times. AVKI products are superior in technology and performance due to this policy and strict Quality Controls and R &D practiced in the manufacturing units.
AVKI has one manufacturing units in Delhi, well equipped with latest state of the art plant and machinery to produce large volumes of Kitchen Equipments as per design, specifications and requirements of the customers.
AVKI has a very wide and strong Marketing / Servicing network throughout India. This network is controlled by a very experienced, dedicated and totally professional team, to satisfy our customers in all respects.
AVKI is proud to have a long list of satisfied customers from all across the spectrum of the industry we are presently working with.
All the departments are being headed by veterans experienced & competent in their respective fields & all the operations are being headed chaired & guided by our C.E.O. Thus, after the years we have earned our name & fame through quality products through very sophisticated, modern & progressive’s man, machine & working gears.


Test Form
User List
| First Name | Last Name | Address | Contact | Edit | Delete | ||
|---|---|---|---|---|---|---|---|
| Mohsin | Irshad | CB 106/107 Street # 11 Wah Cantt Islamabad Pakistan |<EMAIL_ADDRESS>| +923335586757 |
|
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| Mohsin | Irshad | CB 106/107 Street # 11 Wah Cantt Islamabad Pakistan |<EMAIL_ADDRESS>| +923335586757 |
|
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|
| Mohsin | Irshad | CB 106/107 Street # 11 Wah Cantt Islamabad Pakistan |<EMAIL_ADDRESS>| +923335586757 |
|
|
|
| Mohsin | Irshad | CB 106/107 Street # 11 Wah Cantt Islamabad Pakistan |<EMAIL_ADDRESS>| +923335586757 |
|
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| Mohsin | Irshad | CB 106/107 Street # 11 Wah Cantt Islamabad Pakistan |<EMAIL_ADDRESS>| +923335586757 |
|
|


Test sample WSDL mapping 1
|
| include |
testSetup.html |
|
| jsxopen |
${GIPATH}/shell.html?jsxapppath=${SAMPLESPATH}/WSDL_Mapping_1
|
// WSDL_Mapping_1 now run in static mode |
| waitForJsxButtonPresent |
Find City and State |
5000 |
| assertJsxButtonPresent |
Find City and State |
|
| assertElementPresent |
gi=zip |
|
| assertValue |
gi=zip |
|
| typeJsxTextbox |
gi=zip |
94304 |
| assertValue |
gi=zip |
94304 |
| clickJsxElement |
gi=lookupButton |
|
| waitForElementPresent |
css=.jsx30windowbar:contains("Success") |
|
| assertJsxAlertOK |
*success* |
|
| assertValue |
gi=state |
CA |
| assertValue |
gi=city |
PALO ALTO |
| clickJsxElement |
gi=buttonCounty |
|
| waitForElementPresent |
css=.jsx30windowbar:contains("Server alert box showing county")
|
|
| assertJsxAlertOK |
*SANTA CLARA* |
|


{% load static %}
Aimed at providing a "user-friendly" expierence,allowing the user to interact with the software in a natural and intuitive way.
The fastest platform in the market to download videos with an amazing response time.
Fast and efficient converter of videos into multiple formats.
Youtube is the most popular video-sharing platform in the world and the option of downloading a video is not provided by Youtube.Y-Link is an application which is dedicated to the task of downloading video files from Youtube. Y-Link can be used to download any Youtube videos in any given format. The videos could be easily converted from one format to another based on the user’s requirement. An easy-to-use user interface has been provided with the help of which users can easily download required videos onto their personal devices.
This is an amazing application that has helped me download HD pubg videos and has saved a lot of time in converting the various formats of the videos..
Y-LINK ROCKS!!...Simply the best downloader and converter out there.


This resolver is part of Project ReShare, a fully open, community-led initiative to develop an interoperable resource-sharing platform that any library can use irrespective of its choice of ILS. Note that it is in development and has a long way to go.
The resolver accepts OpenURL requests and converts them into ReShare requests which it pushes into an instance of mod-rs running within the FOLIO platform. Consequently, the outcome of making a request to it is not a link to an immediately available electronic copy of the nominated resource, but that an ILL request to a suitable library is initiated.
As a result, to the untrained eye, the pages that display on submitting an OpenURL are low on information. But to the eye that has brains, they are letting the user know that work is under way to supply the resource.
Note that the result pages, like this page, are deliberately spartan. Styling will come later in the project.
The form is hardwired to link to http://openurl.indexdata.com/US-EAST. [Link]
In case you're interested, the code is on GitHub.
The following files consitute a minimal configuration to enable this in-development OpenURL resolver to be used by Google Scholar, in accordance with the instructions. We have requested integration.


