part of the x-data entry for an object and wherein the script process includes a process which interacts with the object file, or, a second object file published by an x-data entry and wherein the script process includes a process which interacts with a file not published by an x-data entry and wherein the script process includes a process which uses authentication information to access the object file, or, to access a second object file published in the x-base and searching for an object based on a keyword, displaying a document page according to the metadata and displaying the HREF link and searching for an object based on a keyword, displaying a document page according to the metadata, displaying the HREF link and executing a script which isin all 4 patients during retropubic prostatectomy. The duration of anaesthesia and the operation, and the intra-operative blood loss did not differ significantly between patients with and without evidence of intra-operative myocardial ischaemia. However, the maximum intra-operative fall in systolic and diastolic blood pressure, as well as the mass of the prostatic tissue removed, were significantly greater in patients with than in those without evidence of intra-operative myocardial ischaemia, suggesting that the latter may be related to the extent of surgery and the degree of intraoperative hypotension. In this study, 7 of 26 patients (27%) showed evidence of myocardial ischaemia during prostatectomy. However, it remains difficult to explain why intra-operative myocardial ischaemia should result in an increased cardiovascular mortality rate several years after the operation.


Q:

2012 POLO 1.2 S hatchback service manual?

Is there an after market service manual for a my new polo? I have already tried haynes but it's not available for my model I need it before I start messing around with the electrics. I want to attempt to fit a keyless entry system with alarm. My dad and my brother in law have one so I feel left out.

A:

A Haynes workshop manual does exist for this vehicle now.

"Work frell you, work!" "See, to me it's unbelievable." "You know" "I can come to the Mall of the Uncharted Territories, buy anthing I want cause I'm rich-- and that leather SM faced wacko Scorpy clone-- he's-he's, locked in here...here  so, you know, I" "anything with all, you know, everything, is going to be just fine, but no-- my friend, she's sick, so we gotta find a place where she can heal-- and you have no idea what I'm talkin' about, do ya?" "No." "What the hell's goin' on out there?" "Gamma disturbances are quite common in this area." "Are you talkin', like, storms?" "Oh, yes." "They're no problem." "John!" "Hey yo, 'Heavy D'!" "Hey man, have you tried one of these things?" "They're terrible, but once


now!" "You have to talk." "I've run the residual storm graph you wanted." "You were right." "The storm took a 90 degree turn to hit us." "90 degrees?" "It seems to have come after us, on purpose." "And there's worse..." "Pilot says there's another storm on the way." "It's gonna hit us in less than two arns and it's bigger than the last one." "Hit us?" "This station can't take another hit." "Yeah, I know that..." "Then let's all get onto Moya and haul out of here." "I can't pull the spike out of Moordil, and I can't just leave him here." " Well, he's gonna die isn't he?" " Well, yes, but..." " Blue..." " What does it matter if we leave him?" "Blue..." "Sparky..." "Just knockcontract to be rebid, could, however, be accorded here with or without Crozier.
FRCP 19(a)(2) states that a person should be joined if he
claims an interest relating to the subject of the action and is so situated that the disposition of the action in the person's absence may (i) as a practical matter impair or impede the person's ability to protect that interest or (ii) leave any of the persons already parties subject to a *34 substantial risk of incurring double, multiple, or otherwise inconsistent obligations by reason of the claimed interest.
Any potential problem under FRCP 19(a)(2) was disposed of by the affidavit submitted by Crozier waiving all right to pursue his interest in this matter against the government in subsequent litigation. Saratoga Motion, exhibit G. The waiver of


severing of the financing criterion because plaintiff had the option during its oral presentation before the Board to object to the action. Having failed to do so at that time, defendants argue, plaintiff should not now be heard to complain about the deletion. This argument does not persuade the Court. Failure on the part of Saratoga to state its opposition to the deletion of a selection criterion was not a waiver by it of the ability to contest whether the deletion was handled in accordance with the applicable laws and regulations. At the time of the oral presentations, defendants had not yet deleted the criterion. Thus Saratoga was not at that time "slumbering on its rights" because no claim had arisen. See Rozen v. District of Columbia, 702F.2d 1202, 1203-04 (D.C.Cir.1983).

E. Reviewability of PADC Action

The last of defendants' procedural defenses is that the PADC's action in this case is unreviewable as a matter of law. Defendants assert that this Court must dismiss plaintiff's lawsuit because the PADC's actions at issue here are committed to the agency's discretion.
Under 5 U.S.C. § 701(a)(2), an agency's actions will be found to be "committed to agency discretion by law," and hence unreviewable, where "statutes are drawn in such broad terms that in a given case there is no law to apply." Citizens to Preserve Overton Park, Inc. v. Volpe, 401 U.S. 402, 410, 91 S.Ct. 814, 820, 28 L.Ed.2d 136 (1971) (quoting S.Rep. No. 752, 79th Cong., 1st Sess., 26 (1945)). In Heckler v. Chaney, 470 U.S. 821, 105


flaws against one another, Delta's was superior to the competition. Courts are ill-equipped to second guess the agency's exercise of discretion.

CONCLUSION
For the reasons stated above, plaintiff's motion for partial summary judgment is denied, and defendants' motion for summary judgment is granted. Judgment is entered for defendants and this case is dismissed.
NOTES
[1]  The PADC had previously written to each team to advise them to be prepared during their oral presentations to address the issue of decoupling the financing criteria from the development competition. AR, tab 11. Saratoga at that time did not state its opposition to this idea. AR, tab 11(a).
[2]  When at full strength, the PADC Board consists of 15 voting members. The 13 ballots cast in this vote reflect the fact that one Board memberPatterns for To-Many Properties
Anyway because I wanted to compute the maximum of the elements it is better to iterate the array than use some tricks to make KVC work.

A:

You can solve this with using Key Value Coding and the collection operators.
NSNumber *result = [sample valueForKeyPath:@"@max.analogDataChannel"];

Update 1
As Arcanfel mentioned, you can join the arrays together:
NSNumber *result = [samples valueForKeyPath:@"@max.@unionOfArrays.@analogChannelData"];

I would suggest reading the documentation that we both linked to.  There are some very powerful features in there.
Update 2
Further to HRD's answer, he has your solution, you need to combine his changes with KVC.
Add a propert to your CMData object for currentChannel. Then you can call
[samples setValue:@(channelIndex) forKey:@"currentChannel"];

Which will set it in every instance in the array. Then call:
[samples valueForKeyPath:@"@max.analogDataForCurrentChannel"];

Then you are done.


with police, he stated that usually this nervousness

diminishes during the stop; Pulley, however, only seemed to grow more nervous

as the stop continued.

       {¶7} Trooper White testified that he observed a bottle of Febreze hanging

on the back of the front seat in a pouch. He also noticed some perfume in the front

passenger compartment. Based on his observations and his training, Trooper

White stated that he called a canine unit to perform a drug sniff on Pulley’s

vehicle.

       {¶8} Trooper White explained that Deputy Bob Roberts and his dog arrived

on the scene, walked around the car, and Deputy Roberts indicated that the dog

alerted on the car. Trooper White stated that Pulley was then removed from the

    citing Okocha v. Fehrenbacher, 101 Ohio App.3d 309, 322 (8th

Dist.1995).

       {¶29} Trial courts have broad discretion in determining whether to admit or

exclude evidence. State v. Heft, 3d Dist. Logan No. 8-09-08, 2009-Ohio-5908, ¶

62, citing State v. Issa, 93 Ohio St.3d 49, 64 (2001), citing State v. Maurer, 15

Ohio St.3d 239 (1984). Accordingly, a trial court’s ruling on the admissibility of

evidence will not be disturbed on appeal absent an abuse of discretion. Id. A trial

court will be found to have abused its discretion when its decision is contrary to

law, unreasonable, not supported by the evidence, or grossly unsound. State v.


                 -11-
Case No. 14-15-21

       C:    I think - -

       D:    If basically what we’re saying is if the marijuana - - if - - and
             the paraphernalia is in her vehicle, then she’s guilty. And I
             don’t believe the case law supports that, your Honor. But if
             that’s your ruling, then we might as well call an endto support either view. On the one hand, to close the doors of the Grand Jury room so tightly that the actions of the prosecuting officer therein cannot be disclosed, however flagrant and unlawful his conduct may have been and however much it may have been responsible for the finding of a wholly unauthorized bill of indictment, would be unfair to the defendant thus indicted even though, if innocent, he could subsequently vindicate himself in a trial upon the merits; it would also permit an over-zealous official to use the power of his office and his influence with the grand jury as an instrument of oppression, with immunity from investigation. On the other hand, to allow such an investigation lightly to be had would afford an opportunity to


The Birmingham City Council is expected to pass a $428 million operating budget on Tuesday, six months after the start of the current fiscal year.

The 2017-18 fiscal year budget -- with changes recommended by new Mayor Randall Woodfin -- includes cutting funding to the Birmingham Construction Industry Authority, a non-profit that works to build minority participation in construction projects.

"Honestly, I would like to see this budget passed tomorrow," Woodfin said to members of the Birmingham City Council during a Monday afternoon committee meeting. "From an operational and department standpoint, it is time."

He asked the councilors to make the budget the first item on the agenda for Tuesday's council meeting so city employees could receive their cost of living raises and longevity pay by Christmas.

The 2017-18 fiscal year startedto receive double-blind subcutaneous pasireotide 600 µg or 900 µg twice daily (bid). Patients with a mean urinary free cortisol (mUFC) level not exceeding the upper limit of the normal range (ULN) or who were considered by the investigator to be achieving clinical benefit from pasireotide at month 12 could continue receiving pasireotide in an open-label phase. If treatment benefit persisted and pasireotide was well tolerated, patients could continue to receive pasireotide until it became commercially available. Increase and decrease of dose was permitted during the open-label phase for efficacy and tolerability issues (permitted dose range, 150--1200 µg bid). The study was approved by an independent ethics committee, research ethics board, or institutional review board at each centre and complied with the Declaration of Helsinki, the Harmonised Tripartite Guideline for Good


striae, bruising, and dorsal and supraclavicular fat pads at month 60 compared with baseline values. Muscle strength scores remained the same in most patients from baseline to month 60 (Supplementary Fig. 3). There were no significant changes seen from baseline to month 60 in median lean body mass (−2.1 kg \[95% CI: −5.4, 0.6\]), total body fat (−3.5 kg \[95% CI: −10.0, 1.9\]) and BMD: lumbar vertebrae, 0.0 mg/cm^3^ (95% CI: −0.1, 0.1); left proximal femur total hip, 0.0 mg/cm^3^ (95% CI: −0.1, 0.0); and left proximal femur neck, 0.0 mg/cm^3^ (95% CI: −0.1, 0.0). No significant changes were seen from baseline to month 60 in blood lipids: total cholesterol, −1.3 mmol/l (95% CI: −1.6, 0.0); low-density lipoprotein cholesterol, −0.7 mmol/l (95% CI: −1.0, 0.5); high-density lipoprotein cholesterol, −0.2 mmol/l (95% CI: −0.7, 0.1); and triglycerides,to elevations in blood glucose), 75.3% (122/162) of patients in the overall population and 93.8% (15/16) of patients who reached month 60 experienced at least one AE related to hyperglycaemia. Of the overall patient population and those who reached month 60: 37.7% (61/162) and 62.5% (10/16) experienced a gallbladder/biliary-related AE; 15.4% (25/162) and 25.0% (4/16) experienced a bradycardia-related AE; and 17.3% (28/162) and 18.8% (3/16) experienced a liver-safety-related AE, respectively.Table 2AEs (regardless of study drug relationship) occurring in ≥10% of the 162 patients who received pasireotidePreferred termOverall population (*N* = 162)Patients reaching month 60 (*N* = 16)Grades 3/4All gradesGrades 3/4All grades*n* (%)*n* (%)*n* (%)*n* (%)Diarrhoea5 (3.1)95 (58.6)07 (43.8)Nausea4 (2.5)87 (53.7)2 (12.5)11 (68.8)Hyperglycaemia21 (13.0)67 (41.4)2 (12.5)9 (56.3)Cholelithiasis3 (1.9)53 (32.7)1 (6.3)8 (50.0)Headache3 (1.9)50 (30.9)1 (6.3)7 (43.8)Abdominal pain4 (2.5)41 (25.3)1 (6.3)8 (50.0)Diabetes mellitus14 (8.6)36 (22.2)2


