The Australian Government, also known as the Commonwealth Government, is the national government of Australia, a federal parliamentary constitutional monarchy. Like other Westminster-style systems of government, the Australian Government is made up of three branches: the executive (the prime minister, the ministers, and government departments), the legislative (the Parliament of Australia), and the judicial.The legislative branch, the federal Parliament, is made up of two chambers: the House of Representatives (lower house) and Senate (upper house). The House of Representatives has 151 members, each representing an individual electoral district of about 165,000 people. The Senate has 76 members: twelve from each of the six states and two each from Australia's internal territories, the Australian Capital Territory and Northern Territory. The Australian monarch, currently Queen Elizabeth II, is represented by the governor-general. The Australian Government in its executive capacity is formed by the party or coalition with a majority in the House of Representatives, with the prime minister being the parliamentary leader who has the support of a majority of members in the House of Representatives. The prime minister is formally appointed to the role by the governor-general.The government is based in the nation's capital, Canberra, in the Australian Capital Territory. The head offices of all fourteen federal departments lie in Canberra, along with Parliament House and the High Court. The judicial branch of government, headed by the High Court of Australia, is independent of the legislative and executive branch, and ensures that government acts according to the constitution and law. As a founding member of the Commonwealth and a former British colony before Federation in 1901, Australia's Constitution is influenced heavily by the British Westminster system of government, as well as the United States Constitution.
The notion of defects in crystalline phases of matter has been extremely powerful for understanding crystal growth, deformation and melting. Many of these discontinuities in the periodic order of crystals are well described by the Burgers vector, derived from the particle displacements, which encapsulates the direction and magnitude of slip relative to the undeformed state. Since the reference structure of the crystal is known a priori, the Burgers vector can be determined experimentally using both imaging and diffraction methods to measure the final lattice distortion, and thus infer the particle displacements. Glasses have structures that lack the periodicity of crystals, and thus a well-defined reference state. Yet, measurable structural parameters can still be obtained from diffraction from a glass. Here we examine the usefulness of these parameters to probe deformation in glasses. We find that co-ordinated transformations in the centrosymmetry of local particle arrangements are a strong marker of plastic events. For a glass, determining the local distortions corresponding to these plastic events requires measurements before and after deformation. We investigate two geometric indicators that can be derived from these distortions, namely the continuous Burgers vector and the quadrupolar strain. We find that the Burgers vector again emerges as a robust and sensitive metric for understanding local structural transformations due to mechanical deformation, even in disordered glasses.
This article investigates factor-augmented sparse MIDAS (Mixed Data Sampling) regressions for high-dimensional time series data, which may be observed at different frequencies. Our novel approach integrates sparse and dense dimensionality reduction techniques. We derive the convergence rate of our estimator under misspecification due to the MIDAS approximation error, tau -mixing dependence, and polynomial tails. Our method's finite sample performance is assessed via Monte Carlo simulations. We apply the methodology to nowcasting U.S. GDP growth and demonstrate that it outperforms both sparse regression and standard factor-augmented regression during the COVID-19 pandemic. These findings indicate that the growth through this period was influenced by both idiosyncratic (sparse) and common (dense) shocks. The approach is implemented in the midasml R package, available on CRAN.
Directed Energy Deposition-Arc (DED-Arc) processes create residual stresses in the material due to their nonuniform thermal gradients. These residual stresses interact with the in-service loads and could negatively impact the material integrity. To understand and mitigate the negative effects of these stresses, in this study, a thin-walled structure out of a high strength low alloy (HSLA) steel was manufactured by DED-Arc process. The formation of residual stresses was studied with neutron diffraction at the centerline of the structure. To incorporate the effects of martensitic phase transformation on the residual stress formation, the microstructure of the material was studied using electron and optical microscopy. Also, the phase fractions were calculated using image segmentation methods. Furthermore, thermodynamics calculations were performed to understand the kinetics of the phase changes. The results show that the structure follows a tensile-compressive-tensile-compressive residual stress regime in the travel direction by moving from the lower side of the substrate to the top side of the thin-walled structure. The main influencing factors in the formation of these stresses are the volume expansion due to martensitic and bainitic phase transformations, contraction due to cooling of the hot material, and bending of the structure due to the interaction between tensile and compressive stresses at different heights of the part.
Alternative protein foods with desirable textural properties are of wide interest. Here we investigated the potential to improve pea protein isolate (PPI) gel strength by the addition of pea protein fibrils (PPF). Firstly, optimal conditions for PPF production were investigated, in particular whether the presence of salt (0.15 M NaCl) improved fibril quality when generated under acidic conditions. Pea protein fibrils were prepared in either water (PPFW) or 0.15 M NaCl (PPFS) at pH 2. Fibrils were formed when PPI proteins were hydrolyzed, unfolded, and aggregated into a fibrillar structure as determined by TEM, particle size analysis, CD, and SAXS. AFM-IR confirmed their long, thin morphology and revealed differences in the secondary structures composition of PPFS and PPFW, with high beta-sheet content and increased aggregation observed when adjusted to pH 7. Rheological examination of gels formed from either PPI or PPF individually showed very weak gel strengths at 60 degrees C. Fibrils mixed with PPI at either pH 2 (native fibril-forming condition) or pH 7 (typical for food applications) at a 1:1 ratio formed strong elastic gels. The highest value of the elastic modulus (G' similar to 30 kPa) resulted from PPFS forming a scaffold network for PPI entrapment at pH 2. The viscoelastic material response of all the gels is well described by the Scott Blair model for a critical gel. Analysis of the resulting model parameters indicated a strong and rigid network formed between PPI and PPFS at pH 2, consistent with an open, highly connected network of rigidly bonded flocs. SEM images showed dense interconnected networks with protein aggregates of PPI within a continuous fibrillar matrix. Overall, the incorporation of PPF formed in the presence of salt into PPI gels could significantly enhance the textural properties of pea protein.
Explicit results are obtained using simple and exact methods for the joint queue-length distribution of the M/M/c queue with an arbitrary number of non-preemptive priority levels. This work is the first to provide explicit results for the joint probability generating function and joint probability mass function for a general number of priority levels. A fixed-point iteration is developed for the stationary balance equations, which enables direct computation of the joint queue-length distribution. A multi-variate probability generating function is also derived, from which the joint probability mass function can be computed by means of a multi-dimensional fast Fourier transform method.