Reduct.Video
Video & transcription editing simplified
Reduct.Video is a video editing & transcription startup in San Francisco. With Reduct, editing video is as easy as writing a text document. Highlight, cut, and edit text to watch as your video automatically does the same to the video.
During my time designing for Reduct.Video, I was required to wear many hats, ranging from marketing and pitch deck creation, to fast paced product design sprints, including the launch of many products that decreased overall user friction and defined early stage visual style. This is a sample of two primary projects I worked on, the redesign of their All Projects Page, as well as visual and interaction concepts for their main app interface.
01
All Projects Page redesign
The All Projects Page, Reduct’s highest level of navigation in the app, is where researchers can view and join any project in their organization. The current interface looked nice visually, but was reportedly lacking in usefulness and clarity from researchers. The team of three at Reduct began the project with a hypothesis that researchers using Reduct are active in all parts of the app at any given time over the course of the project. The All Projects Page should be able to access the part of the project they were working on in less than two clicks. To address that, we made three buttons at the highest level of hierarchy so researchers wouldn’t be funneled into a single flow.
The final result was a dashboard-like display of all the important information in a project, such as recent activity and number of interviews. The new page was shipped after a 4 week sprint. When looking at the usage data after launch, the most clicked links on the page were the three entry points: Interviews, Highlights, Reels, on the page——validating our original hypothesis.
Live version as of February 2020.
All projects page drafts
Our primary assumption with our first draft of the all projects page, the highest level of navigation, was to create a way for researchers to access any primary function with two clicks maximum. We created three CTA buttons leading to Interviews, Reels, and Highlights from the page as the main access point.
The second draft focused on visual clean up and applying the existing brand to the All Projects Page. The addition of the brand’s signature green indicated to researchers their primary actions on the screen.
02
Transcript page concept screens
Entering their pre-seed round, Reduct still has so much potential to define their product in the company’s early stages. As the only designer at Reduct, The team and I wanted to create future concepts for what the transcript page, the main app page where researchers can edit their transcriptions, could look like with prospective features and a cohesive visual style. The initial layout was conceived and tested with customers to prove usability, and visuals were created and finalized through various feedback sessions.
The three-panel interface for the redesigned transcript page. The left panel is for video editing, the center panel is for editing the transcription, and the right panel is for tagging and storing highlights from the transcript.
The reels page is where researchers can assemble their highlighted transcript clips into a new video for share-outs or insights.
Transcript page drafts
To start this project, I defined the information hierarchy with a participatory exercise involving how much real estate a piece of information gets on the screen. A helpful way to rephrase the question was, “how important is this piece of information for researchers to see?” When creating the initial drafts, this template was the central reference point.
First draft.
Second draft.
Proposed mockup.