hyperglycaemia (88.5%), the gallbladder/biliary tract (47.5%), and the liver (27.9%) were highest during the first 6 months of pasireotide treatment (Fig. [3](#Fig3){ref-type="fig"}). Steady decreases in annualised rates were seen after month 6 up to month 72.Fig. 3Annualised rates of first-reported AEs\* related to **a** hyperglycaemia, **b** the gallbladder/biliary tract, **c** the liver, and **d** bradycardia. Data show annualised rates of first-reported AEs by time interval and 95% CI. During the first year of treatment, annualised rates were estimated for 0--6 and \>6--12 months. The numbers of patients who experienced a first-reported AE (*n*) and the total number who were 'at risk' (*N*; ongoing at start of interval and had not already experienced the AE) are shown below each graph for each time interval. \*Common AE terms were grouped, for129.7) and 117.1 mg/dl (95% CI: 91.9, 142.3) at months 6 and 60, respectively (Fig. [4](#Fig4){ref-type="fig"}).Fig. 4Median **a** HbA~1c~ and **b** FPG from baseline up to month 60. Error bars show 95% distribution-free confidence limits for median values. Numbers of patients with evaluable measurements are shown beneath each time point for the overall population. Concomitant treatment with antidiabetic medication was permitted at the discretion of the investigator. Data for the overall population (*n* = 162) have previously been reported up to month 12 \[[@CR7]\] and month 24 \[[@CR8]\]

Two of the 16 patients who reached month 60 were receiving antidiabetic medication at study baseline. A further 11 patients initiated one or more antidiabetic drugs after starting pasireotide; median time from study start to first antidiabetic medication was 52 weeks (range: 1‒226). For those


A capillary electrophoresis chip with hydrodynamic sample injection for measurements from a continuous sample flow.
A microchip-based capillary electrophoresis device supported by a microfluidic network made of poly(dimethylsiloxane), used for measuring target analytes from a continuous sample flow, is presented. The microsystem was fabricated by means of replica molding in combination with standard microfabrication technologies, resulting in microfluidic components and an electrochemical detector. A new hydrodynamic sample injection procedure is introduced, and the maximum number of consecutive measurements that can be made with a poly(dimethylsiloxane) capillary electrophoresis chip with amperometric detection is investigated with respect to reproducibility. The device features a high degree of functional integration, so the benefits associated with miniaturized analysis systems apply to it.relatively poor for lean mixtures, and (3) it is ordinarily limited to providing fuel/air ratios down to only about 1:15.5. There are carburetors available, (e.g. Delco-Rochester's "Quadra Jet"; also, see U.S. Pat. No. 3,310,045, to E. Bartholomew) which do effect good air/fuel mixing at relatively lean air/fuel ratios. However, such carburetors are somewhat limited in their capacity to provide sufficient air/fuel mixture for high engine demand; these carburetors are relatively complex in structure; and finally, their air/fuel blending characteristics for lean mixtures, for example, air/fuel of 18:1 and higher, may not be adequate for good engine performance. These carburetor limitations in general have an adverse effect on the driveability of an automobile -- especially where the engine is equipped with other exhaust emission reducing modifications such as catalytic


this gallery were captured using a combination of plane-polarized light and Hoffman modulation contrast optical microscopy techniques.

Ajoene - Millions of Italian mothers can't be wrong. Eat your garlic, it's good for you. Ajoene is a naturally occurring "nutriceutical" that might reduce the risk of stroke and heart disease.

Butyl Phthalide - It's the distinctive taste and smell of celery, but also offers protection against cancer, high blood pressure and high cholesterol levels. No wonder the ancient Greeks gave stalks of celery as trophies for their athletes.

Calcium Pectate - That crunch in your pickle may help lower your cholesterol levels by removing cholesterol from the bloodstream.

Capsaicin - This chili pepper-derived spice packs the wallop in your hot tamale, but it is also a digestive aid, a topical painkiller, and aknow that Plato was Aristotle's teacher, or anything about the Nag Hammadi library, the Qumran Dead Sea Scrolls, nor be able to read a dead language like Koine Greek. So he or she could be ignorant about many facts and yet recognized as one of the top intellectuals in the world.This same point of Law's should be recognized by believers. Atheists are not stupid either. Of course, many believers have a hard time with that one, since their faith convinces them God is as obvious as the nose on one's face. For believers to admit this fact may be a problem, one that has been made into an argument by J.L. Schellenberg, that:Again, spot on. I too think Christianity is ludicrous and a delusional belief system comparable to


C4::Context;
use HTML::Template::Pro;
use C4::Search;
use C4::Output;
use C4::Koha;
use C4::Branch; # GetBranches
=head1

=cut

sub set_parameters {
	my ($template) = @_;
	my $dbh = C4::Context->dbh;
	my $branches=GetBranches();
	my @branches;
	my @select_branch;
	my %select_branches;
	push @select_branch,"";
	$select_branches{""} = "";
	foreach my $branch (keys %$branches) {
		push @select_branch, $branch;
		$select_branches{$branch} = $branches->{$branch}->{'branchname'};
	}
	my $CGIbranch=CGI::scrolling_list( -name     => 'value',
				-id => 'value_branches',
				-values   => \@select_branch,
				-labels   => \%select_branches,
				-size     => 1,
				-title    => 'Select a branch',
				-multiple => 0 );
	$template->param(CGIbranch => $CGIbranch);
	return $template;
}
sub calculate {
	my ($parameters) = @_;
	my @results =();
	my @branch = split /,/, @$parameters[0];
	my $dbh = C4::Context->dbh;
	my $sth;
	if (@branch) {
		if (C4::Context->preference('item-level_itypes')) {
		$sth = $dbh->prepare("
        SELECT description, items.itype as itemtype, COUNT(*) AS total
			FROM itemtypes,items
		WHERE items.itype=itemtypes.itemtype
		AND items.holdingbranchof a school. The court noted that the purpose of the statute  to reduce drug use by children  was reasonably served by the creation of a drug-free zone around schools that would be enforced by stiff penalties for drug pushers. It was not fatal to the statute that it could apply to drug activity conducted after school hours or in places within the zone not frequented by children, or between persons not involved in making drugs available to children. Similarly, the statute at issue protects children and other tenants of public housing projects from drug-related crime that is, by all accounts, rampant in such areas. See 42 U.S.C.A. § 11901 (West 1992). We find that the distance classification in the subject statute is a reasonable means


seek interdisciplinarity in understanding the health-disease process.

The establishment, evolution, propagation and perpetuation of infectious diseases of humans and animals are closely related to hygienic-sanitary, socioeconomical and demographic factors, and the occurrence of these vector-borne diseases is characterized by spatial and temporal patterns due to the context of residences of individuals and animals, and the aspects of the environment are associated with the proliferation of populations of reservoirs, vectors and infectious agents^[@B5]-[@B7]^.

Therefore, the use of Geographic Information Systems (GIS) and spatial statistical analysis in the health field generate an important recovery of the role of the socio-environmental atmosphere in the production and reproduction of leptospirosis, since it is closely related to the ecological characteristics of the environment, enabling a more complete analysis of the disease and the identification ofChina, Hungary, Canada, USA, Zambia and Brazil^[@B11]-[@B21]^.

Considering the etiological agent of leptospirosis as an inherent structure of the space-climate relationship, and since the space is the means by which the infectious agent circulates, it can be concluded that the epidemiological structure of the disease is modified by the transformation of space and climate over the years, hence requiring continuous technological innovations of surveillance models in a diverse and complex social context, such as the current urban life^[@B22],[@B23]^.

This study aims to conduct a systematic review, through the election of national and international articles, of the main techniques of GIS and spatial analysis used in scientific studies on the identification of risk areas of leptospirosis in the period from 1998 to 2017, as well as to create a ranking table


only one article published in the last 20 years. It was observed that 34 articles were in the human field and six were in the animal field.

Among the 40 articles, only 18 performed spatial statistical analysis, and nine of them used the Kernel density technique. In 22 articles, the authors only performed spatial analysis by constructing thematic maps and distributing cases on these maps to visualize the spatial pattern of leptospirosis distribution, as shown in the [Supplementary Table](#t3){ref-type="table"}. Despite this variation of complexity in the methodologies adopted, all studies achieved the objectives initially proposed by the authors.

Supplementary TableList of the elected articles with their respective descriptions regarding the year of publication, authors, country of origin, title, scientific journal, software and method of analysis in the 2007-2017 periodYear of*32/12. Suppose 0 = h*z + 3*o - 64, o + 8 = -o. Is z a composite number?
False
Let i = -65 - -259. Is i composite?
True
Let p = 6272 - 3153. Suppose -2*k + 2 = 0, 4*w + 2*k + k - p = 0. Is w a prime number?
False
Let q be (-15 + -1)*(-2)/4. Suppose q = -4*m + 420. Is m prime?
True
Let l = 4 + 0. Suppose 5 = -z - l*z, 0 = -2*a - 4*z + 318. Is a prime?
False
Suppose -4*s - 5 = 3*t, 4*t + s + 2*s = -9. Is (10/t)/(2/(-39)) a prime number?
False
Let r(y) = -y + 17. Suppose -g = -2*g + 2*p + 18, 27 = 2*g - p. Let t be r(g). Is (-3)/((-3


Usual and unusual pitfalls of 18F-FDG-PET/CT in lymphoma after treatment: a pictorial review.
Fluorine-18-fluorodeoxyglucose (F-FDG) PET/computed tomography (CT) is now a standard of care in initial staging and treatment evaluation of lymphomas. It is also used in the interim evaluation in diffuse large B cell lymphoma and Hodgkin lymphoma. However, several pitfalls may occur during or after treatment, because of the nonspecificity of F-FDG for lymphoma disease and treatment as immunotherapy, thus possibly induces misinterpretation and wrong treatment decision. The aim of this pictorial review is to provide an illustrated tutorial of the most frequent pitfalls found on F-FDG-PET/CT during or after treatment.Evaluating the efficacy of anti-influenza drugs such as Umifenovir and Oseltamivir against COVID-19 virus is interesting but lacks any biological plausibility. Many antiviral drugs can cause cardiac insufficiency, arrhythmia or other cardiovascular disorders. Antiviral drug induced heart damage during COVID-19 treatment is a major concern and the monitoring of the risk of cardiac toxicity with the use of antiviral drugs is important. In a study of 138 patients with COVID-19, 89.9% were given antiviral drug [@b0005], [@b0235].

Acute cardiac injury in patients with COVID-19 {#s0050}
----------------------------------------------

In a report by Huang et al [@b0015] myocardial injury associated with the SARS-CoV-2 was found in 5 of the first 41 patients diagnosed with COVID-19 in Wuhan. These patients had elevated cardiac troponin I (hs-cTnI) levels (\>28 pg/ml) levels. In this report, four of five patients


can aggravate the pneumonia and increase the severity of symptoms. When infected with SARS-CoV-2, cardiac insufficiency is more likely to occur, in these patients. For patients with cardiac insufficiency who have underlying heart disease, SARS-CoV-2 infection might act as a precipitating factor to worsen the condition and lead to death. However, it has not been shown any causative role of such co-morbidities to SARS-CoV-2 infection. In fact, ACE2 expression had been shown to lower with age [@b0250].

