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OBJECTIVE To investigate the prevalence of hypertensive disorders of pregnancy (HDP), and the roles of polycystic ovary syndrome (PCOS), obesity, weight gain (WG) and hyperandrogenaemia in the development of HDP by age 46. DESIGN prospective population-based cohort. Setting and population The Northern Finland Birth Cohort 1966 (NFBC1966) METHODS Follow-up at ages 14, 31 and 46, including women with (n=408) and without (n=3373) HDP. HDP was combined from the questionnaire data at age 46, hospital discharge records and Finnish Medical Birth Registers. Women with both oligo-amenorrhea and hirsutism at age 31 and/or with PCOS diagnosis by age 46 (self-reported PCOS, srPCOS, n=279) were compared with women without symptoms or PCOS diagnosis (n=1577). Main outcome measures Association of PCOS and WG through life with HDP RESULTS Women with srPCOS had an increased HDP risk ([OR]=1.56 [95%CI:1.03-2.37]), but the association disappeared after BMI adjusting at age 31. Increase of BMI from age 14 to 31 was significantly greater in srPCOS (median [interquartile range]:5.94kg/m2[3.69;11.1], p<0.001) and non-PCOS (4.89kg/m2[3.21;7.57], p<0.001) women with HDP and in srPCOS women without HDP (4.59kg/m2[2.40;7.54], p=0.009) compared to non-PCOS without HDP. Among women with srPCOS, BMI increase was greater in women with than without HDP (5.94kg/m2 [3.69;11.1] vs 4.59kg/m2[2.40;7.54], p=0.015). Hyperandrogenaemia at 31 or 46 did not associate with HDP (OR=1.44[95%CI: 0.98-2.11]). CONCLUSION Obesity and weight gain from adolescence to age 46, but not srPCOS or hyperandrogenaemia, were associated with an increased risk of HDP.
A slip line theory governing states of incipient plane flow at the yield point load is developed for anisotropic rigid/plastic materials which exhibit a reduced yield criterion, governing states of plane flow, that depends only on the deviatoric parts of the in-plane stress tensor. It is shown that every homogeneous, incompressible material which complies with the principle of maximum plastic work, but which is of otherwise arbitrary anisotropy, is of this class. The stress equilibrium requirements are seen to take a remarkably simple form expressing the constancy of the quantities mean in-plane normal stress plus or minus arc length around the governing yield contour in a Mohr stress plane along members of the two slip line families. Further, this generalization of the Hencky equations is valid for every material of the considered class. Some special features of yield contours containing corners and flat segments are discussed, and velocity equations are given for materials complying with the maximum work inequality. The theory is applied to obtain the solution for indentation of an arbitrarily anisotropic half-space with a flat-ended, rigid, frictionless punch. A simple, universal formula, involving only geometrical dimensions of the governing yield contour, is derived for the yield point indentation pressure.
Polymorphism occurs in the family of engineered cocrystals that form from N,N '-bis(p-X-phenyl)melamines (X = H, F, Cl, Br, I, CH3, and CF3) and barbital. X-ray powder diffraction indicates that only one crystalline phase formed for X = Cl, F, and CH3, that primarily one phase occurred for X = H and I, but that a small contribution from an alternative phase or phases was possibly also present, and that at least two different polymorphs exist for both X = Br and CF3. Agreement of positions of peaks in experimental XPD traces and reflections calculated from single-crystal data is good, while agreement in intensities is good in some cases but only fair in others. Reasons for this disagreement are likely to include the physical design of the diffractometer and preferred orientation of crystallites in the sample. Two of the polymorphic forms of X = Br are converted to a third on annealing at 140 °C. Steric effects seem the most probable origin of the polymorphism: the bromine-substituted diphenylmelamine crystallizes in several polymorphs, and the bromine substituent is intermediate in size for the family of substituents examined. This cocrystal forms one polymorph that is formed by cocrystals having larger substituents (I and CH3) and one that packs similarly to a cocrystal having a smaller substituent (Cl).