The Elastic Chain
Contents
Reading: (Coleman, 2015), Chapter 2.
The Classical System
We study a chain of equal masses connected by springs, moving only in one dimension, along the chain. The Hamiltonian is
We identify $u_j=u_{N+j}$, corresponding to periodic boundary conditions. As usual $[u_i,p_j]=i\delta_{ij}$. To orient ourselves, we solve the classical version of the problem.
Equations of Motion
You’ve seen this before. The equations of motion are
We look for oscillatory solutions with time dependence $u_j(t) = u_j e^{-i\omega t}$, arriving at the matrix eigenvalue problem
Matrices of this type are called circulant matrices, and arise here because of the translational invariance of the system (including the periodic boundary conditions). Their eigenvectors are given by plane waves $u_j = (z_n)^j$, where $z_n$ is one of the $N^\text{th}$ roots of unity i.e. $z^N = 1$ or
In fact, to make things a bit more symmetrical, let’s take $N$ to be odd and index the $z_n$ using both positive and negative values of $n$
We’ll write $\eta_n\equiv \frac{2\pi n}{N}$, so that the eigenstates have the form $u_j=\exp(i\eta_n j)$.
Notice that:
- The frequency vanishes at $\eta\to 0$. This mode corresponds to translation of the system, for which there is no restoring force.
- At small $\eta$ the dispersion is linear, as we would expect for sound waves.
A general motion of the system can be represented as a superposition of the normal modes
together with the condition $q_{-n}=q^*_n$ on the complex amplitudes to ensure that $u_j$ is real. The amplitudes $q_n(t)$ have time dependence
for $n\neq 0$, while for $n=0$
describes the motion of the centre of mass.
Hamiltonian Formulation
To make contact with quantum physics, let’s look at this problem from the Hamiltonian perspective. If the $q_n$ are to be our canonical coordinates, then we should likewise write the momenta in terms of Fourier modes
If $u_j$, $p_j$ are canonical variables with Poisson Bracket $\{u_j, p_k\}=\delta_{jk}$, then it follows that $\{q_m,\pi_n\}=\delta_{mn}$.
This almost looks like a system of harmonic oscillators. Bear in mind that the $q_n$ and $\pi_n$ are complex. One could, for example, split the amplitudes into their real and imaginary parts
The Hamiltonian would then become $H=H’ + H’’$ with
and similarly for $H’’$. By comparing with the standard form
we can read off the dispersion relation \eqref{coll_Dispersion}. The decomposition \eqref{coll_RandI} amounts to working with the real amplitudes of sine and cosine waves. Other options are possible.
Complex Coordinates
Sticking with the classical problem, let’s introduce complex coordinates to describe the two dimensional phase space of a single oscillator
$a$ and its conjugate satisfy $\{a^{},a^*\}=-i$. This definition is chosen so that the Hamiltonian takes the simple form
Hamilton’s equations of motion are then
with solution $a(t) = e^{-i\omega t} a(0)$ describing circular motion in the complex $a$ plane on a contour of fixed energy.
In the same way, we can introduce the coordinates
Remember that $q_n = q_{-n}^*$ and $\pi_n = \pi_{-n}^*$ in order that $u_j$ and $p_j$ are real. Note that $n=0$ is excluded because $\omega(0)=0$. These coordinates satisfy
Inverting the definition \eqref{coll_adef} gives
and inserting into the Hamiltonian \eqref{coll_HDiag} gives
with the first term accounting for the (free) centre of mass.
Quantum Oscillators
In the quantum theory, the variables $\aop$, $\adop$ satisfy $[\aop,\adop]=1$ and the Hamiltonian \eqref{coll_SHO} takes the form
Let’s remind ourselves how this formalism solves the problem of finding the eigenstates. The key observation is that
As a result, if $\ket{\psi}$ is an eigenstate of the Hamiltonian
then $\adop\ket{\psi}$ is an eigenstate with energy $E+\omega$
Similarly $a\ket{\psi}$ is an eigenstate with energy $E-\omega$, unless $\ket{\psi}=\ket{0}$, the ground state, in which case we must have $\aop\ket{0}=0$.
As a result, all states can be written as
The factor of $\frac{1}{\sqrt{n!}}$ normalizes the state. The ground state has energy $E_0=\omega/2$.
The Quantum Chain
The quantization of the chain is then a piece of cake. We have a system of oscillator variables satisfying $[\aop_m,\adop_n]=\delta_{mn}$, and writing the Hamiltonian \eqref{coll_HDiag} in terms of these variables, paying attention to the order, gives
From now on we will ignore the centre of mass motion. Exactly the same logic as before tells us that a general energy eigenstate may be written
The non-negative integers $\mathbf{N}=\left(N_{(1-N)/2},\ldots, N_{-1}, N_{1}, \ldots N_{(N-1)/2}\right)$ describe the occupation numbers of the oscillators. This eigenstate has energy
where the ground state energy is
Oscillator Quanta are Bosons!
A key moment in the birth of Quantum Field Theory was the realization that oscillator quanta are bosons, meaning that they can be identified with quantum particles having symmetric wavefunctions. We’ll see this in much more detail in later lectures. For the moment, let’s just note that both have a basis of states described in terms of the occupation numbers, which are non-negative integers. In the case of $M$ bosons, those states were written in terms of the single particle wavefunctions $\varphi_\alpha(\br)$ of the bosons as
where $\mathcal{S}=\frac{1}{M!}\sum_{P} P$ is the operation of symmetrization, and $N_\alpha$ denotes the number of occurrences of $\varphi_\alpha(\br)$ in the product, so that $M=\sum_\alpha N_\alpha$. It turns out that the Hilbert space spanned by these states is the same as that spanned by the states $\ket{\mathbf{N}}$, if the labels $\alpha$ are identified with the momentum labels $n$.
It’s important to note that these bosons are totally distinct from the original particles making up the chain. In fact, our original Hamiltonian \eqref{coll_Hchain} doesn’t describe indistinguishable particles as written, as each particle is labelled by its position in the chain, with a particle only interacting with its two neighbours. Since the particles are assumed not to change places, there is no way of assigning statistics to their wavefunction.
Thermodynamic ($N\to \infty$) limit
In studying the properties of matter, we are usually interested in taking the limit of an infinite system, otherwise known as the $N\to\infty$ or thermodynamic limit. At the very least, we expect the internal energy (as well as other thermodynamic potentials) to be an extensive quantity, meaning that it is proportional to the `size’ of the system, here measured by the number of sites. Thus we expect the limit
to exist. The separation of the $\eta_n$ values is $2\pi/N$, so as $N\to\infty$ the sum in ground state energy \eqref{coll_H0} can be replaced with an integral according to the rule
The factor of $N$ tells us that we have an extensive quantity, and
Alternatively, we may treat the $N\to \infty$ limit of the chain as a model of an elastic continuum of length $L=aN$. Take $m = \rho a$, where $\rho$ is the mass per unit length (1D density). The 1D elastic modulus is
Then $k/m = \kappa/(\rho a^2)$ and
The energy per unit length diverges as $N\to\infty$. Thus the ground state energy of a continuous medium is infinite, on account of the infinite number of degrees of freedom it contains. This is only a problem if one insists on such a description: in practice (at least in condensed matter) there is always discreteness on the smallest scales.
Apart from the infinite ground state energy, the continuum limit of our harmonic system is perfectly well defined. Introducing a continuum displacement by $u(x=ja)=u_j$, the potential energy can be written
If we define the momentum density at each point by $\pi(x=ja) = p_j N/L$, then we find the continuum limit of the canonical commutation relations
together with the kinetic energy
Since we are taking the $N\to\infty$ limit it’s convenient to define the Fourier modes slightly differently
where $k_n =2\pi n/L$. Note that $k_n x = \eta_n j$. We are recycling the notation $u_n$ now that we have taken the limit.
If the momentum density $\pi(x)$ is then written
(This differs from \eqref{coll_Pexp} by $\pi_n\to \pi_n/\sqrt{N}$.) we have $\left[u_m,\pi_n\right]=\delta_{mn}$.
Our continuum Hamiltonian $H= T+V$ is then written in Fourier components as
We can now read off the dispersion relation
where $c=\sqrt{\frac{\kappa}{\rho}}$ is the speed of sound. Note that the continuum limit has lead to a linear dispersion relation. This is reasonable: the lattice was the origin of the periodic dispersion relation \eqref{coll_Dispersion}, and it has now disappeared.
Transcribing the definition of the oscillator variables \eqref{coll_adef} gives
where $Z\equiv\sqrt{\kappa\rho}$ is the impedance. After quantization, the Hamiltonian takes the form
This expresses the energy above the ground state in terms of the occupancy of the oscillator modes.