Klok et al [@b0255] evaluated the incidence of the outcome of venous thromboembolism (VTE) and arterial thrombotic complications in all COVID-19 patients admitted to the ICU of 2 Dutch university hospitals and 1 Dutch teaching hospital and they suggested that the composite outcome consisted of acute pulmonary embolism (PE), deep-vein thrombosis (DVT),communities in an adverse way.”

Little has happened since then, however.

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At a hearing in early fall, Sen. Thomas R. Carper (D-Del.) pressed the EPA’s director of groundwater and drinking water on when the agency might announce its plans to regulate the chemicals and finalize a drinking-water standard. Peter Grevatt, an agency veteran who recently retired, responded that officials were continuing to visit communities and develop a long-term “management plan.” He acknowledged that it could take the agency a “number of years” to put enforceable regulations in place — if it determined that the contaminants were surfacing in enough water systems to be considered a nationwide health concern.

“Is it a national standard that requires all the nation’s systems to sample on some regular basis and has the tools to get


and the smell of hash browns hangs in the air.

“We lost a lot of business, primarily because of fear,” said manager Carrie Klinger, whose father started the diner more than two decades ago. During the month-long water crisis, the family bought 80 pounds of bagged ice a day, made soups with bottled water and served canned sodas because the drink machine was hooked to a water line.

“It’s still not quite back to where it was,” Klinger said. “I still have customers who say they’ll never drink the water again.”

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Echoes of that distrust linger on Glendale Boulevard, where Jennifer and Justin Koehler lived in a tidy, white clapboard house until selling and moving away because of their fears.

“It made me so scared, because our kids are so little. Andbeing in a tug-o-war with two people pulling at either side and not knowing how to adapt to the situation.

He said he was fortunate because he can afford to pay for professional help to deal with his problem, unlike many others.

Earlier, I wondered if I would speak about my problem today in the Dáil. I think it is important that people speak out about this issue.

The Social Democrats’ Catherine Murphy raised the issue of youth mental health.

In the years that I have been a public representative, there have been several incidents of clusters of teen suicides in my area which has a disproportionately young age profile. It causes huge long-term irreparable damage to the families involved and to their communities.

Meanwhile Independent TD Thomas Pringle said funding must be


The Nomadic Hyena Handlers of Nigeria

It all started with the picture above. A friend had emailed photographer Pieter Hugo this bizarre image taken on a cellphone in Lagos, Nigeria. The caption read, ‘The Streets of Lagos’, and a newspaper publishing the photo reported that the men were bank robbers, body guards, drug dealers and debt collectors.

The image went viral online and the myth of these street toughs in Nigeria with Hyenas grew. Pieter was captivated and knew he had to learn more.

Through a journalist friend, Hugo tracked down a Nigerian reporter, Adetokunbo Abiola, who said that he knew the Gadawan Kura as they are known in Hausa (a rough translation: ‘hyena handlers/guides’). A few weeks later, Pieter was on a plane to Lagos.

Abiola met me at the airportof a not too distant sealing device. A burst is manifested by a drop in pressure toward the site of the burst, which drop is sensed by suitable control devices and is utilized for the control of the flow control valve that is positioned upstream relative to the side of the burst.
For the purpose of measuring relatively small pressure differences at rather high absolute pressure, the Barton cells are known, and such operate with two measuring bellows exposed to the pressures to be compared. However, Barton cells normally cannot be considered for the present purpose because the control devices must be arranged in open ground along the natural gas pipe line, and diaphragm or bellows switch elements are less suitable than is desirable for the low temperatures often


that correct? A. Yes, sir. Q. That's correct? A. Yes, sir. Q. You've just had one injury, just your damage to your engine. Now, in one case your measure of damages may be more than in the other case. A. Yes, sir. Q. But you just had one injury. A. Yes, sir. Q. All right. And Columbus Body Works paid you for this injury, didn't they? A. Yes, sir. Q. And you signed a release. A. Yes, sir. Q. And we have the release here, and we have the lawsuit that you filed against Columbus Body Works. A. Yes, sir. Q. All right. Now, do I understand it that when you took the car to Columbus Body Works, that the engine was running excellently when you delivered itso i dont know how my if statement needs to be

A:

You need to reference the indices of the array. Each index in an array is represented by a number that starts at base zero. This is an important and fundamental concept across many programming languages.
It also looks like your array's name is not names and is name.
So you could check to see if the name is "Calculators" by doing something like this:
if (name[i].equals("Calculators")) { ... }


knew of the tenant's prior misconduct against Ritz employees and did nothing.
Appellant's evidence showed that three days before the assault, David Caldwell, the director of human resources, instructed appellant to investigate reports about a certain guest harassing the staff. Almost every female housekeeper reported improper sexual behavior from the Saudi Arabian tenant in room 821. On February 12, appellant told *464 this to Luis Argote, the general manager. Argote responded, "keep a lid on it," "we've known about this all along," and the situation will "blow over in a day or two."
Three days later, on February 15, the Saudi Arabian sexually assaulted Granados. In June 1992, Granados sued The Ritz. During the investigation, Argote asked appellant to prepare a statement about the incident, which appellant thought was forcontends The Ritz failed to prove as a matter of law that he was not fired for the "sole reason" of refusing to perform an illegal act. He claims the evidence was in conflict concerning The Ritz's true motive in firing him. We agree.
The longstanding rule in Texas is that employment for an indefinite term may be terminated at will and without cause. East Line & R.R.R. Co. v. Scott, 72 Tex. 70, 75, 10 S.W. 99, 102 (1888). In Sabine Pilot Service, Inc. v. Hauck, 687 S.W.2d 733, 735 (Tex.1985), the court created a narrow exception to the employment-at-will doctrine. This "public policy exception" allows an employee to sue for wrongful termination if fired "for the sole reason that the employee refused to perform an illegal act."


criminally liable for mail fraud as a principal or as a conspirator. See 18 U.S.C.A. § 2 (1969); 18 U.S.C.A. § 371 (West Supp.1997).
We sustain the third point of error.
The judgment is reversed, and the cause is remanded.
Sunday, July 5, 2009

Rome Wasn't Built in a Day...

...Nothing beautiful and extraordinary ever was!!!

So when I placed an order for the most exquisite hand knitted mittens, gloves and long fingerless mittens from Mel Paton Crochet, I just knew there would have to be a wait... Surprisingly they were all made up for me in such little time for what I've received - and it has definitely been well worth it!

So... Come to the Curious Oyster Shoppe soon and check out these sublime, 100% Australian Wool beauties....

And a little bit of Q & A for the star artisan...

Q. Who are you?A. I'm a 31 year old primary school teacher and crochet designer from Perth, WA.

Q. What do you make?A. I make luxury fingerless mittens, eco-friendly makeup removal wipes and


---
abstract: 'Over the past three decades, black holes have played an important role in quantum gravity, mathematical physics, numerical relativity and gravitational wave phenomenology. However, conceptual settings and mathematical models used to discuss them have varied considerably from one area to another. Over the last five years a new, quasi-local framework was introduced to analyze diverse facets of black holes in a unified manner. In this framework, evolving black holes are modelled by *dynamical horizons* and black holes in equilibrium by *isolated horizons*. We review basic properties of these horizons and summarize applications to mathematical physics, numerical relativity, and quantum gravity. This paradigm has led to significant generalizations of several results in black hole physics. Specifically, it has introduced a more physical setting for black hole thermodynamics andtheorems [@pcreview; @mh] took the community by surprise. The subsequent analysis of the detailed properties of Kerr–Newman solutions [@bc] and perturbations thereof [@chandra] constituted a large fraction of research in mathematical general relativity in the seventies and eighties. Just as the community had come to terms with the uniqueness results, it was surprised yet again by the discovery of hairy black holes [@bm; @pb]. Research in this area continues to be an active branch of mathematical physics [@vgreview]. The situation has been similar in numerical relativity. Since its inception, much of the research in this area has been driven by problems related to black holes, particularly their formation through gravitational collapse [@collapsereview], the associated critical phenomenon [@mc; @cgreview], and the dynamics leading to their coalescence (see, e.g., [@grand1; @closelimit2; @closelimit1; @grazing2; @grazing1; @lhreview]). Finally, black


isolated black hole and carry out its quantization systematically. A pre-requisite for such a program is the availability of a manageable action principle and/or Hamiltonian framework. Unfortunately, however, if one attempts to construct these within the classical frameworks traditionally used to describe black holes, one runs into two difficulties. First, because the event horizon is such a global notion, no action principle is known for the sector of general relativity containing geometries which admit an event horizon as an internal boundary. Second, if one restricts oneself to globally stationary solutions, the phase space has only a finite number of true degrees of freedom and is thus ‘too small’ to adequately incorporate all quantum fluctuations. Thus, again, we are led to ask: Is there a more satisfactory framework whichin numerical simulations where the backscattering effects typically become smaller than the numerical errors rather quickly after the formation of the black hole (see, e.g., [@whiskey; @bks]).

### Definitions {#s2.1.1}

The key idea is to extract from the notion of a Killing horizon the minimal conditions which are necessary to define physical quantities such as the mass and angular momentum of the black hole and to establish the zeroth and the first laws of black hole mechanics. Like Killing horizons, isolated horizons are null, 3-dimensional sub-manifolds of space-time. Let us therefore begin by recalling some essential features of such sub-manifolds, which we will denote by $\Delta$. The intrinsic metric $q_{ab}$ on $\Delta$ has signature (0,+,+), and is simply the pull-back of the space-time metric to $\Delta$, $q_{ab}={\hbox{\lower0.85ex\hbox{${}_{\longleftarrow}$}}\kern-3.0ex{g_{ab}}}$, where an underarrow


*marginally trapped*. (Note incidentally that if $\Theta_{(\ell)}$ vanishes for one null normal $\ell^a$ to $\Delta$, it vanishes for all.) Condition \[cond\_1\_2\] is equivalent to requiring that the *infinitesimal area element* is Lie dragged by the null normal $\ell^a$. In particular, then, Condition \[cond\_1\_2\] implies that the horizon area is ‘constant in time’. We will denote the area of any cross section of $\Delta$ by $a_\Delta$ and define the horizon radius as $R_\Delta:=\sqrt{a_\Delta/4\pi}$.

Because of the Raychaudhuri equation, Condition \[cond\_1\_2\] also implies $$R_{ab}\ell^a\ell^b + \sigma_{ab}\sigma^{ab} = 0,$$ where $\sigma^{ab}$ is the shear of $\ell_a$, defined by $\sigma_{ab} := {\hbox{\lower0.5ex\hbox{${}_{\leftarrow}$}}\kern-1.9ex{\nabla_{(a} \ell_{b)}}} - \frac{1}{2}
\Theta_{{(\ell)}} q_{ab}$, where the underarrow denotes ‘pull-back to $\Delta$’. Now the energy condition \[cond\_1\_3\] implies that $R_{ab}\ell^a \ell^b$ is non-negative, whence we conclude that each of the two terms in the last equationassociated to a space-like 3-surface $M$ representing ‘an instant of time’. Let us begin by recalling these ideas.

Hawking’s *outer trapped surface $S$* is a compact, space-like 2-dimensional sub-manifold in $(\mathcal{M}, g_{ab})$ such that the expansion $\Theta_{(\ell)}$ of the outgoing null normal $\ell^a$ to $S$ is non-positive. Hawking then defined the *trapped region $\mathcal{T}(M)$ in a surface $M$* as the set of all points in $M$ through which there passes an outer-trapped surface, lying entirely in $M$. Finally, Hawking’s *apparent horizon* $\partial \mathcal{T}(M)$ is the boundary of a connected component of $\mathcal{T}(M)$. The idea then was to regard each apparent horizon as the instantaneous surface of a black hole. One can calculate the expansion $\Theta_{(\ell)}$ of $S$ knowing only the intrinsic 3-metric $q_{ab}$ and the extrinsic curvature $K_{ab}$ of


the remainder of our discussion of DHs will be focused on the zero cosmological constant case with 2-sphere topology.*

Energy flux due to gravitational waves {#s3.3}
--------------------------------------

Let us interpret the various terms appearing in the area balance law (\[ab3\]).

