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Knowledge about the effect of regular intake of specific food groups on cardiometabolic health is primarily derived from large prospective cohort studies. With careful study design and analysis, results from observational data offer opportunities for causal inference. Sugar-sweetened beverage intake is consistently associated with increased risk of obesity, cardiovascular disease (CVD), and type 2 diabetes owing to the excess amounts of added sugar, as well as mediation by increased weight gain. Coffee consumption is associated with lower incidence of CVD, with the largest benefit observed around 3–5 cups/day. Higher consumption of fruits and vegetables is associated with lower risk of heart disease, although data on type 2 diabetes is conflicted. Dairy consumption has mixed associations with cardiometabolic diseases, depending on the types of dairy products. Red meat, especially processed red meat, is associated with increased risk of diabetes and CVD. Fish intake is inversely associated with CVD incidence, although high-dose fish oil supplementation does not appear to be beneficial. Regular consumption of whole grains and nuts is associated with lower risk of both diabetes and CVD. Future research should focus on studying food subtypes, as well as adopting a holistic view of nutrition.
Background Asthma and obesity are common diseases with considerable impact on public health. Prospective studies showed that obesity is a risk factor for developing asthma and a causal relation has been proposed. However, there is limited evidence for the existence of shared genetic effects and it is not yet clear how obesity and genetic factors jointly influence the risk of developing asthma. Objective We sought to determine whether obesity (body mass index of 30 or greater) modifies the risk of developing asthma and to assess whether there is evidence for a causal relation linking the genetic risk of developing obesity with asthma. Methods The analyses were performed in genotyped individuals of two northern Finland birth cohorts. The discovery set (NFBC1966) and the in silico replication set (NFBC1986) comprised a sample of 4182 and 1441 individuals. The presence of asthma was determined by self-report of a physician diagnosis of asthma, and body mass index (BMI) was measured at time of clinical examination (at 31 and 16 years old respectively). Sixty SNPs previously associated with asthma or obesity from the GWAS catalogue were analysed. The gene environment interactions were formally tested with a full interaction model using logistic regression. The significant interactions (Pl0.05) found in the discovery dataset were meta-analysed with results of the replication set using fixed and random effects model. Results We prioritized six significant (Pl0.05) SNP interactions in the discovery set for replication (Fig. 1). Only one of the prioritized loci was previously associated with obesity (BMI). After meta-analysis with the replication set, we identified one directionally consistent interaction with obesity (P l 6.5x10-3) in rs2786098 near DENND1B, a SNP previously associated with asthma (Fig. 2). After meta-analysis, we did not find significant or directionally consistent interactions in SNPs previously associated with BMI or Obesity. Conclusion Our limited dataset suggests that obesity modifies the genetic risk of developing asthma. We did not found evidence for the hypothesis that obesity causes asthma.
ADVERTISEMENT RETURN TO ISSUEPREVArticleNEXTA combined chemical-enzymic synthesis of 3-deoxy-D-arabino-heptulosonic acid 7-phosphateNicholas J. Turner and George M. WhitesidesCite this: J. Am. Chem. Soc. 1989, 111, 2, 624–627Publication Date (Print):January 1, 1989Publication History Published online1 May 2002Published inissue 1 January 1989https://pubs.acs.org/doi/10.1021/ja00184a033https://doi.org/10.1021/ja00184a033research-articleACS PublicationsRequest reuse permissionsArticle Views255Altmetric-Citations37LEARN ABOUT THESE METRICSArticle Views are the COUNTER-compliant sum of full text article downloads since November 2008 (both PDF and HTML) across all institutions and individuals. These metrics are regularly updated to reflect usage leading up to the last few days.Citations are the number of other articles citing this article, calculated by Crossref and updated daily. Find more information about Crossref citation counts.The Altmetric Attention Score is a quantitative measure of the attention that a research article has received online. Clicking on the donut icon will load a page at altmetric.com with additional details about the score and the social media presence for the given article. Find more information on the Altmetric Attention Score and how the score is calculated. Share Add toView InAdd Full Text with ReferenceAdd Description ExportRISCitationCitation and abstractCitation and referencesMore Options Share onFacebookTwitterWechatLinked InRedditEmail Other access optionsGet e-Alertsclose Get e-Alerts
Numerical simulations of earthquake failure sequences along a discrete cellular fault zone are performed for a three‐dimensional (3‐D) model representing approximately the central San Andreas fault. The model consists of an upper crust overlying a lower crust and mantle region, together defining an elastic half‐space with a vertical half‐plane fault. The fault contains a region where slip is calculated on a uniform grid of cells governed by a static/kinetic friction law and regions where slip is prescribed so as to represent tectonic loading, aseismic fault creep, and adjacent great earthquakes. The computational region models a 70‐km‐long and 17.5‐km‐deep section of the San Andreas fault to the NW of the great 1857 rupture zone. Different distributions of stress drops on failing computational cells are used to model asperity (“Parkfield asperity”) and nonasperity fault regions. The model is “inherently discrete” and corresponds to a situation in which a characteristic size of geometric disorder within the fault (i.e., cell size, here a few hundreds of meters) is much larger than the “nucleation size” (of the order of tens of centimeters to tens of meters) based on slip weakening or state evolution slip distances. The computational grid is loaded by a constant plate motion imposed at the lower crust, upper mantle, and creeping fault regions and by a “staircase” slip history