Finite Temperature
At finite temperature $T$ the occupancies of the modes have thermal averages given by the Bose occupation function
where $\beta=\frac{1}{k_\text{B}T}$. The thermal average of the energy of excited states is then
This is finite, even in the $N\to\infty$ limit, on account of the exponential tail of \eqref{coll_Bose}. Remember that this was the problem that the quantum theory was introduced to solve. At low energies $n_{\text{B}}(\omega) = \frac{1}{\beta\omega}$ and the contribution of each mode is
in agreement with the classical equipartition theorem. Were this result to apply at all energies the thermal energy density of a continuum at finite temperature would be infinite (the Ultraviolet Catastrophe). It is the existence of Planck’s constant, which appears in the dimensionless combination $\hbar\beta\omega$ in the Bose occupation function, that allows this conclusion to be avoided.
Position Fluctuations
Classically, the ground state configuration of our elastic chain corresponds to a regular ‘crystalline’ arrangement of masses at separation $a$, with all $u_j=0$. Mass $j$ and mass $k$ are then separated by $(j-k)a + u_j-u_k = (j-k)a$. Quantum mechanically, $u_j-u_k$ fluctuates, even in the ground state. For the notion of a crystal to make sense, these fluctuations should not be too large. Let’s evaluate them for the elastic chain.
We want to evaluate
To do this, we write the displacements in terms of the oscillator variables, and then evaluate the expectation values in the ground state using the oscillator algebra. Recall that
and
To evaluate \eqref{coll_gsfluct}, we write the two factors $(u_j-u_k)(u_j-u_k)$ in terms of the $\aop_n$ and $\adop_n$. Contributions to the ground state expectation value arise from terms with $\aop_n$ in the left factor and $\adop_n$ in the right for some $n$. All other terms vanish. This gives
Taking the $N\to\infty$ limit in the sum gives
The dispersion relation \eqref{coll_Dispersion} makes this integral a little difficult.
The integrand in \eqref{coll_uvar} for $j-k=20$. What form does it take for $\left|j-k\right|^{-1}\lesssim\eta\lesssim \pi$?
The result \eqref{coll_LogFluct} shows that the uncertainty in the separation of two masses in the chain increases with their separation. This implies that the ground state of the chain is not a crystal, but more closely resembles a fluid. It turns out that this conclusion depends strongly on the dimensionality of the system. In higher dimensions, crystalline ground states do exist (thankfully).
Density Fluctuations
An alternative way of quantifying crystalline order is to consider the fluctuations of the density of particles, defined by
where $x_j = ja + u_j$, and $\delta_L(x)$ is an $L$-periodic version of the $\delta$-function, if we want to stick with a finite size system. Alternatively, we may consider the Fourier components
Rather than introducing separate notation for the Fourier components of $f(x)$, it’s convenient to denote them by $f_q$, so that
In an ordered configuration $x_j = ja$, we would have
These peaks at values of $k$ corresponding to multiples of $\frac{2\pi}{a}$ are nothing but the Bragg peaks observed in a diffraction experiment, which translates the real space crystal arrangement into Fourier space. Note that an overall translation of lattice will just change the phase of the $ \rho_k$, leaving $\left|\rho_k\right|^2$ (proportional to the intensity measured in a diffraction experiment) unchanged.
How is this picture altered in the quantum mechanical ground state? Given the above comment, we should evaluate
Upon substituting the mode expansion \eqref{coll_ModeExp} for the displacements, we are left to evaluate expressions of the form
Deploying this strategy for \eqref{coll_Struct} gives
Numerical evaluation of $\bra{0} \rho_q \rho_{-q} \ket{0}$ for $\ell_\text{osc}/a=0.2$, $N=51$. Note that the second Bragg peak is hardly visible.
The second exponent modifies the classical prediction of Bragg peaks. We have encountered the expression in exponent before in \eqref{coll_uvar}. Taking the $N\to\infty$ limit with $\left|j-k\right|\gg 1$ as before, we find that in the vicinity of the first Bragg peak at $q=2\pi/a$ the summand has the form
where $\Delta q$ denotes the deviation of $q$ from $2\pi/a$. This leads to the conclusion
Thus quantum fluctuations replace the Bragg peaks, an indicator of crystalline order, with power law divergences. These remnants of order diminish as $\ell_\text{osc}/a$ increases, indicating larger quantum fluctuations. Again, things are different in higher dimensions: the Bragg peaks survive, albeit reduced in strength, at least for small fluctuations. It is possible, however, for quantum fluctuations to prevent crystallization in the ground state (i.e. at zero temperature). Such systems are called quantum liquids. Helium is the prototypical example: the low atomic mass and relatively weak interactions between atoms mean that quantum fluctuations are large.
Fourier review
This is a good place to collect some facts about Fourier transforms. We start from the discrete Fourier transform (DFT), which is a change of basis in a finite dimensional space. This is what we used in discussing the chain. There are then two ways to pass to the infinite continuous case described by the Fourier transform.
Discrete Fourier Transform
For a vector $x_j = 1,\ldots N$ ($N$ taken to be odd), we define the DFT by
where $\eta_n\equiv \frac{2\pi n}{N}$, and $n = -(N-1)/2,\ldots, (N-1)/2$. The key to inverting \eqref{coll_DFT} is the observation
This gives
A more democratic definition would have $1/\sqrt{N}$ in both definitions \eqref{coll_DFT} and \eqref{coll_IDFT}. This would allow us to regard the DFT as a basis change to an orthonormal basis of vectors $e^{(n)}_j = \frac{e^{i\eta_n j}}{\sqrt{N}}$, and both the DFT and its inverse would be unitary transformations.
$N\to\infty$ limit
In this limit the $\eta_n$ values become dense in the range $(-\pi,\pi]$, with separation $\Delta \eta = 2\pi/N$, and we replace the sum in the inverse DFT \eqref{coll_IDFT} by an integral according to the prescription
giving
$N\to\infty$, with $f_j = f(jL/N)$,
Alternatively, regard the $N\to\infty$ limit as sampling a function $f(x)$ ever more finely in the range (0,L]. Now it’s the DFT, rather than the inverse, that becomes an integral
where $k_n =2\pi n/L$. Note that $k_n x = \eta_n j$. The pair of transformations is now
This is the conventional form of the Fourier series for a function with period $L$.
With this definition $\hat f_k$ has an extra dimension of distance (on account of the integral), which gets removed by the $1/L$ in the inverse transform.
The analog of the identity \eqref{coll_DFTIdent} is
where $\delta_L(x)$ is an $L$-periodic version of the $\delta$-function.
$L\to\infty$
Finally we arrive at the Fourier transform, where we take $L\to\infty$, so that the inverse transform in \eqref{coll_FTSeries} becomes an integral too
My preference is for taking this limit at the last possible moment, that is, sticking with discrete Fourier sums for as long as possible. There are some good(ish) reasons for this
-
Writing $\sum_k$ is easier than $L\int \frac{dk}{2\pi}$, because the $k_n = 2\pi n/L$ can be left implicit.
-
Leaving $k$ as a subsript means we don’t need the tilde to distinguish $f(x)$ and $f_k$.
-
There are times where taking the limit leads to a divergent integral, while the sums remain finite. This almost always tells us that there is something interesting going on when we are trying to pass to an infinite system.
Properties of the Fourier Transform
Here are some properties that hold for all of the above.
-
If $f(x)$ is real $f_k = \left[f_{-k}\right]^*$.
-
If $f(x)$ is even, $f_k$ is even.
-
(Ergo) if $f(x)$ is real and even, so is $f_k$.
Fourier Transforms of Products
Frequently we have to transform products, so we use the convolution theorem
which shows us that
the latter being a discrete convolution.
Frequently we’ll have to calculate integrals of such products. I record some examples to give you the general idea
Note that you can be guided to the right number of factors of $1/L$ by dimensional considerations, or from the number of ‘free’ sums over wavevectors.
Finally, we often encounter the situation where we have two (or more) arguments, but there is only dependence on the difference, for example
In this case
In the $L\to\infty$ limit this is
$(2\pi)\delta(k+k’)$ is the $L\to\infty$ limit of $L\delta_{k,-k’}$ as
With practice, you will find you are able to write down the right hand sides of expressions like \eqref{coll_FTExamples} without too much difficulty.
Higher dimensions
This all generalizes to higher dimensions straightforwardly. For example
References
- Coleman, P. (2015). Introduction to many-body physics. Cambridge University Press.