The left side of this equation provides us with the change in the horizon radius caused by the dynamical process under consideration. Since the expansion $\Theta_{(\ell)}$ vanishes, this is also the change in the *Hawking mass* as one moves from the cross section $S_1$ to $S_2$. The first integral on the right side of this equation is the flux $\mathcal{F}^{(R)}_\mathrm{matter}$ of matter energy associated with the vector field $\xi_{(R)}^a$. The second term is purely geometrical and accompanies the term representing the matter energy flux. Hence it is interpreted as *the flux $\mathcal{F}^{(R)}_\mathrm{grav}$ ofhave to introduce any structure, such as coordinates or tetrads, which is auxiliary to the problem, the expression is obviously gauge invariant. This is to be contrasted with definitions involving pseudo-tensors or background fields.

<!-- -->

Positivity

:    \
    The energy flux (\[gravflux1\]) is manifestly non-negative. In the case of the Bondi flux, positivity played a key role in the early development of the gravitational radiation theory. It was perhaps the most convincing evidence that gravitational waves are not coordinate artifacts but carry *physical* energy. It is quite surprising that a simple, manifestly non-negative expression can exist in the strong field regime of DHs. One can of course apply our general strategy to any space-like 3-surface $\bar{H}$, foliated by 2-spheres. However, if $\bar{H}$ is not a DH,


${\mathcal L}_X \mathbf{\Omega} =0$. Since the phase space is topologically trivial, it follows that this condition holds if and only if there is a function $H$ on $\mathbf{\Gamma}$ such that $\mathbf{\Omega}(\delta, X) = \delta H$ for all vector fields $\delta$. The function $H$ is called a Hamiltonian and $X$ its Hamiltonian vector field; alternatively, $H$ is said to generate the infinitesimal canonical transformation $X$.

Since we are interested in energy and angular momentum, the infinitesimal canonical transformations $X$ will correspond to time translations and rotations. As in any generally covariant theory, when the constraints are satisfied, values of Hamiltonians generating such diffeomorphisms can be expressed purely as surface terms. In the present case, the relevant surfaces are the sphere at infinity and the spherical section $S=M\cap \Delta$ of thebinding energy.

The first calculation of binding energy was made by Brill and Lindquist in such a context. They considered two non-spinning black holes initially at rest [@bl]. For large separations, they found that, in a certain mathematical sense, the leading contribution to binding energy comes just from the usual Newtonian gravitational potential. More recently, Dain [@sd] has extended this calculation to the case of black holes with spin and has shown that the spin-spin interaction energy is correctly incorporated in the same sense.

In numerical relativity, the notion of binding energy has been used to locate sequences of quasi-circular orbits. The underlying heuristic idea is to minimize $E\mathrm{b}$ with respect to the proper separation between the holes, keeping the physical parameters of the black holes fixed. The value of the separation


or radiation outside the horizon which contribute to the field multipoles at infinity. The two sets of quantities need not agree even for stationary, vacuum space-times because of contributions from the gravitational field in the exterior region. For the Kerr space-time, the source and field moments are indeed different for $n\ge 2$. However, the difference is small for low $n$ [@aepv].

See [@aepv] for further discussion and for the inclusion of electromagnetic fields, and [@bks] for the numerical implementation of these results.

Waveform extraction {#s5.4}
-------------------

The prospect of receiving gravitational waves offers exciting opportunities for astrophysics and for testing the *dynamical, strong field regime* of general relativity (see, e.g., [@sourcesreview]). Black holes are among the most promising sources both for terrestrial and space-based observatories. Extracting gravitational waveform resulting from, say, gravitational collapse [@collapsereview] or blackexcess energy being radiated away to infinity. In general, however, even if one component of a bound system is unstable, the total system may still be stable if the binding energy is sufficiently large. An example is provided by the deuteron. However, an examination of energetics reveals that this is not the case for colored black holes, so instability should prevail. Furthermore, one can make a few predictions about the nature of instability. We summarize these for the simplest case of spherically symmetric, static black holes for which there is a single quantum number $n$:

1.  All the colored black holes on the $n$th branch have the same number (namely, $2n$) of unstable modes as the $n$th soliton. (The detailed features of these unstable modes can differ especially


because they are subject to different boundary conditions in the two cases.) \[item\_1\]

2.  For a given $n$, colored black holes with larger horizon area are less unstable. For a given horizon area, colored black holes with higher value of $n$ are more unstable. \[item\_2\]

3.  The ‘available energy’ for the process is given by $$\label{avail}
        E_\mathrm{available}^{(n)}= M_\mathrm{sol}^{(n)} -
        |E_\mathrm{binding}^\mathrm{initial}|.$$ Part of it is absorbed by the black hole so that its horizon area increases and the rest is radiated away to infinity. Note that $E_\mathrm{available}^{(n)}$ can be computed *knowing just the initial configuration*. \[item\_3\]

4.  In the process the horizon area necessarily increases. Therefore, the energy radiated to infinity is strictly less than$E_\mathrm{available}^{(n)}$. \[item\_4\]

Expectation \[item\_1\] of the model is known to be correct [@unstable2]. Prediction \[item\_2\] has been shown to be correct in the $n=1$, colored black holes in the sense that the frequency of all unstable modes is a decreasing function of the area, whence the characteristic decay time grows with area [@vgreview; @unstable4]. To our knowledge a detailed analysis of instability, needed to test Predictions \[item\_3\] and \[item\_4\] are yet to be made.

Finally, the notion of horizon mass and the associated stability analysis has also provided an ‘explanation’ of the following fact which, at first sight, seems puzzling. Consider the ‘embedded Abelian black holes’ which are solutions to Einstein–Yang–Mills equations with a specific magnetic charge $P^0_\Delta$. They are isometric to a family of magnetically charged Reissner–Nordström solutions and the isometry maps the Maxwell field


the thermodynamic, black hole entropy through a detailed, statistical mechanical counting of appropriate micro-states. Indeed, this is essentially the only [concrete]{} quantitative hint we have had about the nature of quantum space-time geometry. The isolated horizon framework has been used to address this issue systematically and has led to the only available detailed calculations within a full-fledged approach to quantum gravity that encompass realistic black holes (which carry no or negligible gauge charges and may be distorted). As we will discuss in Section \[s8\], what we know about dynamical horizons does suggest that there should be interesting generalizations of these results also to non-equilibrium situations. But so far there has been no work along these lines.

Preliminaries {#s7.1}
-------------

The first and the second laws of black hole mechanics discussed in Section \[s4\],numerical values *do depend on* $\gamma$. Since the eigenvalues are distinct in different $\gamma$-sectors, it immediately follows that these sectors provide unitarily inequivalent representations of the algebra of geometric operators; there is ‘super-selection’. Put differently, there is a quantization ambiguity, and which $\gamma$-sector is actually realized in Nature is an experimental question. One appropriate experiment, for example a measurement of the smallest non-zero area eigenvalue, would fix the value of $\gamma$ and hence the quantum theory. Every further experiment – e.g., the measurement of higher eigenvalues or eigenvalues of other operators such as those corresponding to the volume of a region – would provide tests of the theory. While such direct measurements are not feasible today we will see that, somewhat surprisingly, the Hawking–Bekenstein formula (\[entropy1\]) for the entropy


of large black holes provides a thought experiment to fix the value of $\gamma$.

Recall next that, because of the horizon internal boundary, the symplectic structure now has an additional surface term. In the classical theory, since all fields are smooth, values of fields on the horizon are completely determined by their values in the bulk. However, a key point about field theories is that their quantum states depend on fields which are arbitrarily discontinuous. Therefore, in quantum theory, a decoupling occurs between fields in the surface and those in the bulk, and independent surface degrees of freedom emerge. *These describe the geometry of the quantum horizon and are responsible for entropy*.

In quantum theory, then, it is natural to begin with a total Hilbert space $\mathcal{H} = \mathcal{H}_{V}\otimes \mathcal{H}_{S}$in the given intervals. Again recent work shows that the state counting yields the Hawking–Bekenstein formula (\[entropy1\]) for minimally coupled matter and its modification (\[entropy3\]) for non-minimally coupled scalar field, *for the same value $\gamma= \gamma_0$ of the Barbero–Immirzi parameter* [@aa4; @aev].

To summarize, the isolated horizon framework serves as a natural point of departure for a statistical mechanical calculation of black hole entropy based on quantum geometry. How does this detailed analysis compare with the ‘It from Bit’ scenario [@wheeler] with which we began? First, the quantum horizon boundary conditions play a key role in the construction of a consistent quantum theory of the horizon geometry. Thus, unlike in the ‘It from Bit’ scenario, the calculation pertains only to those 2-spheres $S$ which are cross-sections of a WIH. One can indeed divide


of black holes is that so little is known about their properties in the fully dynamical and non-linear regime of general relativity. Indeed, we do not even have a fully satisfactory *definition* of a dynamical black hole. Traditionally, one uses event horizons. But as we discussed in detail, they have several undesirable features. First, they are defined only in space-times where one can unambiguously identify infinity. Even in these restricted contexts, event horizons are teleological, can form in a flat region of space-time and grow even though there is no flux of energy of any kind across them. When astronomers tell us that there is a black hole in the center of Milky Way, they are certainly not referring to event horizons.

Numerical simulations [@bks; @gv2] suggest that the outermostmarginally trapped world-tubes become dynamical horizons soon after they are formed. As we saw, dynamical horizons have a number of attractive properties that overcome the limitations of event horizons: they are defined quasi-locally, can not be formed in flat space-time, and their growth is dictated by balance laws with direct physical interpretation. Physically, then, dynamical horizons satisfying the additional physical condition $\mathcal{L}_n
\Theta_{(\ell)} <0 $ (i.e., SFOTHs) appear to be good candidates to represent the surface of a black hole. But so far, our understanding of their uniqueness is rather limited. If a canonical dynamical horizon could be singled out by imposing physically reasonable conditions, one could use it as the physical representation of an evolving black hole.

A plausibility argument for the existence of a canonical dynamical horizon was


code I used was:

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The window.orientation value is 0 (zero) when in portrait and 90/-90 when in landscape. There is no “upside down” portrait value (you can try yourself to rotate by 180 degrees the iPhone, it remains in landscape).

Now you have a good reason to not use .mobi domains.

Thank you, Apple.  '-D'*)
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yet. In another chase sequence we follow Obi-Wan who is chasing Jango to another new planet (props for all of the planets we got to see in this movie), and he finally gets captured. All of this leads back to Anakin and Padme through a droid factory and they get captured too.

John Carter of Mars is a clear influence of the next events. A coliseum where our three heroes must fight three monsters to survive while the alien natives and new big bad villain, Count Dooku, played fantastically by Christopher Lee. A big surprise brings along one of the coolest moments in all of the movies when the several Jedi reveal themselves to rescue our heroes. This is the first time we’ve seen this many Jedi fighting inthere to contract. If this is right, then the ant ends its life as a prisoner in its own body. Its brain is still in the driver’s seat, but the fungus has the wheel.

ICE wants to use machine learning technology and social media monitoring to determine whether an individual is a “positively contributing member of society,” according to documents published on federal contracting websites. More than 50 civil society groups and more than 50 technical experts sent separate letters on Thursday to the Department of Homeland Security saying the vetting program as described was “tailor-made for discrimination” and contending artificial intelligence was unable to provide the information ICE desired.