imposed at the 1857 and 1906 rupture zones. Stress transfer along and outside the fault due to the imposed loadings and failure episodes along the computational grid is calculated using 3‐D elastic dislocation theory. The resulting displacement field in the computational region is compatible with geodetic and seismological observations only when the asperity and nonasperity regions are characterized by significantly different average stress drops. The frequency‐magnitude statistics of the simulated failure episodes are approximately self‐similar for small events, with b ≈ 1.2 (the b value of statistics based on rupture area b A is about 1) but are strongly enhanced with respect to self‐similarity for events larger than a critical size. This is interpreted as a direct manifestation of our 3‐D elastic stress transfer calculations; beyond certain rupture area and potency (seismic moment divided by rigidity) release values, the event is usually unstoppable, and it continues to grow to a size limited by a characteristic model dimension. This effect is not accounted for by cellular automata and block‐spring models in which the adopted simplified stress transfer laws fail to scale properly with increasing rupture size. The simulations suggest that local maxima in observed frequency‐magnitude statistics correspond to dimensions of coherent brittle zones, such as the width of the seismogenic layer or the length of a fault segment bounded by barriers. The analysis indicates that a single cell size, representing approximately a single scale of geometric disorder, cannot induce self‐similarity in a 3‐D elastic model over a broad range of magnitudes. A representation of geometric disorder covering a range of scales may thus be required to generate a wide domain of self‐similar Gutenberg‐Richter statistics. Our simulations show a great diversity in the mode of failure of the Parkfield asperity; the earthquakes themselves define an irregular sequence of events. The modeling, like many other discrete fault models, suggests that expectations for periodic Parkfield earthquakes and/or simple precursory patterns repeating from one event to the other are unrealistic.
In this paper we solve the elasticity problem of two elastic half spaces that are joined together over a region that does not differ much from a circle, i.e., the problem of an external planar crack leaving a nearly circular uncracked connection. The method we use is based on the perturbation technique developed by Rice (1985) for solving the elastic field of a crack whose front deviates slightly from some reference geometry. Quantities such as crack opening displacement and stress intensity factor are derived in detail to the first order of accuracy in the deviation of the shape of the connection from a circle. In addition, some results such as the crack face weight functions and Green's functions for a perfectly circular connection are also discussed under various boundary conditions at infinity. The formulae derived are used to study the configurational stability problem for quasistatic growth of an external circular crack. The results, derived when the crack front is perturbed from circular in a harmonic waveform and is subjected to axisymmetric loading, suggest that a perturbation of wavenumber higher than one is configurationally stable under all boundary conditions at infinity. The perturbation with wavenumber equal to one, which corresponds to a translational shift of the geometric center of the circular connection, turns out to be configurationally stable if any rotation in the remote field is suppressed and configurationally unstable if there is no such restraint.
ADVERTISEMENT RETURN TO ISSUEPREVArticleNEXT.alpha.-Amino aldehyde equivalents as substrates for rabbit muscle aldolase: synthesis of 1,4-dideoxy-D-arabinitol and 2(R),5(R)-bis(hydroxymethyl)-3(R),4(R)-dihydroxypyrrolidineRebecca R. Hung, Julie Ann Straub, and George M. WhitesidesCite this: J. Org. Chem. 1991, 56, 12, 3849–3855Publication Date (Print):June 1, 1991Publication History Published online1 May 2002Published inissue 1 June 1991https://pubs.acs.org/doi/10.1021/jo00012a015https://doi.org/10.1021/jo00012a015research-articleACS PublicationsRequest reuse permissionsArticle Views1150Altmetric-Citations93LEARN ABOUT THESE METRICSArticle Views are the COUNTER-compliant sum of full text article downloads since November 2008 (both PDF and HTML) across all institutions and individuals. These metrics are regularly updated to reflect usage leading up to the last few days.Citations are the number of other articles citing this article, calculated by Crossref and updated daily. Find more information about Crossref citation counts.The Altmetric Attention Score is a quantitative measure of the attention that a research article has received online. Clicking on the donut icon will load a page at altmetric.com with additional details about the score and the social media presence for the given article. Find more information on the Altmetric Attention Score and how the score is calculated. Share Add toView InAdd Full Text with ReferenceAdd Description ExportRISCitationCitation and abstractCitation and referencesMore Options Share onFacebookTwitterWechatLinked InRedditEmail Other access optionsGet e-Alertsclose Get e-Alerts
A simple constitutive framework is proposed to take account of progressive changes in a stress-based criterion of yielding as plastic deformation accumulates. The analysis is relevant to a sheet of isotropic or orthotropic material which is subsequently loaded in its plane by biaxial tensions (σ1, σ2) in arbitrary fixed ratio. Under these circumstances there is evidence that texture development causes significant changes in the shapes of successive yield loci in (σ1, σ2) space. Here such departures from geometric similarity are explicitly linked to a presumed dependence on σ1/σ2 of the exponent m in a standard power-law representation of the stress-strain characteristic under each constant value of σ1/σ2. The linkage is formulated in detail for several types of representation, and it is shown how a family of yield loci associated with any conjectural dependence m(σ1/σ2) can be generated readily by computer graphics. Some typical examples are given, in particular when m (σ1/σ2) reflects the distinctive trends reported for certain kinds of brass and aluminum sheet (e.g., Wagoner, 1980; Stout and Hecker 1983).