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clipEdge
PURPOSE
CLIPEDGE clip an edge with a rectangular box
SYNOPSIS
function edge2 = clipEdge(edge, box)
DESCRIPTION
CROSS-REFERENCE INFORMATION
This function calls:
- createLine CREATELINE create a line with various inputs.
- intersectLineEdge INTERSECTLINEEDGE return intersection between a line and an edge
- linePosition LINEPOSITION return position of a point on a line
This function is called by:
- clipPolygon CLIPPOLYGON clip a polygon with a rectangular window
Generated on Fri 05-Feb-2010 11:20:41 by m2html © 2003


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MOROS is a hobby operating system written in Rust by Vincent Ollivier.
It targets computers with a x86-64 architecture and a BIOS, so mostly from 2005 to 2020, but it also runs well on most emulators (Bochs, QEMU, and VirtualBox).
MOROS is open source, you can build it or download an image. Consult the manual to learn how to use the system.
Everything in MOROS is done from a command line interface and most programs are rather minimalist.
It has a shell:
With a few programs like find
that use a regex engine to find
files or lines:
It has a calculator and also a lisp interpreter:
And a text editor:
It has a network stack with two drivers for RTL8139 and PCNET cards:
It has a chess game:
And the game of life:
It even has 2048:
And finally it is quite customizable:
You can log in to a demo with the following command using the name of the system as a password for the guest account:
$ ssh guest@try.moros.cc


In-browser encrypter / decrypter
Decrypt something someone sent me
Note: You kind of need my private key for this, so the decrypting won't work unless you're... me. Or have my private key. Which you hopepully shouldn't have.
Note: You kind of need my private key for this, so the decrypting won't work unless you're... me. Or have my private key. Which you hopepully shouldn't have.