Security: Quad9 blocks against known malicious domains, preventing your computers and IoT devices from connecting malware or phishing sites. Whenever


a developer will decide to upload all their dot-files in their home directory to github so they can use the same .vimrc and .bashrc aliases everywhere, and will end up uploading their AWS creds).'

how did you solve this problem at Something Awful? You said you wrote a bunch of rules but internet pedants will always find ways to get around them.

The last rule says we can ban you for any reason. It's like the catch-all. We can ban you if it's too hot in the room, we can ban you if we had a bad day, we can ban you if our finger slips and hits the ban button. And that way people know that if they're doing something and it's not technically breaking any rules but they're"The last one... the Malraux..." "I thought they'd been killed off." "According to this, there might be one left." "Hayley." "You looked for five years." "You found nothing." "Suddenly, I get word of a lead." "What if someone else found it, too?" "What if it's a trap?" "("siberian nights" by the kills playing)" "Your royal highness." "And to what do I owe this great honor?" "All right, all right, take it down a notch." "Is he here?" "In the back." "He was just raving about your awesome punctuality." "Good crowd." "Witches, vampires." "Everyone getting along?" "We're like Switzerland, right smack in the heart of the city." "Everything Cami wanted." "Okay, I got to run." "Spinning records all week." "You know... (imitates rhythmic, percussive sounds)" "Vincent." "Appreciate you coming."


for everyone in this city" "If you're here for what's going down." "If you need me to say "please," Vincent, I will." "What have you gotten yourself into, Marcel?" " You about to start a war?" " No." "If this goes the way I expect, I won't have to lift a finger." "All I need from you" "Is a boundary spell." "Anyone can enter, no one can leave." "And it's got to be strong." "Well, how strong?" "Original strength." "You got my venom." "When do I get to go?" "As soon as I know it works." "And when will that be?" "Believe me," "You'll know when you see it." "You have to wake up sleeping beauty, right?" "How do you do that?" "You know, you ask a lot---
abstract: 'The properties are considered in detail of a non-local (integral) equation for the superconducting gap parameter, which is obtained by a coarse-graining procedure applied to the Bogoliubov-de Gennes (BdG) equations over the whole coupling-vs-temperature phase diagram associated with the superfluid phase. It is found that the limiting size of the coarse-graining procedure, which is dictated by the range of the kernel of this integral equation, corresponds to the size of the Cooper pairs over the whole coupling-vs-temperature phase diagram up to the critical temperature, even when Cooper pairs turn into composite bosons on the BEC side of the BCS-BEC crossover. A practical method is further implemented to solve numerically this integral equation in an efficient way, which is based on a novel algorithm for calculating the Fourier


the Fermi function in Eq. (\[Kernel-Q\]) becomes smooth for increasing temperature, the kink singularity in $K(Q)$ is also smoothed out.

In addition, Fig. \[Figure-3\] shows the wave-vector dependence of the kernel $K(Q)$ over a more extended range of Q in the case of unitarity at zero temperature, evidencing how $K(Q)$ converges, in practice, for large enough $Q$ to its asymptotic expression (\[large\_Q-remaining\_part\]) (or, else, to the asymptotic kernel (\[asymptotic-kernel\])).

![(Color online) Radial profile of the kernel $K^{\sigma}(R)$ for various couplings and temperatures: $T=0$ (full line); $T=0.1T_{c}$ (dashed line); $T=0.5T_{c}$ (dotted line); $T=0.95T_{c}$ (dashed-dotted line). In each case, the critical temperature $T_{c}$ refers to the given coupling, while the value $\sigma=10 k_{F}$ is common to all curves. To make the difference among the various curves more visible, $K^{\sigma}(R)$ is multiplied by $R^{4}$.[]{data-label="Figure-4"}](Figure-4.pdf){width="7.2cm"}

[**B. Propertiesside (rhs) of both Eq. (\[useful-identitiy-1\]) (upper panel - dots) and Eq. (\[useful-identitiy-2\]) (lower panel - stars) calculated for different values of $\sigma$, when $T=0$ and $(k_{F} a_{F})^{-1} = -1$.[]{data-label="Figure-7"}](Figure-7.pdf){width="6.5cm"}

[**Numerical checks on the overall shape of $\mathbf{K^{\sigma}(R)}$.**]{} The following identities hold for the kernel $K^{\sigma}(R)$ at any coupling and temperature below $T_{c}$:

$$\begin{aligned}
& & 4 \pi \! \int_{0}^{\infty} \!\! dR \, R^{2} \, K^{\sigma}(R) \, = \, K(\mathbf{Q}=0) \, = \, \mathcal{I}_{0} \, ,
\label{useful-identitiy-1} \\
& & 16 \pi \! \int_{0}^{\infty} \!\! dR \, R^{4} \, K^{\sigma}(R) \, = \, - \, \nabla^{2} \! \left(  K(\mathbf{Q}) \, e^{-\mathbf{Q}^{2}/\sigma^{2}} \right)_{\mathbf{Q}=0}
\nonumber \\
& = & - \, \nabla^{2} \! \left. K(\mathbf{Q}) \right|_{\mathbf{Q}=0} + \frac{6}{\sigma^{2}} \, K(\mathbf{Q}=0) \, =  \, \frac{ 6 \, \mathcal{I}_{1}}{m} + \, \frac{ 6 \, \mathcal{I}_{0}}{\sigma^{2}} \, ,
\label{useful-identitiy-2} \end{aligned}$$

where


$R$, where $K^{\sigma}(R)$ and $K_{\infty}^{\sigma}(R)$ are seen to essentially coincide with each other. An example is shown in Fig. \[Figure-9\] for a given value of $\sigma$ when $T=0$ and $(k_{F} a_{F})^{-1} = (0.0,1.0)$. Since the small-$R$ profile common to $K^{\sigma}(R)$ and $K_{\infty}^{\sigma}(R)$ is associated with the common large-$Q$ behaviour of the corresponding kernels in $Q$-space, which is independent of coupling and temperature, the results of Fig. \[Figure-9\] suggest us to adopt the following procedure which allows us to concentrate on the large-$R$ behaviour of the kernel $K^{\sigma}(R)$, that instead depends on both coupling and temperature.

![(Color online) Coupling dependence of the point $R_{0}$ at which the two kernels $K^{\sigma}(R)$ and $K^{\sigma}_{\infty}(R)$ start to deviate from each other within $2 \%$, for several temperatures. Here, $\sigma = 20 k_{F}$ (dots), $\sigma =30 k_{F}$ (stars), and $\sigma = 40 k_{F}$ (diamonds).[]{data-label="Figure-10"}](Figure-10.pdf){width="6.5cm"}

For given coupling and temperature, we move from $R=0$ outwards and search for the point $R_{0}$ at which the two kernels $K^{\sigma}(R)$ and $K^{\sigma}_{\infty}(R)$ start to deviate from each other, say, within $2 \%$. This can be done for a set of values of $\sigma$, thus monitoring the convergence of the results for $\sigma \rightarrow \infty$. The results of this procedure are shown in Fig. \[Figure-10\] throughout the BCS-BEC crossover, for several temperatures and three different values of $\sigma$. In all cases, the values of $R_{0}$ are not larger than $1/(2 k_{F})$, which represents a small length scale compared with the overall spatial extent of the kernel $K^{\sigma}(R)$ [@footnote-1]. Note also that $R_{0}$ depends weakly on $\sigma$ for all couplings and


where a double coarse-graining procedure was introduced on the BdG equations to end up eventually with the local (differential) LPDA equation for the gap parameter. This equation is similar in spirit to the GL and GP equations, but expands their range of validity over a much wider portion of the coupling-vs-temperature phase diagram in the superfluid phase. In Ref. [@Simonucci-2014] the question of the spatial extent of the “granularity” associated with the coarse-graining procedure was, however, left open, since most attention was concentrated there in studying the outcomes of LPDA equation itself.

In the present paper we have considered this question in detail, by studying the properties of the non-local (integral) NLPDA equation that was also reported in Ref. [@Simonucci-2014] at an intermediate step of the derivation of the local (differential)only in the weak-coupling (BCS) limit, and can now be carried over to the whole BCS-BEC crossover in terms of the non-local (integral) NLPDA equation. This study may also help stimulating a revival of the experiments that adopt a similar geometry and physical arrangement, in line with the original experimental work of Ref. [@Polturak-1991] aimed at determining the temperature dependence of the coherence length in the normal phase.

[**ACKNOWLEDGMENTS**]{}

We are indebted to P. Pieri for having determined the expression (\[large\_Q-remaining\_part\]) for the large-$Q$ behavior of the kernel $K(Q)$ as well as for a critical reading of the manuscript.

ORIGIN OF THE SPATIAL OSCILLATIONS AND THE LONG-RANGE TAIL OF THE KERNEL $\mathbf{K^{\sigma}(R)}$: A MODEL STUDY {#sec:appendix-A}
================================================================================================================

The origin of the spatial oscillations, that affect the kernel $K^{\sigma}(R)$ of the non-local gap equation (\[non-local-LPDA-equation\])


of $\Delta$ previously calculated on the coarse mesh of $M$ points.

(v) Repeat the process until self-consistency is attained. \[For the isolated vortex of subsection \[sec:solving-NLPDA-equation\]-A, typically $10$ cycles are sufficient.\]

(vi) Test the stability of the obtained self-consistent solution, by performing cycles of self-consistency with different values of $N$ and $\lambda$. \[For the isolated vortex of subsection \[sec:solving-NLPDA-equation\]-A, values $N \approx 10^{3} \div 10^{4}$ and $\lambda \approx Q_{c}^{\mathrm{L}}$ of Eq. (\[Q\_c-Landau-criterion\]) prove appropriate essentially for all couplings and temperatures.\]

![(Color online) Comparison between the Fourier transform of the functions (\[test-function-1\]) (a) and (\[test-function-2\]) (c), as obtained analytically (full lines) and by our numerical method (dashed lines). A similar comparison between the original functions (\[test-function-1\]) and (\[test-function-2\]) (full lines) and their Fourier transforms taken twice (dots) is shown in (b) and (d).[]{data-label="Figure-19"}](Figure-19.pdf){width="8.5cm"}

There remains toThe matrix elements of the $S$ matrix eventually result from their definition (\[S-matrix\]).

We conclude this Appendix by presenting a few tests about the accuracy of the method we have developed to calculate numerically the Fourier transform of a function via Eqs. (\[explicit-expression-Delta-R\]) and (\[explicit-expression-Delta-Q\]). To this end, we consider two non-trivial (one even and one odd) functions, of the form $$\begin{aligned}
f_{1}(x) & = & \exp{(-x^{2}/10)} \, \sin(x^{2})
\label{test-function-1} \\
f_{2}(x) & = & \frac{ i \, 64 x}{64 x^{2} + 1}
\label{test-function-2}\end{aligned}$$ whose Fourier transform can be obtained analytically by standard methods, yielding:

$$\begin{aligned}
\tilde{f}_{1}(Q) & = & \sqrt{\frac{5 \pi}{101}} \, e^{-10 Q^{2}/101} \, \left[ \sqrt{ \sqrt{101}-1} \, \cos\left(\frac{100 Q^{2}}{101}\right) \right.
\nonumber \\
& - & \left. \sqrt{ \sqrt{101}+1} \, \sin\left(\frac{100 Q^{2}}{101}\right) \right]
\label{FT-test-function-1} \\
\tilde{f}_{2}(Q) & = & \pi \, e^{-|Q|/4} \, {\text{sgn}}{(Q)} \, .
\label{FT-test-function-2}\end{aligned}$$

An additional test


American protection service for freeloading Europeans, it was intended to keep the Europeans unified and yoked to American leadership. Not only would they never again threaten the United States, their reliance on American power enlists them on its behalf.