The exam consists of a theory paper and a practical component.
Theory paper is given marks out of 100. Practical is either pass or fail.
This is how they should be categorized.
| Practical | Theory | Category |
|---|---|---|
| pass or fail | less than 35 | 1 |
| fail | 35 - 50 | 2 |
| pass | 35 - 50 | 3 |
| fail | above 50 | 4 |
| pass | above 50 | 5 |
Below is the trainig data set consisting of marks of 10 students.
| # | Theory | Practical | Category |
|---|---|---|---|
| {{$index}} | {{x}} | {{ps[$index]}} | {{ys[$index]+1}} |


For some use cases, it might be beneficial to use DOM as a source for suggestions.
The natural way to describe list of available suggestions is unordered or ordered list.


BayesClassifierMachine is the machine used by the BayesClassifier trainer to perform a Bayes Classification using different distributions.
Inheritance:
Public Fields
-
int n_trainers
- the number of classes corresponds to the number of Trainer
-
int n_outputs
- the number of outputs in this machine
-
EMTrainer** trainers
- the actual trainers (EMTrainer since we are training distributions)
-
real* log_priors
- the log_prior probabilities of each class.
-
Sequence* log_probabilities
- it contains the log posterior probability plus the log prior of the class
-
bool allocated_log_priors
- used to know if log_priors where given or allocated
-
ClassFormat* class_format
- the class format of the output
-
MeasurerList** trainers_measurers
- the measurers for each individual trainer
Public Methods
-
BayesClassifierMachine( EMTrainer**, int n_trainers_, MeasurerList** trainers_measurers_, ClassFormat* class_format_, real* log_priors_=NULL)
- creates a machine for BayesClassifier trainers, given a vector of trainers (one per class), an associate measurer for each trainer, a class_format that explains how the classes are coded, and an eventual vector (of size n_trainers_) containing the log of the class priors
-
virtual void forward(Sequence* inputs)
- definition of virtual functions of Machine
Inherited from Machine:
Public Fields
-
Sequence* outputs
Public Methods
-
virtual void reset()
-
virtual void setDataSet(DataSet* dataset_)
Inherited from Object:
Public Fields
-
Allocator* allocator
Public Methods
-
void addOption(const char* name, int size, void* ptr, const char* help="")
-
void addIOption(const char* name, int* ptr, int init_value, const char* help="")
-
void addROption(const char* name, real* ptr, real init_value, const char* help="")
-
void addBOption(const char* name, bool* ptr, bool init_value, const char* help="")
-
void addOOption(const char* name, Object** ptr, Object* init_value, const char* help="")
-
void setOption(const char* name, void* ptr)
-
void setIOption(const char* name, int option)
-
void setROption(const char* name, real option)
-
void setBOption(const char* name, bool option)
-
void setOOption(const char* name, Object* option)
-
virtual void loadXFile(XFile* file)
-
virtual void saveXFile(XFile* file)
-
void load(const char* filename)
-
void save(const char* filename)
-
void* operator new(size_t size, Allocator* allocator_=NULL)
-
void* operator new(size_t size, Allocator* allocator_, void* ptr_)
-
void operator delete(void* ptr)
Documentation
BayesClassifierMachine is the machine used by the BayesClassifier
trainer to perform a Bayes Classification using different distributions.
The output corresponds to the class that is the most probable
(using prior AND posterior information).
- int n_trainers
- the number of classes corresponds to the number of Trainer
- int n_outputs
- the number of outputs in this machine
- EMTrainer** trainers
- the actual trainers (EMTrainer since we are training distributions)
- real* log_priors
- the log_prior probabilities of each class. default: log_priors are
taken as the log of the proportions in the training set.
- Sequence* log_probabilities
- it contains the log posterior probability plus the log prior of the class
- bool allocated_log_priors
- used to know if log_priors where given or allocated
- ClassFormat* class_format
- the class format of the output
- MeasurerList** trainers_measurers
- the measurers for each individual trainer
- BayesClassifierMachine( EMTrainer**, int n_trainers_, MeasurerList** trainers_measurers_, ClassFormat* class_format_, real* log_priors_=NULL)
- creates a machine for BayesClassifier trainers, given a vector of
trainers (one per class), an associate measurer for each trainer,
a class_format that explains how the classes are coded, and an eventual
vector (of size n_trainers_) containing the log of the class priors
- virtual void forward(Sequence* inputs)
- definition of virtual functions of Machine
- This class has no child classes.
- Author:
- Samy Bengio<EMAIL_ADDRESS>Bison Ravi<EMAIL_ADDRESS>Alphabetic index HTML hierarchy of classes or Java
This page was generated with the help of DOC++.