Mr. Trump has boasted of increasing American military spending to $623 billion this year, from $603 billion in 2016. But American collective defense with NATO effectively adds $312 billion — the combined defense budgets of fellow members — in military power. That power applies to actual wars as well as the less visible but consequential projection of unused firepower, whether in deterring Russian or Chinese ambitions or keeping seafaring lanes clear.

But NATO, like other aspects of the American-led order, consists of more than its collective hardware. It is held togetherof operating system, including Windows 10, 8.1, 7, or Ubuntu, as well as the option of 4K and touch displays. The notebooks are expected to go on sale sometime in the fourth quarter this year, with the P70 also offering something some PC users will have forgotten about: an optional DVD-RW drive.


HARTZ, Circuit Judges.

       Daniel Starr, a state inmate appearing pro se, seeks review of the district court’s

dismissal of his discrimination claim brought pursuant to 42 U.S.C. § 1983. This court

exercises jurisdiction pursuant to 28 U.S.C. § 1291 and we AFFIRM.

       The underlying facts of this case are described in a prior opinion from this court,

and only a brief description of them will be provided here. See Starr v. Downs, 117 Fed.

Appx. 64, 66-67 (10th Cir. 2004). Mr. Starr, an African-American living in Tulsa,

Oklahoma, visited a friend’s basement in a building allegedly used for drug trafficking in

       *
        This order and judgment is notstated that Mr. Starr “had no notice that his equal-

protection claim was subject to summary judgment and therefore had no opportunity to

support his accusations of discriminatory enforcement.” Id. We also affirmed the district

court’s denial of Mr. Starr’s motion to join the police officer who conducted the search of

his vehicle, as he only sought to include her in the Fourth Amendment claim. In addition,

we stated that on remand “the district court should determine whether Plaintiff should be

allowed to pursue a motion to amend and add the city of Tulsa in connection with his

equal-protection claim.” Id. at 71.

       On remand, the district court granted Officer Downs’ motion for summary

judgment on the equal-protection claim and denied Mr. Starr’s motion for leave to amend

his complaint in


Q:

CREATE FULLTEXT INDEX/CATALOG statement cannot be used inside a user transaction

I have a db versioning app to update deployed databases. It runs smoothly with almost all SQL statements but when I decided to use FullText Search  and generated scripts to use statements like following it broke.
CREATE FULLTEXT CATALOG [ProductCatalog]

--Create fulltext index on Product
CREATE FULLTEXT INDEX ON [tblProduct] KEY INDEX [PK_Catalog]
    ON ([ProductCatalog]) WITH (CHANGE_TRACKING AUTO)
ALTER FULLTEXT INDEX ON [tblProduct] ADD ([ProductName] LANGUAGE [English])
ALTER FULLTEXT INDEX ON [tblProduct] ENABLE

I use the following code to execute SQL file within a C# SqlTransaction
SqlConnection cnn = new SqlConnection("cstring");
SqlTransaction trn = cnn.BeginTransaction();

cnn.Open();

using (SqlCommand cmd = cnn.CreateCommand())
{
    cmd.Connection = cnn;
    cmd.Transaction = trn;

    cmd.CommandText= SQLScript;
    cmd.CommandType = CommandType.Text;
    cmd.ExecuteNonQuery();
}

trn.Commit();
cnn.Close();

How can I run my scripts without a transaction?

A:

I've modified my code to execute scripts
SqlConnection cnn = new SqlConnection("cstring");
SqlTransaction trn = null;

cnn.Open();

using (SqlCommand cmd = cnn.CreateCommand())
{
    cmd.Connection = cnn;

    if(!SQLScript.Contains("FULLTEXT"))
    {
        trn = cnn.BeginTransaction();
        cmd.Transaction = trn;
    }

    cmd.CommandText = SQLScript;
    cmd.CommandType = CommandType.Text;
    cmd.ExecuteNonQuery();
}

if(trn!=null)
    trn.Commit();

cnn.Close();


he'd been trying for and hadn't had luck on for a couple years. Now we're trying to get the Raptor for him/me, the tiger for me, and the horse for him. ^_^ Since Zul is being phased out for Cata.

Garrosh has been evolving from the emo sack of crap he was and pathetic excuse for the Hellscream name.

And yea guild exp will lead to the mount which will be awesome, I have my ten man group already set up and ready to go from a bunch of people I know in Rl through meeting them at Blizzcon or just playing with them since game release on and off these last few years.

I used to play, but my highest leveled character was only a level 33 warlock. I hadreceptors with PDGF at 4 degrees C did not expedite subsequent enzyme activation at 37 degrees C. Removal of PDGF in the media after the 4 degrees C pretreatment did not affect the enzyme activation response, indicating that the continued presence of PDGF in the medium is not necessary after receptor binding is saturated. Results of sequential addition of PDGF, EGF, and insulin indicated a refractory period in the response system. This property is evident even when the second addition involved a different growth factor and is independent of the sequence of addition of the factors. There was little additivity in the actions of the three growth factors in effecting enzyme activation and suggests a common intermediate element in the three signalling pathways.


Collaborative Consumption: Love Home Swap Raises Further $1.28M From MMC Ventures, Angels To Scale By Acquisition

0

Collaborative consumption continues to be a hot trend in the eyes of investors as news comes today that Love Home Swap, the holiday home exchange marketplace, has raised a further £800k (approx. $1.28m) from MMC Ventures, along with a number of unnamed angels. The new capital will be used to scale the company, including through acquisition, and to continue to develop the service and launch a new bespoke insurance product, a much-needed feature post-Airbnb woes.

MMC is a previous backer of UK-based Love Home Swap, having previously invested £850k, bringing the total raised by Love Home Swap to £1.65m.

Founded by Debbie Wosskow, and launched in October 2011, Love Home Swap builds on the age-old:= suite.handler.GetCache(context.Background(), &job.GetCacheRequest{Id: id})
	suite.Error(err)
}

func (suite *JobHandlerTestSuite) TestJobGetCache_FailToLoadRuntime() {
	id := &peloton.JobID{
		Value: "my-job",
	}

	// Test fail to get job runtime cache
	suite.mockedJobFactory.EXPECT().
		GetJob(gomock.Any()).Return(suite.mockedCachedJob)
	suite.mockedCachedJob.EXPECT().
		GetRuntime(gomock.Any()).Return(nil, fmt.Errorf("get runtime err"))
	_, err := suite.handler.GetCache(context.Background(), &job.GetCacheRequest{Id: id})
	suite.Error(err)
}

func (suite *JobHandlerTestSuite) TestJobGetCache_FailToGetJobConfig() {
	id := &peloton.JobID{
		Value: "my-job",
	}
	jobRuntime := &job.RuntimeInfo{State: job.JobState_RUNNING}

	// Test fail to get job config cache
	suite.mockedJobFactory.EXPECT().
		GetJob(gomock.Any()).Return(suite.mockedCachedJob)
	suite.mockedCachedJob.EXPECT().
		GetRuntime(gomock.Any()).Return(jobRuntime, nil)
	suite.mockedCachedJob.EXPECT().
		GetConfig(gomock.Any()).Return(nil, fmt.Errorf("get runtime err"))
	_, err := suite.handler.GetCache(context.Background(), &job.GetCacheRequest{Id: id})
	suite.Error(err)
}

func (suite *JobHandlerTestSuite) TestJobGetCache_SUCCESS() {
	id := &peloton.JobID{
		Value: "my-job",
	}
	jobConfig := &job.JobConfig{
		InstanceCount: 4,
		Type:          job.JobType_BATCH,
	}
	jobRuntime := &job.RuntimeInfo{State: job.JobState_RUNNING}

	// Test succeed path
	suite.mockedJobFactory.EXPECT().
		GetJob(gomock.Any()).Return(suite.mockedCachedJob)
	suite.mockedCachedJob.EXPECT().
		GetRuntime(gomock.Any()).Return(jobRuntime, nil)
	suite.mockedCachedJob.EXPECT().
		GetConfig(gomock.Any()).Return(cachedtest.NewMockJobConfig(suite.ctrl, jobConfig), nil)
	resp, err := suite.handler.GetCache(context.Background(), &job.GetCacheRequest{Id: id})
	suite.NoError(err)
	suite.Equal(resp.Config.Type, jobConfig.Type)
	suite.Equal(resp.Config.InstanceCount, jobConfig.InstanceCount)
	suite.Equal(resp.Runtime.State, jobRuntime.State)
}

// TestJobGetActiveJobsFail tests failure to get active jobs list from DB
func (suite *JobHandlerTestSuite) TestJobGetActiveJobsFail() {
	suite.mockedActiveJobsOps.EXPECT().GetAll(context.Background()).
		Return(nil, fmt.Errorf("get active jobs err"))
	_, err := suite.handler.GetActiveJobs(context.Background(),
		&job.GetActiveJobsRequest{})
	suite.Error(err)
}

// TestJobGetActiveJobs tests failure to get active jobs list from DB
func (suite *JobHandlerTestSuite) TestJobGetActiveJobs() {
	expectedJobIDs := []*peloton.JobID{
		{Value: "my-job-1"},
	}
	suite.mockedActiveJobsOps.EXPECT().
		GetAll(context.Background()).
		Return(expectedJobIDs, nil)

	resp,


triangular with a sharp edge and was attached to the acetabulum by the base. Homogeneous low signal intensity was observed in labral segments. Fourteen of the 19 patients were examined by MRI. Six patients (6/14, 42.9%) showed various degrees of labrum tears. On STIR, the labrum was irregular in shape and the signal intensity was inhomogeneous with spotted or patchy anomalous high intensity scattered around ([Figure 4B](#F0004){ref-type="fig"}), or a linear high signal extending to the articular surface was demonstrated between the acetabular cartilage and the base of the labrum ([Figure 4C](#F0004){ref-type="fig"}). Among cases, only 5 patients presented with joint effusion (5 of 14 cases, 35.7%, [Figure 4D](#F0004){ref-type="fig"}), and in only 3 cases was there bone marrow edema of the femoral head on fs-FRFSE-T2 ([Figure 4E](#F0004){ref-type="fig"}).

![MRI manifestations of theacetabular labral tear patients had FAI \[[@CIT0005]\]. In agreement with the literature report, we found that 17 of the 19 patients (89.5%) had FAI under arthroscopy, which indicated that FAI had much to do with acetabular labral tears. Assessment of these arthrographs revealed that 68.4% (13 of 19 cases) of the acetabular labral tears were most often located in the anterosuperior part of the labrum, which suggested that the most common site of labrum tears was the anterosuperior labrum. The preferential involvement of the anterosuperior labrum may be due to FAI. Hip abnormalities in FAI limit motion, in particular flexion and internal rotation, as repetitive impact of the proximal femoral neck occurs against the acetabular labrum and/or its adjacent cartilage \[[@CIT0009], [@CIT0010]\].

The FAI occurs when the femoral head


comfy of all the TB bras except the convertible strap. More of the above mentioned colors please! P.

True Body Scoop Neck Adjustable Strap Bra,
Dulce

Renee

Size:
S

☆ ☆ ☆ ☆ ☆

They’re right it’s the best bra ever. It’s a great bra if you are post breastfeeding or on the tail end of nursing. Buttery soft. Not a push up bra but flattering and does not gap at the sides which was my problem. You completely forget about it after you put it on. With the pink you can see the inserts which is kind of weird - so I would to for another color the second time.