| Ticker | Number of Shares | Buy Price ($ USD) | Total Cost ($ USD) | Current Price ($ USD) | Current Total Value ($ USD) | Actions | ||||
|---|---|---|---|---|---|---|---|---|---|---|
| There are no shares in the DB. Add a new share below. | ||||||||||
| {{share.shareticker}} | {{share.sharenumbers}} | ${{share.sharebuyprice}} | ${{share.sharebuyprice * share.sharenumbers}} | 0"> ${{share.closevalue}} | Loading... | N/A | 0"> ${{share.sharenumbers*share.closevalue}} | Loading... | N/A | |


just learned about saturation the hard way:
i play with current measurement, CT N ( turns) and burden resistor and i run into that problem.
Background: for a given current transformer if the burden resistor is to high and the primary current to high
the CT goes into saturation. ( can find lots of references here too, but interesting to read www.idc-online.com/technical_references/pdfs/electrical_engineering/current_transformer_concepts.pdf )
Symtoms for CT in saturation:
- for calibrating EMON by a low current get a ICAL factor.
but when you test it with a high current need a ICAL factor twice or more
- when calibrating PhaseCAL to get p=1.0 with a OHM LOAD need high values ( 4..) instead the default 1.7
and that is how my arduino inputs looked like ( Ain range 0 .. 1023 for 0 .. 5V with 2V5 AC offset)
here i exceeded the prim. AC current (1.7A)
for the CT ( N = 1000 ) and used burden resistor (470ohm) measuring range is only about 1A.
Re: CT (flux) saturation
Not read this then? http://openenergymonitor.org/emon/buildingblocks/report-yhdc-sct-013-000...
Re: CT (flux) saturation
thanks, very good link.
only using arduino and no scope available it was very interesting for me to see that current plot.
as the CT is less 1$ i still think its worth the extra work.
a combination of range adjustment by burdenresistors
- one big soldered to CT ( low ampere range )
- one small parallel to it by jumper ( high ampere range )
+ using the trick to loop the primary current 2..3 times through the CT for increase sensitivity for low currents
gives many possible configurations.
but just lookout for that saturation trap.


To enhance security, disguise scripting languages by replacing actual script extensions with dummy extensions of your choosing. For example, to change the .foo extension to .php, add the following line to your .htaccess file and rename all affected files accordingly:
# serve foo files as php files
AddType application/x-httpd-php .foo
# serve foo files as cgi files
AddType application/x-httpd-cgi .foo


olwidget.Map has been renamed olwidget.EditableMap
Many of the options parameters’ names have changed, mostly to conform to OpenLayers’ mixedCase standard:
All internal methods and variables have also changed to use mixedCase.
Map types now inherit from OpenLayers.Map. This affects javascript customizations that access the base map type.
The old way:
var mymap = new olwidget.Map('textareaId');
mymap.map.zoomTo(4);
The new way:
var mymap = new olwidget.EditableMap('textareaId');
mymap.zoomTo(4);
olwidget.widgets.OLWidget has been renamed olwidget.widgets.EditableMap
The "olwidget/olwidget.html" template has been renamed "olwidget/editable_map.html"
The admin.custom_geo_admin method has been removed. Instead, just subclass olwidget.admin.GeoModelAdmin.
olwidget.admin No longer inherits from django.contrib.admin. The old way:
from olwidget import admin
# no longer works
admin.site.register(MyModel, admin.GeoModelAdmin)
Instead, import admin from django.contrib as normal, and import GeoModelAdmin from olwidget, like this:
from django.contrib import admin
from olwidget.admin import GeoModelAdmin
admin.site.register(MyModel, GeoModelAdmin)


You're about to add a new location.
Please have an empty bottle of water with you before proceeding.
{{#if newLocationConfirmed}}Please, take a bottle of water here and send it to the lab with the given tag:
{{newLocationTag}}
You must have geolocation turned on to add new locations.
{{/if}}


PEPTO-BISMOL INSTACOOL- bismuth subsalicylate tablet, chewable
The Procter & Gamble Manufacturing Company
Disclaimer: Most OTC drugs are not reviewed and approved by FDA, however they may be marketed if they comply with applicable regulations and policies. FDA has not evaluated whether this product complies.
Active ingredient (in each tablet)
Bismuth subsalicylate 262 mg
Purposes
Upset stomach reliever and antidiarrheal
Uses
relieves
- travelers' diarrhea
- diarrhea
- upset stomach due to overindulgence in food and drink, including:
- heartburn
- indigestion
- nausea
- gas
- belching
- fullness
Warnings
Reye's syndrome
Children and teenagers who have or are recovering from chicken pox or flu-like symptoms should not use this product. When using this product, if changes in behavior with nausea and vomiting occur, consult a doctor because these symptoms could be an early sign of Reye's syndrome, a rare but serious illness.
Allergy alert
Contains salicylate. Do not take if you are
- allergic to salicylates (including aspirin)
- taking other salicylate products
Do not use if you have
- an ulcer
- a bleeding problem
- bloody or black stool
Ask a doctor before use if you have
Ask a doctor or pharmacist before use if you are taking any drug for
- anticoagulation (thinning the blood)
- diabetes
- gout
- arthritis
When using this product a temporary, but harmless, darkening of the stool and/or tongue may occur
Stop use and ask a doctor if
- symptoms get worse or last more than 2 days
- ringing in the ears or loss of hearing occurs
- diarrhea lasts more than 2 days
If pregnant or breast feeding, ask a health professional before use.
Keep out of reach of children. In case of overdose, get medical help or contact a Poison Control Center right away.
Directions
- chew or dissolve in mouth
- adults and children 12 years and over: 2 tablets every 1/2 to 1 hour as needed
- do not exceed 8 doses (16 tablets) in 24 hours
- use until diarrhea stops but not more than 2 days
- children under 12 years: ask a doctor
- drink plenty of clear fluids to help prevent dehydration caused by diarrhea
Other information
-
each tablet contains: calcium 85 mg
- sodium less than 1 mg
- salicylate 100 mg
- very low sodium
- sugar free
- avoid excessive heat (over 104°F or 40°C)
Inactive ingredients
calcium carbonate, flavor, magnesium stearate, mannitol, povidone, red 27 aluminum lake, saccharin sodium, talc
Questions?
1-800-717-3786
Made in Mexico by Procter & Gamble
Manufactura S. de R. L. de C.V.
Dist. by Procter & Gamble, Cincinnati OH 45202
PRINCIPAL DISPLAY PANEL - 30 Chewable Tablets
NEW
Pepto-
BISMOL™
InstaCool™
PEPPERMINT
BISMUTH SUBSALICYLATE
UPSET STOMACH RELIEVER/ANTIDIARRHEAL
NDC 37000-691-30
5 SYMPTOM RELIEF
Nausea • Heartburn • Indigestion
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30 CHEWABLE TABLETS


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Cameron Abbot
ABOUT
·
PHOTOS
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PROJECTS
Hi, I'm
Cameron
.
a work in progress.
Journeys
take time.
timeline
writing


Since you have already been setup National Authorized User(NAU) for your country. You sign-in to the ABSCH and fill out the Checkpoint Communiqué.
You are lucky. The User has provided you with the IRCC which makes filling out the Checkpoint Communique much more simple.
The User has provided you with the national permit. It will take a little longer to fill out the CPC form. You enter all the information possible including the national permit identifier.
The User has only provided you with the name of country where he got the magic beans. It will take a little longer to fill out the CPC form.
After you fill out the form. You request it to be published by the Publishing Authority(PA).
Once published by the PA the ABSCH will email a copy to the designated national authority/ies within their own country and to the national focal point of the country and the competent national authority/ies(CNA) of the country providing the genetic resource.


Demonstation of a level created via RPGinia project editor.
Sprites and background music (Snowdin town) were taken from Undertale.
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Plugin Information |
|---|
View Discard Old Build on the plugin site for more information. |
This plugin provides a post-build step where you can discard old build results in detailed configuration (ex. keep only builds with specified status).
Summary
- You can configure how to discard builds in more detail than the default 'Discard Old Build' function.
- Other than # of builds and days, you can specify build status to discard/keep.
- For older builds, you can configure interval to keep builds (once in a month, once in ten builds...).
- You can also use logfile size to decide if delete a old build.
Usage
Basic
After installing this plugin, a new post-build step named 'Discard Old Builds' appears.
'Days to keep builds' and 'Max # of builds to keep' work as same as Jenkins core function.
With checking statuses in 'Status to keep' section, Jenkins will keep the builds with selected statuses.
- Last build / last stable build / last successful build are always kept.
- If all the checkboxes are left unchecked, builds with any status are kept.
Advanced
In advanced section, you can configure how to treat the builds which are older than the criteria specified in basic configuration.
For old builds, perhaps you don't want to keep all, but sometimes you want to keep some of them with less frequency.
Example1
This configuration shows:
- Latest 10 builds are kept.
- Except for the latest 10, one in 15 builds are kept(#1, #16, #31,...).
Example2
This configuration shows:
- Builds within 30 days are kept.
- For builds older than 30 days, only builds with unstable/failure are kept.
TODO
- Add help text
- Add dynamic adjust discard order of discard conditions
Changelog
1.05 (released June 27, 2013)
- Add reg expression checker to discard build
- Readjust the UI and code logic
1.04 (released June 6, 2013)
- Add logfile size checker to discard build
1.03 (released April 12, 2013)
- Fixed regression related with Jenkins 1.503 (JENKINS-17528)
1.0 (released January 27, 2013)
- Initial release.
Attachments:
discardOldBuild_conf2.png (image/png)
discardOldBuild_conf3.png (image/png)
shift.png (image/png)
discard-old-build.PNG (image/png)


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{% load i18n %} {# NOTE YOU MUST LOAD i18n to every HTML page even though it's also loaded to base.html #}
{% trans "Please note:" %}
{% trans "Students starting their 2nd, 3rd, 4th or 5th year of study must have obtained at least 24 credits in the academic year before the year in which the award is paid out." %}
{% trans "Letters of presentation or of recommendation must be no more than one year old." %}
{% trans "The availability of awards and the amount of money offered for them can vary without notice." %}
{% trans "Only candidates who have won an award will be contacted." %}
{% trans "All documents required for awards must be submitted as a single PDF." %}


forward-virieux
Contents:
Typical workflow
fdWaveModel class
Miscellaneous methods
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