True Body Scoop Neck Adjustable Strap Bra,
Retro Pink

Guest

Age:
24

Size:
L

☆ ☆ ☆ ☆ ☆

I love this bra! I just had a baby in August and I havethis bra on! The FABRIC!!! There are no words as there is nothing else on the market like it. So silky and luxurious. This was my first purchase from True & Co. but I just ordered more items from your TrueBody line. LOVE the thin, adjustable straps. I wear a 38D and this bra offers natural feeling, light support and stayed in place. I often go braless rather than enduring the discomfort of wires and padding. Now I have another option for times when I must be a bit more discreet. THANK YOU for creating such a fabulous product!

True Body Scoop Neck Adjustable Strap Bra,
Dulce

Kendra

Age:
37

Size:
M

☆ ☆ ☆ ☆ ☆

This bra is as close to perfect as I can imagine: it is EXTREMELY comfortable, no underwire, it is smooth


Strap Bra,
Mink

Lois

Size:
L

☆ ☆ ☆ ☆ ☆

Simply the most amazing bra I have ever worn !!! As others have said " you forget you even have a bra on" "I don't want to wear any other bra". I am 38C with "dense" ( heavy) girls and this bra holds them up and separated. I highly recommend this bra! Favorite Bra Ever!// Code generated by protoc-gen-gogo. DO NOT EDIT.
// source: combos/marshaler/theproto3.proto

/*
Package theproto3 is a generated protocol buffer package.

It is generated from these files:
	combos/marshaler/theproto3.proto

It has these top-level messages:
	Message
	Nested
	AllMaps
	AllMapsOrdered
	MessageWithMap
	FloatingPoint
	Uint128Pair
	ContainsNestedMap
	NotPacked
*/
package theproto3

import testing "testing"
import math_rand "math/rand"
import time "time"
import github_com_gogo_protobuf_proto "github.com/gogo/protobuf/proto"
import github_com_gogo_protobuf_jsonpb "github.com/gogo/protobuf/jsonpb"
import fmt "fmt"
import go_parser "go/parser"
import proto "github.com/gogo/protobuf/proto"
import math "math"
import _ "github.com/gogo/protobuf/gogoproto"
import _ "github.com/gogo/protobuf/test/combos/both"

// Reference imports to suppress errors if they are not otherwise used.
var _ = proto.Marshal
var _ = fmt.Errorf
var _ = math.Inf

func TestMessageProto(t *testing.T) {
	seed := time.Now().UnixNano()
	popr := math_rand.New(math_rand.NewSource(seed))
	p := NewPopulatedMessage(popr, false)
	dAtA, err := github_com_gogo_protobuf_proto.Marshal(p)
	if err != nil {
		t.Fatalf("seed = %d, err = %v", seed, err)
	}
	msg := &Message{}
	if err := github_com_gogo_protobuf_proto.Unmarshal(dAtA, msg); err != nil {
		t.Fatalf("seed = %d, err = %v", seed, err)
	}
	littlefuzz := make([]byte, len(dAtA))
	copy(littlefuzz, dAtA)
	for i := range dAtA {
		dAtA[i] = byte(popr.Intn(256))
	}
	if err := p.VerboseEqual(msg); err != nil {
		t.Fatalf("seed


= %d, %#v !VerboseProto %#v, since %v", seed, msg, p, err)
	}
	if !p.Equal(msg) {
		t.Fatalf("seed = %d, %#v !Proto %#v", seed, msg, p)
	}
	if len(littlefuzz) > 0 {
		fuzzamount := 100
		for i := 0; i < fuzzamount; i++ {
			littlefuzz[popr.Intn(len(littlefuzz))] = byte(popr.Intn(256))
			littlefuzz = append(littlefuzz, byte(popr.Intn(256)))
		}
		// shouldn't panic
		_ = github_com_gogo_protobuf_proto.Unmarshal(littlefuzz, msg)
	}
}

func TestMessageMarshalTo(t *testing.T) {
	seed := time.Now().UnixNano()
	popr := math_rand.New(math_rand.NewSource(seed))
	p := NewPopulatedMessage(popr, false)
	size := p.Size()
	dAtA := make([]byte, size)
	for i := range dAtA {
		dAtA[i] = byte(popr.Intn(256))
	}
	_, err := p.MarshalTo(dAtA)
	if err != nil {
		t.Fatalf("seed = %d, err = %v", seed, err)
	}
	msg := &Message{}
	if err := github_com_gogo_protobuf_proto.Unmarshal(dAtA, msg); err != nil {
		t.Fatalf("seed = %d, err = %v", seed, err)
	}
	for i := range dAtA {
		dAtA[i] = byte(popr.Intn(256))
	}
	if err := p.VerboseEqual(msg); err != nil {
		t.Fatalf("seed = %d, %#v !VerboseProto %#v, since %v", seed, msg, p, err)
	}
	if !p.Equal(msg) {
		t.Fatalf("seed = %d, %#verr)
	}
	if err := p.VerboseEqual(msg); err != nil {
		t.Fatalf("seed = %d, %#v !VerboseProto %#v, since %v", seed, msg, p, err)
	}
	if !p.Equal(msg) {
		t.Fatalf("seed = %d, %#v !Json Equal %#v", seed, msg, p)
	}
}
func TestAllMapsOrderedJSON(t *testing.T) {
	seed := time.Now().UnixNano()
	popr := math_rand.New(math_rand.NewSource(seed))
	p := NewPopulatedAllMapsOrdered(popr, true)
	marshaler := github_com_gogo_protobuf_jsonpb.Marshaler{}
	jsondata, err := marshaler.MarshalToString(p)
	if err != nil {
		t.Fatalf("seed = %d, err = %v", seed, err)
	}
	msg := &AllMapsOrdered{}
	err = github_com_gogo_protobuf_jsonpb.UnmarshalString(jsondata, msg)
	if err != nil {
		t.Fatalf("seed = %d, err = %v", seed, err)
	}
	if err := p.VerboseEqual(msg); err != nil {
		t.Fatalf("seed = %d, %#v !VerboseProto %#v, since %v", seed, msg, p, err)
	}
	if !p.Equal(msg) {
		t.Fatalf("seed = %d, %#v !Json Equal %#v", seed, msg, p)
	}
}
func TestMessageWithMapJSON(t *testing.T) {
	seed := time.Now().UnixNano()
	popr := math_rand.New(math_rand.NewSource(seed))
	p := NewPopulatedMessageWithMap(popr, true)
	marshaler := github_com_gogo_protobuf_jsonpb.Marshaler{}
	jsondata, err := marshaler.MarshalToString(p)
	if err != nil {
		t.Fatalf("seed = %d, err = %v", seed, err)
	}
	msg :=


&MessageWithMap{}
	err = github_com_gogo_protobuf_jsonpb.UnmarshalString(jsondata, msg)
	if err != nil {
		t.Fatalf("seed = %d, err = %v", seed, err)
	}
	if err := p.VerboseEqual(msg); err != nil {
		t.Fatalf("seed = %d, %#v !VerboseProto %#v, since %v", seed, msg, p, err)
	}
	if !p.Equal(msg) {
		t.Fatalf("seed = %d, %#v !Json Equal %#v", seed, msg, p)
	}
}
func TestFloatingPointJSON(t *testing.T) {
	seed := time.Now().UnixNano()
	popr := math_rand.New(math_rand.NewSource(seed))
	p := NewPopulatedFloatingPoint(popr, true)
	marshaler := github_com_gogo_protobuf_jsonpb.Marshaler{}
	jsondata, err := marshaler.MarshalToString(p)
	if err != nil {
		t.Fatalf("seed = %d, err = %v", seed, err)
	}
	msg := &FloatingPoint{}
	err = github_com_gogo_protobuf_jsonpb.UnmarshalString(jsondata, msg)
	if err != nil {
		t.Fatalf("seed = %d, err = %v", seed, err)
	}
	if err := p.VerboseEqual(msg); err != nil {
		t.Fatalf("seed = %d, %#v !VerboseProto %#v, since %v", seed, msg, p, err)
	}
	if !p.Equal(msg) {
		t.Fatalf("seed = %d, %#v !Json Equal %#v", seed, msg, p)
	}
}
func TestUint128PairJSON(t *testing.T) {
	seed := time.Now().UnixNano()
	popr := math_rand.New(math_rand.NewSource(seed))
	p := NewPopulatedUint128Pair(popr, true)
	marshaler := github_com_gogo_protobuf_jsonpb.Marshaler{}
	jsondata, errseed, msg, p)
	}
}

func TestTheproto3Description(t *testing.T) {
	Theproto3Description()
}
func TestMessageVerboseEqual(t *testing.T) {
	popr := math_rand.New(math_rand.NewSource(time.Now().UnixNano()))
	p := NewPopulatedMessage(popr, false)
	dAtA, err := github_com_gogo_protobuf_proto.Marshal(p)
	if err != nil {
		panic(err)
	}
	msg := &Message{}
	if err := github_com_gogo_protobuf_proto.Unmarshal(dAtA, msg); err != nil {
		panic(err)
	}
	if err := p.VerboseEqual(msg); err != nil {
		t.Fatalf("%#v !VerboseEqual %#v, since %v", msg, p, err)
	}
}
func TestNestedVerboseEqual(t *testing.T) {
	popr := math_rand.New(math_rand.NewSource(time.Now().UnixNano()))
	p := NewPopulatedNested(popr, false)
	dAtA, err := github_com_gogo_protobuf_proto.Marshal(p)
	if err != nil {
		panic(err)
	}
	msg := &Nested{}
	if err := github_com_gogo_protobuf_proto.Unmarshal(dAtA, msg); err != nil {
		panic(err)
	}
	if err := p.VerboseEqual(msg); err != nil {
		t.Fatalf("%#v !VerboseEqual %#v, since %v", msg, p, err)
	}
}
func TestAllMapsVerboseEqual(t *testing.T) {
	popr := math_rand.New(math_rand.NewSource(time.Now().UnixNano()))
	p := NewPopulatedAllMaps(popr, false)
	dAtA, err := github_com_gogo_protobuf_proto.Marshal(p)
	if err != nil {
		panic(err)
	}
	msg := &AllMaps{}
	if err := github_com_gogo_protobuf_proto.Unmarshal(dAtA, msg); err != nil {
		panic(err)
	}
	if err := p.VerboseEqual(msg); err != nil {
		t.Fatalf("%#v !VerboseEqual %#v, since %v", msg, p, err)
	}
}
func TestAllMapsOrderedVerboseEqual(t *testing.T) {
	popr := math_rand.New(math_rand.NewSource(time.Now().UnixNano()))
	p


are impressive financial professionals who steer the fortunes of their companies and organizations. Join IBJ to celebrate them on Dec. 1.

Nominations

Do you know an individual or organization that goes above and beyond to improve health care in the Indianapolis area? Let them know their contributions matter. Nominate them for IBJ’s 2017 Health Care Heroes Awards program. For more information or to submit a nomination, visit www.ibj.com/nominations// The parsing starts here.
    unsigned char *data = bstr_ptr(h->value);
    size_t len = bstr_len(h->value);
    size_t pos = 9; // Start after "form-data"

    // Main parameter parsing loop (once per parameter).
    while (pos < len) {
        // Ignore whitespace.
        while ((pos < len) && isspace(data[pos])) pos++;
        if (pos == len) {
            part->parser->multipart.flags |= HTP_MULTIPART_CD_SYNTAX_INVALID;


    if (pos == len) {
            part->parser->multipart.flags |= HTP_MULTIPART_CD_SYNTAX_INVALID;
            return HTP_DECLINED;
        }

        // Equals.
        if (data[pos] != '=') {
            part->parser->multipart.flags |= HTP_MULTIPART_CD_SYNTAX_INVALID;
            return HTP_DECLINED;
        }
              return HTP_DECLINED;
                }

                // Allow " and \ to be escaped.
                if ((data[pos + 1] == '"')||(data[pos + 1] == '\\')) {
                    // Go over the quoted character.
                    pos++;


NULL) {
            unlink(part->file->tmpname);
            free(part->file->tmpname);
        }

        free(part->file);
        part->file = NULL;
    }

    if ((!gave_up_data) || (part->type != MULTIPART_PART_TEXT)) {
        bstr_free(part->name);
        bstr_free(part->value);
    }

    bstr_free(part->content_type);

    if (part->headers != NULL) {
        htp_header_t *h = NULL;
        for (size_t i = 0, n = htp_table_size(part->headers); i < n; i++)                   strncpy(buf, part->parser->extract_dir, 254);
                        strncat(buf, "/libhtp-multipart-file-XXXXXX", 254 - strlen(buf));

                        part->file->tmpname = strdup(buf);
                        if (part->file->tmpname == NULL) {


parser->multipart.flags |= HTP_MULTIPART_HAS_PREAMBLE;
            parser->current_part_mode = MODE_DATA;
        } else {
            // Part after preamble.
            parser->current_part_mode = MODE_LINE;
        }

        // Add part to the list.
        htp_list_push(parser->multipart.parts, parser->current_part);

        #ifdef HTP_DEBUG
        fprintf(stderr, "Created new part type %d\n", parser->current_part->type);
        #endif
     htp_mpartp_t *parser = calloc(1, sizeof (htp_mpartp_t));
    if (parser == NULL) return NULL;

    parser->cfg = cfg;

    parser->boundary_pieces = bstr_builder_create();
    if (parser->boundary_pieces == NULL) {
        htp_mpartp_destroy(parser);
        return NULL;
    }

    parser->part_data_pieces = bstr_builder_create();
    if (parser->part_data_pieces == NULL) {
        htp_mpartp_destroy(parser);
        return NULL;
    }

    parser->part_header_pieces = bstr_builder_create();
    if (parser->part_header_pieces == NULL) {
        htp_mpartp_destroy(parser);
        return NULL;
    }


// what we have in the buffer as data, except for the CR byte,
                            // which we're going to leave for later. If it happens that a
                            // CR is followed by a LF and then a boundary, the CR is going
                            // to be discarded.
              htp_martp_process_aside(parser, /* no match */ 0);

                        // Return back where data parsing left off.
                        if (parser->current_part_mode == MODE_LINE) {
                            // In line mode, we process the line.


                      // Process stored (buffered) data.
                        htp_martp_process_aside(parser, /* boundary match */ 1);

                        // Process data prior to the boundary in the current input buffer.
                        // Because we know this is the last chunk before boundary, we can
          parser->multipart.flags |= HTP_MULTIPART_CRLF_LINE;
                    parser->parser_state = STATE_DATA;
                } else {
                    // Not a line ending; start again, but do not process this byte.
                    parser->multipart.flags |= HTP_MULTIPART_BBOUNDARY_NLWS_AFTER;
                    parser->parser_state = STATE_BOUNDARY_EAT_LWS;


      if (!htp_is_space(data[pos])) {
            seen_non_space = 1;
        } else {
            seen_space = 1;
        }

        pos++;
    }

    // Raise INVALID if we see any non-space characters,
    // but raise UNUSUAL if we see _only_ space characters.
    if (seen_non_space) {
        *flags |= HTP_MULTIPART_HBOUNDARY_INVALID;
    } else if (seen_space) {
        *flags |= HTP_MULTIPART_HBOUNDARY_UNUSUAL;
  costs and increasing the speed of production. Traditionally, several manufacturing techniques have been utilized for economically and quickly forming tortillas on commercial production lines. A first popular method is known as die-cutting and a second popular method is known as pressing, both of which are described below.
In the die-cutting technique, tortilla dough is first formed in a commercial mixer. The dough is then transferred to an extruder that extrudes a sheet of dough onto a conveyor belt of a rolling and cutting machine to form a dough ribbon. In this step, the dough ribbon is gradually reduced to a predetermined thickness by sheeting and cross-rolling.
Once the dough has reached a desired thickness, a die is actuated to cut the dough into the desired form. The formed dough products


Q:

A wired array's length is always 0 in angular2

I read data.csv file's content through browse, then I save part of this file's content to an array. I can use console.log() to print this array, but I always get 0 of this array's length.
Here is my code:
app.component.html
<form id="file-input-form" #fileInputForm>

Sample Infomation

      <input type="file"
      (change)="onChange($event, 'sample_info', 'not_defined')"
      class="custom-file-input"
      accept=".csv"
      required>

</form>

app.component.ts
import { Component } from '@angular/core';

@Component({
  selector: 'my-app',
  templateUrl: './app.component.html',
  styleUrls: [ './app.component.css' ]
})
export class AppComponent  {
  public sampleInfoStatus = [];
  public sampleNameInSampleInfo = [];

          _sampleInfoStatus.push(8);
        }
        if (_sampleInfoStatus.length === 0) {
          sampleInfo.forEach(ele => {
            _sampleNames.push(ele[0]);
          });
        }
      }

      console.log(_sampleInfoStatus);
      console.log(typeof(_sampleInfoStatus));
      console.log(_sampleInfoStatus.length);
      console.log(_sampleNames);  // length is 12
      console.log(_sampleNames.length);  //<---- here is always zero
      console.log(_sampleNames.slice(0, 5));  //<---- always


July temperatures baked South Florida this year, the noon summer sun made city streets feel like the surface of Venus. If the trend continues, it could spell disaster for outdoor laborers, backyard pets, the sick, and the elderly. Studies have warned that anywhere from 200 to 1,400 more deaths due to heat exposure could occur each year in Miami by 2100 if trends don't reverse.

In July, McNoldy noted it is almost certain that human meddling is what's turning Miami into a rotisserie oven.

"Take a look at the chart with the full-year temperatures going back through our history," he said. "You really see that upward trend in the last 40, 50 years. Even the cool years dipped down; they’re higher than what the average used to be."

              dropTargetAsView);
        event.action.touch = Action.DRAGDROP;

        dragObj.dragSource.fillInLaunchSourceData(null, dragObj.originalDragInfo,
                event.srcTarget[0], event.srcTarget[1]);

        if (dropTargetAsView instanceof LaunchSourceProvider) {
            ((LaunchSourceProvider) dropTargetAsView).fillInLaunchSourceData(null,
                    dragObj.dragInfo, event.destTarget[0], event.destTarget[1]);

        }
        event.actionDurationMillis = SystemClock.uptimeMillis() - mActionDurationMillis;
        dispatchUserEvent(event, null);


[Rating T13][Action][Drama][Mystery][Complete][Noir]

Alan is back at it again with this sequel.The story follows Nick as he attempts to find Gideon Grey after he goes missing. The entire fic has a nice flow and pacing which will keep you on the edge of your seat throughout the whole story. Alan is able to craft a setting that gives off a very noir vibe, which I enjoyed greatly. Overall a very well done story and one that comes highly recommended, especially if you enjoy noir type fics. ~Namicle

Author: Alan Schezar

Description :

There are some things that even the relentless march of time can never erase, and some secrets that refuse to remain buried. On a rain drenched autumn evening, with Judy out of town for work, Nick receives a chilling phone callCalvin got a new bed today and he wouldn't even let me get the tags off before snuggling right in for a nap.

Byron,GA> Charleston, SC> Jacksonville, FL> Guilford, CT> Rohnert Park, CA! A southern drawl in sunny Cali! . The amount of time from slipping on the peel and landing on the pavement is exactly one bananosecond.I do have a secret yen for pink in unexpected places. ~ninja dogI've decided that I'll never get down to my original weight, and I'm OK with that--After all, 8 pounds 2 oz. is just not realistic.

I don't even like cats much, but I want a calico if we ever get one. I had a calico kitty growing up and I miss her so much, she was an awesome kitty. All these


have a secret yen for pink in unexpected places. ~ninja dogI've decided that I'll never get down to my original weight, and I'm OK with that--After all, 8 pounds 2 oz. is just not realistic.in the area when the shooting started.

"My sympathy goes out to the victims and their families," Trenton Mayor Eric Jackson said at a Sunday morning press conference. "All shootings are a crisis. This is not just a random act of violence – this is a public health issue."

"Woke up to news of another terrible shooting, and this time in our own backyard. Praying for those affected in Trenton today," said Sen. Bob Menendez, D-NJ.

Murphy, who just signed six gun-control bills into law this past week, said "there's still more work to do" in trying to prevent gun violence in local communities. He decried other states for being permissive in their gun laws and enabling people to easily transport firearms into New Jersey from elsewhere.

"We're getting stronger and better


against his detention without trial AFP/Getty In pictures: Palestinian flotilla Palestinian protester A Palestinian protester waves his national flag and shouts slogans during a demonstration in support of Palestinian prisoner Khader Adnan, a senior member of Islamic Jihad, under administrative detention in an Israeli jail AFP/Getty In pictures: Palestinian flotilla Palestinian flotilla Palestinians wave their national flag as they ride boats during a rally in support of activists aboard a Pro-Gaza flotilla made up of four boats aimed at defying Israel's blockade of Gaza, at the seaport of Gaza City In pictures: Palestinian flotilla Palestinian flotilla Palestinians wave their national flag as they ride boats during a rally in support of activists aboard a Pro-Gaza flotilla made up of four boats aimed at defying Israel's blockade of Gaza,is that such an instruction is required "only where substantially all the evidence is circumstantial." (People v. Schwab, 136 Cal.App.2d 280, 290 [288 P.2d 627].) [3b] Application of the rule to the facts at hand shows that it was not error to refuse to give the requested instruction because a substantial portion of the evidence, as to each count, was direct. As to the transactions involving Bonin (August 23, 24 and 31) the evidence consists of the testimony of Officer Rutherford that Bonin accompanied him on each of these occasions to a location indicated by Bonin; that the officer handed Bonin money for the purchase of narcotics, and that on each occasion Bonin later handed the officer a paper bindle containing heroin. The officer's testimony was obviously direct


from the Order Entered March 24, 2016
                In the Court of Common Pleas of Beaver County
                       Civil Division at No(s): 10815-2014

BEFORE: BENDER, P.J.E., BOWES, J., and SOLANO, J.

OPINION BY BENDER, P.J.E.:                             FILED March 1, 2017

        Appellants, Universal Medical Services, Inc. and Roderick K. Reeder,

CFO, appeal from the trial court’s March 24, 2016 order granting Appellee’s,

Jeffrey P.award to $14,604.90.

            [Appellee] requested attorney[s’] fees and costs, and this
     [c]ourt scheduled a hearing on that matter on March 3, 2016.
     At the hearing, [Appellee] presented evidence regarding his
     claim for attorney[s’] fees and costs, and counsel for both
     parties argued certain matters to the [c]ourt, including an issue
     of first impression. For the reasons specified below, this [c]ourt
     granted [Appellee’s] claim for attorney[s’] fees.

           As stated above, [Appellee] made claims for both breach
     of contract and [a]


violation of the [WPCL]. The essence of the
     claims is that [Appellee] permitted use of his credit card by an
     employee working for [Appellant] Universal. [Appellee] was the
     chief executive officer of [Appellant] Universal and left his
     employment with Universal in dispute. The evidence at trial
     revealed that Universal had an employee by the name of Bill
     Dunford. Universal had an account with a corporate customer by
     the name of Welsh Allen. Dunford worked on this account and
     was required to travel to service the account. Dunford could not
     meet the financialrequirements of the travel on his own, and
     [Appellee] arranged for Dunford to have access to his
     ([Appellee’s]) credit card for use on these business trips.

           [Appellee] submitted the expenses on the credit card for
     reimbursement by [Appellant] Universal, and the expenses were
     paid for a period of time. [Appellee] claimed that he was not
     fully reimbursed for the expenses and made claim for the
     outstanding balance due.

           [Appellant Universal] contended that many of the
     expenses were Dunford’s personal expenses